Galois Theory
Tom Leinster, University of Edinburgh
Version of 31 March 2023
Note to the reader
2
1 Overview of Galois theory
4
1.1 The view of C from Q . . . . . . . . . . . . . . . . . . . . . . . . 4
1.2 Every polynomial has a symmetry group. . . . . . . . . . . . . . .
9
1.3 . . . which determines whether it can be solved . . . . . . . . . . . 11
2 Group actions, rings and fields
14
2.1 Group actions . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14
2.2 Rings . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20
2.3 Fields . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26
3 Polynomials
34
3.1 The ring of polynomials . . . . . . . . . . . . . . . . . . . . . . . 34
3.2 Factorizing polynomials . . . . . . . . . . . . . . . . . . . . . . . 39
3.3 Irreducible polynomials . . . . . . . . . . . . . . . . . . . . . . . 43
4 Field extensions
49
4.1 Definition and examples . . . . . . . . . . . . . . . . . . . . . . . 49
4.2 Algebraic and transcendental elements . . . . . . . . . . . . . . . 54
4.3 Simple extensions . . . . . . . . . . . . . . . . . . . . . . . . . . 58
5 Degree
66
5.1 The degree of an extension . . . . . . . . . . . . . . . . . . . . . 66
5.2 Algebraic extensions . . . . . . . . . . . . . . . . . . . . . . . . 73
5.3 Ruler and compass constructions . . . . . . . . . . . . . . . . . . 76
6 Splitting fields
83
6.1 Extending homomorphisms . . . . . . . . . . . . . . . . . . . . . 84
6.2 Existence and uniqueness of splitting fields . . . . . . . . . . . . 86
6.3 The Galois group . . . . . . . . . . . . . . . . . . . . . . . . . . 92
7 Preparation for the fundamental theorem
97
7.1 Normality . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 98
7.2 Separability . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 105
7.3 Fixed fields . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 111
8 The fundamental theorem of Galois theory
114
8.1 Introducing the Galois correspondence . . . . . . . . . . . . . . . 114
8.2 The theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 118
8.3 A specific example . . . . . . . . . . . . . . . . . . . . . . . . . 123
9 Solvability by radicals
129
9.1 Radicals . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 130
9.2 Solvable polynomials have solvable groups . . . . . . . . . . . . . 133
9.3 An unsolvable polynomial . . . . . . . . . . . . . . . . . . . . . 139
10 Finite fields
144
10.1 Classification of finite fields . . . . . . . . . . . . . . . . . . . . . 145
10.2 Multiplicative structure . . . . . . . . . . . . . . . . . . . . . . . 147
10.3 Galois groups for finite fields . . . . . . . . . . . . . . . . . . . . 148
1
Note to the reader
These are the course notes for Galois Theory, University of Edinburgh, 2022-23.
Structure Each chapter corresponds to one week of the semester. You are
expected to read Chapter π before the lectures in Week π, except for Chapter 1. I
may make small changes to these notes as we go along (e.g. to correct errors), so I
recommend that you download a fresh copy before you start each week’s reading.
Exercises looking like this are sprinkled through the notes. The idea
is that you try them immediately, before you continue reading.
Most of them are meant to be quick and easy, much easier than assignment or workshop questions. If you can do them, you can take it
as a sign that you’re following successfully. For those that defeat you,
talk with others in the class, ask on Piazza, or ask me.
I promise you that if you make a habit of trying every exercise, you’ll
enjoy the course more and understand it better than if you don’t.
Here you’ll see
titles of relevant
videos, made two
years ago when the
class was online.
They are entirely
optional but may
help your
understanding.
Digressions like this are optional and not examinable, but might interest
you. They’re usually on points that I find interesting, and often describe
connections between Galois theory and other parts of mathematics.
References to theorem numbers, page numbers, etc., are clickable links.
What to prioritize You know by now that the most important things in almost
any course are the definitions and the results called Theorem. But I also want to
emphasize the proofs. This course presents a wonderful body of theory, and the
idea is that you learn it all, including the proofs that are its beating heart.
Less idealistically, the exam will test not only that you know the proofs, but
also something harder: that you understand them. So the proofs will need your
attention and energy.
2
Compulsory prerequisites To take this course, you must have already taken
these two courses:
• Honours Algebra: We’ll need some abstract linear algebra, corresponding to
Chapter 1 of that course. We’ll also need everything from Honours Algebra
about rings and polynomials (Chapter 3 there), including ideals, quotient
rings (factor rings), the universal property of quotient rings, and the first
isomorphism theorem for rings.
• Group Theory: From that course, we’ll need fundamentals such as normal
subgroups, quotient groups, the universal property of quotient groups, and
the first isomorphism theorem for groups. You should know lots about the
symmetric groups ππ , alternating groups π΄π , and cyclic groups πΆπ , as well
as a little about the dihedral groups π· π , and I hope you can list all of the
groups of order < 8 without having to think too hard.
Chapter 8 of Group Theory, on solvable groups, will be crucial for us. For
example, you’ll need to understand what it means that π4 is solvable but π΄5
is not.
We won’t need anything on free groups, the Sylow theorems, or the Jordan–
Hölder theorem.
If you’re a visiting or MSc student and didn’t take those courses, please contact
me so that we can decide whether your background is suitable.
Mistakes I’ll be grateful to hear of mistakes in these notes (Tom.Leinster@
ed.ac.uk), even if it’s something very small and even if you’re not sure.
3
Chapter 1
Overview of Galois theory
Introduction to
Week 1
This chapter stands apart from all the others,
Modern treatments of Galois theory take advantage of several well-developed
branches of algebra: the theories of groups, rings, fields, and vector spaces. This
is as it should be! However, assembling all the algebraic apparatus will take us
several weeks, during which it’s easy to lose sight of what it’s all for.
Galois theory came from two basic insights:
• every polynomial has a symmetry group;
• this group determines whether the polynomial can be solved by radicals (in
a sense I’ll define).
In this chapter, I’ll explain these two ideas in as short and low-tech a way as I can
manage. In Chapter 2 we’ll start again, beginning the modern approach that will
take up the rest of the course. But I hope that all through that long build-up, you’ll
keep in mind the fundamental ideas you learn in this chapter.
1.1
The view of C from Q
Imagine you lived several centuries ago, before the discovery of complex numbers.
Your whole mathematical world is the real numbers, and there is no square root of
−1. This situation frustrates you, and you decide to do something about it.
So, you invent a new symbol π (for ‘imaginary’) and decree that π 2 = −1. You
still want to be able to do all the usual arithmetic operations (+, ×, etc.), and you
want to keep all the rules that govern them (associativity, commutativity, etc.). So
you’re also forced to introduce new numbers such as 2 + 3 × π, and you end up with
what today we call the complex numbers.
So far, so good. But then you notice something strange. When you invented
the complex numbers, you only intended to introduce one square root of −1. But
4
accidentally, you introduced a second one at the same time: −π. (You wait centuries
for a square root of −1, then two come along at once.) Maybe that’s not so strange
in itself; after all, positive reals have two square roots too. But then you realize
something genuinely weird:
There’s nothing you can do to distinguish π from −π.
Try as you might, you can’t find any reasonable statement that’s true for π but not
−π. For example, you notice that π is a solution of
π§ 3 − 3π§2 − 16π§ − 3 =
17
,
π§
but then you realize that −π is too.
Of course, there are unreasonable statements that are true for π but not −π, such
as ‘π§ = π’. We should restrict to statements that only refer to the known world of
real numbers. More precisely, let’s consider statements of the form
π 1 (π§) π 3 (π§)
=
,
π 2 (π§) π 4 (π§)
where π 1 , π 2 , π 3 , π 4 are polynomials with real coefficients. Any such equation
can be rearranged to give
π(π§) = 0,
where again π is a polynomial with real coefficients, so we might as well just
consider statements of that form. The point is that if π(π) = 0 then π(−π) = 0.
Let’s make this formal. We could say that two complex numbers are ‘indistinguishable when seen from R’ if they satisfy the same polynomials over R. But the
official term is ‘conjugate’:
Definition 1.1.1 Two complex numbers π§ and π§′ are conjugate over R if for all
polynomials π with coefficients in R,
π(π§) = 0 ⇐⇒ π(π§′) = 0.
For example, π and −π are conjugate over R. This follows from a more general
result, stating that conjugacy in this new sense is closely related to complex
conjugacy:
Lemma 1.1.2 Let π§, π§′ ∈ C. Then π§ and π§′ are conjugate over R if and only if
π§′ = π§ or π§′ = π§.
5
Proof ‘Only if’: suppose that π§ and π§′ are conjugate over R. Write π§ = π₯ + ππ¦ with
π₯, π¦ ∈ R. Then (π§ − π₯) 2 + π¦ 2 = 0. Since π₯ and π¦ are real, conjugacy implies that
(π§′ − π₯) 2 + π¦ 2 = 0, so π§′ − π₯ = ±ππ¦, so π§′ = π₯ ± ππ¦.
‘If’: obviously π§ is conjugate to itself, so it’s enough to prove that π§ is conjugate
to π§. I’ll give two proofs. Each one teaches us a lesson that will be valuable later.
First proof: recall that complex conjugation satisfies
π€1 + π€2 = π€1 + π€2,
π€1 · π€2 = π€1 · π€2
for all π€ 1 , π€ 2 ∈ C. Also, π = π for all π ∈ R. It follows by induction that for any
polynomial π over R,
π(π€) = π(π€)
for all π€ ∈ C. So
π(π§) = 0 ⇐⇒ π(π§) = 0 ⇐⇒ π(π§) = 0.
Second proof: write π§ = π₯ + ππ¦ with π₯, π¦ ∈ R. Let π be a polynomial over
R such that π(π§) = 0. We will prove that π(π§) = 0. This is trivial if π¦ = 0, so
suppose that π¦ ≠ 0.
Consider the real polynomial π(π‘) = (π‘ − π₯) 2 + π¦ 2 . Then π(π§) = 0. You know
from Honours Algebra that
π(π‘) = π(π‘)π(π‘) + π (π‘)
(1.1)
for some real polynomials π and π with deg(π) < deg(π) = 2 (so π is either a
constant or of degree 1). Putting π‘ = π§ in (1.1) gives π (π§) = 0. It’s easy to see
that this is impossible unless π is the zero polynomial (using the assumption that
π¦ ≠ 0). So π(π‘) = π(π‘)π(π‘). But π(π§) = 0, so π(π§) = 0, as required.
We have just shown that for all polynomials π over R, if π(π§) = 0 then π(π§) = 0.
Exchanging the roles of π§ and π§ proves the converse. Hence π§ and π§ are conjugate
over R.
β‘
Exercise 1.1.3 Both proofs of ‘if’ contain little gaps: ‘It follows by
induction’ in the first proof, and ‘it’s easy to see’ in the second. Fill
them.
Digression 1.1.4 With complex analysis in mind, we could imagine a stricter
definition of conjugacy in which polynomials are replaced by arbitrary convergent power series (still with coefficients in R). This would allow functions
such as exp, cos and sin, and equations such as exp(ππ) = −1.
But this apparently different definition of conjugacy is, in fact, equivalent. A
complex number is still conjugate to exactly itself and its complex conjugate.
(For example, exp(−ππ) = −1 too.) Do you see why?
6
Example 1.1.5
Lemma 1.1.2 tells us that conjugacy over R is rather simple. But the same idea
becomes much more interesting if we replace R by Q. And in this course, we will
mainly focus on polynomials over Q.
Define conjugacy over Q by replacing R by Q in Definition 1.1.1. Again, when
you see the words ‘conjugate over Q’, you can think to yourself ‘indistinguishable
when seen from Q’. From now on, I will usually just say ‘conjugate’, dropping the
‘over Q’.
√
√
Example 1.1.5 I claim that 2 and − 2 are conjugate. And I’ll give you two
different proofs, closely analogous to the two proofs of the ‘if’ part of Lemma 1.1.2.
First proof: write
√
√
Q( 2) = {π + π 2 : π, π ∈ Q}.
√
√
√
For π€ ∈ Q( 2), there are unique π, π ∈ Q such that π€ = π + π 2, because 2 is
irrational. So it is logically valid to define
√
√
π€
e = π − π 2 ∈ Q( 2).
(Question: what did the uniqueness
of π and π have to do with the logical validity
√
of that definition?) Now, Q( 2) is closed under addition and multiplication, and
it is straightforward to check that
π€Β
f1 + π€
f2 ,
π€
Β
f1 · π€
f2
1 + π€2 = π€
1 · π€2 = π€
√
π = π for all π ∈ Q. So just as in the √
proof of
for all π€ 1 , π€ 2 ∈ Q( 2). Also, e
Lemma 1.1.2,
e are conjugate for √every π€ ∈ Q( 2). In
√ it follows that π€ and π€
particular, 2 is conjugate to (‘indistinguishable from’) − 2.
√Second proof: let π = π(π‘) be a polynomial with coefficients in Q such that
π( 2) = 0. You know from Honours Algebra that
π(π‘) = (π‘ 2 − 2)π(π‘) + π (π‘)
√
for√some polynomials
π(π‘) and π (π‘) over Q with deg π < 2. Putting π‘ = 2 gives
√
π ( 2) = 0. But 2 is irrational and π (π‘) is of the form ππ‘ + π with π,√π ∈ Q, so π
must be the zero polynomial. Hence π(π‘) = (π‘ 2 − 2)π(π‘), giving π(−
√ 2) = 0.
We
√ have just shown that for all polynomials π √over Q, if
√ π( 2) = 0 then
π(− 2) = 0. The same
argument
with
the
roles
of
2
and
−
2 reversed proves
√
the converse. Hence ± 2 are conjugate.
Exercise 1.1.6 Let π§ ∈ Q. Show that π§ is not conjugate to π§′ for any
complex number π§′ ≠ π§.
One thing that makes conjugacy more subtle over Q than over R is that over Q,
more than two numbers can be conjugate:
7
π
π2
1
π3
π4
Figure 1.1: The 5th roots of unity.
Example 1.1.7 The 5th roots of unity are
1, π, π2 , π3 , π4 ,
where π = π 2ππ/5 (Figure 1.1). Now 1 is not conjugate to any of the rest, since it
is a root of the polynomial π‘ − 1 and the others are not. (See also Exercise 1.1.6.)
But it turns out that π, π2 , π3 , π4 are all conjugate to each other.
Complex conjugate numbers are conjugate over R, so they’re certainly conjugate over Q. (If you’ve got a pair of complex numbers that you can’t tell apart
using only the reals, you certainly can’t tell them apart using only the rationals.)
Since π4 = 1/π = π, it follows that π and π4 are conjugate over Q. By the same
argument, π2 and π3 are conjugate. What’s not so obvious is that π and π2 are
conjugate. I know two proofs, which are like the two proofs of Lemma 1.1.2 and
Example 1.1.5. But we’re not equipped to do either yet.
Example 1.1.8 More generally, let π be any prime and put π = π 2ππ/π . Then
π, π2 , . . . , π π−1 are all conjugate to one another.
So far, we have asked when one complex number can be distinguished from
another, using only polynomials over Q. But what about more than one?
Definition 1.1.9 Let π ≥ 0 and let (π§1 , . . . , π§ π ) and (π§′1 , . . . , π§′π ) be π-tuples of
complex numbers. Then (π§1 , . . . , π§ π ) and (π§′1 , . . . , π§′π ) are conjugate over Q if for
all polynomials π(π‘1 , . . . , π‘ π ) over Q in π variables,
π(π§ 1 , . . . , π§ π ) = 0 ⇐⇒ π(π§′1 , . . . , π§′π ) = 0.
When π = 1, this is just the earlier definition of conjugacy.
8
Exercise 1.1.10 Suppose that (π§1 , . . . , π§ π ) and (π§′1 , . . . , π§′π ) are conjugate. Show that π§π and π§′π are conjugate, for each π ∈ {1, . . . , π }.
Example 1.1.11 For any π§1 , . . . , π§ π ∈ C, the π-tuples (π§1 , . . . , π§ π ) and (π§1 , . . . , π§ π )
are conjugate. For let π(π‘ 1 , . . . , π‘ π ) be a polynomial over Q. Then
π(π§1 , . . . , π§ π ) = π(π§1 , . . . , π§ π )
since the coefficients of π are real, by a similar argument to the one in the first
proof of Lemma 1.1.2. Hence
π(π§1 , . . . , π§ π ) = 0 ⇐⇒ π(π§1 , . . . , π§ π ) = 0,
which is what we had to prove.
Example 1.1.12 Let π = π 2ππ/5 , as in Example 1.1.7. Then
(π, π2 , π3 , π4 )
and
(π4 , π3 , π2 , π)
are conjugate, by Example 1.1.11. It can also be shown that
(π, π2 , π3 , π4 )
and
(π2 , π4 , π, π3 )
are conjugate, although the proof is beyond us for now. But
(π, π2 , π3 , π4 )
and
(π2 , π, π3 , π4 )
(1.2)
are not conjugate, since if we put π(π‘1 , π‘2 , π‘3 , π‘4 ) = π‘ 2 − π‘12 then
π(π, π2 , π3 , π4 ) = 0 ≠ π(π2 , π, π3 , π4 ).
Warning 1.1.13 The converse of Exercise 1.1.10 is false: just because
π§π and π§′π are conjugate for all π, it doesn’t follow that (π§1 , . . . , π§ π ) and
(π§′1 , . . . , π§′π ) are conjugate. For we saw in Example 1.1.7 that π, π2 ,
π3 and π4 are all conjugate to each other, but we just saw that the
4-tuples (1.2) are not conjugate.
1.2
Every polynomial has a symmetry group. . .
We are now ready to describe the first main idea of Galois theory: every polynomial
has a symmetry group.
9
Definition 1.2.1 Let π be a polynomial with coefficients in Q. Write πΌ1 , . . . , πΌ π
for its distinct roots in C. The Galois group of π is
Gal( π ) = {π ∈ π π : (πΌ1 , . . . , πΌ π ) and (πΌπ(1) , . . . , πΌπ(π) ) are conjugate}.
‘Distinct roots’ means that we ignore any repetition of roots: e.g. if π (π‘) =
π‘ 5 (π‘ − 1) 9 then π = 2 and {πΌ1 , πΌ2 } = {0, 1}.
Exercise 1.2.2 Show that Gal( π ) is a subgroup of π π . (This one is
harder. Hint: if you permute the variables of a polynomial, you get
another polynomial.)
Exercise 1.2.2
Digression 1.2.3 I brushed something under the carpet. The definition
of Gal( π ) depends on the order in which the roots are listed. Different
orderings gives different subgroups of π π . However, these subgroups are
all conjugate to each other (conjugacy in the sense of group theory!), and
therefore isomorphic as abstract groups. So Gal( π ) is well-defined as an
abstract group, independently of the choice of ordering.
Example 1.2.4 Let π be a polynomial over Q whose complex roots πΌ1 , . . . , πΌ π
are all rational. If π ∈ Gal( π ) then πΌπ(π) and πΌπ are conjugate for each π, by Exercise 1.1.10. But since they are rational, that forces πΌπ(π) = πΌπ (by Exercise 1.1.6),
and since πΌ1 , . . . , πΌ π are distinct, π(π) = π. Hence π = id. So the Galois group of
π is trivial.
Example 1.2.5 Let π be a quadratic over Q. If π has rational roots then as we
have just seen, Gal( π ) is trivial. If π has two non-real roots then they are complex
conjugate, so Gal( π ) = π2 by Example 1.1.11. The remaining case is where π has
two distinct roots that are real but not rational, and it can be shown that in that case
too, Gal( π ) = π2 .
Warning 1.2.6 On terminology: note that just now I said ‘non-real’.
Sometimes people casually say ‘complex’ to mean ‘not real’. But try
not to do this yourself. It makes as little sense as saying ‘real’ to mean
‘irrational’, or ‘rational’ to mean ‘not an integer’.
Example 1.2.7 Let π (π‘) = π‘ 4 + π‘ 3 + π‘ 2 + π‘ + 1. Then (π‘ − 1) π (π‘) = π‘ 5 − 1, so π has
roots π, π2 , π3 , π4 where π = π 2ππ/5 . We saw in Example 1.1.12 that
1 2 3 4
1 2 3 4
1 2 3 4
,
∈ Gal( π ),
∉ Gal( π ).
4 3 2 1
2 4 1 3
2 1 3 4
10
In fact, it can be shown that
Gal( π ) =
1 2 3 4
2 4 1 3
πΆ4 .
Example 1.2.8 Let π (π‘) = π‘ 3 + ππ‘ 2 + ππ‘ + π be a cubic over Q with no rational
roots. Then
(
√
π΄3 if −27π 2 + 18πππ − 4π3 − 4π 3 π + π 2 π2 ∈ Q,
Gal( π ) π3 otherwise.
This appears as Proposition 22.4 in Stewart, but is way beyond us for now. Calculating Galois groups is hard.
Galois groups,
intuitively
1.3
. . . which determines whether it can be solved
Here we meet the second main idea of Galois theory: the Galois group of a
polynomial determines whether it can be solved. More exactly, it determines
whether the polynomial can be ‘solved by radicals’.
To explain what this means, let’s begin with the quadratic formula. The roots
of a quadratic ππ‘ 2 + ππ‘ + π are
√
−π ± π 2 − 4ππ
.
2π
After much struggling, it was discovered that there is a similar formula for cubics
ππ‘ 3 + ππ‘ 2 + ππ‘ + π: the roots are given by
√οΈ
√
√
3
√οΈ
3
−27π 2 π+9πππ−2π 3 +3π 3(27π 2 π 2 −18ππππ+4ππ3 +4π 3 π−π 2 π2 ) + −27π 2 π+9πππ−2π 3 −3π 3(27π 2 π 2 −18ππππ+4ππ3 +4π 3 π−π 2 π2 )
.
√
3
3 2π
(No, you don’t need to memorize that!) This is a complicated formula, and there’s
also something strange about it. Any nonzero complex number
has three cube roots,
√3
√
and there are two 3 signs in the formula (ignoring the 2 in the denominator), so
it looks as if the formula gives nine roots for the cubic. But a cubic can only have
three roots. What’s going on?
It turns out that some of the nine aren’t roots of the cubic at all. You have to
choose your cube roots carefully. Section 1.4 of Stewart’s book has much more on
this point, as well as an explanation of how the cubic formula was obtained. We
won’t be going into this ourselves.
As Stewart also explains, there is a similar but even more complicated formula
for quartics (polynomials of degree 4).
11
Digression 1.3.1 Stewart doesn’t actually write out the explicit formula for
the cubic, let alone the much worse one for the quartic. He just describes
algorithms by which they can be solved. But if you unwind the algorithm for
the cubic, you get the formula above. I have done this exercise once and do
not recommend it.
Once mathematicians discovered how to solve quartics, they naturally looked
for a formula for quintics (polynomials of degree 5). But it was eventually proved
by Abel and Ruffini, in the early 19th century, that there is no formula like the
quadratic, cubic or quartic formula for polynomials of degree ≥ 5. A bit more
precisely, there is no formula for the roots in terms of the coefficients that uses
only the usual arithmetic operations (+, −, ×, ÷) and πth roots (for integers π).
Spectacular as this result was, Galois went further—and so will we.
Informally, let us say that a complex number is radical if it can be obtained
from the rationals using only the usual arithmetic operations and πth roots. For
example,
√οΈ3 √
√2
7
1
+
2− 7
2
√οΈ
√οΈ
4
6 + 5 23
is radical, whichever square root, cube root, etc., we choose. A polynomial over
Q is solvable (or soluble) by radicals if all of its complex roots are radical.
Example 1.3.2 Every quadratic
√ over Q is solvable by radicals. This follows from
the quadratic formula: (−π ± π 2 − 4ππ)/2π is visibly a radical number.
Example 1.3.3 Similarly, the cubic formula shows that every cubic over Q is
solvable by radicals. The same goes for quartics.
Example 1.3.4 Some quintics are solvable by radicals. For instance,
(π‘ − 1)(π‘ − 2)(π‘ − 3)(π‘ − 4)(π‘ − 5)
is solvable by radicals, since all its roots are rational and, therefore, radical. A bit
less trivially, (π‘ − 123) 5 √
+ 456 is solvable by radicals, since its roots are the five
5
complex numbers 123 + −456, which are all radical.
What determines whether a polynomial is solvable by radicals? Galois’s
amazing achievement was to answer this question completely:
12
Theorem 1.3.5 (Galois) Let π be a polynomial over Q. Then
π is solvable by radicals ⇐⇒ Gal( π ) is a solvable group.
Example 1.3.6 Definition 1.2.1 implies that if π has degree π then Gal( π ) is
isomorphic to a subgroup of ππ . You saw in Group Theory that π4 is solvable,
and that every subgroup of a solvable group is solvable. Hence the Galois group
of any polynomial of degree ≤ 4 is solvable. It follows from Theorem 1.3.5 that
every polynomial of degree ≤ 4 is solvable by radicals.
Example 1.3.7 Put π (π‘) = π‘ 5 − 6π‘ + 3. Later we’ll show that Gal( π ) = π5 . You
saw in Group Theory that π5 is not solvable. Hence π is not solvable by radicals.
If there was a quintic formula then all quintics would be solvable by radicals,
for the same reason as in Examples 1.3.2 and 1.3.3. But since this is not the case,
there is no quintic formula.
Galois’s result is much sharper than Abel and Ruffini’s. They proved that there
is no formula providing a solution by radicals of every quintic, whereas Galois
found a way of determining which quintics (and higher) can be solved by radicals
and which cannot.
Digression 1.3.8 From the point of view of modern numerical computation,
this is all a bit odd. Computationally speaking, there is probably not much
difference
between solving π‘ 5 + 3 = 0 to 100 decimal places (that is, finding
√5
−3) and solving π‘ 5 − 6π‘ + 3 = 0 to 100 decimal places (that is, solving
a polynomial that isn’t solvable by radicals). Numerical computation and
abstract algebra have different ideas about what is easy and what is hard!
∗
∗
∗
This completes our overview of Galois theory. What’s next?
Mathematics increasingly emphasizes abstraction over calculation. Individual
mathematicians’ tastes vary, but the historical trend is clear. In the case of Galois
theory, this means dealing with abstract algebraic structures, principally fields,
instead of manipulating explicit algebraic expressions such as polynomials. The
cubic formula already gave you a taste of how hairy that can get.
Developing Galois theory using abstract algebraic structures helps us to see its
connections to other parts of mathematics, and also has some fringe benefits. For
example, we’ll solve some notorious geometry problems that perplexed the ancient
Greeks and remained unsolved for millennia. For that and many other things, we’ll
need some of the theory of groups, rings and fields—and that’s what’s next.
13
Chapter 2
Group actions, rings and fields
We now start again. This chapter is a mixture of revision and material that is
likely to be new to you. The revision is from Fundamentals of Pure Mathematics,
Honours Algebra, and Introduction to Number Theory (if you took it, which I
won’t assume). Because much of it is revision, it’s a longer chapter than usual.
Introduction to
Week 2
2.1
Group actions
Let’s begin with a definition from Fundamentals of Pure Mathematics (Figure 2.1).
Definition 2.1.1 Let πΊ be a group and π a set. An action of πΊ on π is a function
πΊ × π → π, written as (π, π₯) β¦→ ππ₯, such that
(πβ)π₯ = π(βπ₯)
for all π, β ∈ πΊ and π₯ ∈ π, and
1π₯ = π₯
for all π₯ ∈ π. Here 1 denotes the identity element of πΊ.
Figure 2.1: Action of a group πΊ on a set π. (Image adapted from @rowvector.)
14
Examples 2.1.2
i. Let π be a set. There is a group Sym(π) whose elements
are the bΔ³ections π → π, with composition as the group operation and
the identity function id π : π → π as the identity of the group. When
π = {1, . . . , π}, this group is nothing but ππ .
There is an action of Sym(π) on π defined by
Sym(π) × π →
π
(π, π₯)
β¦→ π(π₯).
Acting on π is what Sym(π) was born to do!
ii. Similar examples can be given for many kinds of mathematical object, not
just sets. Generally, an automorphism of an object π is an isomorphism
π → π (preserving whatever structure π has), and the automorphisms of
π form a group Aut(π) under composition. It acts on π just as in (i):
ππ₯ = π(π₯), for π ∈ Aut(π) and π₯ ∈ π.
For instance, when π is a real vector space, the linear automorphisms form
a group Aut(π) which acts on the vector space π. When π is finitedimensional, we can describe this action in more concrete terms. Writing
π = dim π, the vector space π is isomorphic to Rπ , whose elements we will
view as column vectors. The group Aut(π) is isomorphic to the group of
π × π real invertible matrices under multiplication, usually called GLπ (R)
(‘general linear’ group). Under these isomorphisms, the action of Aut(π)
on π becomes
GLπ (R) × Rπ → Rπ
(π, v)
β¦→ πv,
where πv is the usual matrix product.
iii. Let πΊ be the 48-element group of isometries (rotations and reflections) of a
cube. Then πΊ acts on the 6-element set of faces of the cube: any isometry
maps faces to faces. It also acts in a similar way on the 12-element set of
edges, the 8-element set of vertices, and a little less obviously, the 4-element
set of long diagonals. (The long diagonals are the lines between a vertex
and its opposite, furthest-away, vertex.)
iv. For any group πΊ and set π, the trivial action of πΊ on π is given by ππ₯ = π₯
for all π and π₯. Nothing moves anything!
Take an action of a group πΊ on a set π. Every group element π gives rise to a
function
π¯ : π → π
15
defined by
π(π₯)
¯
= ππ₯.
In fact, π¯ is a bΔ³ection, because π −1 is the inverse function of π.
¯ So π¯ ∈ Sym(π)
for each π ∈ πΊ. For instance, consider the usual action of the isometry group πΊ
of the cube on the set π of faces (Example 2.1.2(iii)). If π is a particular isometry,
then π¯ is whatever permutation of the set of faces the isometry induces.
We have just seen that whenever πΊ acts on π, every element π of the group πΊ
gives rise to an element π¯ of the group Sym(π). So, we have defined a function
Σ:
πΊ → Sym(π)
π β¦→
π.
¯
You can check that Σ is a group homomorphism.
Exercise 2.1.3 Check that π¯ is a bΔ³ection for each π ∈ πΊ. Also check
that Σ is a homomorphism.
In summary: any action of a group πΊ on π gives rise to a homomorphism
πΊ → Sym(π), in a natural way.
Examples 2.1.4
i. Let π be a set, and consider the action of Sym(π) on π
described in Example 2.1.2(i). For each π ∈ Sym(π), the function π¯ : π →
π is just π itself. Hence the homomorphism Σ : Sym(π) → Sym(π) is the
identity.
ii. Similarly, take a real vector space π and consider the action of Aut(π)
on π described in Example 2.1.2(ii). The resulting homomorphism
Σ : Aut(π) → Sym(π) is the inclusion; that is, Σ(π) = π for all π ∈ Aut(π).
(The domain of Σ is the group of linear bΔ³ections π → π, whereas the
codomain is the group of all bΔ³ections π → π.)
iii. Consider the usual action of the isometry group πΊ of the cube on the set π
of edges (Example 2.1.2(iii)). Since π has 12 elements, Sym(π) π12 , and
Σ amounts to a homomorphism πΊ → π12 .
iv. The trivial action of a group πΊ on a set π (Example 2.1.2(iv)) corresponds
to the trivial homomorphism πΊ → Sym(π).
Remark 2.1.5 When π is finite, we often choose an ordering of its elements,
writing π = {π₯ 1 , . . . , π₯ π }. Then Sym(π) π π (assuming the π₯π s are all distinct).
For each π ∈ πΊ and π ∈ {1, . . . , π }, the element ππ₯π of π must be equal to π₯ π for
some π. Write that π as ππ (π), so that
ππ₯π = π₯ ππ (π) .
16
Then ππ ∈ π π , and the composite homomorphism
Σ
πΊ −→ Sym(π) π π
is π β¦→ ππ .
Digression 2.1.6 In fact, an action of πΊ on π is the same thing as a
homomorphism πΊ → Sym(π). What I mean is that there is a natural
one-to-one correspondence between actions of πΊ on π and homomorphisms
πΊ → Sym(π). Some books even define an action of πΊ on π to be a
homomorphism πΊ → Sym(π).
In detail: we’ve just seen how an action of πΊ on π gives rise to a homomorphism Σ : πΊ → Sym(π). In the other direction, take any homomorphism
Σ : πΊ → Sym(π). Define a function πΊ × π → π by
(π, π₯) β¦→ Σ(π) (π₯).
(To make sense of the right-hand side: Σ(π) is an element of the group
Sym(π), which is the set of bΔ³ections π → π, so we can apply the function
Σ(π) to the element π₯ to obtain another element (Σ(π)) (π₯) of π.) You can
check that this function πΊ × π → π is an action of πΊ on π. So, we’ve now
seen how to convert an action into a homomorphism and vice versa. These
two processes are mutually inverse. Hence actions of πΊ on π correspond
one-to-one with homomorphisms πΊ → Sym(π).
At the purely set-theoretic level (ignoring the group structures), the key is
that for any sets π΄, π΅ and πΆ, there’s a natural bΔ³ection
πΆ π΄×π΅ (πΆ π΅ ) π΄ .
Here πΆ π΅ means the set of functions π΅ → πΆ. The general proof is very
similar to what we’ve just done (where π΄ = πΊ and π΅ = πΆ = π). In words, a
function π΄ × π΅ → πΆ can be seen as a way of assigning to each element of π΄
a function π΅ → πΆ. In a picture:
Here π΄ = π΅ = πΆ = R. By slicing up the surface as shown, a function R2 → R
can be seen as a function from R to {functions R → R}.
17
Definition 2.1.7 An action of a group πΊ on a set π is faithful if for π, β ∈ πΊ,
ππ₯ = βπ₯ for all π₯ ∈ π ⇒ π = β.
Faithfulness means that if two elements of the group do the same, they are the
same. Here are some other ways to express it.
Lemma 2.1.8 For an action of a group πΊ on a set π, the following are equivalent:
i. the action is faithful;
ii. for π ∈ πΊ, if ππ₯ = π₯ for all π₯ ∈ π then π = 1;
iii. the homomorphism Σ : πΊ → Sym(π) is injective;
iv. ker Σ is trivial.
¯ then π = β. But
Proof Faithfulness states that whenever π, β ∈ πΊ with π¯ = β,
Σ(π) = π,
¯ so (i) ⇐⇒ (iii). Similarly, (ii) ⇐⇒ (iv). Finally, it is a standard fact that
a homomorphism is injective if and only if its kernel is trivial, so (iii) ⇐⇒ (iv).β‘
Many common actions are faithful:
Examples 2.1.9
i. The natural action of Sym(π) on a set π (Examples 2.1.2(i) and 2.1.4(i)) is faithful, since the corresponding homomorphism
id : Sym(π) → Sym(π) is injective.
ii. Similarly, the natural action of Aut(π) on a vector space (Examples 2.1.2(ii)
and 2.1.4(ii)) is faithful, since the corresponding homomorphism Aut(π) →
Sym(π) is injective.
iii. The action of the isometry group πΊ of the cube on the set of faces (Examples 2.1.2(iii) and 2.1.4(iii)) is faithful, since an isometry is determined by
its effect on faces. The same is true for edges and vertices.
But the action of πΊ on the 4-element set π of long diagonals is not faithful:
for πΊ has 48 elements, whereas Sym(π) has only 4! = 24 elements, so the
homomorphism Σ : πΊ → Sym(π) cannot be injective.
iv. The trivial action of a group πΊ on a set π is never faithful unless πΊ itself is
trivial, since ππ₯ = π₯ for all π ∈ πΊ and π₯ ∈ π.
Exercise 2.1.10 Example 2.1.9(iii) shows that the action of the isometry cube πΊ of the cube on the set π of long diagonals is not faithful.
By Lemma 2.1.8, there must be some non-identity isometry of the
cube that fixes all four long diagonals. In fact, there is exactly one.
What is it?
18
When a group πΊ acts faithfully on a set π, there is a copy of πΊ sitting inside
Sym(π) as a subgroup (a ‘faithful representation’ of πΊ):
Lemma 2.1.11 Let πΊ be a group acting faithfully on a set π. Then πΊ is isomorphic
to the subgroup
im Σ = { π¯ : π ∈ πΊ}
of Sym(π), where Σ : πΊ → Sym(π) and π¯ are defined as above.
Proof By Lemma 2.1.8, Σ is injective, and it is a general group-theoretic fact that
any injective homomorphism π : πΊ → π» induces an isomorphism between πΊ and
im π.
β‘
Example 2.1.12 Consider the usual action of the isometry group πΊ of the cube
on the 8-element set π of vertices. As we have seen, this action is faithful. Hence
the associated homomorphism
Σ:
πΊ → Sym(π)
π β¦→
π¯
induces an isomorphism between πΊ and the subgroup { π¯ : π ∈ πΊ} of Sym(π).
The subgroup consists of all permutations of the set of vertices that come from
some isometry. For instance, there is no isometry that exchanges two vertices but
leaves the rest fixed, so this subgroup contains no 2-cycles.
Remark 2.1.13 How does Lemma 2.1.11 look when π is a finite set with elements
π₯ 1 , . . . , π₯ π ? Then Sym(π) π π , and as in Remark 2.1.5, we can write ππ₯π = π₯ ππ (π) .
It follows from that lemma and remark that πΊ is isomorphic to the subgroup
{ππ : π ∈ πΊ} of π π (which is a subgroup). The isomorphism is given by π β¦→ ππ .
Faithfulness is about which elements of the group fix everything in the set. We
can also ask which elements of the set are fixed by everything in the group—or
more generally, by some prescribed set π of group elements.
Definition 2.1.14 Let πΊ be a group acting on a set π. Let π ⊆ πΊ. The fixed set
of π is
Fix(π) = {π₯ ∈ π : π π₯ = π₯ for all π ∈ π}.
Later, we’ll need the following lemma.
Lemma 2.1.15 Let πΊ be a group acting on a set π, let π ⊆ πΊ, and let π ∈ πΊ.
Then Fix(πππ −1 ) = π Fix(π).
Here πππ −1 = {ππ π −1 : π ∈ π} and π Fix(π) = {ππ₯ : π₯ ∈ Fix(π)}.
19
Proof For π₯ ∈ π, we have
π₯ ∈ Fix(πππ −1 ) ⇐⇒ ππ π −1 π₯ = π₯ for all π ∈ π
⇐⇒ π π −1 π₯ = π −1 π₯ for all π ∈ π
⇐⇒ π −1 π₯ ∈ Fix(π)
⇐⇒ π₯ ∈ π Fix(π).
2.2
β‘
Rings
We’ll begin this part with some stuff you know—but with a twist.
In this course, the word ring means commutative ring with 1 (multiplicative
identity). Noncommutative rings and rings without 1 are important in some parts
of mathematics, but since we’ll be focusing on commutative rings with 1, it will
be easier to just call them ‘rings’.
Example 2.2.1 There are many ways of building new rings from old. One of the
most fundamental is that from any ring π
, we can build the ring π
[π‘] of polynomials
over π
. We will define π
[π‘] formally and study it in detail in Chapter 3.
Given rings π
and π, a homomorphism from π
to π is a function π : π
→ π
satisfying the equations
π(π + π ′) = π(π) + π(π ′),
π(ππ ′) = π(π)π(π ′),
π(0) = 0,
π(1) = 1 (note this!)
π(−π) = −π(π),
for all π, π ′ ∈ π
. For example, complex conjugation is a homomorphism C → C.
It is a very useful lemma that if
π(π + π ′) = π(π) + π(π ′),
π(ππ ′) = π(π)π(π ′),
π(1) = 1
for all π, π ′ ∈ π
then π is a homomorphism. In other words, to show that π is a
homomorphism, you only need to check it preserves +, · and 1; preservation of 0
and negatives then comes for free. But you do need to check it preserves 1. That
doesn’t follow from the other conditions.
A subring of a ring π
is a subset π ⊆ π
that contains 0 and 1 and is closed
under addition, multiplication and negatives. Whenever π is a subring of π
, the
inclusion π : π → π
(defined by π(π ) = π ) is a homomorphism.
20
Warning 2.2.2 In Honours Algebra, rings had 1s but homomorphisms
were not required to preserve 1. Similarly, subrings of π
had to have
a 1, but it was not required to be the same as the 1 of π
.
For example, take the ring C, the noncommutative ring π of 2 × 2
matrices over C, and the function π : C → π defined by
π§ 0
π(π§) =
.
0 0
In the terminology of Honours Algebra, π is a homomorphism and
its image im π is a subring of π. But in our terminology, π is not
a homomorphism (as π(1) ≠ πΌ) and im π is not a subring of π (as
πΌ ∉ im π).
Lemma 2.2.3 Let π
be a ring and let S be any set (perhaps infinite) of subrings
Ñ
of π
. Then their intersection π∈S π is also a subring of π
.
In contrast, in the Honours Algebra setup, even the intersection of two subrings
need not be a subring.
Ñ
Proof Write π = π∈S π.
For each π ∈ S , we have 0 ∈ π since π is a subring. Hence 0 ∈ π by definition
of intersection.
Let π, π ∈ π. For each π ∈ S , we have π, π ∈ π by definition of intersection,
so π + π ∈ π since π is a subring. Hence π + π ∈ π by definition of intersection.
Similar arguments show that π ∈ π ⇒ −π ∈ π, that 1 ∈ π, and that π, π ∈ π ⇒
π π ∈ π.
β‘
Example 2.2.4 For any ring π
, there is exactly one homomorphism Z → π
. Here
is a sketch of the proof.
To show there is at least one homomorphism π : Z → π
, we construct one.
Define π inductively on integers π ≥ 0 by π(0) = 0 and π(π + 1) = π(π) + 1 π
.
Thus,
π(π) = 1 π
+ · · · + 1 π
.
Define π on negative integers π by π(π) = −π(−π). A series of tedious checks
shows that π is indeed a ring homomorphism.
To show there is only one homomorphism Z → π
, let π be any homomorphism
Z → π
; we have to prove that π = π. Certainly π(0) = 0 = π(0). Next prove
by induction on π that π(π) = π(π) for nonnegative integers π. I leave the details
to you, but the crucial point is that because homomorphisms preserve 1, we must
have
π(π + 1) = π(π) + π(1) = π(π) + 1 π
21
for all π ≥ 0. Once we have shown that π and π agree on the nonnegative integers,
it follows that for negative π,
π(π) = −π(−π) = −π(−π) = π(π).
The meaning of
‘π · 1’, and
Exercise 2.3.13
Hence π(π) = π(π) for all π ∈ Z; that is, π = π.
Usually we write π(π) as π · 1 π
, or simply as π if it is clear from the context
that π is to be interpreted as an element of π
. So for π ≥ 0,
π · 1π
= 1π
+ · · · + 1π
.
| {z }
π times
The dot in the expression ‘π · 1 π
’ is not multiplication in any ring, since π ∈ Z but
1 π
∈ π
. It’s just notation.
Every ring homomorphism π : π
→ π has an image im π, which is a subring
of π, and a kernel ker π, which is an ideal of π
.
Warning 2.2.5 Subrings are analogous to subgroups, and ideals are
analogous to normal subgroups. But whereas normal subgroups are
a special kind of subgroup, ideals are not a special kind of subring!
Subrings must contain 1, but most ideals don’t.
Exercise 2.2.6 Prove that the only subring of a ring π
that is also an
ideal is π
itself.
Quotient rings
Given an ideal πΌ P π
, we obtain the quotient ring or factor ring π
/πΌ and the
canonical homomorphism π πΌ : π
→ π
/πΌ, which is surjective and has kernel πΌ.
As explained in Honours Algebra, the quotient ring together with the canonical
homomorphism has a ‘universal property’: given any ring π and any homomorphism π : π
→ π satisfying ker π ⊇ πΌ, there is exactly one homomorphism
π¯ : π
/πΌ → π such that this diagram commutes:
π
π
ππΌ
π
/πΌ
π¯
!
/ π.
(For a diagram to commute means that whenever there are two different paths
from one object to another, the composites along the two paths are equal. Here, it
means that π = π¯ β¦ π πΌ .) The first isomorphism theorem says that if π is surjective
and has kernel equal to πΌ then π¯ is an isomorphism. So π πΌ : π
→ π
/πΌ is essentially
the only surjective homomorphism out of π
with kernel πΌ.
22
Digression 2.2.7 Loosely, the ideals of a ring π
correspond one-to-one with
the surjective homomorphisms out of π
. This means four things:
•
given an ideal πΌ P π
, we get a surjective homomorphism out of π
(namely, π πΌ : π
→ π
/πΌ);
•
given a surjective homomorphism π out of π
, we get an ideal of π
(namely, ker π);
•
if we start with an ideal πΌ of π
, take its associated surjective homomorphism π πΌ : π
→ π
/πΌ, then take its associated ideal, we end up where
we started (that is, ker(π πΌ ) = πΌ);
•
if we start with a surjective homomorphism π : π
→ π, take its associated ideal ker π, then take its associated surjective homomorphism
πker π : π
→ π
/ker π, we end up where we started (at least ‘up to isomorphism’, in that we have the isomorphism π¯ : π
/ker π → π making
the triangle commute). This is the first isomorphism theorem.
Analogous stories can be told for groups and modules.
An integral domain is a ring π
such that 0 π
≠ 1 π
and for π, π ′ ∈ π
,
ππ ′ = 0 ⇒ π = 0 or π ′ = 0.
Exercise 2.2.8 The trivial ring or zero ring is the one-element set
with its only possible ring structure. Show that the only ring in which
0 = 1 is the trivial ring.
Equivalently, an integral domain is a nontrivial ring in which cancellation is
valid: π π = π ′ π implies π = π ′ or π = 0.
Warning 2.2.9 In an arbitrary ring, you can’t reliably cancel by
nonzero elements. For example, in the ring Z/β¨6β© of integers mod 6,
we have 1 × 2 = 4 × 2 but 1 ≠ 4.
Digression 2.2.10 Why is the condition 0 ≠ 1 in the definition of integral
domain?
My answer begins with a useful general point: the sum of no things should
always be interpreted as 0. (The amount you pay in a shop is the sum of the
prices of the individual things. If you buy no things, you pay £0.) This is
ultimately because 0 is the identity for addition.
Similarly, the product of no things should be interpreted as 1. One justification is that 1 is the identity for multiplication. Another is that if we want
23
Í
Î
laws like exp( π₯ π ) = exp(π₯ π ) to hold, and if we believe that the sum of
no things is 0, then the product of no things should be 1. Or if we want every
positive integer to be a product of primes, we’d better say that 1 is the product
of no primes. It’s a convention to let us handle trivial cases smoothly.
Now consider the following condition on a ring π
: for all π ≥ 0 and
π 1 , . . . , π π ∈ π
,
π 1π 2 · · · π π = 0 ⇒ there exists π ∈ {1, . . . , π} such that π π = 0.
(2.1)
For π = 2, this is the main condition in the definition of integral domain.
For π = 0, it says: if 1 = 0 then there exists π ∈ ∅ such that π π = 0. But
any statement beginning ‘there exists π ∈ ∅’ is false! So in the case π = 0,
condition (2.1) states that 1 ≠ 0. Hence ‘1 ≠ 0’ is the 0-fold analogue of the
main condition.
On the other hand, if (2.1) holds for π = 0 and π = 2 then a simple induction
shows that it holds for all π ≥ 0. Conclusion: an integral domain can
equivalently be defined as a ring in which (2.1) holds for all π ≥ 0.
Let π be a subset of a ring π
. The ideal β¨π β© generated by π is defined as the
intersection of all the ideals of π
containing π . You can show that any intersection
of ideals is an ideal (much as for subrings in Lemma 2.2.3). So β¨π β© is an ideal.
We can also characterize β¨π β© as the smallest ideal of π
containing π . That is, β¨π β©
is an ideal containing π , and if πΌ is another ideal containing π then β¨π β© ⊆ πΌ.
This definition of the ideal generated by π is top-down: we obtain β¨π β© as the
intersection of bigger ideals. But there is also a useful bottom-up description of
β¨π β©. Here it is when π is finite.
Lemma 2.2.11 Let π
be a ring and let π = {π 1 , . . . , π π } be a finite subset. Then
β¨π β© = {π 1π 1 + · · · + π π π π : π 1 , . . . , π π ∈ π
}.
Proof Write πΌ for the right-hand side. It is straightforward to check that πΌ is an
ideal of π
, and it contains π because, for instance, π 1 = 1π 1 + 0π 2 + · · · + 0π π .
Now let π½ be any ideal of π
containing π . Let π 1 , . . . , π π ∈ π
. For each π,
we have ππ ∈ π½ since π½ contains π , and so ππ ππ ∈ π½ since π½ is an ideal. Hence
Í
ππ ππ ∈ π½, again since π½ is an ideal. So πΌ ⊆ π½.
Hence πΌ is the smallest ideal of π
containing π , that is, πΌ = β¨π β©.
β‘
Digression 2.2.12 A similar interplay between top-down and bottom-up
appears in other parts of mathematics.
For example, in topology, the closure of a subset of a metric or topological
space is the intersection of all closed subsets containing it. In linear algebra,
24
the span of a subset of a vector space is the intersection of all linear subspaces
containing it. In group theory, the subgroup generated by a subset of a group
is the intersection of all subgroups containing it.
These are all top-down definitions, but there are equivalent bottom-up definitions, describing explicitly which elements belong to the subset. Sometimes
we’re lucky and those descriptions are simple. For instance, closures can
easily be described in terms of limit points, and spans are just sets of linear
combinations. But sometimes it gets more complicated. For example, the
subgroup of a group πΊ generated by a subset π can be described informally
as the set of elements of πΊ that can be obtained from π by taking products
and inverses, but expressing that precisely is a little bit fiddly.
It’s worth getting comfortable with the top-down style of definition, as it
works well in cases where the bottom-up approach is prohibitively complicated, and we’ll need it later.
When π = {π 1 , . . . , π π }, we write β¨π β© as β¨π 1 , . . . , π π β© rather than β¨{π 1 , . . . , π π }β©.
In particular, when π = 1, Lemma 2.2.11 implies that
β¨πβ© = {ππ : π ∈ π
}.
Ideals of the form β¨πβ© are called principal ideals. A principal ideal domain is
an integral domain in which every ideal is principal.
Example 2.2.13 Z is a principal ideal domain. Indeed, if πΌ PZ then either πΌ = {0},
in which case πΌ = β¨0β©, or πΌ contains some positive integer, in which case we can
define π to be the least positive integer in πΌ and use the division algorithm to show
that πΌ = β¨πβ©.
Exercise 2.2.14 Fill in the details of Example 2.2.13.
Let π and π be elements of a ring π
. We say that π divides π , and write π | π , if
there exists π ∈ π
such that π = ππ. This condition is equivalent to π ∈ β¨πβ©, and to
β¨π β© ⊆ β¨πβ©.
An element π’ ∈ π
is a unit if it has a multiplicative inverse, or equivalently
if β¨π’β© = π
. The units form a group π
× under multiplication. For instance,
Z× = {1, −1}.
Exercise 2.2.15 Let π and π be elements of an integral domain. Show
that π | π | π ⇐⇒ β¨πβ© = β¨π β© ⇐⇒ π = π’π for some unit π’.
Elements π and π of a ring are coprime if for π ∈ π
,
π | π and π | π ⇒ π is a unit.
25
Proposition 2.2.16 Let π
be a principal ideal domain and π, π ∈ π
. Then
π and π are coprime ⇐⇒ ππ + ππ = 1 for some π, π ∈ π
.
Proof ⇒: suppose that π and π are coprime. Since π
is a principal ideal domain,
β¨π, π β© = β¨π’β© for some π’ ∈ π
. Since π ∈ β¨π, π β© = β¨π’β©, we must have π’ | π, and
similarly π’ | π . But π and π are coprime, so π’ is a unit. Hence 1 ∈ β¨π’β© = β¨π, π β©.
But by Lemma 2.2.11,
β¨π, π β© = {ππ + ππ : π, π ∈ π
},
and the result follows.
⇐: suppose that ππ + ππ = 1 for some π, π ∈ π
. If π’ ∈ π
with π’ | π and π’ | π
then π’ | (ππ + ππ ) = 1, so π’ is a unit. Hence π and π are coprime.
β‘
2.3
Fields
A field is a ring πΎ in which 0 ≠ 1 and every nonzero element is a unit. Equivalently,
it is a ring such that πΎ × = πΎ \ {0}. Every field is an integral domain.
Exercise 2.3.1 Write down all the examples of fields that you know.
As we go on, we’ll see several ways of making new fields out of old. Here’s
the simplest.
Example 2.3.2 Let πΎ be a field. A rational expression over πΎ is a ratio of two
polynomials
π (π‘)
,
π(π‘)
where π (π‘), π(π‘) ∈ πΎ [π‘] with π ≠ 0. Two such expressions, π1 /π1 and π2 /π2 , are
regarded as equal if π1 π2 = π2 π1 in πΎ [π‘]. So formally, a rational expression is an
equivalence class of pairs ( π , π) under the equivalence relation in the last sentence.
The set of rational expressions over πΎ is denoted by πΎ (π‘).
Rational expressions are added, subtracted and multiplied in the ways you’d
expect, making πΎ (π‘) into a field. We will look at it more carefully in Chapter 3.
A field πΎ has exactly two ideals: {0} and πΎ. For if {0} ≠ πΌ P πΎ then π’ ∈ πΌ for
some π’ ≠ 0; but then π’ is a unit, so β¨π’β© = πΎ, so πΌ = πΎ.
Lemma 2.3.3 Every homomorphism between fields is injective.
26
A ‘homomorphism between fields’ means a ring homomorphism.
Proof Let π : πΎ → πΏ be a homomorphism between fields. Then ker π P πΎ, so
ker π is either {0} or πΎ. If ker π = πΎ then π(1) = 0; but π(1) = 1 by definition
of homomorphism, so 0 = 1 in πΏ, contradicting the assumption that πΏ is a field.
Hence ker π = {0}, that is, π is injective.
β‘
Warning 2.3.4 With the Honours Algebra definition of homomorphism, Lemma 2.3.3 would be false, since the map with constant value
0 would be a homomorphism.
Exercise 2.3.5 Let π : πΎ → πΏ be a homomorphism of fields and let
0 ≠ π ∈ πΎ. Prove that π(π −1 ) = π(π) −1 . Why is π(π) −1 defined?
A subfield of a field πΎ is a subring that is a field.
Lemma 2.3.6 Let π : πΎ → πΏ be a homomorphism between fields.
i. For any subfield πΎ ′ of πΎ, the image ππΎ ′ is a subfield of πΏ.
ii. For any subfield πΏ ′ of πΏ, the preimage π−1 πΏ ′ is a subfield of πΎ.
Proof For (i), you know from Proposition 3.4.28 of Honours Algebra that ππΎ ′ is
a subring of πΏ, and you can use Exercise 2.3.5 above to show that if 0 ≠ π ∈ ππΎ ′
then π −1 ∈ ππΎ ′. The proof of (ii) is similar.
β‘
Whenever we have a collection of homomorphisms between the same pair of
fields, we get a subfield in the following way.
Definition 2.3.7 Let π and π be sets, and let π ⊆ {functions π → π }. The
equalizer of π is
Eq(π) = {π₯ ∈ π : π (π₯) = π(π₯) for all π , π ∈ π}.
In other words, it is the part of π where all the functions in π are equal.
Lemma 2.3.8 Let πΎ and πΏ be fields, and let π ⊆ {homomorphisms πΎ → πΏ}.
Then Eq(π) is a subfield of πΎ.
Proof We must show that 0, 1 ∈ Eq(π), that if π ∈ Eq(π) then −π ∈ Eq(π) and
1/π ∈ Eq(π) (for π ≠ 0), and that if π, π ∈ Eq(π) then π + π, ππ ∈ Eq(π). I will
show just the last of these, leaving the rest to you.
Suppose that π, π ∈ Eq(π). For all π, π ∈ π, we have
π(ππ) = π(π)π(π) = π (π)π (π) = π (ππ),
so ππ ∈ Eq(π).
β‘
27
Example 2.3.9 Let πΎ = πΏ = C. Let π = {idC , π
}, where π
: C → C is complex
conjugation. Then
Eq(π) = {π§ ∈ C : π§ = π§} = R,
and R is indeed a subfield of C.
Next we ask: when is 1 + · · · + 1 equal to 0?
Let π
be any ring. By Example 2.2.4, there is a unique homomorphism
π : Z → π
. Its kernel is an ideal of the principal ideal domain Z. Hence
ker π = β¨πβ© for a unique integer π ≥ 0. This π is called the characteristic of π
,
and written as char π
. So for π ∈ Z, we have π · 1 π
= 0 if and only if π is a
multiple of char π
. Or equivalently,
(
the least π > 0 such that π · 1 π
= 0 π
, if such an π exists;
char π
=
(2.2)
0,
otherwise.
The concept of characteristic is mostly used in the case of fields.
Examples 2.3.10
i. Q, R and C all have characteristic 0.
ii. For a prime number π, we write F π for the field Z/β¨πβ© of integers modulo
π. Then char F π = π.
iii. For any field πΎ, the field πΎ (π‘) of rational expressions has the same characteristic as πΎ.
Lemma 2.3.11 The characteristic of an integral domain is 0 or a prime number.
Proof Let π
be an integral domain and write π = char π
. Suppose that π > 0; we
must prove that π is prime.
Since 1 ≠ 0 in an integral domain, π ≠ 1. (Remember that 1 is not a prime!
So that step was necessary.) Now let π, π > 0 with ππ = π. Writing π for the
unique homomorphism Z → π
, we have
π(π) π(π) = π(ππ) = π(π) = 0,
and π
is an integral domain, so π(π) = 0 or π(π) = 0. WLOG, π(π) = 0. But
ker π = β¨πβ©, so π | π, so π = π. Hence π is prime.
β‘
In particular, the characteristic of a field is always 0 or a prime. But there is
no way of mapping between fields of different characteristics:
Lemma 2.3.12 Let π : πΎ → πΏ be a homomorphism of fields. Then char πΎ =
char πΏ.
28
Proof Write ππΎ and ππΏ for the unique homomorphisms from Z to πΎ and πΏ,
respectively. Since ππΏ is the unique homomorphism Z → πΏ, the triangle
Z
ππΎ
ππΏ
πΎ
π
/πΏ
commutes. (Concretely, this says that π(π · 1πΎ ) = π · 1 πΏ for all π ∈ Z.) Hence
ker(π β¦ ππΎ ) = ker ππΏ . But π is injective by Lemma 2.3.3, so ker(π β¦ ππΎ ) = ker ππΎ .
Hence ker ππΎ = ker ππΏ , or equivalently, char πΎ = char πΏ.
β‘
For example, the inclusion Q → R is a homomorphism of fields, and both have
characteristic 0.
Exercise 2.3.13 This proof of Lemma 2.3.12 is quite abstract. Find
a more concrete proof, taking equation (2.2) as your definition of
characteristic. (You will still need the fact that π is injective.)
The meaning of
‘π · 1’, and
Exercise 2.3.13
The prime subfield of πΎ is the intersection of all the subfields of πΎ. It is
straightforward to show that any intersection of subfields is a subfield (much as in
Lemma 2.2.3). Hence the prime subfield is a subfield. It is the smallest subfield
of πΎ, in the sense that any other subfield of πΎ contains it.
Concretely (‘bottom-up’), the prime subfield of πΎ is
π · 1πΎ
: π, π ∈ Z with π · 1πΎ ≠ 0 .
π · 1πΎ
To see this, first note that this set is a subfield of πΎ. It is the smallest subfield of πΎ:
for if πΏ is a subfield of πΎ then 1πΎ ∈ πΏ by definition of subfield, so π · 1πΎ ∈ πΏ for
all integers π, so (π · 1πΎ )/(π · 1πΎ ) ∈ πΏ for all integers π and π such that π · 1πΎ ≠ 0.
Examples 2.3.14
i. The field Q has no proper subfields, so the prime subfield
of Q is Q itself.
ii. Let π be a prime. The field F π has no proper subfields, so the prime subfield
of F π is F π itself.
Exercise 2.3.15 What is the prime subfield of R? Of C?
The prime subfields appearing in Examples 2.3.14 were Q and F π . In fact,
these are the only prime subfields of anything:
29
Lemma 2.3.16 Let πΎ be a field.
i. If char πΎ = 0 then the prime subfield of πΎ is Q.
ii. If char πΎ = π > 0 then the prime subfield of πΎ is F π .
In the statement of this lemma, as so often in mathematics, the word ‘is’ means
‘is isomorphic to’. I hope you’re comfortable with that by now.
Proof For (i), suppose that char πΎ = 0. By definition of characteristic, π · 1πΎ ≠ 0
for all integers π ≥ 0. One can check that there is a well-defined homomorphism
π : Q → πΎ defined by π/π β¦→ (π · 1πΎ )/(π · 1πΎ ). (The check uses the fact that
π : π β¦→ π · 1πΎ is a homomorphism.) Now π is injective (being a homomorphism
of fields), so im π Q. But im π is a subfield of πΎ, and since Q has no proper
subfields, it is the prime subfield.
For (ii), suppose that char πΎ = π > 0. By Lemma 2.3.11, π is prime. The
unique homomorphism π : Z → πΎ has kernel β¨πβ©, by definition. By the first
isomorphism theorem, im π Z/β¨πβ© = F π . But im π is a subfield of πΎ, and since
F π has no proper subfields, it is the prime subfield.
β‘
Lemma 2.3.17 Every finite field has positive characteristic.
Proof By Lemma 2.3.16, a field of characteristic 0 contains a copy of Q and is
therefore infinite.
β‘
Warning 2.3.18 There are also infinite fields of positive characteristic.
An example is the field F π (π‘) of rational expressions over F π .
Square roots usually √come in pairs: how many times in your life have you
written a ± sign before a ? But in characteristic 2, plus and minus are the same,
so the two square roots become one. We’ll see that this pattern persists: πth roots
behave strangely in characteristic π. First, an important little lemma:
Lemma 2.3.19 Let π be a prime and 0 < π < π. Then π | ππ .
For example, the 7th row of Pascal’s triangle is 1, 7, 21, 35, 35, 21, 7, 1, and the
lemma predicts that 7 divides all of these numbers apart from the first and last.
Proof We have π!( π − π)! ππ = π!. Now π divides
π! but not π! or ( π − π)! (since
π is prime and 0 < π < π), so π must divide ππ .
β‘
Proposition 2.3.20 Let π be a prime number and π
a ring of characteristic π.
30
i. The function
π
→ π
π β¦→ π π
π:
is a homomorphism.
ii. If π
is a field then π is injective.
iii. If π
is a finite field then π is an automorphism of π
.
Proof For (i), certainly π preserves multiplication and 1. To show that π preserves
addition, let π, π ∈ π
: then by Lemma 2.3.19 and the hypothesis that char π
= π,
π
π (π + π ) = (π + π ) =
π ∑οΈ
π
π π π π−π = π π + π π = π (π) + π (π ).
π
π=0
Now (ii) follows since every homomorphism between fields is injective, and (iii)
since every injection from a finite set to itself is bΔ³ective.
β‘
The homomorphism π : π β¦→ π π is called the Frobenius map, or, in the case
of finite fields, the Frobenius automorphism.
That π is a homomorphism is a shocker. Writing (π₯ + π¦) π = π₯ π + π¦ π is a classic
algebra mistake. But here, it’s true!
Example 2.3.21 The Frobenius automorphism of F π = Z/β¨πβ© is not very interesting. When πΊ is a finite group of order π, Lagrange’s theorem implies that π π = 1
for all π ∈ πΊ. Applying this to the multiplicative group F×π = F π \ {0} gives
π π−1 = 1 whenever 0 ≠ π ∈ F π . It follows that π π = π for all π ∈ F π . That is, π is
the identity. Everything is its own πth root!
Unfortunately, we can’t give any interesting examples of the Frobenius map
just now, because we have so few examples of fields. That will change later.
Corollary 2.3.22 Let π be a prime number.
i. In a field of characteristic π, every element has at most one πth root.
ii. In a finite field of characteristic π, every element has exactly one πth root.
Proof Part (i) says that the Frobenius map is injective, and part (ii) says that it is
bΔ³ective, as Proposition 2.3.20 states.
β‘
Examples 2.3.23
i. In a field of characteristic 2, every element has at most
one square root.
31
ii. In C, there are π different πth roots of unity. But in a field of characteristic
π, there is only one: 1 itself.
iii. Let πΎ be a field of characteristic π and π ∈ πΎ. Corollary 2.3.22(i) says that
π has at most one πth root. It may have none. For instance, you’ll show in
Exercise 3.1.13 that the element π‘ of F π (π‘) has no πth root.
Here’s a construction that will let us manufacture many more examples of
fields.
An element π of a ring π
is irreducible if π is not 0 or a unit, and if for π, π ∈ π
,
Building blocks
π = ππ ⇒ π or π is a unit.
For example, the irreducibles in Z are ±2, ±3, ±5, . . .. An element of a ring is
reducible if it is not 0, a unit, or irreducible.
Warning 2.3.24 The 0 and units of a ring count as neither reducible
nor irreducible, in much the same way that the integers 0 and 1 are
neither prime nor composite.
Exercise 2.3.25 What are the irreducible elements of a field?
Proposition 2.3.26 Let π
be a principal ideal domain and 0 ≠ π ∈ π
. Then
π is irreducible ⇐⇒ π
/β¨πβ© is a field.
Proof Write π for the canonical homomorphism π
→ π
/β¨πβ©.
⇒: suppose that π is irreducible. To show that 1 π
/β¨πβ© ≠ 0 π
/β¨πβ© , note that since
π is not a unit, 1 π
∉ β¨πβ© = ker π, so
1 π
/β¨πβ© = π(1 π
) ≠ 0 π
/β¨πβ© .
Next we have to show that every nonzero element of π
/β¨πβ© is a unit, or
equivalently that π(π ) is a unit whenever π ∈ π
with π ∉ β¨πβ©. We have π β€ π ,
and π is irreducible, so π and π are coprime. Hence by Proposition 2.2.16 and the
assumption that π
is a principal ideal domain, we can choose π, π ∈ π
such that
ππ + ππ = 1 π
.
Applying π to each side gives
π(π)π(π) + π(π)π(π ) = 1 π
/β¨πβ© .
32
But π(π) = 0, so π(π)π(π ) = 1, so π(π ) is a unit.
⇐: suppose that π
/β¨πβ© is a field. Then 1 π
/β¨πβ© ≠ 0 π
/β¨πβ© , that is, 1 π
∉ ker π = β¨πβ©,
that is, π β€ 1 π
. Hence π is not a unit.
Next we have to show that if π, π ∈ π
with π = ππ then π or π is a unit. We
have
0 = π(π) = π(π)π(π)
and π
/β¨πβ© is an integral domain, so WLOG π(π) = 0. Then π ∈ ker π = β¨πβ©, so
π = ππ′ for some π′ ∈ π
. This gives
π = ππ = ππ′ π.
But π ≠ 0 by hypothesis, and π
is an integral domain, so π′ π = 1. Hence π is a
unit.
β‘
Example 2.3.27 When π is an integer, Z/β¨πβ© is a field if and only if π is irreducible
(that is, ± a prime number).
Proposition 2.3.26 enables us to construct fields from irreducible elements. . . but irreducible elements of a principal ideal domain. Right now that’s
not much help, because we don’t have many examples of principal ideal domains.
But we will do soon.
33
Chapter 3
Polynomials
This chapter revisits and develops some themes you met in Honours Algebra.
Before you begin, it may help you to reread Section 3.3 (Polynomials) of the
Honours Algebra notes.
Introduction to
Week 3
3.1
The ring of polynomials
You already know the definition of polynomial, but I want to make a point by
phrasing it in an unfamiliar way.
Definition 3.1.1 Let π
be a ring. A polynomial over π
is an infinite sequence
(π 0 , π 1 , π 2 , . . .) of elements of π
such that {π : ππ ≠ 0} is finite.
The set of polynomials over π
forms a ring as follows:
(π 0 , π 1 , . . .) + (π 0 , π 1 , . . .) = (π 0 + π 0 , π 1 + π 1 , . . .),
(π 0 , π 1 , . . .) · (π 0 , π 1 , . . .) = (π 0 , π 1 , . . .)
∑οΈ
where π π =
ππ π π ,
(3.1)
(3.2)
(3.3)
π, π : π+ π=π
the zero of the ring is (0, 0, . . .), and the multiplicative identity is (1, 0, 0, . . .).
Of course, we almost always write (π 0 , π 1 , π 2 , . . .) as π 0 + π 1 π‘ + π 2 π‘ 2 + · · · , or
the same with some other symbol in place of π‘. In that notation, formulas (3.1)
and (3.2) look like the usual formulas for addition and multiplication of polynomials. Nevertheless:
Warning 3.1.2 A polynomial is not a function!
A polynomial gives rise to a function, as we’ll recall in a moment. But
a polynomial itself is a purely formal object. To emphasize this, we
sometimes call the symbol π‘ an indeterminate rather than a ‘variable’.
34
Why study
polynomials?
The set of polynomials over π
is written as π
[π‘] (or π
[π’], π
[π₯], etc.). Since
π
[π‘] is itself a ring π, we can consider the ring π[π’] = (π
[π‘]) [π’], usually written
as π
[π‘, π’]. And then there’s π
[π‘, π’, π£] = (π
[π‘, π’]) [π£], and so on.
Polynomials are typically written as either π or π (π‘), interchangeably. A
polynomial π = (π 0 , π 1 , . . .) over π
gives rise to a function
π
→
π
π β¦→ π 0 + π 1π + π 2π 2 + · · · .
(The sum on the right-hand side makes sense because only finitely many ππ s are
nonzero.) This function is usually denoted by π too. But calling it that is slightly
dangerous, because:
Warning 3.1.3 Different polynomials can give rise to the same function. For example, consider π‘, π‘ 2 ∈ F2 [π‘]. They are different polynomials: going back to Definition 3.1.1, they’re alternative notation for
the sequences
(0, 1, 0, 0, . . .)
and
(0, 0, 1, 0, . . .),
which are plainly not the same. On the other hand, they induce the
same function F2 → F2 , because π = π 2 for all (both) π ∈ F2 .
Exercise 3.1.4 Show that whenever π
is a finite nontrivial ring, it is
possible to find distinct polynomials over π
that induce the same function π
→ π
. (Hint: are there finitely or infinitely many polynomials
over π
? Functions π
→ π
?)
Remark 3.1.5 In Example 2.3.2, we met the field πΎ (π‘) of rational expressions over
a field πΎ. People sometimes say ‘rational function’ to mean ‘rational expression’.
But just as for polynomials, I want to emphasize that rational expressions are not
functions. For instance, 1/(π‘ − 1) is a totally respectable element of πΎ (π‘). You
don’t have to worry about what happens ‘when π‘ = 1’, because π‘ is just a formal
symbol (a mark on a piece of paper), not a variable. And 1/(π‘ − 1) is just a formal
expression, not a function.
The ring of polynomials has a universal property: a homomorphism from π
[π‘]
to some other ring π΅ is determined by its effect on scalars and on π‘ itself, in the
following sense.
The universal
property of π
[π‘]
35
Proposition 3.1.6 (Universal property of the polynomial ring) Let π
and π΅ be
rings. For every homomorphism π : π
→ π΅ and every π ∈ π΅, there is exactly one
homomorphism π : π
[π‘] → π΅ such that
π (π) = π(π)
π (π‘) = π.
for all π ∈ π
,
(3.4)
(3.5)
On the left-hand side of (3.4), the ‘π’ means the polynomial π + 0π‘ + 0π‘ 2 + · · · .
Proof To show there is at most one such π, take any homomorphism π : π
[π‘] → π΅
Í
satisfying (3.4) and (3.5). Then for every polynomial π ππ π‘ π over π
,
∑οΈ
∑οΈ
ππ π‘ π =
π (ππ )π (π‘) π
since π is a homomorphism
π
π
=
π
∑οΈ
π(ππ )ππ
by (3.4) and (3.5).
π
So π is uniquely determined.
To show there is at least one such π, define a function π : π
[π‘] → π΅ by
∑οΈ
∑οΈ
π(ππ )ππ
π
ππ π‘ π =
π
π
Í
( π ππ π‘ π ∈ π
[π‘]). Then π clearly satisfies conditions (3.4) and (3.5). It remains to
check that π is a homomorphism. I will do the worst part of this, which is to check
that π preserves multiplication, and leave the rest to you.
Í
Í
So, take polynomials π (π‘) = π ππ π‘ π and π(π‘) = π π π π‘ π . Then π (π‘)π(π‘) =
Í
π
π π π π‘ , where π π is as defined in equation (3.3). We have
∑οΈ
π ( π π) = π
ππ π‘ π
∑οΈ π
=
π(π π )π π
by definition of π
π
=
∑οΈ ∑οΈ
π
ππ π π π π
π
π, π : π+ π=π
=
∑οΈ
∑οΈ
by definition of π π
π(ππ )π(π π )π π
since π is a homomorphism
π π, π : π+ π=π
=
∑οΈ
=
∑οΈ
π(ππ )π(π π )ππ+ π
π, π
π(ππ )ππ
π
∑οΈ
π(π π )π π
π
= π ( π )π (π)
by definition of π.
36
β‘
Here are three uses for the universal property of the ring of polynomials. First:
Definition 3.1.7 Let π : π
→ π be a ring homomorphism. The induced homomorphism
π∗ : π
[π‘] → π[π‘]
is the unique homomorphism π
[π‘] → π[π‘] such that π∗ (π) = π(π) for all π ∈ π
and π∗ (π‘) = π‘.
The universal property guarantees that there is one and only one homomorphism π∗ with these properties. Concretely,
∑οΈ
∑οΈ
π
ππ π‘ =
π(ππ )π‘ π
π∗
π
π
Í
for all π ππ π‘ π ∈ π
[π‘].
Second, let π
be a ring and π ∈ π
. By the universal property, there is a unique
homomorphism evπ : π
[π‘] → π
such that evπ (π) = π for all π ∈ π
and evπ (π‘) = π.
Concretely,
∑οΈ
∑οΈ
evπ
ππ π‘ π =
ππ π π
π
π
Í
for all π ππ π‘ π ∈ π
[π‘]. This map evπ is called evaluation at π.
Í
(The notation ππ π‘ π for what is officially (π 0 , π 1 , . . .) makes it look obvious that
we can evaluate a polynomial at an element, and that this gives a homomorphism:
of course ( π · π)(π) = π (π)π(π), for instance! But that’s only because of the
notation: there was actually something to prove here.)
Third, let π
be a ring and π ∈ π
. For any π (π‘) ∈ π
[π‘], we can ‘substitute
π‘ = π’ + π’ to get a polynomial in π’. What exactly does this mean? Formally, there
is a unique homomorphism π : π
[π‘] → π
[π’] such that π (π) = π for all π ∈ π
and
π (π‘) = π’ + π. Concretely,
∑οΈ
∑οΈ
π
ππ (π’ + π) π .
π
ππ π‘ =
π
π
This particular substitution is invertible. Informally, the inverse is ‘substitute
π’ = π‘ − π’. Formally, there is a unique homomorphism π ′ : π
[π’] → π
[π‘] such that
π ′ (π) = π for all π ∈ π
and π ′ (π’) = π‘ − π. These maps π and π ′ carrying out the
substitutions are inverse to each other, as you can deduce from either the universal
property or the concrete descriptions. So, the substitution maps
π
[π‘] o
π
π′
37
/
π
[π’]
(3.6)
define an isomorphism between π
[π‘] and π
[π’]. For example, since isomorphism
preserve irreducibility (and everything else that matters!), π (π‘) is irreducible if
and only if π (π‘ − π) is irreducible.
Exercise 3.1.8 What happens to everything in the previous paragraph
if we substitute π‘ = π’ 2 + π instead?
The rest of this section is about degree.
Í
Definition 3.1.9 The degree, deg( π ), of a nonzero polynomial π (π‘) = ππ π‘ π is
the largest π ≥ 0 such that π π ≠ 0. By convention, deg(0) = −∞, where −∞ is a
formal symbol which we give the properties
−∞ < π,
(−∞) + π = −∞,
(−∞) + (−∞) = −∞
for all integers π.
Digression 3.1.10 Defining deg(0) like this is helpful because it allows us
to make statements about all polynomials without annoying exceptions for
the zero polynomial (e.g. Lemma 3.1.11(i)).
But putting deg(0) = −∞ also makes intuitive sense. At least for polynomials
over R, the degree of a nonzero polynomial tells us how fast it grows: when π₯
is large, π (π₯) behaves roughly like π₯ deg( π ) . What about the zero polynomial?
Well, whether or not π₯ is large, 0(π₯) = 0. And π₯ −∞ can sensibly be interpreted
as limπ→−∞ π₯ π = 0, so it makes sense to put deg(0) = −∞.
Lemma 3.1.11 Let π
be an integral domain. Then:
i. deg( π π) = deg( π ) + deg(π) for all π , π ∈ π
[π‘];
ii. π
[π‘] is an integral domain.
Proof This was proved in Honours Algebra (Section 3.3).
β‘
Example 3.1.12 For any integral domain π
, the ring π
[π‘1 , . . . , π‘ π ] of polynomials
over π
in π variables is also an integral domain, by Lemma 3.1.11(ii) and induction.
In particular, this is true when π
is a field.
Exercise 3.1.13 Let π be a prime and consider the field F π (π‘) of
rational expressions over F π . Show that π‘ has no πth root in F π (π‘).
(Hint: consider degrees of polynomials.)
The one and only polynomial of degree −∞ is the zero polynomial. The
polynomials of degree 0 are the nonzero constants. The polynomials of degree
> 0 are, therefore, the nonconstant polynomials.
38
Lemma 3.1.14 Let πΎ be a field. Then:
i. the units in πΎ [π‘] are the nonzero constants;
ii. π ∈ πΎ [π‘] is irreducible if and only if π is nonconstant and cannot be
expressed as a product of two nonconstant polynomials.
Proof Part (i) was also in Honours Algebra (Section 3.3), and part (ii) follows
from the general definition of irreducible element of a ring.
β‘
3.2
Factorizing polynomials
Every nonzero integer can be expressed as a product of primes in an essentially
unique way. But the analogous statement is not true in all rings, or even all
integral domains. Some rings have elements that can’t be expressed as a product
of irreducibles at all. In other rings, factorizations into irreducibles exist but are
not unique. (By ‘not unique’ I mean more than just changing the order of the
factors or multiplying them by units.)
The big theorem of this section is that, happily, every polynomial over a field
can be factorized into irreducibles, essentially uniquely.
We begin with a result on division of polynomials from Section 3.3 of Honours
Algebra.
Proposition 3.2.1 Let πΎ be a field and π , π ∈ πΎ [π‘] with π ≠ 0. Then there is
exactly one pair of polynomials π, π ∈ πΎ [π‘] such that π = ππ + π and deg(π) <
deg(π).
β‘
We use this to prove an extremely useful fact:
Proposition 3.2.2 Let πΎ be a field. Then πΎ [π‘] is a principal ideal domain.
Proof First, πΎ [π‘] is an integral domain, by Lemma 3.1.11(ii).
Now let πΌ P πΎ [π‘]. If πΌ = {0} then πΌ = β¨0β©. Otherwise, put π = min{deg( π ) :
0 ≠ π ∈ πΌ} and choose π ∈ πΌ such that deg(π) = π.
I claim that πΌ = β¨πβ©. To prove this, let π ∈ πΌ; we must show that π | π .
By Proposition 3.2.1, π = ππ + π for some π, π ∈ πΎ [π‘] with deg(π) < π. Now
π = π − ππ ∈ πΌ since π , π ∈ πΌ, so the minimality of π implies that π = 0. Hence
π = ππ, as required.
β‘
If you struggled with Exercise 2.2.14, that proof should give you a clue.
39
Warning 3.2.3 We just saw that πΎ [π‘] is a principal ideal domain, and
we saw in Example 3.1.12 that πΎ [π‘1 , . . . , π‘ π ] is an integral domain.
But it is not a principal ideal domain if π > 1. For example, the ideal
β¨π‘1 , π‘2 β© = { π (π‘ 1 , π‘2 ) ∈ Q[π‘ 1 , π‘2 ] : π has constant term 0}
of Q[π‘ 1 , π‘2 ] is not principal.
Also, Proposition 3.2.2 really needed the hypothesis that πΎ is a field;
it’s not enough for it to be a principal ideal domain. For example, Z is
a principal ideal domain, but in Z[π‘], the ideal
β¨2, π‘β© = { π (π‘) ∈ Z[π‘] : the constant term of π is even}
is not principal.
Exercise 3.2.4 Prove that the ideals in Warning 3.2.3 are indeed not
principal.
Exercise 3.2.4: a
non-principal ideal
At the end of Chapter 2, I promised I’d give you a way of manufacturing lots
of new fields. Here it is!
Corollary 3.2.5 Let πΎ be a field and let 0 ≠ π ∈ πΎ [π‘]. Then
π is irreducible ⇐⇒ πΎ [π‘]/β¨ π β© is a field.
Proof This follows from Propositions 2.3.26 and 3.2.2.
β‘
To make new fields using Corollary 3.2.5, we’ll need a way of knowing which
polynomials are irreducible. That’s the topic of Section 3.3. But for now, let’s
stick to our mission: proving that every polynomial factorizes into irreducibles in
an essentially unique way.
To achieve our mission, we’ll need two more lemmas.
Lemma 3.2.6 Let πΎ be a field and let π (π‘) ∈ πΎ [π‘] be a nonconstant polynomial.
Then π (π‘) is divisible by some irreducible in πΎ [π‘].
Proof Let π be a nonconstant polynomial of smallest possible degree such that
π | π . (For this to make sense, there must be at least one nonconstant polynomial
dividing π , and there is: π .) I claim that π is irreducible. Proof: if π = π1 π2 then
each ππ divides π , so by minimality of deg(π), each ππ has degree 0 or deg(π).
They cannot both have degree deg(π), since deg(π1 ) + deg(π2 ) = deg(π) > 0. So
at least one has degree 0, which by Lemma 3.1.14(i) means that it is a unit.
β‘
40
Lemma 3.2.7 Let πΎ be a field and π , π, β ∈ πΎ [π‘]. Suppose that π is irreducible
and π | πβ. Then π | π or π | β.
This behaviour is familiar in the integers: if a prime π divides some product
ππ, then π | π or π | π. In fact, our proof works in any principal ideal domain.
Proof Suppose that π β€ π. Since π is irreducible, π and π are coprime. Since πΎ [π‘]
is a principal ideal domain, Proposition 2.2.16 implies that there are π, π ∈ πΎ [π‘]
satisfying
π π + ππ = 1.
Multiplying both sides by β gives
π π β + ππβ = β.
But π | π π β and π | πβ, so π | β.
β‘
Theorem 3.2.8 Let πΎ be a field and 0 ≠ π ∈ πΎ [π‘]. Then
π = π π1 π2 · · · π π
for some π ≥ 0, π ∈ πΎ and monic irreducibles π1 , . . . , ππ ∈ πΎ [π‘]. Moreover, π
and π are uniquely determined by π , and π1 , . . . , ππ are uniquely determined
up to reordering.
In the case π = 0, the product π1 · · · ππ should be interpreted as 1 (as in
Digression 2.2.10). Monic means that the leading coefficient is 1.
Proof First we prove that such a factorization exists, by induction on deg( π ). If
deg( π ) = 0 then π is a constant π and we take π = 0. Now suppose that deg( π ) > 0
and assume the result for polynomials of smaller degree. By Lemma 3.2.6, there
is an irreducible π dividing π , and we can assume that π is monic by dividing by
a constant if necessary. Then π /π is a nonzero polynomial of smaller degree than
π , so by inductive hypothesis,
π /π = πβ1 · · · βπ
for some π ∈ πΎ and monic irreducibles β1 , . . . , βπ . Rearranging gives
π = πβ1 · · · βπ π,
completing the induction.
41
Now we prove uniqueness, again by induction on deg( π ). If deg( π ) = 0 then
π is a constant π and the only possible factorization is the one with π = 0. Now
suppose that deg( π ) > 0, and take two factorizations
π π1 · · · ππ = π = ππ1 · · · ππ
(3.7)
where π, π ∈ πΎ and ππ , π π are monic irreducible. Since deg( π ) > 0, we have
π, π ≥ 1. Now ππ | ππ1 · · · ππ , so by Lemma 3.2.7, ππ | π π for some π. By
rearranging, we can assume that π = π. But ππ is also irreducible, so ππ = πππ
for some nonzero π ∈ πΎ, and both ππ and ππ are monic, so π = 1. Hence ππ = ππ .
Cancelling in (3.7) (which we can do as πΎ [π‘] is an integral domain) gives
π π1 · · · ππ−1 = ππ1 · · · ππ−1 .
By inductive hypothesis, π − 1 = π − 1, π = π, and the lists π1 , . . . , ππ−1 and
π1 , . . . , ππ−1 are the same up to reordering. This completes the induction.
β‘
One way to find an irreducible factor of a polynomial π (π‘) ∈ πΎ [π‘] is to find a
root (an element π ∈ πΎ such that π (π) = 0):
Lemma 3.2.9 Let πΎ be a field, π (π‘) ∈ πΎ [π‘] and π ∈ πΎ. Then
π (π) = 0 ⇐⇒ (π‘ − π) | π (π‘).
Proof ⇒: suppose that π (π) = 0. By Proposition 3.2.1,
π (π‘) = (π‘ − π)π(π‘) + π (π‘)
(3.8)
for some π, π ∈ πΎ [π‘] with deg(π) < 1. Then π is a constant, so putting π‘ = π
in (3.8) gives π = 0.
⇐: if π (π‘) = (π‘ − π)π(π‘) for some polynomial π then π (π) = 0.
β‘
A field is algebraically closed if every nonconstant polynomial has at least one
root. For example, C is algebraically closed (the fundamental theorem of algebra).
A straightforward induction shows:
Lemma 3.2.10 Let πΎ be an algebraically closed field and 0 ≠ π ∈ πΎ [π‘]. Then
π (π‘) = π(π‘ − π 1 ) π1 · · · (π‘ − π π ) π π ,
where π is the leading coefficient of π , and π 1 , . . . , π π are the distinct roots of π in
πΎ, and π 1 , . . . , π π ≥ 1.
β‘
42
3.3
Irreducible polynomials
Determining whether an integer is prime is generally hard, so it’s no surprise that
determining whether a polynomial is irreducible is hard too. This section presents
a few techniques for doing so.
Let’s begin with the simplest cases. Recall Lemma 3.1.14(ii): a polynomial
over a field is irreducible if and only if it is nonconstant (has degree > 0) and
cannot be expressed as a product of two nonconstant polynomials.
Lemma 3.3.1 Let πΎ be a field and π ∈ πΎ [π‘].
i. If π is constant then π is not irreducible.
ii. If deg( π ) = 1 then π is irreducible.
iii. If deg( π ) ≥ 2 and π has a root then π is reducible.
iv. If deg( π ) ∈ {2, 3} and π has no root then π is irreducible.
Proof Parts (i) and (ii) follow from what we just recalled, and (iii) follows
from Lemma 3.2.9. For (iv), suppose for a contradiction that π = πβ with
deg(π), deg(β) ≥ 1. We have deg(π) + deg(β) ∈ {2, 3}, so without loss of generality, deg(π) = 1. Also without loss of generality, π is monic, say π(π‘) = π‘ + π; but
then π (−π) = 0, a contradiction.
β‘
Warning 3.3.2 To show a polynomial is irreducible, it’s generally
not enough to show it has no root. The converse of (iii) is false! For
instance, (π‘ 2 + 1) 2 ∈ Q[π‘] has no root but is reducible.
Warning 3.3.3 Make sure you’ve digested Warning 3.3.2!
This is an extremely common mistake.
Examples 3.3.4
i. Let π be a prime. Then π (π‘) = 1 + π‘ + · · · + π‘ π−1 ∈ F π [π‘] is
reducible, since π (1) = 0.
ii. Let π (π‘) = π‘ 3 − 10 ∈ Q[π‘]. Then deg( π ) = 3 and π has no root in Q, so π is
irreducible by part (iv) of the lemma.
iii. Over C or any other algebraically closed field, the irreducibles are exactly
the polynomials of degree 1.
43
Exercise 3.3.5 If I gave you a quadratic over Q, how would you decide
whether it was reducible or irreducible?
From now on we focus on πΎ = Q. Any polynomial over Q can be multiplied
by a nonzero integer to get a polynomial over Z, and that’s often a helpful move,
so we’ll look at Z[π‘] too.
Definition 3.3.6 A polynomial over Z is primitive if its coefficients have no
common divisor except for ±1.
For example, 15 + 6π‘ + 10π‘ 2 is primitive but 15 + 6π‘ + 30π‘ 2 is not.
Lemma 3.3.7 Let π (π‘) ∈ Q[π‘]. Then there exist a primitive polynomial πΉ (π‘) ∈
Z[π‘] and πΌ ∈ Q such that π = πΌπΉ.
Í
Proof Write π (π‘) = π (ππ /ππ )π‘ π , where ππ ∈ Z and 0 ≠ ππ ∈ Z. Take any common
Í
multiple π of the ππ s; then writing ππ = ππ π/ππ ∈ Z, we have π (π‘) = (1/π) ππ π‘ π .
Now let π be the greatest common divisor of the ππ s, put ππ = ππ /π ∈ Z, and put
Í
πΉ (π‘) = ππ π‘ π . Then πΉ (π‘) is primitive and π (π‘) = (π/π)πΉ (π‘).
β‘
If the coefficients of a polynomial π (π‘) ∈ Q[π‘] happen to all be integers, the
word ‘irreducible’ could mean two things: irreducibility in the ring Q[π‘] or in the
ring Z[π‘]. We say that π is irreducible over Q or Z to distinguish between the two.
Suppose we have a polynomial over Z that’s irreducible over Z. In principle it
could still be reducible over Q: although there’s no nontrivial way of factorizing
it over Z, perhaps it can be factorized when you give yourself the freedom of
non-integer coefficients. But the next result tells us that you can’t.
Lemma 3.3.8 (Gauss)
primitive.
i. The product of two primitive polynomials over Z is
ii. If a nonconstant polynomial over Z is irreducible over Z, it is irreducible
over Q.
Proof For (i), let π and π be primitive polynomials over Z. Let π be a prime
number. (We’re going to show that π doesn’t divide all the coefficients of π π.)
Write π : Z → Z/πZ = F π for the canonical homomorphism, which induces a
homomorphism π∗ : Z[π‘] → F π [π‘] as in Definition 3.1.7.
Since π is primitive, π does not divide all the coefficients of π . Equivalently,
π∗ ( π ) ≠ 0. Similarly, π∗ (π) ≠ 0. But F π [π‘] is an integral domain, so
π∗ ( π π) = π∗ ( π )π∗ (π) ≠ 0,
44
so π does not divide all the coefficients of π π. This holds for all primes π, so π π
is primitive.
For (ii), let π ∈ Z[π‘] be a nonconstant polynomial irreducible over Z. Let
π, β ∈ Q[π‘] with π = πβ. By Lemma 3.3.7, π = πΌπΊ and β = π½π» for some
πΌ, π½ ∈ Q and primitive πΊ, π» ∈ Z[π‘]. Then πΌπ½ = π/π for some coprime integers
π and π, giving
π π = ππΊπ».
(All three of these polynomials are over Z.) Now π divides every coefficient of
π π , hence every coefficient of ππΊπ». Since π and π are coprime, π divides every
coefficient of πΊπ». But πΊπ» is primitive by (i), so π = ±1, so π = ±ππΊπ». Since π
is irreducible over Z, either πΊ or π» is constant, so π or β is constant, as required.β‘
Gauss’s lemma quickly leads to a test for irreducibility. It involves taking a
polynomial over Z and reducing it mod π, for some prime π. This means applying
the map π∗ : Z[π‘] → F π [π‘] from the last proof. As we saw after Definition 3.1.7,
Í
Í
if π (π‘) = ππ π‘ π then π∗ ( π )(π‘) = π(ππ )π‘ π , where π(ππ ) is the congruence class of
ππ mod π. I’ll write π(π) as π and π∗ ( π ) as π . That is, π is ‘ π mod π’.
Proposition 3.3.9 (Mod π method) Let π (π‘) = π 0 + π 1 π‘ + · · · + π π π‘ π ∈ Z[π‘]. If
there is some prime π such that π β€ π π and π ∈ F π [π‘] is irreducible, then π is
irreducible over Q.
I’ll give some examples first, then the proof.
Examples 3.3.10
i. Let’s use the mod π method to show that π (π‘) = 9 + 14π‘ −
3
8π‘ is irreducible over Q. Take π = 7: then π (π‘) = 2 − π‘ 3 ∈ F7 [π‘], so it’s
enough to show that 2 − π‘ 3 is irreducible over F7 . Since this has degree 3, it’s
enough to show that π‘ 3 = 2 has no solution in F7 (by Lemma 3.3.1(iv)). And
you can easily check this by computing 03 , (±1) 3 , (±2) 3 and (±3) 3 mod 7.
ii. The condition in Proposition 3.3.9 that π β€ π π can’t be dropped. For instance,
consider π (π‘) = 6π‘ 2 + π‘ and π = 2.
Warning 3.3.11 Take π (π‘) as in Example 3.3.10(i), but this time take
π = 3. Then π (π‘) = −π‘ + π‘ 3 ∈ F3 [π‘], which is reducible. But that
doesn’t mean π is reducible! The mod π method only ever lets you
show that a polynomial is irreducible over Q, not reducible.
Proof of Proposition 3.3.9 Take a prime π satisfying the stated conditions.
First suppose that π is primitive. By Gauss’s lemma, it is enough to prove that
π is irreducible over Z.
45
Since π is irreducible, deg( π ) > 0, so deg( π ) > 0.
Let π = πβ in Z[π‘]. We have π = πβ and π is irreducible, so without loss of
generality, π is constant. The leading coefficient of π is the product of the leading
coefficients of π and β, and is not divisible by π, so the leading coefficient of π is
not divisible by π. Hence deg(π) = deg(π). But deg(π) = 0, so deg(π) = 0, so
π ∈ Z[π‘] is a constant π ∈ Z. Finally, π = πβ = πβ and π is primitive, so π = ±1,
which is a unit in Z[π‘]. It follows that π is irreducible over Z.
Now take an arbitrary π satisfying the hypotheses. We have π = ππΉ where
π ∈ Z is the greatest common divisor of the coefficients and πΉ ∈ Z[π‘] is primitive.
Then π = ππΉ, and π is a unit in F π because π β€ π. Since π is irreducible, this
implies that πΉ is irreducible, and so by what we’ve just proved, πΉ is irreducible
over Q. But π ≠ 0, so π is a unit in Q, so π = ππΉ is also irreducible over Q.
β‘
We finish with an irreducibility test that turns out to be surprisingly powerful.
Not Einstein.
Proposition 3.3.12 (Eisenstein’s criterion) Let π (π‘) = π 0 + · · · + π π π‘ π ∈ Z[π‘],
with π ≥ 1. Suppose there exists a prime π such that:
• π β€ ππ;
• π | ππ for all π ∈ {0, . . . , π − 1};
• π2 β€ π0.
Then π is irreducible over Q.
To prove this, we will use the concept of the codegree codeg( π ) of a polynomial
Í
π (π‘) = π ππ π‘ π , which is defined to be the least π such that ππ ≠ 0 (if π ≠ 0), or as
the formal symbol ∞ if π = 0. For polynomials π and π over an integral domain,
codeg( π π) = codeg( π ) + codeg(π).
Clearly codeg( π ) ≤ deg( π ) unless π = 0.
Proof We may assume π is primitive: if not, divide π through by the greatest
common divisor of its coefficients, which does not affect their divisibility by
powers of π or the reducibility of π over Q. By Gauss’s lemma, it is enough to
show that π is irreducible over Z. Let π, β ∈ Z[π‘] with π = πβ. Continue to write
π (π‘) ∈ F π [π‘] for π reduced mod π; then π = πβ. Since
π 2 β€ π 0 = π (0) = π(0)β(0),
we may assume without loss of generality that π β€ π(0). Hence codeg(π) = 0.
Also, codeg( π ) = π, since π divides each of π 0 , . . . , π π−1 but not π π . So
π = codeg( π ) = codeg(π) + codeg(β) = codeg(β) ≤ deg(β) ≤ deg(β),
46
(3.9)
giving π ≤ deg(β). But π = πβ with deg( π ) = π, so deg(β) = π and deg(π) = 0.
Hence π is constant. Since π is primitive, π = ±1, so π is a unit in Z[π‘].
β‘
Exercise 3.3.13 The last step in (3.9) was ‘deg(β) ≤ deg(β)’. Why
is that true? And when does equality hold?
Example 3.3.14 Let
2
5
1
π(π‘) = π‘ 5 − π‘ 4 + π‘ 3 + ∈ Q[π‘].
9
3
3
Then π is irreducible over Q if and only if
9π(π‘) = 2π‘ 5 − 15π‘ 4 + 9π‘ 3 + 3
Testing for
irreducibility
is irreducible over Q, which it is by Eisenstein’s criterion with π = 3.
Exercise 3.3.15 Use Eisenstein’s criterion to show that for every
π ≥ 1, there is an irreducible polynomial over Q of degree π.
I’ll give you one more example, and it’s an important one.
Example 3.3.16 Let π be a prime. The πth cyclotomic polynomial is
Φ π (π‘) = 1 + π‘ + · · · + π‘ π−1 =
π‘π − 1
.
π‘−1
(3.10)
I claim that Φ π is irreducible. We can’t apply Eisenstein to Φ π as it stands, because
whichever prime we choose (whether it’s π or another one) doesn’t divide any of
the coefficients. However, we saw on p. 38 that Φ π (π‘) is irreducible if and only if
Φ π (π‘ − π) is irreducible, for any π ∈ Q. We’ll take π = −1. We have
(π‘ + 1) π − 1
(π‘ + 1) − 1
π 1 ∑οΈ π π
=
π‘
π‘ π=1 π
π
π
π‘ π−2 + π‘ π−1 .
= π+
π‘ +···+
π−1
2
Φ π (π‘ + 1) =
So Φ π (π‘ + 1) is irreducible by Eisenstein’s criterion and Lemma 2.3.19, hence
Φ π (π‘) is irreducible too.
47
Digression 3.3.17 I defined the πth cyclotomic polynomial Φ π only when
π is prime. The definition of Φπ for general π ≥ 1 is not the obvious
generalization of (3.10). Instead, it’s this:
Ö
Φπ (π‘) =
(π‘ − π),
π
where the product runs over all primitive πth roots of unity π. (In this
context, ‘primitive’ means that π is the smallest number satisfying π π = 1;
it’s a different usage from ‘primitive polynomial’.)
Many surprising things are true. It’s not obvious that the coefficients of Φπ
are real, but they are. Even given that they’re real, it’s not obvious that they’re
rational, but they are. Even given that they’re rational, it’s not obvious that
they’re integers, but they are (Workshop 4, question 14). The degree of Φπ
is π(π), the number of integers between 1 and π that are coprime with π
(Euler’s function). It’s also true that the polynomial Φπ is irreducible for all
π, not just primes.
Some of these things are quite hard to prove, and results from Galois theory
help. We won’t get into all of this, but you can read more here.
48
Chapter 4
Field extensions
Introduction to
Week 4
Roughly speaking, an ‘extension’ of a field πΎ is a field π that contains πΎ as a
subfield. It’s not much of an exaggeration to say that field extensions are the central
objects of Galois theory, in much the same way that vector spaces are the central
objects of linear algebra.
It will be a while before it becomes truly clear why field extensions are so
important, but here are a couple of indications:
• For any polynomial π over Q, we can take the smallest subfield π of C that
contains all the complex roots of π , and that’s an extension of Q.
• For any irreducible polynomial π over a field πΎ, the quotient ring π =
πΎ [π‘]/β¨ π β© is a field. The constant polynomials form a subfield of π isomorphic to πΎ, so π is an extension of πΎ.
It’s important to distinguish between these two types of example. The first extends
Q by all the roots of π , whereas the second extends πΎ by just one root of π —as
we’ll see.
4.1
Definition and examples
Before we do anything else, we need to think about some set theory. What follows
might seem trivial, but it’s worth taking the time to get it straight.
Given a set π΄ and a subset π΅ ⊆ π΄, there is an inclusion function π : π΅ → π΄
defined by π(π) = π for all π ∈ π΅. (That’s a Greek letter iota.) Remember that by
definition, every function has a specified domain and codomain, so this is not the
same as the identity on π΅. The inclusion π is injective.
On the other hand, given any injective function between sets, say π : π → π΄,
the image im π is a subset of π΄, and there is a bΔ³ection π′ : π → im π given by
49
π′ (π₯) = π(π₯) (π₯ ∈ π). Hence the set π is isomorphic to (in bΔ³ection with) the
subset im π of π΄.
So given any subset of π΄, we get an injection into π΄, and vice versa. These
two back-and-forth processes are mutually inverse (up to isomorphism), so subsets
and injections are more or less the same thing.
Now here’s an example to show you that the concept of subset is not as clearcut as it might seem—at least when you look at what mathematicians actually do,
rather than what we claim we do.
• It’s common to define the set C as R2 .
• Everyone treats R as a subset of C.
• But almost no one would say that R is a subset of R2 . (If you think it is, and
you agree that R has an element called 6, then you must think that R2 has an
element called 6—which you probably don’t.)
So, is R a subset of C or not? In truth, while we almost always ‘know what we
mean’, the common conventions are inconsistent.
Probably you’re thinking that this all seems rather distant from ‘real mathematics’. Nothing important should depend on whether R is literally a subset of C.
I agree! But the challenge is to set up the formal definitions so that we never have
to worry about irrelevant-seeming questions like this again. And the solution is to
work with injections rather than subsets.
So: we intuitively want to define an ‘extension’ of a field πΎ as a field π that
contains πΎ as a subfield. But if we defined it that way, we’d run into the annoying
question of whether C really is an extension of R. So instead, we define an
extension of πΎ to be a field π together with an injective homomorphism πΎ → π.
Lemma 2.3.3 tells us that every homomorphism between fields is injective, so our
actual definition is as follows.
Definition 4.1.1 Let πΎ be a field. An extension of πΎ is a field π together with a
homomorphism π : πΎ → π.
Often we blur the distinction between injections and subsets, speaking as if πΎ
is literally a subfield of π and π is the inclusion. We then write π : πΎ (read ‘π
over πΎ’) to mean that π is an extension of πΎ, not bothering to mention π.
Examples 4.1.2
i. The field C, together with the inclusion π : Q → C, is an
extension of Q. We write it as C : Q. Similarly, there are field extensions
C : R and R : Q.
50
ii. Let
√
√
Q( 2) = {π + π 2 : π, π ∈ Q}.
√
Then Q( 2) is a subring of C (easily), and in fact it’s a subfield: for if
(π, π) ≠ (0, 0) then
√
π−π 2
1
√ =
π + π 2 π 2 − 2π 2
√
(noting that the denominators
are not 0 because 2 √
is irrational). So we
√
have an extension
√ C : Q( 2). Also, because Q ⊆ Q( 2), we have another
extension Q( 2) : Q.
iii. Write
√
√
√
Q( 2, π) = {π + π 2 + ππ + π 2π : π, π, π, π ∈ Q.}
By√direct calculation or later theory (which will make it much
√ easier),
Q( √2, π) is also a subfield of C, so we have extensions C : Q( 2, π) and
Q( 2, π) : Q.
iv. Let πΎ be a field, and consider the field πΎ (π‘) of rational expressions over
πΎ (Example 2.3.2). There is a homomorphism π : πΎ → πΎ (π‘) given by
π(π) = π/1 (π ∈ πΎ). In other words, πΎ (π‘) contains a copy of πΎ as the
constant rational expressions. So, we have a field extension πΎ (π‘) : πΎ.
v. There is a homomorphism π
: C → C defined by π
(π§) = π§. So C together
with π
is an extension of C! You might feel that this example obeys the letter
but not the spirit of Definition 4.1.1, but it is an example.
Exercise
4.1.3 Find two examples of fields πΎ such that Q β« πΎ β«
√
Q( 2, π). (The symbol β« means proper subset.)
Sometimes we fix a field πΎ and think about fields that contain it—extensions
of πΎ. Other times, we fix a field πΎ and think about fields it contains—subfields of
πΎ. It may be that we are given a mere subset π of πΎ and want to generate a subfield
from it. Recalling the top-down/bottom-up distinction of Digression 2.2.12, we
define this as follows.
Definition 4.1.4 Let πΎ be a field and π a subset of πΎ. The subfield of πΎ generated
by π is the intersection of all the subfields of πΎ containing π.
Let πΉ be the subfield of πΎ generated by π. Since any intersection of subfields is
a subfield, πΉ really is a subfield of πΎ. It contains π. By definition of intersection,
πΉ is the smallest subfield of πΎ containing π, in the sense that any subfield of πΎ
containing π contains πΉ.
51
Exercise 4.1.5 Check the truth of all the statements in the previous
paragraph.
Examples 4.1.6
of πΎ.
i. The subfield of πΎ generated by ∅ is the prime subfield
ii. Let πΏ be the subfield of C generated by {π}. I claim that
πΏ = {π + ππ : π, π ∈ Q}.
To prove this, we have to show that πΏ is the smallest subfield of C containing
π. First, it is a subfield of C (by an argument similar to Example 4.1.2(ii))
and it contains 0 + 1π = π. Now let πΏ ′ be any subfield of C containing π. Then
πΏ ′ contains the prime subfield of C (by definition of prime subfield), which
is Q. So whenever π, π ∈ Q, we have π, π, π ∈ πΏ ′ and so π + ππ ∈ πΏ ′. Hence
πΏ ⊆ πΏ ′, as required.
√
iii. A very similar argument shows
√ that the subfield of C generated by 2 is
what we have been calling Q( 2).
Exercise 4.1.7 What is the subfield of C generated by {7/8}? By
{2 + 3π}? By R ∪ {π}?
We will be very interested in chains of fields
πΎ⊆πΏ⊆π
in which πΎ and π are regarded as fixed and πΏ as variable. You can think of πΎ as
the floor, π as the ceiling, and πΏ as varying in between.
Definition 4.1.8 Let π : πΎ be a field extension and π ⊆ π. We write πΎ (π ) for
the subfield of π generated by πΎ ∪π . We call it πΎ with π adjoined, or the subfield
of π generated by π over πΎ.
So, πΎ (π ) is the smallest subfield of π containing both πΎ and π .
When π is a finite set {πΌ1 , . . . , πΌπ }, we write πΎ ({πΌ1 , . . . , πΌπ }) as
πΎ (πΌ1 , . . . , πΌπ ).
√
Examples 4.1.9
i. Take π : πΎ to be C : Q and π =
√ { 2}. By definition,
πΎ (π ) is the smallest subfield of C containing Q ∪ { 2}. But every subfield
of C contains Q: that’s what it means for Q to be
√ the prime subfield of C.
So, πΎ (π ) is the smallest subfield of C containing
2. By Example 4.1.6(iii),
√
√
that’s exactly
what
we’ve
been
calling
Q(
2)
all
along.
We
refer
to
Q(
2)
√
as ‘Q with 2 adjoined’.
52
ii. Similarly, Q with π adjoined is
Q(π) = {π + ππ : π, π ∈ Q}
√
(Example
4.1.6(ii)), and Q with { 2, π} adjoined is the subfield denoted by
√
Q( 2, π) in Example 4.1.2(iii).
iii. Let π be a field and π ⊆ π. Write πΎ for the prime subfield of π. Then
πΎ (π) is the smallest subfield of π containing πΎ and π. But every subfield
of π contains πΎ, by definition of prime subfield. So πΎ (π) is the smallest
subfield of π containing π; that is, it’s the subfield of π generated by π.
√
We already saw this argument in (i), in the case π = C and π = { 2}.
iv. Let πΎ be any field and let π be the field πΎ (π‘) of rational expressions over πΎ,
which is an extension of πΎ. You might worry that there’s some ambiguity
in the notation: πΎ (π‘) could either mean the field of rational expressions
over πΎ (as defined in Example 4.1.2(iv)) or the subfield of πΎ (π‘) obtained by
adjoining the element π‘ of πΎ (π‘) to πΎ (as in Definition 4.1.8).
In fact, they’re the same. In other words, the smallest subfield of πΎ (π‘)
containing πΎ and π‘ is πΎ (π‘) itself. Or equivalently, the only subfield of πΎ (π‘)
containing πΎ and π‘ is πΎ (π‘) itself. To see this, let πΏ be any such subfield. For
Í
any polynomial π (π‘) = ππ π‘ π over πΎ, we have π (π‘) ∈ πΏ, since ππ , π‘ ∈ πΏ and
πΏ is closed under multiplication and addition. Hence for any polynomials
π (π‘), π(π‘) over πΎ with π(π‘) ≠ 0, we have π (π‘), π(π‘) ∈ πΏ, so π (π‘)/π(π‘) ∈ πΏ
as πΏ is closed under division by nonzero elements. So πΏ = πΎ (π‘).
Warning 4.1.10 It is not true in general that
πΎ (πΌ) = {π + ππΌ : π, π ∈ πΎ }
(false!)
(4.1)
√
Examples
like Q( 2) and Q(π) do satisfy this, but that’s only because
√
2 and π satisfy quadratic equations. Certainly the right-hand side is
a subset of πΎ (πΌ), but in general it’s much smaller, and isn’t a subfield.
You’ve just seen an example: the field πΎ (π‘) of rational expressions is
much bigger than the set {π + ππ‘ : π, π ∈ πΎ } of polynomials of degree
≤ 1. And that set of polynomials isn’t closed under multiplication.
Another example: let π be the real cube root of 2. You can show that
π 2 cannot be expressed as π + ππ for any π, π ∈ Q (a fact we’ll come
back to in Example 4.2.11(ii)). But π ∈ Q(π), so π 2 ∈ Q(π), so (4.1)
fails in this case. In fact,
Q(π) = {π + ππ + ππ 2 : π, π, π ∈ Q}.
We’ll see why next week.
53
Exercise 4.1.11 Let π : πΎ be a field extension. Show that πΎ (π ∪ π) =
(πΎ (π ))(π) whenever π , π ⊆ π. (For example, πΎ (πΌ, π½) = (πΎ (πΌ))(π½)
whenever πΌ, π½ ∈ π.)
Remark 4.1.12 For a field extension π : πΎ, I’ll generally use small Greek letters
πΌ, π½, . . . for elements of π and small English letters π, π, . . . for elements of πΎ.
4.2
Algebraic and transcendental elements
A complex number πΌ is said to be ‘algebraic’ if
π 0 + π 1 πΌ + · · · + π π πΌπ = 0
for some rational numbers ππ , not all zero. (You may have seen this definition with
‘integer’ instead of ‘rational number’. It makes no difference, as you can always
clear the denominators.) This concept generalizes to arbitrary field extensions:
Definition 4.2.1 Let π : πΎ be a field extension and πΌ ∈ π. Then πΌ is algebraic
over πΎ if there exists π ∈ πΎ [π‘] such that π (πΌ) = 0 but π ≠ 0, and transcendental
otherwise.
Exercise 4.2.2 Show that every element of πΎ is algebraic over πΎ.
Examples 4.2.3
i. Let π ≥ 1. Then π 2ππ/π ∈ C is algebraic over Q, since
π
π (π‘) = π‘ − 1 is a nonzero polynomial such that π (π 2ππ/π ) = 0.
ii. The numbers π and π are both transcendental over Q. Both statements are
hard to prove (and we won’t prove them). By Exercise 4.2.2, any complex
number transcendental over Q is irrational. Proving the irrationality of π
and π is already a challenge; proving they’re transcendental is even harder.
iii. Although π is transcendental over Q, it is algebraic over R, since it’s an
element of R. (Again, we’re using Exercise 4.2.2.) Moral: you shouldn’t say
an element of a field is just ‘algebraic’ or ‘transcendental’; you should say
it’s ‘algebraic/transcendental over πΎ’, specifying your πΎ. Or at least, you
should do this when there’s any danger of confusion.
iv. Take the field πΎ (π‘) of rational expressions over a field πΎ. Then π‘ ∈ πΎ (π‘) is
transcendental over πΎ, since π (π‘) = 0 ⇐⇒ π = 0.
54
The set of complex numbers algebraic over Q is written as Q. It’s a fact that Q
is a subfield of C, but this is extremely hard to prove by elementary means. Next
week I’ll show you that with a surprisingly small amount of abstract algebra, you
can transform this from a very hard problem into an easy one (Proposition 5.2.7).
So that you appreciate the miracle later, I give you this unusual exercise now.
Exercise 4.2.4 Attempt to prove any part of the statement that Q is a
subfield of C. For example, try to show that Q is closed under addition,
or multiplication, or reciprocals. I have no idea how to do any of these
using only our current tools, but it’s definitely worth a few minutes of
doomed effort to get a sense of the difficulties.
Digression 4.2.5 The field Q is, in fact, algebraically closed, as you’ll see
in Workshop 3, question 8. So you might ask whether it’s possible for every
field πΎ to build an algebraically closed field containing πΎ. It turns out
that it is. Better still, there is a unique ‘smallest’ algebraically closed field
containing πΎ, called its algebraic closure πΎ. For example, the algebraic
closure of Q is Q. We won’t have time to do algebraic closure properly, but
you can read about it in most Galois theory texts.
Let π : πΎ be a field extension and πΌ ∈ π. An annihilating polynomial of πΌ
is a polynomial π ∈ πΎ [π‘] such that π (πΌ) = 0. So, πΌ is algebraic if and only if it
has some nonzero annihilating polynomial.
It is natural to ask not only whether πΌ is annihilated by some nonzero polynomial, but which polynomials annihilate it. The situation is pleasantly simple:
Lemma 4.2.6 Let π : πΎ be a field extension and πΌ ∈ π. Then there is a
polynomial π(π‘) ∈ πΎ [π‘] such that
β¨πβ© = {annihilating polynomials of πΌ over πΎ }.
(4.2)
If πΌ is transcendental over πΎ then π = 0. If πΌ is algebraic over πΎ then there is a
unique monic polynomial π satisfying (4.2).
Proof By the universal property of polynomial rings (Proposition 3.1.6), there is
a unique homomorphism
π : πΎ [π‘] → π
such that π (π) = π for all π ∈ πΎ and π (π‘) = πΌ. (Here we’re taking the ‘π’ of
Proposition 3.1.6 to be the inclusion πΎ → π.) Then
∑οΈ
∑οΈ
π
π
ππ π‘ =
π π πΌπ
55
for all
Í
ππ π‘ π ∈ πΎ [π‘], so
ker π = {annihilating polynomials of πΌ over πΎ }.
But ker π is an ideal of the principal ideal domain πΎ [π‘] (using Proposition 3.2.2),
so ker π = β¨πβ© for some π ∈ πΎ [π‘].
If πΌ is transcendental then ker π = {0}, so π = 0.
If πΌ is algebraic then π ≠ 0. Multiplying a polynomial by a nonzero constant
does not change the ideal it generates (by Exercise 2.2.15 and Lemma 3.1.14(i)),
so we can assume that π is monic. It remains to prove that π is the only monic
polynomial such that β¨πβ© = ker π. If π
e is another monic polynomial such that
β¨π
eβ© = ker π then π
e = ππ for some nonzero constant π (again by Exercise 2.2.15
and Lemma 3.1.14(i)), and both are monic, so π = 1 and π
e = π.
β‘
Definition 4.2.7 Let π : πΎ be a field extension and let πΌ ∈ π be algebraic over πΎ.
The minimal polynomial of πΌ is the unique monic polynomial π satisfying (4.2).
Warning 4.2.8 We do not define the minimal polynomial of a transcendental element. So for an arbitrary field extension π : πΎ, some
elements of π may have no minimal polynomial.
Exercise 4.2.9 What is the minimal polynomial of an element of πΎ?
This is an important definition, so we give some equivalent conditions.
Lemma 4.2.10 Let π : πΎ be a field extension, let πΌ ∈ π be algebraic over πΎ,
and let π ∈ πΎ [π‘] be a monic polynomial. The following are equivalent:
i. π is the minimal polynomial of πΌ over πΎ;
ii. π(πΌ) = 0, and π | π for all annihilating polynomials π of πΌ over πΎ;
iii. π(πΌ) = 0, and deg(π) ≤ deg( π ) for all nonzero annihilating polynomials
π of πΌ over πΎ;
iv. π(πΌ) = 0 and π is irreducible over πΎ.
Part (iii) says the minimal polynomial is a monic annihilating polynomial of
least degree.
56
Proof (i)⇒(ii) follows from the definition of minimal polynomial.
(ii)⇒(iii) because if π | π ≠ 0 then deg(π) ≤ deg( π ).
(iii)⇒(iv): assume (iii). First, π is not constant: for if π is constant then π = 1
(since π is monic); but π(πΌ) = 0, so 1 = 0 in πΎ, a contradiction. Next, suppose
that π = π π for some π , π ∈ πΎ [π‘]. Then 0 = π(πΌ) = π (πΌ)π(πΌ), so without loss
of generality, π (πΌ) = 0. By (iii), deg( π ) ≥ deg(π), so deg( π ) = deg(π) and
deg(π) = 0. This proves (iv).
(iv)⇒(i): assume (iv), and write π πΌ for the minimal polynomial of πΌ. We
have π πΌ | π by definition of π πΌ and since π(πΌ) = 0. But π is irreducible and π πΌ
is not constant, so π is a nonzero constant multiple of π πΌ . Since both are monic,
π = π πΌ , proving (i).
β‘
√
Examples 4.2.11
i. The minimal polynomial of 2 over Q is π‘ 2 − 2. There
are several ways to see this.
√
One argument: π‘ 2 − 2 is a monic annihilating polynomial
of
2, and no
√
nonzero polynomial of degree ≤ 1 over Q annihilates 2 since it is irrational.
Then use Lemma 4.2.10(iii).
Another: π‘ 2 − 2 is an irreducible monic annihilating polynomial. It is
irreducible because π‘ 2 − 2 has degree 2 and has no rational roots (using
Lemma 3.3.1(iv)). Then use Lemma 4.2.10(iv).
√3
ii. The minimal polynomial of 2 over Q is π‘ 3 − 2. This will follow from
Lemma 4.2.10(iv) as long as π‘ 3 − 2 is irreducible, which you can show using
either Lemma 3.3.1(iv) or Eisenstein.
But unlike in (i), it’s not so easy to show directly that π‘ 3 −2 is the annihilating
√3
polynomial of least degree. Try proving with your bare hands that 2
satisfies no quadratic equation over Q, i.e. that the equation
√3 2
√3
2 = π 2+π
has no solution for π, π ∈ Q. It’s not impossible, but it’s a mess. (You
naturally begin by cubing both sides, but look what happens next. . . ) So
the theory really gets us something here.
Two traps
iii. Let π be a prime number, and put π = π 2ππ/π ∈ C. Then π is a root of π‘ π − 1,
but that is not the minimal polynomial of π, since it is reducible:
π‘ π − 1 = (π‘ − 1)π(π‘)
where
π(π‘) = π‘ π−1 + · · · + π‘ + 1.
Since π π −1 = 0 but π−1 ≠ 0, we must have π(π) = 0. By Example 3.3.16,
π is irreducible over Q. Hence π is the minimal polynomial of π over Q.
57
4.3
Simple extensions
Suppose I give you a field πΎ and a nonconstant polynomial π over πΎ. Can you
find an extension of πΎ containing a root of π ?
If πΎ = Q, it’s easy. The fundamental theorem of algebra guarantees that π
has a root πΌ in C, so you can take your extension to be C. Or, if you’re feeling
economical, you can take Q(πΌ) as your extension, that being the smallest subfield
of C containing your root πΌ.
But what if πΎ is not Q?
It’s a bit like this. Say you want to go rock-climbing. If you live next to
Arthur’s Seat, no problem: just walk out of your door and get started. There’s a
ready-made solution. But if you live in the middle of the fields in the Netherlands,
you’re going to have to build your own climbing wall.
When πΎ = Q, we have a ready-made algebraically closed field C containing
πΎ, so it’s easy to find an extension of πΎ containing a root of π . For a general πΎ,
it’s not so easy. We’re going to have to build an extension of our own. But it’s not
so hard either!
Rather than taking a general polynomial π , we will just consider irreducibles.
That’s fine, because Theorem 3.2.8 guarantees that π has some irreducible factor
π, and any root of π is automatically a root of π . We will also restrict to monic
irreducibles, which makes no real difference to anything.
So, we have a field πΎ and a monic irreducible polynomial π ∈ πΎ [π‘]. We are
trying to construct an extension π of πΎ and an element πΌ ∈ π such that π(πΌ) = 0.
By Lemma 4.2.10, π will then be the minimal polynomial of πΌ.
This construction can be done as follows. By Corollary 3.2.5, the quotient
πΎ [π‘]/β¨πβ© is a field. We have ring homomorphisms
π
πΎ → πΎ [π‘] −→ πΎ [π‘]/β¨πβ©,
(4.3)
where the first homomorphism sends π ∈ πΎ to the constant polynomial π ∈ πΎ [π‘]
and π is the canonical homomorphism. Their composite is a homomorphism
of
fields πΎ → πΎ [π‘]/β¨πβ©. So, we have a field extension πΎ [π‘]/β¨πβ© : πΎ. And one of
the elements of πΎ [π‘]/β¨πβ© is π(π‘), which I will call πΌ.
Í
For a polynomial ππ π‘ π ∈ πΎ [π‘],
∑οΈ
∑οΈ
π
π
ππ π‘ =
π π πΌπ .
(4.4)
π
π
Í
Since π is surjective, every element of πΎ [π‘]/β¨πβ© is of the form ππ πΌπ . You can
think of πΎ [π‘]/β¨πβ© as the ring of polynomials over πΎ, but with two polynomials
seen as equal if they differ by a multiple of π. (Compare how you think of Z/β¨πβ©.)
58
Part (i) of the following lemma says that πΌ is a root of π, and that if we’re looking
for an extension of πΎ containing a root of π, then πΎ [π‘]/β¨πβ© is an economical
choice: it’s no bigger than it needs to be.
Part (ii) answers an analogous but easier question: what if we start with a field
πΎ and want to extend it by an element that satisfies no nonzero polynomial over
πΎ?
Lemma 4.3.1 Let πΎ be a field.
i. Let π ∈ πΎ [π‘] be monic and irreducible. Write πΌ ∈ πΎ [π‘]/β¨πβ© for the image
of π‘ under the canonical homomorphism πΎ [π‘] → πΎ [π‘]/β¨πβ©. Then πΌ has
minimal polynomial π over πΎ, and πΎ [π‘]/β¨πβ© is generated by πΌ over πΎ.
ii. The element π‘ of the field πΎ (π‘) of rational expressions over πΎ is transcendental over πΎ, and πΎ (π‘) is generated by π‘ over πΎ.
In part (i), we are viewing πΎ [π‘]/β¨πβ© as an extension of πΎ, as in (4.3).
Proof For (i), write π = πΎ [π‘]/β¨πβ©. Equation (4.4) implies that the set of
annihilating polynomials of πΌ over πΎ is ker π, which is β¨πβ©. So π is by definition
the minimal polynomial of πΌ over πΎ.
Any subfield πΏ of π containing πΎ and πΌ contains every polynomial in πΌ over
πΎ, so πΏ = π. Hence π is generated by πΌ over πΎ.
For (ii), we have already seen that π‘ is transcendental over πΎ (Example 4.2.3(iv)).
Let πΏ be a subfield of πΎ (π‘) containing πΎ and π‘. Then any polynomials
π , π ∈ πΎ [π‘] are in πΏ, so if π ≠ 0 then π /π ∈ πΏ. Hence πΏ = π, and π is
generated by π‘ over πΎ.
β‘
So far, we’ve seen that given a monic irreducible polynomial π over a field πΎ,
we can build an extension of πΎ containing a root of π. In fact, there are many
such extensions. For instance:
√
Example 4.3.2 If πΎ = Q and π(π‘) = π‘ 2 − 2 then all three of the extensions Q( 2),
R and C contain a root of π.
But πΎ [π‘]/β¨πβ© is the canonical or minimal choice. In fact, πΎ [π‘]/β¨πβ© has a
universal property. To express it, we need a definition.
Definition 4.3.3 Let πΎ be a field, and let π : πΎ → π and π′ : πΎ → π ′ be extensions
of πΎ. A homomorphism π : π → π ′ is said to be a homomorphism over πΎ if
/ π′
>
π
π`
π′
π
πΎ
commutes.
59
For the triangle to commute means that π(π(π)) = π′ (π) for all π ∈ πΎ. Very
often, the homomorphisms π and π′ are thought of as inclusions, and we write both
π(π) and π′ (π) as just π. Then for π to be a homomorphism over πΎ means that
π(π) = π for all π ∈ πΎ.
Example 4.3.4 Define π
: C → C by π
(π§) = π§. Then π
is a homomorphism, and
it is a homomorphism over R since π = π for all π ∈ R.
Exercise 4.3.5 Let π : πΎ and πΏ : πΎ be field extensions, and let
π : π → πΏ be a homomorphism over πΎ. Show that if πΌ ∈ π
has minimal polynomial π over πΎ then π(πΌ) ∈ πΏ also has minimal
polynomial π over πΎ.
Here’s an extremely useful lemma about homomorphisms over a field.
Lemma 4.3.6 Let π and π ′ be extensions of a field πΎ, and let π, π : π → π ′
be homomorphisms over πΎ. Let π be a subset of π such that π = πΎ (π ). If
π(πΌ) = π(πΌ) for all πΌ ∈ π then π = π.
Proof We have π(π) = π = π(π) for all π ∈ πΎ, since π and π are homomorphisms
over πΎ. But we are assuming that π(πΌ) = π(πΌ) for all πΌ ∈ π , so πΎ ∪ π is a subset
of the equalizer Eq{π, π} (Definition 2.3.7). Hence by Lemma 2.3.8, Eq{π, π}
is a subfield of π containing πΎ ∪ π . But πΎ (π ) is the smallest subfield of π
containing πΎ ∪ π , so Eq{π, π} = πΎ (π ) = π. Hence π = π.
β‘
Now we can formulate the universal property of πΎ [π‘]/β¨πβ©, and similarly that
of πΎ (π‘).
Proposition 4.3.7 (Universal properties of π²[π]/β¨πβ© and π² (π)) Let πΎ be a
field.
i. Let π ∈ πΎ [π‘] be monic and irreducible, let πΏ : πΎ be an extension of πΎ,
and let π½ ∈ πΏ with minimal polynomial π. Write πΌ for the image of π‘ under
the canonical homomorphism πΎ [π‘] → πΎ [π‘]/β¨πβ©. Then there is exactly one
homomorphism π : πΎ [π‘]/β¨πβ© → πΏ over πΎ such that π(πΌ) = π½.
ii. Let πΏ : πΎ be an extension of πΎ, and let π½ ∈ πΏ be transcendental. Then there
is exactly one homomorphism π : πΎ (π‘) → πΏ over πΎ such that π(π‘) = π½.
60
Diagram for (i):
3π½
πΌ
(
3 FπΏ
π
πΎ [π‘]/β¨πβ©
c
πΎ
I’ve drawn πΏ higher than πΎ [π‘]/β¨πβ© to convey the idea that πΏ may be bigger. Before
I give the proof, here’s an example.
√
Example 4.3.8 Let πΎ = Q and π(π‘) = π‘ 2 − 2. Let πΏ = C and let π½ = − 2 ∈ C.
Proposition 4.3.7(i) tells us that there is a unique field homomorphism
π : Q[π‘]/β¨π‘ 2 − 2β© → C
√
over Q mapping the equivalence class of π‘ to − 2.
Proof of Proposition 4.3.7 For (i), first we show there is at least one homomorphism π : πΎ [π‘]/β¨πβ© → πΏ over πΎ such that π(πΌ) = π½. By the universal
property of polynomial rings (Proposition 3.1.6), there is exactly one homomorphism π : πΎ [π‘] → πΏ such that π (π) = π for all π ∈ πΎ and π (π‘) = π½. Then
π (π(π‘)) = π(π½) = 0, so β¨πβ© ⊆ ker π. Hence by the universal property of quotients (p. 22), there is exactly one homomorphism π : πΎ [π‘]/β¨πβ© → πΏ such that
πΎ [π‘]
π
π
πΎ [π‘]/β¨πβ©
π
/$ πΏ
commutes. Then π is a homomorphism over πΎ, since for all π ∈ πΎ we have
π(π) = π(π(π)) = π (π) = π.
Moreover,
π(πΌ) = π(π(π‘)) = π (π‘) = π½,
so π(πΌ) = π½.
Now we show there is at most one homomorphism πΎ [π‘]/β¨πβ© → πΏ over πΎ
such that πΌ β¦→ π½. Let π and π′ be two such. Then π(πΌ) = π′ (πΌ), and πΌ generates
πΎ [π‘]/β¨πβ© over πΎ (Lemma 4.3.1(i)), so π = π′ by Lemma 4.3.6.
For (ii), first we show there is at least one homomorphism π : πΎ (π‘) → πΏ over
πΎ such that π(π‘) = π½. Every element of πΎ (π‘) can be represented as π /π where
61
π , π ∈ πΎ [π‘] with π ≠ 0. Since π½ is transcendental over πΎ, we have π(π½) ≠ 0,
and so π (π½)/π(π½) is a well-defined element of πΏ. One can check that this gives a
well-defined homomorphism
π:
πΎ (π‘) →
πΏ
π (π‘)
π (π½)
β¦→
.
π(π‘)
π(π½)
Evidently π is a homomorphism over πΎ (that is, π(π) = π for all π ∈ πΎ), and
evidently π(π‘) = π½.
The proof that there is at most one homomorphism πΎ (π‘) → πΏ over πΎ such that
π‘ β¦→ π½ is similar to the uniqueness proof in part (i).
β‘
Exercise 4.3.9 Fill in the details of the last paragraph of that proof.
We know now that for a monic irreducible polynomial π over πΎ, the extension
πΎ [π‘]/β¨πβ© contains a root of π and is generated by that root. As we’re about to
see, Proposition 4.3.7 implies that πΎ [π‘]/β¨πβ© is the only extension of πΎ with this
property. But the word ‘only’ has to be interpreted in an up-to-isomorphism sense
(as you’re used to from statements like ‘there is only one group of order 5’). The
appropriate notion of isomorphism is as follows.
Let π and π ′ be extensions of a field πΎ. A homomorphism π : π → π ′ is
an isomorphism over πΎ if it is a homomorphism over πΎ and an isomorphism of
fields. (You can check that π−1 is then also a homomorphism over πΎ.) If such a π
exists, we say that π and π ′ are isomorphic over πΎ.
Warning 4.3.10 Let π and π ′ be extensions of a field πΎ. It can
happen that π and π ′ are isomorphic, but not isomorphic over πΎ.
In other words, just because it’s possible to find an isomorphism
π : π → π ′, it doesn’t mean you can find one making the triangle in
Definition 4.3.3 commute. Workshop 3, question 16 leads you through
a counterexample.
Corollary 4.3.11 Let πΎ be a field.
i. Let π ∈ πΎ [π‘] be monic and irreducible, let πΏ : πΎ be an extension of πΎ,
and let π½ ∈ πΏ with minimal polynomial π and with πΏ = πΎ (π½). Write πΌ
for the image of π‘ under the canonical homomorphism πΎ [π‘] → πΎ [π‘]/β¨πβ©.
Then there is exactly one isomorphism π : πΎ [π‘]/β¨πβ© → πΏ over πΎ such that
π(πΌ) = π½.
62
ii. Let πΏ : πΎ be an extension of πΎ, and let π½ ∈ πΏ be transcendental with
πΏ = πΎ (π½). Then there is exactly one isomorphism π : πΎ (π‘) → πΏ over πΎ
such that π(π‘) = π½.
(Spot the differences between this corollary and Proposition 4.3.7. . . )
Proof For (i), Proposition 4.3.7(i) implies that there is a unique homomorphism
π : πΎ [π‘]/β¨πβ© → πΏ over πΎ such that π(πΌ) = π½. So we only have to show that π
is an isomorphism. Since homomorphisms of fields are injective, we need only
show that π is surjective. Now by Lemma 2.3.6(i), im π is a subfield of πΏ, and it
contains both πΎ (since π is a homomorphism over πΎ) and π½ (since π(πΌ) = π½). But
πΏ = πΎ (π½), so im π = πΏ.
The proof of (ii) is similar.
β‘
Examples 4.3.12
i. Let π be a monic irreducible polynomial over Q. Choose
a complex root π½ of π. Then the subfield Q(π½) of C is an extension of Q
generated by π½. So by Corollary 4.3.11(i), Q[π‘]/β¨πβ© Q(π½).
ii. Let π½ be a transcendental complex number. Then by Corollary 4.3.11(ii),
the field Q(π‘) of rational expressions is isomorphic to Q(π½) ⊆ C.
Field extensions generated by a single element have a special name.
Definition 4.3.13 A field extension π : πΎ is simple if there exists πΌ ∈ π such
that π = πΎ (πΌ).
Examples
i. Surprisingly many extensions are simple. For instance,
√ 4.3.14
√
Q( √2, √3) : Q is√a simple
√ extension (despite appearances), because in fact
Q( 2, 3) = Q( 2 + 3).
ii. πΎ (π‘) : πΎ is simple, where πΎ (π‘) is the field of rational expressions over πΎ.
√ √
√
√
Exercise 4.3.15
Prove that Q( 2, 3) = Q( 2 + 3). Hint: begin
√
√
by finding ( 2 + 3) 3 .
How to understand
simple algebraic
extensions
We’ve now shown that simple extensions can be classified completely:
Theorem 4.3.16 (Classification of simple extensions) Let πΎ be a field.
i. Let π ∈ πΎ [π‘] be a monic irreducible polynomial. Then there exist an
extension π : πΎ and an algebraic element πΌ ∈ π such that π = πΎ (πΌ)
and πΌ has minimal polynomial π over πΎ.
Moreover, if (π, πΌ) and (π ′, πΌ′) are two such pairs, there is exactly
one isomorphism π : π → π ′ over πΎ such that π(πΌ) = πΌ′.
63
ii. There exist an extension π : πΎ and a transcendental element πΌ ∈ π
such that π = πΎ (πΌ).
Moreover, if (π, πΌ) and (π ′, πΌ′) are two such pairs, there is exactly
one isomorphism π : π → π ′ over πΎ such that π(πΌ) = πΌ′.
Proof For (i), we can take π = πΎ [π‘]/β¨πβ© and πΌ to be the image of π‘ under
the canonical homomorphism πΎ [π‘] → π. Lemma 4.3.1(i) implies that πΌ has
minimal polynomial π over πΎ and that π = πΎ (πΌ), and Corollary 4.3.11(i) gives
‘Moreover’.
Part (ii) follows from Lemma 4.3.1(ii) and Corollary 4.3.11(ii) in the same
way.
β‘
Conclusion: given any field πΎ (not necessarily Q!) and any monic irreducible
π(π‘) ∈ πΎ [π‘], we can say the words ‘adjoin to πΎ a root πΌ of π’, and this unambiguously defines an extension πΎ (πΌ) : πΎ. (At least, unambiguously up to isomorphism
over πΎ—but who could want more?) Similarly, we can unambiguously adjoin to
πΎ a transcendental element.
Examples 4.3.17
i. Let πΎ be any field not containing a square root of 2. Then
2
2
π‘ − 2 is irreducible
√ over πΎ. So we can adjoin to πΎ a root of π‘ − 2, giving
an extension πΎ ( 2) : πΎ.
We√have already seen this example many times when πΎ = Q, in which case
πΎ ( 2) can be seen as a subfield of C. But the construction works for √
any
πΎ. For instance, 2 has no square root in F3 , so there is an extension F3 ( 2)
of F3 . It can be constructed as F3 [π‘]/β¨π‘ 2 − 2β©.
ii. The polynomial π(π‘) = 1 + π‘ + π‘ 2 is irreducible over F2 , so we may adjoin to
F2 a root πΌ of π. Then F2 (πΌ) = F2 [π‘]/β¨1 + π‘ + π‘ 2 β©.
√
Exercise 4.3.18 How many elements does the field F3 ( 2) have?
What about F2 (πΌ), where πΌ is a root of 1 + π‘ + π‘ 2 ?
Warning 4.3.19 Take πΎ = Q and π(π‘) = π‘ 3 − 2, which is irreducible.
Write πΌ1 , πΌ2 , πΌ3 for the roots of π in C. Then Q(πΌ1 ), Q(πΌ2 ) and
Q(πΌ3 ) are all different as subsets of C. For example, one of the πΌπ
is the real cube root of 2 (say πΌ1 ), which implies that Q(πΌ1 ) ⊆ R,
whereas the other two are not real, so Q(πΌπ ) β R for π ≠ 1. However,
Q(πΌ1 ) : Q, Q(πΌ2 ) : Q and Q(πΌ3 ) : Q are all isomorphic as abstract
field extensions of Q. This follows from Theorem 4.3.16, since all the
πΌπ have the same minimal polynomial, π.
64
You’re already very familiar with this kind of situation in other
branches of algebra. For instance, in linear algebra, take three vectors
v1 , v2 , v3 in R2 , none a scalar multiple of any other. Then span(v1 ),
span(v2 ) and span(v3 ) are all different as subsets of R2 , but they are all
isomorphic as abstract vector spaces (since they’re all 1-dimensional).
A similar example could be given with a group containing several subgroups that are all isomorphic.
You’ve seen that Galois theory involves aspects of group theory and ring theory.
In the next chapter, you’ll see how linear algebra enters the picture too.
65
Chapter 5
Degree
We’ve seen that if you adjoin to Q a square root of 2, then each element of the
resulting field can be specified using two rational numbers, π and π:
√
√
Q( 2) = π + π 2 : π, π ∈ Q .
Introduction to
Week 5
I also mentioned that if you adjoin to Q a cube root of 2, then it takes three rational
numbers to specify each element of the resulting field:
n
o
√3
√3
√3 2
Q( 2) = π + π 2 + π 2 : π, π, π ∈ Q
√3
(Warning 4.1.10). This might
lead
us
to
suspect
that
Q(
2) : Q is in some sense
√
a ‘bigger’ extension than Q( 2) : Q.
The first thing we’ll do in this chapter is to make√this intuition rigorous.
We’ll
√3
define the ‘degree’ of an extension and see that Q( 2) : Q and Q( 2) : Q have
degrees 2 and 3, respectively.
The concept of degree is incredibly useful, and not only in Galois theory.
In fact, I’ll show you how it can be used to solve three problems that remained
unsolved for literally millennia, since the time of the ancient Greeks.
5.1
The degree of an extension
Let π : πΎ be a field extension. Then π is a vector space over πΎ in a natural way.
Addition and subtraction in the vector space π are the same as in the field π.
Scalar multiplication in the vector space is just multiplication of elements of π by
elements of πΎ, which makes sense because πΎ is embedded as a subfield of π.
This little observation is amazingly useful. It is an excellent illustration of a
powerful mathematical technique: forgetting. When we view π as a vector space
over πΎ rather than a field extension of πΎ, we are forgetting how to multiply together
elements of π that aren’t in πΎ.
66
Definition 5.1.1 The degree [π : πΎ] of a field extension π : πΎ is the dimension
of π as a vector space over πΎ.
If π is a finite-dimensional vector space over πΎ, it’s clear what this means. If
π is infinite-dimensional over πΎ, we write [π : πΎ] = ∞, where ∞ is a formal
symbol which we give the properties
π < ∞,
π·∞=∞
(π ≥ 1),
∞·∞=∞
for integers π. An extension π : πΎ is finite if [π : πΎ] < ∞.
Digression 5.1.2 You know that whenever π is a finite-dimensional vector
space, (i) there exists a basis of π, and (ii) there is a bΔ³ection between any
two bases. This makes it possible to define the dimension of a vector space
as the number of elements in a basis. In fact, both (i) and (ii) are true for
every vector space, not just the finite-dimensional ones. So we can define
the dimension of an arbitrary vector space as the ‘number’ of elements in a
basis, where now ‘number’ means cardinal, i.e. isomorphism class of sets.
We could interpret Definition 5.1.1 using this general definition of dimension.
For instance, suppose we had one field extension π : πΎ such that π had a
countably infinite basis over πΎ, and another, π ′ : πΎ, such that π ′ had an
uncountably infinite basis over πΎ. Then [π : πΎ] and [π ′ : πΎ] would be
different.
However, we’ll lump all the infinite-dimensional extensions together and say
that their degrees are all ∞. We’ll mostly be dealing with finite extensions
anyway, and won’t need to distinguish between sizes of ∞. It’s a bit like the
difference between a house that costs a million pounds and a house that costs
ten million: although the difference is vast, most of us would lump them
together in a single category called ‘unaffordable’.
Examples 5.1.3
i. Every field π contains at least one nonzero element,
namely, 1. So [π : πΎ] ≥ 1 for every field extension π : πΎ.
If π = πΎ then {1} is a basis, so [π : πΎ] = 1. On the other hand, if
[π : πΎ] = 1 then the one-element linearly independent set {1} must be a
basis, which implies that every element of π is equal to π · 1 = π for some
π ∈ πΎ, and so π = πΎ. Hence
[π : πΎ] = 1 ⇐⇒ π = πΎ.
ii. Every element of C is equal to π₯ + π¦π for a unique pair (π₯, π¦) of elements of
R. That is, {1, π} is a basis of C over R. Hence [C : R] = 2.
67
iii. Let πΎ be a field and πΎ (π‘) the field of rational expressions over πΎ. Then
1, π‘, π‘ 2 , . . . are linearly independent over πΎ, so [πΎ (π‘) : πΎ] = ∞.
Warning 5.1.4 The degree [πΎ : πΎ] of πΎ over itself is 1, not 0.
Degrees of extensions are never 0. See Example 5.1.3(i).
Theorem 5.1.5 Let πΎ (πΌ) : πΎ be a simple extension.
i. Suppose that πΌ is algebraic over πΎ. Write π ∈ πΎ [π‘] for the minimal
polynomial of πΌ and π = deg(π). Then
1, πΌ, . . . , πΌπ−1
is a basis of πΎ (πΌ) over πΎ. In particular, [πΎ (πΌ) : πΎ] = deg(π).
ii. Suppose that πΌ is transcendental over πΎ. Then 1, πΌ, πΌ2 , . . . are linearly
independent over πΎ. In particular, [πΎ (πΌ) : πΎ] = ∞.
Proof For (i), to show that 1, πΌ, . . . , πΌπ−1 is a basis of πΎ (πΌ) over πΎ, we will
show that every element of πΎ (πΌ) can be expressed as a πΎ-linear combination of
1, πΌ, . . . , πΌπ−1 in a unique way.
By Lemma 4.3.1(i) and Theorem 4.3.16(i), we might as well take πΎ (πΌ) =
πΎ [π‘]/β¨πβ© and πΌ = π(π‘), where π : πΎ [π‘] → πΎ [π‘]/β¨πβ© is the canonical homomorphism.
Since π is surjective, every element of πΎ (πΌ) is equal to π( π ) for some π ∈ πΎ [π‘].
By Proposition 3.2.1, there are unique π, π ∈ πΎ [π‘] such that π = ππ + π and
deg(π) < π. In particular, there is a unique polynomial π ∈ πΎ [π‘] such that
π − π ∈ β¨πβ© and deg(π) < π. Equivalently, there are unique π 0 , . . . , π π−1 ∈ πΎ such
that
π (π‘) − π 0 + π 1 π‘ + · · · + π π−1 π‘ π−1 ∈ β¨πβ©.
Equivalently, there are unique π 0 , . . . , π π−1 ∈ πΎ such that
π( π ) = π π 0 + π 1 π‘ + · · · + π π−1 π‘ π−1 .
Equivalently (since π(π‘) = πΌ), there are unique π 0 , . . . , π π−1 ∈ πΎ such that
π( π ) = π 0 + π 1 πΌ + · · · π π−1 πΌπ−1 ,
as required.
For (ii), Theorem 4.3.16(ii) implies that πΎ (πΌ) is isomorphic over πΎ to the field
πΎ (π‘) of rational expressions. The result now follows from Example 5.1.3(iii). β‘
68
Examples 5.1.6
i. Let πΌ ∈ C be an algebraic number over Q whose minimal
polynomial is quadratic. Then by Theorem 5.1.5(i),
Q(πΌ) = {π + ππΌ : π, π ∈ Q}.
√
We’ve already seen this in many examples, such as πΌ = 2 and πΌ = π.
ii. Let π be a prime. We saw in Example 4.2.11(iii) that π 2ππ/π has minimal
polynomial 1+π‘ +· · ·+π‘ π−1 . This has degree π−1, so [Q(π 2ππ/π ) : Q] = π−1.
Warning 5.1.7 For a prime π, the degree of π 2ππ/π over Q is π − 1,
not π!
Example 5.1.8 Apart from finite fields of the form F π , the simplest finite field
is F2 (πΌ), where πΌ is a root of the irreducible polynomial 1 + π‘ + π‘ 2 over F2
(Example 4.3.17(ii)). By Theorem 5.1.5(i),
F2 (πΌ) = {π + ππΌ : π, π ∈ F2 } = {0, 1, πΌ, 1 + πΌ}.
Since 1 + πΌ + πΌ2 = 0 and F2 (πΌ) has characteristic 2,
πΌ2 = 1 + πΌ,
(1 + πΌ) 2 = πΌ.
So the Frobenius automorphism of F2 (πΌ) interchanges πΌ and 1 + πΌ. Like all
automorphisms, it fixes 0 and 1.
Exercise 5.1.9 Write out the addition and multiplication tables of
F2 (πΌ).
Theorem 5.1.5(i) implies that when πΌ ∈ π is algebraic over πΎ, with minimal
polynomial of degree π, the subset {π 0 + π 1 πΌ + · · · + π π−1 πΌπ−1 : ππ ∈ πΎ } is a
subfield of π. This isn’t particularly obvious: for instance, why is it closed under
taking reciprocals? But it’s true.
For a field extension π : πΎ and πΌ ∈ π, the degree of πΌ over πΎ is [πΎ (πΌ) : πΎ].
We write it as degπΎ (πΌ). Theorem 5.1.5 immediately implies:
Corollary 5.1.10 Let π : πΎ be a field extension and πΌ ∈ π. Then
degπΎ (πΌ) < ∞ ⇐⇒ πΌ is algebraic over πΎ.
β‘
If πΌ is algebraic over πΎ then by Theorem 5.1.5(i), the degree of πΌ over πΎ is the
degree of the minimal polynomial of πΌ over πΎ.
69
π
π½
[πΎ (π½):πΎ]
[πΏ(π½):πΏ]
πΏ
πΎ
Figure 5.1: Visualization of Corollary 5.1.12 (not to be taken too seriously).
Example 5.1.11 Let π be the real cube root of 2. By Example 4.2.11(ii), the
minimal polynomial of π over Q is π‘ 3 − 2, so degQ (π) = 3. It follows that
Q(π) ≠ {π + ππ : π, π ∈ Q}, since otherwise the two-element set {1, π} would
span the three-dimensional vector space Q(π). So we have another proof that
22/3 cannot be written as a Q-linear combination of 1 and 21/3 . As observed in
Example 4.2.11(ii), this is messy to prove directly.
Theorem 5.1.5 is powerful. Here are two more of its corollaries.
Corollary 5.1.12 Let π : πΏ : πΎ be field extensions and π½ ∈ π. Then [πΏ(π½) :
πΏ] ≤ [πΎ (π½) : πΎ].
Informally, I think of Corollary 5.1.12 as in Figure 5.1. The degree of π½ over
πΎ measures how far π½ is from being in πΎ. Since πΏ contains πΎ, it might be that π½ is
closer to πΏ than to πΎ (i.e. [πΏ(π½) : πΏ] < [πΎ (π½) : πΎ]), and it’s certainly no further
away.
Proof If [πΎ (π½) : πΎ] = ∞ then the inequality is clear. Otherwise, π½ is algebraic
over πΎ (by Corollary 5.1.10), with minimal polynomial π ∈ πΎ [π‘], say. Then π is
an annihilating polynomial for π½ over πΏ, so the minimal polynomial of π½ over πΏ
has degree ≤ deg(π). The result follows from Theorem 5.1.5(i).
β‘
Exercise 5.1.13 Give an example to show that the inequality in Corollary 5.1.12 can be strict. Your example can be as trivial as you like.
Corollary 5.1.14 Let π : πΎ be a field extension. Let πΌ1 , . . . , πΌπ ∈ π, with πΌπ
algebraic over πΎ of degree ππ . Then every element πΌ ∈ πΎ (πΌ1 , . . . , πΌπ ) can be
expressed as a polynomial in πΌ1 , . . . , πΌπ over πΎ. More exactly,
∑οΈ
πΌ=
ππ1 ,...,π π πΌ1π1 · · · πΌππ π
π 1 ,...,π π
for some ππ1 ,...,π π ∈ πΎ, where ππ ranges over 0, . . . , ππ − 1.
70
For example, here’s what this says in the case π = 2. Let π : πΎ be a field
extension, and take algebraic elements πΌ1 , πΌ2 of π. Write π1 and π2 for their
degrees over πΎ. Then every element of πΎ (πΌ1 , πΌ2 ) is equal to
π∑οΈ
1 −1 π∑οΈ
2 −1
ππ π πΌ1π πΌ2π
π=0 π =0
for some coefficients ππ π ∈ πΎ. A fundamental point in the proof is that a polynomial
in two variables can be seen as a polynomial in one variable whose coefficients are
themselves polynomials in one variable, and similarly for more than two variables.
Proof When π = 0, this is trivial. Now let π ≥ 1 and suppose inductively that the
result holds for π − 1. Let
πΌ ∈ πΎ (πΌ1 , . . . , πΌπ ) = πΎ (πΌ1 , . . . , πΌπ−1 ) (πΌπ ).
By Theorem 5.1.5(i) applied to the extension (πΎ (πΌ1 , . . . , πΌπ−1 ))(πΌπ )
πΎ (πΌ1 , . . . , πΌπ−1 ), noting that degπΎ (πΌ1 ,...,πΌπ−1 ) (πΌπ ) ≤ degπΎ (πΌπ ) = ππ , we have
πΌ=
π∑οΈ
π −1
ππ πΌππ
:
(5.1)
π=0
for some π 0 , . . . , π ππ −1 ∈ πΎ (πΌ1 , . . . , πΌπ−1 ). By inductive hypothesis, for each π we
have
∑οΈ
π π−1
ππ =
ππ1 ,...,π π−1 ,π πΌ1π1 · · · πΌπ−1
(5.2)
π 1 ,...,π π−1
for some ππ1 ,...,π π−1 ,π ∈ πΎ, where ππ ranges over 0, . . . , ππ − 1. Substituting (5.2)
into (5.1) completes the induction.
β‘
Example 5.1.15 Back in Example 4.1.9(ii), I claimed that
√
√
√
Q( 2, π) = {π + π 2 + ππ + π 2π : π, π, π, π ∈ Q}.
√
√
Corollary 5.1.14 applied to Q( 2, π) : Q proves this, since degQ ( 2) = degQ (π) =
2.
Exercise 5.1.16 Let π : πΎ be a field extension and πΌ a transcendental element of π. Can every element of πΎ (πΌ) be represented as a
polynomial in πΌ over πΎ?
For extensions obtained by adjoining several elements, the following result is
invaluable.
71
Theorem 5.1.17 (Tower law) Let π : πΏ : πΎ be field extensions.
i. If (πΌπ )π∈πΌ is a basis of πΏ over πΎ and (π½ π ) π ∈π½ is a basis of π over πΏ, then
(πΌπ π½ π ) (π, π)∈πΌ×π½ is a basis of π over πΎ.
ii. π : πΎ is finite ⇐⇒ π : πΏ and πΏ : πΎ are finite.
iii. [π : πΎ] = [π : πΏ] [πΏ : πΎ].
The sets πΌ and π½ here could be infinite. I’ll say that a family (ππ )π∈πΌ of elements
of a field is finitely supported if the set {π ∈ πΌ : ππ ≠ 0} is finite.
Proof To prove (i), we show that (πΌπ π½ π ) (π, π)∈πΌ×π½ is a linearly independent spanning
set of π over πΎ.
For linear independence, let (ππ π ) (π, π)∈πΌ×π½ be a finitely supported family of eleÍ
Í Í
Í
ments of πΎ such that π, π ππ π πΌπ π½ π = 0. Then π ( π ππ π πΌπ ) π½ π = 0, with π ππ π πΌπ ∈ πΏ
Í
for each π ∈ π½. Since (π½ π ) π ∈π½ is linearly independent over πΏ, we have π ππ π πΌπ = 0
for each π ∈ π½. But (πΌπ )π∈πΌ is linearly independent over πΎ, so ππ π = 0 for each π ∈ πΌ
and π ∈ π½.
To show (πΌπ π½ π ) (π, π)∈πΌ×π½ spans π over πΎ, let π ∈ π. Since (π½ π ) π ∈π½ spans π over
Í
πΏ, we have π = π π π π½ π for some finitely supported family (π π ) π ∈π½ of elements of
Í
πΏ. Since (πΌπ )π∈πΌ spans πΏ over πΎ, for each π ∈ π½ we have π π = π ππ π πΌπ for some
Í
finitely supported family (ππ π )π∈πΌ of πΎ. Hence π = π, π ππ π πΌπ π½ π , as required.
Parts (ii) and (iii) follow.
β‘
√ √
Example 5.1.18 What is [Q( 2, 3) : Q]? The tower law gives
√ √
√ √
√ √
Q( 2, 3) : Q = Q( 2, 3) : Q( 2) Q( 2) : Q
√ √ √
= 2 Q( 2, 3) : Q( 2) .
Now on the one hand,
√ √
√ √
Q( 2, 3) : Q( 2) ≤ Q( 3) : Q = 2
√
√ √
√
√
by Corollary
5.1.12.
On
the
other,
3
∉
Q(
2),
so
Q(
2,
3)
≠
Q(
√ √
√
√ √
√ 2), so
> 1 √by Example 5.1.3(i). So [Q( 2, 3) : Q( 2)] = 2,
[Q( 2, 3) : Q( 2)] √
giving the answer: [Q( 2, 3) : Q] = 4.
√ √ √
√ √
By the same argument as in Example √
5.1.15,
{1,
2,
3,
6}
spans
Q(
2, 3)
√
4
over
Q.
Hence
over Q. But we have just shown that Q( 2, 3) has dimension
√ √
this spanning set is a basis. That is, for every element πΌ ∈ Q( 2, 3), there is one
and only one 4-tuple (π, π, π, π) of rational numbers such that
√
√
√
πΌ = π + π 2 + π 3 + π 6.
72
Corollary 5.1.19 Let π : πΏ ′ : πΏ : πΎ be field extensions. If π : πΎ is finite then
[πΏ ′ : πΏ] divides [π : πΎ].
Proof By the tower law twice, [π : πΎ] = [π : πΏ ′] [πΏ ′ : πΏ] [πΏ : πΎ].
β‘
That result might remind you of Lagrange’s theorem on group orders. The
resemblance is no coincidence, as we’ll see.
Exercise 5.1.20 Show that a field extension whose degree is a prime
number must be simple.
That result might remind you of the fact that a group of prime order must be
cyclic, and that’s no coincidence either!
A second corollary of the tower law:
Corollary 5.1.21 Let π : πΎ be a field extension and πΌ1 , . . . , πΌπ ∈ π. Then
[πΎ (πΌ1 , . . . , πΌπ ) : πΎ] ≤ [πΎ (πΌ1 ) : πΎ] · · · [πΎ (πΌπ ) : πΎ].
Proof By the tower law and then Corollary 5.1.12,
[πΎ (πΌ1 , . . . , πΌπ ) : πΎ]
= [πΎ (πΌ1 , . . . , πΌπ ) : πΎ (πΌ1 , . . . , πΌπ−1 )] · · · [πΎ (πΌ1 , πΌ2 ) : πΎ (πΌ1 )] [πΎ (πΌ1 ) : πΎ]
≤ [πΎ (πΌπ ) : πΎ] · · · [πΎ (πΌ2 ) : πΎ] [πΎ (πΌ1 ) : πΎ].
β‘
Example 5.1.22 What is [Q(121/4 , 61/15 ) : Q]? You can check (hint, hint)
that degQ (121/4 ) = 4 and degQ (61/15 ) = 15. So by Corollary 5.1.19,
[Q(121/4 , 61/15 ) : Q] is divisible by 4 and 15. But also, Corollary 5.1.21 implies that [Q(121/4 , 61/15 ) : Q] ≤ 4 × 15 = 60. Since 4 and 15 are coprime, the
answer is 60.
Exercise 5.1.23 Generalize Example 5.1.22. In other words, what
general result does the argument of Example 5.1.22 prove, not involving the particular numbers chosen there?
5.2
Algebraic extensions
We defined a field extension π : πΎ to be finite if [π : πΎ] < ∞, that is, π is
finite-dimensional as a vector space over πΎ. Here are two related conditions.
73
algebraic
finite
finitely
generated
Figure 5.2: Finiteness conditions on a field extension
Definition 5.2.1 A field extension π : πΎ is finitely generated if π = πΎ (π ) for
some finite subset π ⊆ π.
Definition 5.2.2 A field extension π : πΎ is algebraic if every element of π is
algebraic over πΎ.
Recall from Corollary 5.1.10 that πΌ is algebraic over πΎ if and only if πΎ (πΌ) : πΎ
is finite. So for a field extension to be algebraic is also a kind of finiteness condition.
Examples 5.2.3
i. For any field πΎ, the extension πΎ (π‘) : πΎ is finitely generated
(take the ‘π ’ above to be {π‘}) but not finite, by Corollary 5.1.10.
ii. In Section 4.2 you met the set Q of complex numbers algebraic over Q. We’ll
very soon prove that it’s a subfield of C. It is algebraic over Q, by definition.
But you’ll show in Workshop 3, question 13 that it is not finite over Q.
Our three finiteness conditions are related as follows (Figure 5.2).
Proposition 5.2.4 The following conditions on a field extension π : πΎ are equivalent:
i. π : πΎ is finite;
ii. π : πΎ is finitely generated and algebraic;
iii. π = πΎ (πΌ1 , . . . , πΌπ ) for some finite set {πΌ1 , . . . , πΌπ } of elements of π algebraic over πΎ.
Proof (i)⇒(ii): suppose that π : πΎ is finite.
To show that π : πΎ is finitely generated, take a basis πΌ1 , . . . , πΌπ of π over
πΎ. Every subfield πΏ of π containing πΎ is a πΎ-linear subspace of π, so if
πΌ1 , . . . , πΌπ ∈ πΏ then πΏ = π. This proves that the only subfield of π containing
πΎ ∪ {πΌ1 , . . . , πΌπ } is π itself; that is, π = πΎ (πΌ1 , . . . , πΌπ ). So π : πΎ is finitely
generated.
74
To show that π : πΎ is algebraic, let πΌ ∈ π. Then by part (ii) of the tower law
(Theorem 5.1.17), πΎ (πΌ) : πΎ is finite, so by Corollary 5.1.10, πΌ is algebraic over
πΎ.
(ii)⇒(iii) is immediate from the definitions.
(iii)⇒(i): suppose that π = πΎ (πΌ1 , . . . , πΌπ ) for some πΌπ ∈ π algebraic over πΎ.
Then
[π : πΎ] ≤ [πΎ (πΌ1 ) : πΎ] · · · [πΎ (πΌπ ) : πΎ]
by Corollary 5.1.21. For each π, we have [πΎ (πΌπ ) : πΎ] < ∞ since πΌπ is algebraic
over πΎ (using Corollary 5.1.10 again). So [π : πΎ] < ∞.
β‘
We already saw that when π = πΎ (πΌ1 , . . . , πΌπ ) with each πΌπ algebraic, every
element of π is a polynomial in πΌ1 , . . . , πΌπ (Corollary 5.1.14). So for any finite
extension π : πΎ, there is some finite set of elements such that everything in π
can be expressed as a polynomial over πΎ in these elements.
Exercise 5.2.5 Let π : πΎ be a field extension and πΎ ⊆ πΏ ⊆ π. In
the proof of Proposition 5.2.4, I said that if πΏ is a subfield of π then
πΏ is a πΎ-linear subspace of π. Why is that true? And is the converse
also true? Give a proof or a counterexample.
Corollary 5.2.6 Let πΎ (πΌ) : πΎ be a simple extension. The following are equivalent:
i. πΎ (πΌ) : πΎ is finite;
ii. πΎ (πΌ) : πΎ is algebraic;
iii. πΌ is algebraic over πΎ.
Proof (i)⇒(ii) follows from (i)⇒(ii) of Proposition 5.2.4.
(ii)⇒(iii) is immediate from the definitions.
(iii)⇒(i) follows from (iii)⇒(i) of Proposition 5.2.4.
Here’s a spectacular application of Corollary 5.2.6.
Proposition 5.2.7 Q is a subfield of C.
Proof By Corollary 5.2.6,
Q = {πΌ ∈ C : [Q(πΌ) : Q] < ∞}.
For all πΌ, π½ ∈ Q,
[Q(πΌ, π½) : Q] ≤ [Q(πΌ) : Q] [Q(π½) : Q] < ∞
75
β‘
by Corollary 5.1.21. Now πΌ + π½ ∈ Q(πΌ, π½), so Q(πΌ + π½) ⊆ Q(πΌ, π½), so
[Q(πΌ + π½) : Q] ≤ [Q(πΌ, π½) : Q] < ∞,
giving πΌ + π½ ∈ Q. Similarly, πΌ · π½ ∈ Q. For all πΌ ∈ Q,
[Q(−πΌ) : Q] = [Q(πΌ) : Q] < ∞,
giving −πΌ ∈ Q. Similarly, 1/πΌ ∈ Q (if πΌ ≠ 0). And clearly 0, 1 ∈ Q.
β‘
If you did Exercise 4.2.4, you’ll appreciate how hard that result is to prove from
first principles, and how amazing it is that the proof above is so clean and simple.
Exercise 5.2.8 Let π : πΎ be a field extension, and write πΏ for the
set of elements of π algebraic over πΎ. By imitating the proof of
Proposition 5.2.7, prove that πΏ is a subfield of π.
5.3
Ruler and compass constructions
This section is a truly wonderful application of the algebra we’ve developed so far.
Using it, we will solve problems that lay unsolved for thousands of years.
The arguments here have a lot in common with those we’ll use in Chapter 9
for the problem of solving polynomials by radicals. It’s well worth getting used to
these arguments now, since the polynomial problem involves some extra subtleties
that will need your full attention then. In other words, treat this as a warm-up.
The ancient Greeks developed planar geometry to an extraordinary degree,
discovering how to perform a very wide range of constructions using only ruler
and compasses. But there were three particular constructions that they couldn’t
figure out how to do using only these instruments:
• Trisect the angle: given an angle π, construct the angle π/3.
• Duplicate the cube: given a length, construct a new length whose cube is
twice the cube of the original.√ That is, given two points distance πΏ apart,
3
construct two points distance 2πΏ apart.
• Square the circle: given a circle, construct a square with the same area.
That
is, given two points distance πΏ apart, construct two points distance
√
ππΏ apart.
The challenge of finding constructions lay unanswered for millennia. And it
wasn’t for lack of attention. My Galois theory lecture notes from when I was an
undergraduate contain the following words:
76
Thomas Hobbes claimed to have solved these. John Wallis disagreed.
A 17th century pamphlet war ensued.
Ruler and compass
constructions
Twitter users may conclude that human nature has not changed.
It turns out that the reason why no one could find a way to do these constructions
is that they’re impossible. We’ll prove it using field theory.
In order to prove that you can’t do these things using ruler and compasses, it’s
necessary to know that you can do certain other things using ruler and compasses.
I’ll take some simple constructions for granted (but there’s a video if you want the
details).
Digression 5.3.1 The standard phrase is ‘ruler and compass constructions’,
but it’s slightly misleading. A ruler has distance markings on it, whereas
for the problems of ancient Greece, you’re supposed to use only a ‘straight
edge’: a ruler without markings (and no, you’re not allowed to mark it). As
Stewart explains (Section 7.1), with a marked or markable straight edge, you
can solve all three problems. Also, for what it’s worth, an instrument for
drawing circles is strictly speaking a pair of compasses. But like everyone
else, we’ll say ‘ruler and compass’—
—when we really mean ‘straight edge and compasses’—
The problems as stated above are maybe not quite precise; let’s formalize them.
Starting from a subset Σ of the plane, our instruments allow the following
constructions:
• given two distinct points π΄, π΅ of Σ, draw the (infinite) line through π΄ and π΅;
• given two distinct points π΄, π΅ of Σ, draw the circle with centre π΄ passing
through π΅.
A point in the plane is immediately constructible from Σ if it is a point of
intersection between two distinct lines, or two distinct circles, or a line and a
77
circle, of the form above. A point πΆ in the plane is constructible from Σ if
there is a finite sequence πΆ1 , . . . , πΆπ = πΆ of points such that πΆπ is immediately
constructible from Σ ∪ {πΆ1 , . . . , πΆπ−1 } for each π. Broadly, the question is: which
points are constructible from which?
The key idea of the solution is that when you’re doing Greek-style geometry,
then in terms of coordinates, you’re repeatedly solving linear or quadratic equations. (The Greeks didn’t use coordinates, but we will.) This is because equations
of lines and circles are linear or quadratic.
For instance, suppose we start with the points (0, 0) and (1, 0). Draw the circle
with centre (0, 0) passing through
√ (1, 0), and vice versa. The intersection points
of the two circles are (1/2, ± 3/2), where the square root came from solving a
quadratic. If we do
ruler and compass constructions, we might end up with
√οΈ√further
√3
√
coordinates like
2 + 3. But we can never get coordinates like 2, because
where would a cube root come from? We’re only solving quadratics here.
To translate this idea into field terms, we make the following definition. Take
a subfield πΎ ⊆ R. We say that the extension πΎ : Q is iterated quadratic if there
is some finite sequence of subfields
Q = πΎ0 ⊆ πΎ1 ⊆ · · · ⊆ πΎπ = πΎ
such that [πΎπ : πΎπ−1 ] = 2 for all π ∈ {1, . . . , π}.
√οΈ√
√ 2 + 3 is an iterated quadratic extension of Q, because we
Example 5.3.2 Q
have a chain of subfields
√οΈ
√ √ √
√
√ √ √
2+ 3
Q ⊆ Q 2 ⊆ Q 2, 3 = Q 2 + 3 ⊆ Q
where each has degree 2 over the last. (For the equality, see Exercise 4.3.15.)
√οΈ√
√
There is an iterated quadratic extension √οΈ
of Q containing
2 + 3, and by
√
√
the same argument, there is one containing
5 + 7. Is there one containing
both? We will prove a general result guaranteeing that there is. The following
terminology will be useful.
Definition 5.3.3 Let πΏ and πΏ ′ be subfields of a field π. The compositum πΏπΏ ′ of
πΏ and πΏ ′ is the subfield of π generated by πΏ ∪ πΏ ′.
That is, πΏπΏ ′ is the smallest subfield of π containing both πΏ and πΏ ′. In the
notation of Definition 4.1.8, we could also write πΏπΏ ′ as either πΏ (πΏ ′) or πΏ ′ (πΏ).
√
√
Example
√ √ 5.3.4 The compositum of the subfields Q( 2) and Q( 3) of R is
Q( 2, 3).
78
Warning 5.3.5 Despite the notation,
πΏπΏ ′ ≠ {πΌπΌ′ : πΌ ∈ πΏ, πΌ′ ∈ πΏ ′ }.
But it is true that πΏπΏ ′ is the subfield of π generated by the right-hand
side. (Why?)
To show that any two iterated quadratic extensions of Q can be merged into
one, we first consider extensions of degree 2.
Lemma 5.3.6 Let π : πΎ be a field extension and let πΏ, πΏ ′ be subfields of π
containing πΎ. If [πΏ : πΎ] = 2 then [πΏπΏ ′ : πΏ ′] ∈ {1, 2}.
π
πΏπΏ ′
πΏ′
πΏ
πΎ
Actually, it is true more generally that [πΏπΏ ′ : πΏ ′] ≤ [πΏ : πΎ] (Workshop 3,
question 18), but we will not need this fact.
Proof Choose some π½ ∈ πΏ \ πΎ. By applying the tower law to πΏ : πΎ (π½) : πΎ and
using the hypothesis that [πΏ : πΎ] = 2, we see that πΎ (π½) = πΏ.
Next we show that πΏπΏ ′ = πΏ ′ (π½). Certainly πΏ ′ (π½) ⊆ πΏπΏ ′, since πΏ ′ ⊆ πΏπΏ ′ and
π½ ∈ πΏ ⊆ πΏπΏ ′. Conversely, πΏ ′ (π½) is a subfield of π that contains both πΎ (π½) = πΏ
and πΏ ′, so it contains πΏπΏ ′. Hence πΏπΏ ′ = πΏ ′ (π½), as claimed.
It follows that [πΏπΏ ′ : πΏ ′] = [πΏ ′ (π½) : πΏ ′] ≤ [πΎ (π½) : πΎ] = 2, where the
inequality comes from Corollary 5.1.12.
β‘
Exercise 5.3.7 Find an example of Lemma 5.3.6 where [πΏπΏ ′ : πΏ ′] = 2,
and another where [πΏπΏ ′ : πΏ ′] = 1.
Lemma 5.3.8 Let πΎ and πΏ be subfields of R such that the extensions πΎ : Q and
πΏ : Q are iterated quadratic. Then there is some subfield π of R such that the
extension π : Q is iterated quadratic and πΎ, πΏ ⊆ π.
Proof Take subfields
Q = πΎ0 ⊆ πΎ1 ⊆ · · · ⊆ πΎπ = πΎ ⊆ R,
Q = πΏ0 ⊆ πΏ1 ⊆ · · · ⊆ πΏπ = πΏ ⊆ R
with [πΎπ : πΎπ−1 ] = 2 = [πΏ π : πΏ π−1 ] for all π, π. Consider the chain of subfields
Q = πΎ0 ⊆ πΎ1 ⊆ · · · ⊆ πΎπ = πΎ = πΎ πΏ 0 ⊆ πΎ πΏ 1 ⊆ · · · ⊆ πΎ πΏ π = πΎ πΏ
(5.3)
of R. It is enough to show that πΎ πΏ is an iterated quadratic extension of πΎ.
In the chain (5.3), [πΎπ : πΎπ−1 ] = 2 for all π. Moreover, for each π we have
[πΏ π : πΏ π−1 ] = 2, so Lemma 5.3.6 implies that [πΎ πΏ π : πΎ πΏ π−1 ] ∈ {1, 2} (taking the
‘πΎ’ of that lemma to be πΏ π−1 ). Hence in (5.3), all the successive degrees are 1
or 2. An extension of degree 1 is an equality, so by ignoring repeats, we see that
πΎ πΏ : Q is an iterated quadratic extension.
β‘
79
The general theory of ruler and compass constructibility starts with any set
Σ ⊆ R2 of given points. But for simplicity, we will stick to the case where Σ
consists of just two points, and we’ll choose our coordinate axes so that they
have coordinates (0, 0) and (1, 0). This will still enable us to solve the notorious
problems of ancient Greece.
Proposition 5.3.9 Let (π₯, π¦) ∈ R2 . If (π₯, π¦) is constructible from {(0, 0), (1, 0)}
then there is an iterated quadratic extension of Q containing π₯ and π¦.
Proof Suppose that (π₯, π¦) is constructible from {(0, 0), (1, 0)} in π steps. If π = 0
then (π₯, π¦) is (0, 0) or (1, 0), so π₯, π¦ ∈ Q, and Q is trivially an iterated quadratic
extension of Q.
Now let π ≥ 1. Suppose inductively that each coordinate of each point
constructible from {(0, 0), (1, 0)} in < π steps lies in some iterated quadratic
extension of Q. By definition, (π₯, π¦) is an intersection point of two distinct
lines/circles through points constructible in < π steps. By inductive hypothesis,
each coordinate of each of those points lies in some iterated quadratic extension of
Q, so by Lemma 5.3.8, there is an iterated quadratic extension πΏ of Q containing
all the points’ coordinates. The coefficients in the equations of the lines/circles
then also lie in πΏ.
We now show that deg πΏ (π₯) ∈ {1, 2}.
If (π₯, π¦) is the intersection point of two distinct lines, then π₯ and π¦ satisfy two
linearly independent equations
ππ₯ + ππ¦ + π = 0,
π π₯ + π ′ π¦ + π′ = 0
′
with π, π, π, π′, π′, π′ ∈ πΏ. Solving gives π₯ ∈ πΏ. (In more detail, π₯ is a rational
function of π, π, . . .—write it down if you want!—and so π₯ ∈ πΏ.)
If (π₯, π¦) is an intersection point of a line and a circle, then
ππ₯ + ππ¦ + π = 0,
2
2
π₯ + π¦ + ππ₯ + ππ¦ + π = 0
with π, π, π, π, π, π ∈ πΏ. If π = 0 then π ≠ 0 and π₯ = −π/π ∈ πΏ. Otherwise, we
can eliminate π¦ to give a quadratic over πΏ satisfied by π₯, so that deg πΏ (π₯) ∈ {1, 2}.
If (π₯, π¦) is an intersection point of two circles, then
π₯ 2 + π¦ 2 + ππ₯ + ππ¦ + π = 0,
π₯ 2 + π¦ 2 + π ′π₯ + π′ π¦ + π ′ = 0
with π, π, π , π ′, π′, π ′ ∈ πΏ. Subtracting, we reduce to the case of a line and a circle,
again giving deg πΏ (π₯) ∈ {1, 2}.
80
(π₯, π¦)
(0, 0)
(1, 0)
Figure 5.3: The impossibility of trisecting 60β¦ .
Hence deg πΏ (π₯) ∈ {1, 2}. If deg πΏ (π₯) = 1 then π₯ ∈ πΏ, and πΏ is an iterated
quadratic extension of Q. If deg πΏ (π₯) = 2, i.e. [πΏ (π₯) : πΏ] = 2, then πΏ(π₯) is an
iterated quadratic extension of Q. In either case, π₯ lies in some iterated quadratic
extension of Q. The same is true of π¦. Hence by Lemma 5.3.8, there is an iterated
quadratic extension of Q containing π₯ and π¦. This completes the induction.
β‘
Theorem 5.3.10 Let (π₯, π¦) ∈ R2 . If (π₯, π¦) is constructible from {(0, 0), (1, 0)}
then π₯ and π¦ are algebraic over Q, and their degrees over Q are powers of 2.
Proof By Proposition 5.3.9, there is an iterated quadratic extension π of Q with
π₯ ∈ π. Then [π : Q] = 2π for some π ≥ 0, by the tower law. But then
degQ (π₯) = [Q(π₯) : Q] divides 2π by Corollary 5.1.19, and is therefore a power of
2. And similarly for π¦.
β‘
Now we solve the problems of ancient Greece.
Proposition 5.3.11 The angle cannot be trisected by ruler and compass.
Proof Suppose it can be. Construct an equilateral triangle with (0, 0) and (1, 0)
as two of its vertices (which can be done by ruler and compass; Figure 5.3).
Trisect the angle of the triangle at (0, 0). Plot the point (π₯, π¦) where the trisector
meets the circle with centre (0, 0) through (1, 0). Then π₯ = cos(π/9), so by
Theorem 5.3.10, degQ (cos(π/9)) is a power of 2. But you showed in Assignment 2
that degQ (cos(π/9)) = 3, a contradiction.
β‘
Proposition 5.3.12 The cube cannot be duplicated by ruler and compass.
Proof Suppose it can be. Since (0, 0) and (1, 0)
√3 are distance 1 apart, we can
construct from them two points π΄ and π΅ distance
√3 2 apart. From√3 π΄ and π΅ we can
construct, using ruler and compass, the point ( 2, 0). So degQ ( 2) is a power of
√3
2, by Theorem 5.3.10. But degQ ( 2) = 3 by Example 5.1.11, a contradiction. β‘
81
Proposition 5.3.13 The circle cannot be squared by ruler and compass.
This one is the most outrageously impossible, yet the hardest to prove.
Proof Suppose it can be. Since the circle with centre (0, 0) through (1, 0) √has
area π, we can construct by ruler and compass a square with side-length
π,
√
and from that, we√can construct by ruler and compass the point ( π, 0). So by
Theorem 5.3.10, π is algebraic over Q with degree a power of 2. Since Q is a
subfield of C, it follows that π is algebraic over Q. But it is a (hard) theorem that
π is transcendental over Q.
β‘
Digression 5.3.14 Stewart has a nice alternative approach to all this, in his
Chapter 7. He treats the plane as the complex plane, and he shows that the
set of all points in C constructible from 0 and 1 is a subfield. In fact, it is the
smallest subfield of C closed under taking square roots. He calls it Qpy , the
‘Pythagorean closure’ of Q. It can also be described as the set of complex
numbers contained in some iterated quadratic extension of Q.
There is one more famous ruler and compass problem: for which integers π is
the regular π-sided polygon constructible, starting from just a pair of points in the
plane?
The answer has to do with Fermat primes, which are prime numbers of the
form 2π’ + 1 for some π’ ≥ 1. A little exercise in number theory shows that if 2π’ + 1
is prime then π’ must itself be a power of 2. The only known Fermat primes are
0
22 + 1 = 3,
1
22 + 1 = 5,
2
22 + 1 = 17,
3
22 + 1 = 257,
4
22 + 1 = 65537.
Whether there are any others is a longstanding open question. In any case, it can
be shown that the regular π-sided polygon is constructible if and only if
π = 2π π 1 · · · π π
for some π, π ≥ 0 and distinct Fermat primes π 1 , . . . , π π .
We will not do the proof, but it involves cyclotomic polynomials. A glimpse
of the connection: let π be a prime such that the regular π-sided polygon is
constructible. Consider the regular π-sided polygon inscribed in the unit circle
in C, with one of its vertices at 1. Then another vertex is at π 2ππ/π , and from
constructibility, it follows that degQ (π 2ππ/π ) is a power of 2. But we saw in
Example 5.1.6(ii) that degQ (π 2ππ/π ) = π − 1. So π − 1 is a power of 2, that is,
π is a Fermat prime. Field theory, number theory and Euclidean geometry come
together!
82
Chapter 6
Splitting fields
Introduction to
Week 6
In Chapter 1, we met a definition of the symmetry group of a polynomial over Q.
It was phrased in terms of conjugate tuples, it was possibly a little mysterious, and
it was definitely difficult to work with (e.g. we couldn’t compute the symmetry
group of 1 + π‘ + π‘ 2 + π‘ 3 + π‘ 4 ).
In this chapter, we’re going to give a different but equivalent definition of the
symmetry group of a polynomial. It’s a two-step process:
1. We show how every polynomial π over πΎ gives rise to an extension of πΎ,
called the ‘splitting field’ of π .
2. We show how every field extension has a symmetry group.
The symmetry group, or ‘Galois group’, of a polynomial is then defined to be the
symmetry group of its splitting field extension.
How does these two steps work?
1. When πΎ = Q, the splitting field of π is the smallest subfield of C containing
all the complex roots of π . For a general field πΎ, it’s constructed by adding
the roots of π one at a time, using simple extensions, until we obtain an
extension of πΎ in which π splits into linear factors.
2. The symmetry group of a field extension π : πΎ is defined as the group of
automorphisms of π over πΎ. This is the same idea you’ve seen many times
before, for symmetry groups of other mathematical objects.
Why bother? Why not define the symmetry group of π directly, as in Chapter 1?
• Because this strategy works over every field πΎ, not just Q.
• Because there are field extensions that do not arise from a polynomial, and
their symmetry groups are sometimes important. For example, an important
83
structure in number theory, somewhat mysterious to this day, is the symmetry
group of the algebraic numbers Q over Q.
• Because using abstract algebra means you can cut down on explicit calculations with polynomials. (By way of analogy, you’ve seen how abstract
linear algebra with vector spaces and linear maps allows you to cut down on
calculations with matrices.) It also reveals connections with other parts of
mathematics.
6.1
Extending homomorphisms
In your degree so far, you’ll have picked up the general principle that for many
kinds of mathematical object (such as groups, rings, fields, vector spaces, modules,
metric spaces, topological spaces, measure spaces, . . . ), it’s important to consider
the appropriate notion of mapping between them (such as homomorphisms, linear
maps, continuous maps, . . . ). And since Chapter 4, you’ve known that the basic
objects of Galois theory are field extensions.
So it’s no surprise that sooner or later, we have to think about mappings from
one field extension to another. That moment is now. We’ll need what’s in this
section in order to establish fundamental facts about splitting fields.
When we think about a field extension π : πΎ, we generally regard the field
πΎ as our starting point and π as a field that extends it. Similarly, we might start
with a homomorphism π : πΎ → πΎ ′ between fields, together with extensions π of
πΎ and π ′ of πΎ ′, and look for a homomorphism π → π ′ that extends π. The
language is as follows.
Definition 6.1.1 Let π : πΎ → π and π′ : πΎ ′ → π ′ be field extensions. Let
π : πΎ → πΎ ′ be a homomorphism of fields. A homomorphism π : π → π ′
extends π if the square
π
Extension problems
πO
/ π′
O
π′
π
/ πΎ′
πΎ
π
commutes (π β¦ π = π′ β¦ π).
Here I’ve used the strict definition of a field extension as a homomorphism π
of fields (Definition 4.1.1). Most of the time we view πΎ as a subset of π and πΎ ′
as a subset of π ′, with π and π′ being the inclusions. In that case, for π to extend
π just means that
π(π) = π(π) for all π ∈ πΎ.
84
Examples 6.1.2
i. Let π and π ′ be two extensions of a field πΎ. For a
homomorphism π : π → π ′ to extend idπΎ means that π is a homomorphism
over πΎ.
ii. The conjugation homomorphism C → C extends the conjugation homomorphism Q(π) → Q(π).
The basic questions about extending homomorphisms are: given the two field
extensions and the homomorphism π, is there some π that extends π? If so, how
many extensions π are there?
We’ll get to these questions later. In this section, we simply prove two general
results about extensions of field homomorphisms.
Recall that any ring homomorphism π : π
→ π induces a homomorphism
π∗ : π
[π‘] → π[π‘] (Definition 3.1.7). To reduce clutter, I’ll write π∗ ( π ) as π∗ π .
Explanation of
Lemma 6.1.3
π
πΌ
πO
π
πΎ
π
/ π ′ π(πΌ)
O
/ πΎ ′ π∗ π
Lemma 6.1.3 Let π : πΎ and π ′ : πΎ ′ be field extensions, let π : πΎ → πΎ ′ be
a homomorphism, and let π : π → π ′ be a homomorphism extending π. Let
πΌ ∈ π and π (π‘) ∈ πΎ [π‘]. Then
π (πΌ) = 0 ⇐⇒ (π∗ π )(π(πΌ)) = 0.
Í
Í
Proof Write π (π‘) = π ππ π‘ π , where ππ ∈ πΎ. Then (π∗ π )(π‘) = π π(ππ )π‘ π ∈ πΎ ′ [π‘],
so
∑οΈ
∑οΈ
(π∗ π )(π(πΌ)) =
π(ππ )π(πΌ) π =
π(ππ )π(πΌ) π = π( π (πΌ)),
π
π
where the second equality holds because π extends π. Since π is injective
(Lemma 2.3.3), the result follows.
β‘
Example 6.1.4 Let π and π ′ be extensions of a field πΎ, and let π : π → π ′ be a
homomorphism over πΎ. Then the annihilating polynomials of an element πΌ ∈ π
are the same as those of π(πΌ). This is the case π = idπΎ of Lemma 6.1.3.
Exercise 6.1.5 Show that if a ring homomorphism π is injective then
so is π∗ , and if π is an isomorphism then so is π∗ .
An isomorphism between fields, rings, groups, vector spaces, etc., can be
understood as simply a renaming of the elements. For example, if I tell you that
the ring π
is left Noetherian but not right Artinian, and that π is isomorphic to π
,
then you can deduce that π is left Noetherian but not right Artinian without having
the slightest idea what those words mean. Just as long as they don’t depend on the
names of the elements of the ring concerned (which such definitions never do),
you’re fine.
85
Proposition 6.1.6 Let π : πΎ → πΎ ′ be an isomorphism of fields. Let πΎ (πΌ) : πΎ be
a simple extension where πΌ has minimal polynomial π over πΎ, and let πΎ ′ (πΌ′) : πΎ ′
be a simple extension where πΌ′ has minimal polynomial π∗ π over πΎ ′. Then
there is exactly one isomorphism π : πΎ (πΌ) → πΎ ′ (πΌ′) that extends π and satisfies
π(πΌ) = πΌ′.
Diagram:
πΎ (πΌ)
O
πΎ
π
/ πΎ ′ (πΌ′)
O
π
/ πΎ′
We often use a dotted arrow to denote a map whose existence is part of the
conclusion of a theorem.
Proof View πΎ ′ (πΌ′) as an extension of πΎ via the composite homomorphism
π
πΎ −→ πΎ ′ → πΎ ′ (πΌ′). Then the minimal polynomial of πΌ′ over πΎ is π. (If
this isn’t intuitively clear to you, think of the isomorphism π as renaming.) Hence
by the classification of simple extensions, Theorem 4.3.16, there is exactly one
isomorphism π : πΎ (πΌ) → πΎ ′ (πΌ′) over πΎ such that π(πΌ) = πΌ′. The result follows.β‘
6.2
Existence and uniqueness of splitting fields
Let π be a polynomial over a field πΎ. Informally, a splitting field for π is an
extension of πΎ where π has all its roots, and which is no bigger than it needs to be.
Warning 6.2.1 If π is irreducible, we know how to create an extension
of πΎ where π has at least one root: take the simple extension πΎ [π‘]/β¨ π β©,
in which the equivalence class of π‘ is a root of π (Lemma 4.3.1(i)).
But πΎ [π‘]/β¨ π β© is not usually a splitting field for π . For example, take
πΎ = Q and π (π‘) = π‘ 3 − 2, as in Warning 4.3.19. Write π for the real
cube root of 2. (Half the counterexamples in Galois theory involve the
real cube root of 2.) Then Q[π‘]/β¨ π β© is isomorphic to the subfield Q(π)
of R, which only contains one root of π : the other two are non-real,
hence not in Q(π).
Definition 6.2.2 Let π be a polynomial over a field π. Then π splits in π if
π (π‘) = π½(π‘ − πΌ1 ) · · · (π‘ − πΌπ )
for some π ≥ 0 and π½, πΌ1 , . . . , πΌπ ∈ π.
86
Equivalently, π splits in π if all its irreducible factors in π [π‘] are linear.
Examples 6.2.3
i. A field π is algebraically closed if and only if every polynomial over π splits in π.
√
ii. Let π (π‘) = π‘ 4 − 4π‘ 2 − 5. Then π splits in Q(π, 5), since
π (π‘) = (π‘ 2 + 1)(π‘ 2 − 5)
√
√
= (π‘ − π)(π‘ + π)(π‘ − 5)(π‘ + 5).
But π does not split in Q(π), as its factorization into irreducibles in Q(π) [π‘]
is
π (π‘) = (π‘ − π)(π‘ + π)(π‘ 2 − 5),
which contains a nonlinear factor.
Warning 6.2.4 As Example 6.2.3(ii) shows, a polynomial over
π may have one root or even several roots in π, but still not split in π.
Example 6.2.5 Let π = F2 (πΌ), where πΌ is a root of π (π‘) = 1 + π‘ + π‘ 2 , as in
Example 4.3.17(ii). We have
π (1 + πΌ) = 1 + (1 + πΌ) + (1 + 2πΌ + πΌ2 ) = 1 + πΌ + πΌ2 = 0,
so π has two distinct roots in π, giving
π (π‘) = (π‘ − πΌ)(π‘ − (1 + πΌ))
in π [π‘]. Hence π splits in π.
In this example, adjoining one root of π gave us a second root for free. But
this doesn’t typically happen (Warning 6.2.1).
Definition 6.2.6 Let π be a nonzero polynomial over a field πΎ. A splitting field
of π over πΎ is an extension π of πΎ such that:
i. π splits in π;
ii. π = πΎ (πΌ1 , . . . , πΌπ ), where πΌ1 , . . . , πΌπ are the roots of π in π.
Exercise 6.2.7 Show that (ii) can equivalently be replaced by: ‘if πΏ
is a subfield of π containing πΎ, and π splits in πΏ, then πΏ = π’.
87
Examples 6.2.8
i. Let 0 ≠ π ∈ Q[π‘]. Write πΌ1 , . . . , πΌπ for the complex roots
of π . Then Q(πΌ1 , . . . , πΌπ ), the smallest subfield of C containing πΌ1 , . . . , πΌπ ,
is a splitting field of π over Q.
Splitting fields over Q are easy because we have a ready-made algebraically
closed field containing Q, namely, C.
ii. If a polynomial π ∈ πΎ [π‘] splits in πΎ then πΎ itself is a splitting field of π
over πΎ. For instance, since C is algebraically closed, it is a splitting field of
every nonzero polynomial over C.
iii. Let π (π‘) = π‘ 3 − 2 ∈ Q[π‘]. Its complex roots are π, ππ and π2 π, where π is
the real cube root of 2 and π = π 2ππ/3 . Hence a splitting field of π over Q is
Q(π, ππ, π2 π) = Q(π, π).
Now degQ (π) = 3 as π is irreducible, and degQ (π) = 2 as π has minimal
polynomial 1 + π‘ + π‘ 2 . By an argument like that in Example 5.1.22, it follows
that [Q(π, π) : Q] = 6. On the other hand, [Q(π) : Q] = 3. So again, the
extension we get by adjoining all the roots of π is bigger than the one we get
by adjoining just one root of π .
iv. Take π (π‘) = 1 + π‘ + π‘ 2 ∈ F2 [π‘], as in Example 6.2.5. By Theorem 5.1.5(i),
{1, πΌ} is a basis of F2 (πΌ) over F2 , so
F2 (πΌ) = {0, 1, πΌ, 1 + πΌ}
= F2 ∪ {the roots of π in F2 (πΌ)}.
Hence F2 (πΌ) is a splitting field of π over F2 .
Exercise 6.2.9 In Example 6.2.8(iii), I said that Q(π, ππ, π2 π) =
Q(π, π). Why is that true?
Our mission for the rest of this section is to show that every nonzero polynomial
π has exactly one splitting field. So that’s actually two tasks: first, show that π has
at least one splitting field, then, show that π has only one splitting field. The first
task is easy, and in fact we prove a little bit more:
Lemma 6.2.10 Let π ≠ 0 be a polynomial over a field πΎ. Then there exists a
splitting field π of π over πΎ such that [π : πΎ] ≤ deg( π )!.
Proof We prove this by induction on deg( π ), for all fields πΎ simultaneously.
If deg( π ) = 0 then πΎ is a splitting field of π over πΎ, and the result holds
trivially.
88
Now suppose that deg( π ) ≥ 1. We may choose an irreducible factor π of
π . By Theorem 4.3.16, there is an extension πΎ (πΌ) of πΎ with π(πΌ) = 0. Then
(π‘ − πΌ) | π (π‘) in πΎ (πΌ) [π‘], giving a polynomial π(π‘) = π (π‘)/(π‘ − πΌ) over πΎ (πΌ).
We have deg(π) = deg( π ) − 1, so by inductive hypothesis, there is a splitting
field π of π over πΎ (πΌ) with [π : πΎ (πΌ)] ≤ deg(π)!. Then π is a splitting field of
π over πΎ. (Check that you understand why.) Also, by the tower law,
[π : πΎ] = [π : πΎ (πΌ)] [πΎ (πΌ) : πΎ] ≤ (deg( π ) − 1)! · deg(π) ≤ deg( π )!,
completing the induction.
β‘
Proving that every polynomial has only one splitting field is harder. As ever,
‘only one’ has to be understood up to isomorphism: after all, if you’re given a
splitting field, you can always rename its elements to get an isomorphic copy that’s
not literally identical to the original one. But isomorphism is all that matters.
Our proof of the uniqueness of splitting fields depends on the following result,
which will also be useful for other purposes as we head towards the fundamental
theorem of Galois theory.
Proposition 6.2.11 Let π : πΎ → πΎ ′ be an isomorphism of fields, let 0 ≠ π ∈ πΎ [π‘],
let π be a splitting field of π over πΎ, and let π ′ be a splitting field of π∗ π over
πΎ ′. Then:
π
πO
π
πΎ
π
/ π′
O
i. there exists an isomorphism π : π → π ′ extending π;
/ πΎ ′ π∗ π
ii. there are at most [π : πΎ] such extensions π.
We’ll often use this result in the case where πΎ ′ = πΎ and π = idπΎ . (What does
it say then?)
Proof We prove both statements by induction on deg( π ). If deg( π ) = 0 then both
field extensions are trivial, so there is exactly one isomorphism π extending π.
Now suppose that deg( π ) ≥ 1. We can choose a monic irreducible factor π of
π . Then π splits in π since π does and π | π ; choose a root πΌ ∈ π of π. We have
π (πΌ) = 0, so (π‘ − πΌ) | π (π‘) in πΎ (πΌ) [π‘], giving a polynomial π(π‘) = π (π‘)/(π‘ − πΌ)
over πΎ (πΌ). Then π is a splitting field of π over πΎ (πΌ), and deg(π) = deg( π ) − 1.
Also, π∗ π splits in π ′ since π∗ π does and π∗ π | π∗ π . Write πΌ1′ , . . . , πΌ′π for
the distinct roots of π∗ π in π ′. Note that
1 ≤ π ≤ deg(π∗ π) = deg(π).
Counting
isomorphisms: the
proof of
Proposition 6.2.11
(6.1)
Since π∗ is an isomorphism, π∗ π is monic and irreducible, and is therefore the
minimal polynomial of πΌ′π for each π ∈ {1, . . . , π }. Hence by Proposition 6.1.6,
89
for each π, there is a unique isomorphism π π : πΎ (πΌ) → πΎ ′ (πΌ′π ) that extends π and
satisfies π π (πΌ) = πΌ′π . (See diagram below.)
For each π ∈ {1, . . . , π }, we have a polynomial
π π∗ (π) =
π π∗ ( π )
π∗ π
=
π π∗ (π‘ − πΌ) π‘ − πΌ′π
over πΎ ′ (πΌ′π ), and π ′ is a splitting field of π∗ π over πΎ ′, so π ′ is also a splitting
field of π π∗ (π) over πΎ ′ (πΌ′π ).
To prove that there is at least one isomorphism π extending π, choose any
π ∈ {1, . . . , π } (as we may since π ≥ 1). By applying the inductive hypothesis to
π and π π , there is an isomorphism π extending π π :
π
/ π′
O
ππ
/ πΎ ′ (πΌ′ )
O π
πO
πΎ (πΌ)
O
/ πΎ′
πΎ
π
But then π also extends π, as required.
To prove there are at most [π : πΎ] isomorphisms π : π → π ′ extending
π, first note that any such π satisfies (π∗ π)(π(πΌ)) = 0 (by Lemma 6.1.3), so
π(πΌ) = πΌ′π for some π ∈ {1, . . . , π }. Hence
(number of isos π extending π) =
π
∑οΈ
(number of isos π extending π such that π(πΌ) = πΌ′π ).
π=1
If π extends π then ππΎ = ππΎ = πΎ ′, and if also π(πΌ) = πΌ′π then π(πΎ (πΌ)) = πΎ ′ (πΌ′π ).
Since homomorphisms of fields are injective, π then restricts to an isomorphism
πΎ (πΌ) → πΎ ′ (πΌ′π ) satisfying πΌ β¦→ πΌ′π . By the uniqueness part of Proposition 6.1.6,
this restricted isomorphism must be π π . Thus, π extends π π . Hence
(number of isos π extending π) =
π
∑οΈ
(number of isos π extending π π ).
π=1
For each π, the number of isomorphisms π extending π π is ≤ [π : πΎ (πΌ)], by
inductive hypothesis. So, using the tower law and (6.1),
(number of isos π extending π) ≤ π · [π : πΎ (πΌ)] = π ·
completing the induction.
[π : πΎ]
≤ [π : πΎ],
deg(π)
β‘
90
Exercise 6.2.12 Why does the proof of Proposition 6.2.11 not show
that there are exactly [π : πΎ] isomorphisms π extending π? How
could you strengthen the hypotheses in order to obtain that conclusion?
(The second question is a bit harder, and we’ll see the answer next
week.)
This brings us to the foundational result on splitting fields. Recall that an
automorphism of an object π is an isomorphism π → π.
Theorem 6.2.13 Let π be a nonzero polynomial over a field πΎ. Then:
i. there exists a splitting field of π over πΎ;
ii. any two splitting fields of π are isomorphic over πΎ;
iii. when π is a splitting field of π over πΎ,
(number of automorphisms of π over πΎ) ≤ [π : πΎ] ≤ deg( π )!.
Proof Part (i) is immediate from Lemma 6.2.10, and part (ii) follows from Proposition 6.2.11 by taking πΎ ′ = πΎ and π = idπΎ . The first inequality in (iii) follows
from Proposition 6.2.11 by taking πΎ ′ = πΎ, π ′ = π and π = idπΎ , and the second
follows from Lemma 6.2.10.
β‘
Up to now we have been saying ‘a’ splitting field. Parts (i) and (ii) of Theorem 6.2.13 give us the right to speak of the splitting field of a given polynomial π
over a given field πΎ. We write it as SFπΎ ( π ).
We finish with a left over lemma that will be useful later.
Lemma 6.2.14
i. Let π : π : πΎ be field extensions, 0 ≠ π ∈ πΎ [π‘], and
π ⊆ π. Suppose that π is the splitting field of π over πΎ. Then π(π ) is the
splitting field of π over πΎ (π ).
ii. Let π ≠ 0 be a polynomial over a field πΎ, and let πΏ be a subfield of SFπΎ ( π )
containing πΎ (so that SFπΎ ( π ) : πΏ : πΎ). Then SFπΎ ( π ) is the splitting field of
π over πΏ.
Proof For (i), π splits in π, hence in π(π ). Writing π for the set of roots of π
in π, we have π = πΎ (π) and so π(π ) = πΎ (π)(π ) = πΎ (π ∪ π ) = πΎ (π )(π); that
is, π(π ) is generated over πΎ (π ) by π. This proves (i), and (ii) follows by taking
π = SFπΎ ( π ) and π = πΏ.
β‘
91
6.3
The Galois group
Before you get stuck into this section, you may want to review Section 2.1, especially the parts about homomorphisms πΊ → Sym(π). We’ll need all of it.
What gives Galois theory its special flavour is the use of groups to study fields
and polynomials. Here is the central definition.
Definition 6.3.1 The Galois group Gal(π : πΎ) of a field extension π : πΎ is the
group of automorphisms of π over πΎ, with composition as the group operation.
Exercise 6.3.2 Check that this really does define a group.
In other words, an element of Gal(π : πΎ) is an isomorphism π : π → π such
that π (π) = π for all π ∈ πΎ.
Examples 6.3.3
i. What is Gal(C : R)? Certainly the identity is an automorphism of C over R. So is complex conjugation π
, as implicitly shown
in the first proof of Lemma 1.1.2. So {id, π
} ⊆ Gal(C : R). I claim that
Gal(C : R) has no other elements. For let π ∈ Gal(C : R). Then
(π (π)) 2 = π (π 2 ) = π (−1) = −π (1) = −1
as π is a homomorphism, so π (π) = ±π. If π (π) = π then π = id, by
Lemma 4.3.6 and the fact that C = R(π). Similarly, if π (π) = −π then π = π
.
So Gal(C : R) = {id, π
} πΆ2 .
ii. Let π be the real cube root of 2. For each π ∈ Gal(Q(π) : Q), we have
(π (π)) 3 = π (π 3 ) = π (2) = 2
and π (π) ∈ Q(π) ⊆ R, so π (π) = π. It follows from Lemma 4.3.6 that π = id.
Hence Gal(Q(π) : Q) is trivial.
Exercise 6.3.4 Prove that Gal(Q(π 2ππ/3 ) : Q) = {id, π
}, where π
(π§) =
π§. (Hint: imitate Example 6.3.3(i).)
The Galois group of a polynomial is defined to be the Galois group of its
splitting field extension:
Definition 6.3.5 Let π be a nonzero polynomial over a field πΎ. The Galois group
GalπΎ ( π ) of π over πΎ is Gal(SFπΎ ( π ) : πΎ).
92
So the definitions fit together like this:
polynomial β¦−→ field extension β¦−→ group.
We will soon prove that Definition 6.3.5 is equivalent to the definition of Galois
group in Chapter 1, where we went straight from polynomials to groups.
Theorem 6.2.13(iii) says that
| GalπΎ ( π )| ≤ [SFπΎ ( π ) : πΎ] ≤ deg( π )!.
(6.2)
In particular, GalπΎ ( π ) is always a finite group.
Examples 6.3.6
i. If π ∈ πΎ [π‘] splits in πΎ then SFπΎ ( π ) = πΎ (Example 6.2.8(ii)), so GalπΎ ( π ) is trivial. In particular, the Galois group of
any polynomial over an algebraically closed field is trivial.
ii. GalQ (π‘ 2 + 1) = Gal(Q(π) : Q) = {id, π
} πΆ2 , where π
is complex conjugation on Q(π). The second equality is proved by the same argument as in
Example 6.3.3(i), replacing C : R by Q(π) : Q.
iii. Generally, let π ∈ Q[π‘]. We can view SFQ ( π ) as the subfield of C generated
by the complex roots of π , and if πΌ ∈ C is a root of π then so is πΌ. Hence
complex conjugation, as an automorphism of C, restricts to an automorphism
π
of SFQ ( π ).
Calculating the
Galois group with
bare hands, part 1
Calculating the
Galois group with
bare hands, part 2
If all the complex roots of π are real then π
= id ∈ GalQ ( π ). Otherwise, π
is an element of GalQ ( π ) of order 2.
iv. Let π (π‘)√ = (π‘ 2 + 1)(π‘ 2 − 2). Then GalQ ( π ) is the group of automorphisms
of Q(π, 2) over Q. Similar arguments to those in Examples
√
√6.3.3 show that
every π ∈ GalQ ( π ) must satisfy π (π) = ±π and π ( 2) = ± 2, and that the
two choices of sign determine π completely. And one can show that all four
choices are possible, so that | GalQ ( π )| = 4. There are two groups of order
four, πΆ4 and πΆ2 × πΆ2 . But each element of GalQ ( π ) has order 1 or 2, so
GalQ ( π ) is not πΆ4 , so GalQ ( π ) πΆ2 × πΆ2 .
I’ve been sketchy with the details here, because it’s not really sensible to try
to calculate Galois groups until we have a few more tools at our disposal.
We start to assemble them now.
By definition, GalπΎ ( π ) acts on SFπΎ ( π ) (Example 2.1.2(ii)). The action is
(π, πΌ) β¦→ π (πΌ)
(π ∈ GalπΎ ( π ), πΌ ∈ SFπΎ ( π )). In the examples so far, we’ve seen that if πΌ is a root
of π then so is π (πΌ) for every π ∈ GalπΎ ( π ). This is true in general: the action
of GalπΎ ( π ) on SFπΎ ( π ) restricts to an action on the set of roots. In a slogan: the
Galois group permutes the roots.
93
Lemma 6.3.7 Let π be a nonzero polynomial over a field πΎ. Then the action of
GalπΎ ( π ) on SFπΎ ( π ) restricts to an action on the set of roots of π in SFπΎ ( π ).
Terminology: given a group πΊ acting on a set π and a subset π΄ ⊆ π, the action
restricts to π΄ if ππ ∈ π΄ for all π ∈ πΊ and π ∈ π΄.
Proof We have to show that if π ∈ GalπΎ ( π ) and πΌ is a root of π in SFπΎ ( π ) then
π (πΌ) is also a root. This follows from Example 6.1.4.
β‘
The action of the
Galois group
Better still, the Galois group acts faithfully on the roots:
Lemma 6.3.8 Let π be a nonzero polynomial over a field πΎ. Then the action of
GalπΎ ( π ) on the roots of π is faithful.
Proof Write π for the set of roots of π in SFπΎ ( π ). Then SFπΎ ( π ) = πΎ (π). Hence
by Lemma 4.3.6, if π ∈ GalπΎ ( π ) with π (π₯) = π₯ for all π₯ ∈ π, then π = id.
β‘
In other words, an element of the Galois group of π is completely determined
by how it permutes the roots of π . So you can view elements of the Galois group
as being permutations of the roots.
However, not every permutation of the roots belongs to the Galois group.
To understand the situation, recall Remark 2.1.13, which tells us the following.
Suppose that π ∈ πΎ [π‘] has distinct roots πΌ1 , . . . , πΌ π in its splitting field. For each
π ∈ GalπΎ ( π ), there is a permutation ππ ∈ π π defined by
π (πΌπ ) = πΌππ (π)
(π ∈ {1, . . . , π }). Then GalπΎ ( π ) is isomorphic to the subgroup {ππ : π ∈ GalπΎ ( π )}
of π π (and this is indeed a subgroup). The isomorphism is given by π β¦→ ππ .
All this talk of the Galois group as a subgroup of π π may have set your antennae
tingling. Back in Chapter 1, we provisionally defined the Galois group to be a
certain subgroup of π π (Definition 1.2.1). We can now show that the two definitions
are equivalent.
That definition was in terms of conjugacy. Let’s now make the concept of
conjugacy official, also generalizing from Q to an arbitrary field.
Definition 6.3.9 Let π : πΎ be a field extension, let π ≥ 0, and let (πΌ1 , . . . , πΌ π ) and
(πΌ1′ , . . . , πΌ′π ) be π-tuples of elements of π. Then (πΌ1 , . . . , πΌ π ) and (πΌ1′ , . . . , πΌ′π )
are conjugate over πΎ if for all π ∈ πΎ [π‘1 , . . . , π‘ π ],
π(πΌ1 , . . . , πΌ π ) = 0 ⇐⇒ π(πΌ1′ , . . . , πΌ′π ) = 0.
In the case π = 1, we omit the brackets and say that πΌ and πΌ′ are conjugate to mean
that (πΌ) and (πΌ′) are.
94
We now show that the two definitions of the Galois group of π are equivalent.
Proposition 6.3.10 Let π be a nonzero polynomial over a field πΎ, with distinct
roots πΌ1 , . . . , πΌ π in SFπΎ ( π ). Then
{π ∈ π π : (πΌ1 , . . . , πΌ π ) and (πΌπ(1) , . . . , πΌπ(π) ) are conjugate over πΎ }
(6.3)
is a subgroup of π π isomorphic to GalπΎ ( π ).
Proof As above, each π ∈ GalπΎ ( π ) gives rise to a permutation ππ ∈ π π , defined
by π (πΌπ ) = πΌππ (π) . For the purposes of this proof, let us say that a permutation
π ∈ π π is ‘good’ if it belongs to the set (6.3). By Remark 2.1.13, it suffices to
show that a permutation π is good if and only if π = ππ for some π ∈ GalπΎ ( π ).
First suppose that π = ππ for some π ∈ GalπΎ ( π ). For every π ∈ πΎ [π‘1 , . . . , π‘ π ],
π(πΌπ(1) , . . . , πΌπ(π) ) = π(π (πΌ1 ), . . . , π (πΌ π )) = π ( π(πΌ1 , . . . , πΌ π )),
where the first equality is by definition of ππ and the second is because π is a
homomorphism over πΎ. But π is an isomorphism, so it follows that
π(πΌπ(1) , . . . , πΌπ(π) ) = 0 ⇐⇒ π(πΌ1 , . . . , πΌ π ) = 0.
Hence π is good.
Conversely, suppose that π is good. By Corollary 5.1.14, every element of
SFπΎ ( π ) can be expressed as π(πΌ1 , . . . , πΌ π ) for some π ∈ πΎ [π‘1 , . . . , π‘ π ]. Now for
π, π ∈ πΎ [π‘1 , . . . , π‘ π ], we have
π(πΌ1 , . . . , πΌ π ) = π(πΌ1 , . . . , πΌ π ) ⇐⇒ π(πΌπ(1) , . . . , πΌπ(π) ) = π(πΌπ(1) , . . . , πΌπ(π) )
(by applying Definition 6.3.9 of conjugacy with π − π as the ‘π’). So there is a
well-defined, injective function π : SFπΎ ( π ) → SFπΎ ( π ) satisfying
π ( π(πΌ1 , . . . , πΌ π )) = π(πΌπ(1) , . . . , πΌπ(π) )
(6.4)
for all π ∈ πΎ [π‘1 , . . . , π‘ π ]. Moreover, π is surjective because π is a permutation,
and π (π) = π for all π ∈ πΎ (by taking π = π in (6.4)), and π (πΌπ ) = πΌπ(π) for all
π (by taking π = π‘π in (6.4)). You can check that π is a homomorphism of fields.
Hence π ∈ GalπΎ ( π ) with ππ = π, as required.
β‘
Exercise 6.3.11 I skipped two small bits in that proof: ‘π is surjective
because π is a permutation’ (why?), and ‘You can check that π is a
homomorphism of fields’. Fill in the gaps.
95
It’s important in Galois theory to be able to move between fields. For example,
you might start with a polynomial whose coefficients belong to one field πΎ, but
later decide to interpret the coefficients as belonging to some larger field πΏ. Here’s
what happens to the Galois group when you do that.
Corollary 6.3.12 Let πΏ : πΎ be a field extension and 0 ≠ π ∈ πΎ [π‘]. Then Gal πΏ ( π )
is isomorphic to a subgroup of GalπΎ ( π ).
Proof This follows from Proposition 6.3.10 together with the observation that if
two π-tuples are conjugate over πΏ, they are conjugate over πΎ.
β‘
Example 6.3.13 Let’s find the Galois group of π (π‘) = (π‘ 2 + 1)(π‘ 2 − 2) over Q, R
and C in turn.
In Example 6.3.6(iv), we saw that GalQ ( π ) πΆ2 × πΆ2 .
Since both roots of π‘ 2 − 2 are real, SFR ( π ) = SFR (π‘ 2 + 1) = C. So GalR ( π ) =
Gal(C : R) πΆ2 , where the last step is by Example 6.3.3(i).
Finally, GalC ( π ) is trivial since C is algebraically closed (Example 6.3.6(i)).
So as Corollary 6.3.12 predicts, GalC ( π ) is isomorphic to a subgroup of
GalR ( π ), which is isomorphic to a subgroup of GalQ ( π ).
Corollary 6.3.14 Let π be a nonzero polynomial over a field πΎ, with π distinct
roots in SFπΎ ( π ). Then |GalπΎ ( π )| divides π!.
Proof By Proposition 6.3.10, GalπΎ ( π ) is isomorphic to a subgroup of π π , which
has π! elements. The result follows from Lagrange’s theorem.
β‘
The inequalities (6.2) already gave us | GalπΎ ( π )| ≤ deg( π )!. Corollary 6.3.14
improves on this in two respects. First, it implies that | GalπΎ ( π )| ≤ π!. It’s always
the case that π ≤ deg( π ) in all cases, and π < deg( π ) if π has repeated roots in its
splitting field. A trivial example: if π (π‘) = π‘ 2 then π = 1 and deg( π ) = 2. Second,
it tells us that | GalπΎ ( π )| is not only less than or equal to π!, but a factor of it.
Galois theory is about the interplay between field extensions and groups. In
the next chapter, we’ll see that just as every field extension gives rise to a group
of automorphisms (its Galois group), every group of automorphisms gives rise to
a field extension. We’ll also go deeper into the different types of field extension:
normal extensions (the mirror image of normal subgroups) and separable extensions (which have to do with repeated roots). All of that will lead us towards the
fundamental theorem of Galois theory.
96
Chapter 7
Preparation for the fundamental
theorem
Introduction to
Week 7
Very roughly, the fundamental theorem of Galois theory says that you can tell a
lot about a field extension by looking at its Galois group. A bit more specifically,
it says that the subgroups and quotients of Gal(π : πΎ), and their orders, give
us information about the subfields of π containing πΎ, and their degrees. For
example, one part of the fundamental theorem is that
[π : πΎ] = | Gal(π : πΎ)|.
The theorem doesn’t hold for all extensions, just those that are ‘nice enough’.
Crucially, this includes splitting field extensions SFQ ( π ) : Q of polynomials π
over Q—the starting point of classical Galois theory.
Let’s dip our toes into the water by thinking about why it might be true that
[π : πΎ] = | Gal(π : πΎ)|, at least for extensions that are nice enough.
The easiest nontrivial extensions are the simple algebraic extensions, π =
πΎ (πΌ). Write π for the minimal polynomial of πΌ over πΎ and πΌ1 , πΌ2 , . . . , πΌπ for
the distinct roots of π in π. For every element π of Gal(π : πΎ), we have
π(π(πΌ)) = 0 by Example 6.1.4, and so π(πΌ) = πΌ π for some π ∈ {1, . . . , π }. On
the other hand, for each π ∈ {1, . . . , π }, there is exactly one π ∈ Gal(π : πΎ) such
that π(πΌ) = πΌ π , by Proposition 6.1.6. So | Gal(π : πΎ)| = π .
On the other hand, [π : πΎ] = deg(π). So [π : πΎ] = | Gal(π : πΎ)| if and
only if deg(π) is equal to π , the number of distinct roots of π in π. Certainly
π ≤ deg(π). But are π and deg(π) equal?
There are two reasons why √
they might not be. First, π might not split in π.
3
For√instance, if πΎ =√Q and πΌ = 2 then π(π‘) = π‘ 3 − 2, which has only one root in
3
3
Q( 2), so | Gal(Q( 2) : Q)| = 1 < 3 = deg(π). An algebraic extension is called
‘normal’ if this problem doesn’t occur, that is, if the minimal polynomial of every
element does split. That’s what Section 7.1 is about.
97
Second, we might have π < deg(π) because some of the roots of π in π are
repeated. If they are, the number π of distinct roots will be less then deg(π). An
algebraic extension is called ‘separable’ if this problem doesn’t occur, that is, if the
minimal polynomial of every element has no repeated roots in its splitting field.
That’s what Section 7.2 is about.
If we take any finite extension π : πΎ (not necessarily simple) that is both
normal and separable, then it is indeed true that | Gal(π : πΎ)| = [π : πΎ]. And in
fact, these conditions are enough to make the whole fundamental theorem work,
as we’ll see next week.
I hesitated before putting normality and separability into the same chapter,
because you should think of them in quite different ways:
• Normality has a clear conceptual meaning, and its importance was recognized by Galois himself. Despite the name, most field extensions aren’t
normal. Normality isn’t something to be taken for granted.
• In contrast, Galois never considered separability, because it holds automatically over Q (his focus), and in fact over any field of characteristic 0, as
well as any finite field. It takes some work to find an extension that isn’t
separable. You can view separability as more of a technicality.
There’s one more concept in this chapter: the ‘fixed field’ of a group of
automorphisms (Section 7.3). Every Galois theory text I’ve seen contains at least
one proof that makes you ask ‘how did anyone think of that?’ I would argue that
the proof of Theorem 7.3.3 is the one and only truly ingenious argument in this
course: maybe not the hardest, but the most ingenious. This is not a compliment.
7.1
Normality
Definition 7.1.1 An algebraic field extension π : πΎ is normal if for all πΌ ∈ π,
the minimal polynomial of πΌ splits in π.
We also say π is normal over πΎ to mean that π : πΎ is normal.
Lemma 7.1.2 Let π : πΎ be an algebraic extension. Then π : πΎ is normal if and
only if every irreducible polynomial over πΎ either has no roots in π or splits in π.
Put another way, normality means that any irreducible polynomial over πΎ with
at least one root in π has all its roots in π.
Proof Suppose that π : πΎ is normal, and let π be an irreducible polynomial over
πΎ. If π has a root πΌ in π then the minimal polynomial of πΌ is π /π, where π ∈ πΎ
98
is the leading coefficient of π . Since π : πΎ is normal, π /π splits in π, so π does
too.
Conversely, suppose that every irreducible polynomial over πΎ either has no
roots in π or splits in π. Let πΌ ∈ π. Then the minimal polynomial of πΌ has at
least one root in π (namely, πΌ), so it splits in π.
β‘
√3
Examples 7.1.3
i. Let π = 2 ∈ R, and consider Q(π) : Q. The minimal
polynomial of π over Q is π‘ 3 − 2, whose roots in C are π ∈ R and ππ, π2 π ∈
C \ R, where π = π 2ππ/3 . Since Q(π) ⊆ R, the minimal polynomial π‘ 3 − 2
does not split in Q(π). Hence Q(π) is not normal over Q.
Alternatively, using the equivalent condition in Lemma 7.1.2, Q(π) : Q is
not normal because π‘ 3 − 2 is an irreducible polynomial over Q that has a root
in Q(π) but does not split there.
What does it mean
to be normal?
One way to think about the non-normality of Q(π) : Q is as follows. The
three roots of π‘ 3 − 2 are conjugate (‘indistinguishable’) over Q, since they
have the same minimal polynomial. But if they’re indistinguishable, it
would be strange for an extension to contain some but not all of them—that
would be making a distinction between elements that are supposed to be
indistinguishable. In this sense, Q(π) : Q is ‘abnormal’.
ii. Let π be a nonzero polynomial over a field πΎ. Then SFπΎ ( π ) : πΎ is always
normal, as we shall see (Theorem 7.1.5).
iii. Every extension of degree 2 is normal (just as, in group theory, every
subgroup of index 2 is normal). You’ll be asked to show this in Workshop 4,
question 4, but you also know enough to prove it now.
Exercise 7.1.4 What happens if you drop the word ‘irreducible’ from
Lemma 7.1.2? Is it still true?
Normality of field extensions is intimately related to normality of subgroups,
and conjugacy in field extensions is also related to conjugacy in groups. (The
video ‘What does it mean to be normal?’ explains both kinds of normality and
conjugacy in intuitive terms.)
Here’s the first of our two theorems about normal extensions. It describes
which extensions arise as splitting field extensions.
Theorem 7.1.5 Let π : πΎ be a field extension. Then
π = SFπΎ ( π ) for some nonzero π ∈ πΎ [π‘] ⇐⇒ π : πΎ is finite and normal.
99
SF πO (π)
π = πΎ (πΌ1O , . . . , πΌπ )
π
/ πΎ (πΌ1 , . . . , πΌπ , π)
O
πΎ (πΏ) g
π
/ πΎ (π)
7
πΎ
Figure 7.1: Maps used in the proof that splitting field extensions are normal.
Splitting field
extensions are
normal
Proof For ⇐, suppose that π : πΎ is finite and normal. By finiteness, there is a
basis πΌ1 , . . . , πΌπ of π over πΎ, and each πΌπ is algebraic over πΎ (by Proposition 5.2.4).
For each π, let ππ be the minimal polynomial of πΌπ over πΎ; then by normality, ππ
splits in π. Hence π = π 1 π 2 · · · π π ∈ πΎ [π‘] splits in π. The set of roots of π in
π contains {πΌ1 , . . . , πΌπ }, and π = πΎ (πΌ1 , . . . , πΌπ ), so π is generated over πΎ by
the set of roots of π in π. Thus, π is a splitting field of π over πΎ.
For ⇒, take a nonzero π ∈ πΎ [π‘] such that π = SFπΎ ( π ). Write πΌ1 , . . . , πΌπ for
the roots of π in π. Then π = πΎ (πΌ1 , . . . , πΌπ ). Each πΌπ is algebraic over πΎ (since
π ≠ 0), so by Proposition 5.2.4, π : πΎ is finite.
We now show that π : πΎ is normal, which is the most substantial part of the
proof (Figure 7.1). Let πΏ ∈ π, with minimal polynomial π ∈ πΎ [π‘]. Certainly π
splits in SF π (π), so to show that π splits in π, it is enough to show that every
root π of π in SF π (π) lies in π.
Since π is a monic irreducible annihilating polynomial of π over πΎ, it is
the minimal polynomial of π over πΎ. Hence by Theorem 4.3.16, there is an
isomorphism π : πΎ (πΏ) → πΎ (π) over πΎ such that π (πΏ) = π. Now observe that:
• π = SFπΎ (πΏ) ( π ), by Lemma 6.2.14(ii);
• πΎ (πΌ1 , . . . , πΌπ , π) = SFπΎ (π) ( π ), by Lemma 6.2.14(i);
• π ∗ π = π , since π ∈ πΎ [π‘] and π is a homomorphism over πΎ.
So we can apply Proposition 6.2.11, which implies that there is an isomorphism
π : π → πΎ (πΌ1 , . . . , πΌπ , π) extending π. It is an isomorphism over πΎ, since π is.
Since πΏ ∈ πΎ (πΌ1 , . . . , πΌπ ) and π is a homomorphism over πΎ, we have π(πΏ) ∈
πΎ (π(πΌ1 ), . . . , π(πΌπ )). Now π(πΏ) = π (πΏ) = π, so π ∈ πΎ (π(πΌ1 ), . . . , π(πΌπ )).
Moreover, for each π we have π (π(πΌπ )) = 0 (by Example 6.1.4) and so π(πΌπ ) ∈
{πΌ1 , . . . , πΌπ }. Hence π ∈ πΎ (πΌ1 , . . . , πΌπ ) = π, as required.
β‘
100
Corollary 7.1.6 Let π : πΏ : πΎ be field extensions. If π : πΎ is finite and normal
then so is π : πΏ.
Proof Follows from Theorem 7.1.5 and Lemma 6.2.14(ii).
β‘
Warning 7.1.7
does not follow
that πΏ : πΎ is normal. For instance,
√3
√3 It2ππ/3
) : Q( 2) : Q. The first field is the√ splitting
consider Q( 2, π
3
3
field of π‘ − 2 over Q, and therefore normal over Q, but Q( 2) is not
(Example 7.1.3(i)).
Theorem 7.1.5 is the first of two theorems about normality. The second is to
do with the action of the Galois group of an extension.
Warning 7.1.8 By definition, the Galois group Gal(π : πΎ) of an
extension π : πΎ acts on π. But if π is the splitting field of some
polynomial π over πΎ then the action of Gal(π : πΎ) on π restricts to
an action on the roots of π (a finite set), as we saw in Section 6.3. So
there are two actions of the Galois group in play, one the restriction of
the other. Both are important.
When a group acts on a set, a basic question is: what are the orbits? For
Gal(π : πΎ) acting on π, the answer is: the conjugacy classes of π over πΎ. Or at
least, that’s the case when π : πΎ is finite and normal:
Proposition 7.1.9 Let π : πΎ be a finite normal extension and πΌ, πΌ′ ∈ π. Then
πΌ and πΌ′ are conjugate over πΎ ⇐⇒ πΌ′ = π(πΌ) for some π ∈ Gal(π : πΎ).
Proof For ⇐, let π ∈ Gal(π : πΎ) with πΌ′ = π(πΌ). Then πΌ and πΌ′ are conjugate
over πΎ, by Example 6.1.4.
For ⇒, suppose that πΌ and πΌ′ are conjugate over πΎ. Since π : πΎ is finite,
both are algebraic over πΎ, and since they are conjugate over πΎ, they have the same
minimal polynomial π ∈ πΎ [π‘]. By Theorem 4.3.16, there is an isomorphism
π : πΎ (πΌ) → πΎ (πΌ′) over πΎ such that π (πΌ) = πΌ′ (see diagram below).
By Theorem 7.1.5, π is the splitting field of some polynomial π over πΎ. Hence
π is also the splitting field of π over both πΎ (πΌ) and πΎ (πΌ′), by Lemma 6.2.14(ii).
Moreover, π ∗ π = π since π is a homomorphism over πΎ and π is a polynomial over
πΎ. So by Proposition 6.2.11(i), there is an automorphism π of π extending π:
πO
π
/π
O
πΎ (πΌ)b
π
/ πΎ (πΌ′)
<
πΎ
101
Then π ∈ Gal(π : πΎ) with π(πΌ) = π (πΌ) = πΌ′, as required.
β‘
Example 7.1.10 Consider the finite normal extension C : R. Let πΌ, πΌ′ ∈ C.
Lemma 1.1.2 states that πΌ and πΌ′ are conjugate over R if and only if πΌ′ is either
πΌ or πΌ. Example 6.3.3(i) states that Gal(C : R) = {id, π
}, where π
is complex
conjugation. This confirms Proposition 7.1.9 in the case C : R.
Proposition 7.1.9 is about the action of Gal(π : πΎ) on the whole field π, but
it has a powerful corollary involving the action of the Galois group on just the
roots of an irreducible polynomial π , in the case π = SFπΎ ( π ):
Corollary 7.1.11 Let π be an irreducible polynomial over a field πΎ. Then the
action of GalπΎ ( π ) on the roots of π in SFπΎ ( π ) is transitive.
Recall what transitive means, for an action of a group πΊ on a set π: for all
π₯, π₯ ′ ∈ π, there exists π ∈ πΊ such that ππ₯ = π₯ ′.
Proof Since π is irreducible, the roots of π in SFπΎ ( π ) all have the same minimal
polynomial, namely, π divided by its leading coefficient. So they are all conjugate
over πΎ. Since SFπΎ ( π ) : πΎ is finite and normal (by Theorem 7.1.5), the result
follows from Proposition 7.1.9.
β‘
Exercise 7.1.12 Show by example that Corollary 7.1.11 becomes false
if you drop the word ‘irreducible’.
Example 7.1.13 Let π (π‘) = 1 + π‘ + · · · + π‘ π−1 ∈ Q[π‘], where π is prime. Since
(1 − π‘) π (π‘) = 1 − π‘ π , the roots of π in C are π, π2 , . . . , π π−1 , where π = π 2ππ/π .
By Example 3.3.16, π is irreducible over Q. Hence by Corollary 7.1.11, for each
π ∈ {1, . . . , π − 1}, there is some π ∈ GalQ ( π ) such that π(π) = ππ .
This is spectacular! Until now, we’ve been unable to prove such things without
a huge amount of explicit checking, which, moreover, only works on a case-by-case
basis. For example, if you watched the video ‘Calculating Galois groups with bare
hands, part 2’, you’ll have seen how much tedious calculation went into the single
case π = 5, π = 2:
102
But the theorems we’ve proved make all this unnecessary.
In fact, for each π ∈ {1, . . . , π − 1}, there’s exactly one element ππ of GalQ ( π )
such that ππ (π) = ππ . For since SFQ ( π ) = Q(π), two elements of GalQ ( π ) that
take the same value on π must be equal. Hence
GalQ ( π ) = {π1 , . . . , π π−1 }.
In fact, GalQ ( π ) πΆ π−1 (Workshop 4, question 13).
Example 7.1.14 Let’s calculate πΊ = GalQ (π‘ 3 − 2). Since π‘ 3 − 2 has 3 distinct
roots in C, it has 3 distinct roots in its splitting field. By Proposition 6.3.10, πΊ is
isomorphic to a subgroup of π3 . Now πΊ acts transitively on the 3 roots, so it has at
least 3 elements, so it is isomorphic to either π΄3 or π3 . Since two of the roots are
non-real complex conjugates, one of the elements of πΊ is complex conjugation,
which has order 2 (Example 6.3.6(iii)). Hence 2 divides |πΊ |, forcing πΊ π3 .
We now show how a normal field extension gives rise to a normal subgroup.
Whenever in life you meet a normal subgroup, you should immediately want to
form the quotient, so we do that too.
Theorem 7.1.15 Let π : πΏ : πΎ be field extensions with π : πΎ finite and
normal.
i. πΏ : πΎ is a normal extension ⇐⇒ ππΏ = πΏ for all π ∈ Gal(π : πΎ).
ii. If πΏ : πΎ is a normal extension then Gal(π : πΏ) is a normal subgroup of
Gal(π : πΎ) and
Gal(π : πΎ)
Gal(πΏ : πΎ).
Gal(π : πΏ)
Before the proof, here’s some context and explanation.
Part (i) answers the question implicit in Warning 7.1.7: we know from Corollary 7.1.6 that π : πΏ is normal, but when is πΏ : πΎ normal? The notation ππΏ
means {π(πΌ) : πΌ ∈ πΏ}. For ππΏ to be equal to πΏ means that π fixes πΏ as a set (in
other words, permutes it within itself), not that π fixes each element of πΏ.
In part (ii), it’s true for all π : πΏ : πΎ that Gal(π : πΏ) is a subset of Gal(π : πΎ),
since
Gal(π : πΏ) = {automorphisms π of π such that π(πΌ) = πΌ for all πΌ ∈ πΏ}
⊆ {automorphisms π of π such that π(πΌ) = πΌ for all πΌ ∈ πΎ }
= Gal(π : πΎ).
And it’s always true that Gal(π : πΏ) is a subgroup of Gal(π : πΎ), as you can
easily check. But part (ii) tells us something much more substantial: it’s a normal
subgroup when πΏ : πΎ is a normal extension.
103
Proof of Theorem 7.1.15 For (i), first suppose that πΏ is normal over πΎ, and let
π ∈ Gal(π : πΎ). For all πΌ ∈ πΏ, Proposition 7.1.9 implies that πΌ and π(πΌ) are
conjugate over πΎ, so they have the same minimal polynomial, so π(πΌ) ∈ πΏ by
normality. Hence ππΏ ⊆ πΏ. The same argument with π−1 in place of π gives
π−1 πΏ ⊆ πΏ, and applying π to each side then gives πΏ ⊆ ππΏ. So ππΏ = πΏ.
Conversely, suppose that ππΏ = πΏ for all π ∈ Gal(π : πΎ). Let πΌ ∈ πΏ with
minimal polynomial π. Since π : πΎ is normal, π splits in π. Each root πΌ′ of
π in π is conjugate to πΌ over πΎ, so by Proposition 7.1.9, πΌ′ = π(πΌ) for some
π ∈ Gal(π : πΎ), giving πΌ′ ∈ ππΏ = πΏ. Hence π splits in πΏ and πΏ : πΎ is normal.
For (ii), suppose that πΏ : πΎ is normal. To prove that Gal(π : πΏ) is a normal
subgroup of Gal(π : πΎ), let π ∈ Gal(π : πΎ) and π ∈ Gal(π : πΏ). We show that
π−1 ππ ∈ Gal(π : πΏ), or equivalently,
π−1 ππ(πΌ) = πΌ for all πΌ ∈ πΏ,
or equivalently,
ππ(πΌ) = π(πΌ) for all πΌ ∈ πΏ.
But by (i), π(πΌ) ∈ πΏ for all πΌ ∈ πΏ, so π (π(πΌ)) = π(πΌ) since π ∈ Gal(π : πΏ).
This completes the proof that Gal(π : πΏ) P Gal(π : πΎ).
Finally, we prove the statement on quotients (still supposing that πΏ : πΎ is a
normal extension). Every automorphism π of π over πΎ satisfies ππΏ = πΏ (by (i)),
and therefore restricts to an automorphism πˆ of πΏ. The function
π:
Gal(π : πΎ) → Gal(πΏ : πΎ)
π
β¦→
πˆ
is a group homomorphism, since it preserves composition. Its kernel is Gal(π :
πΏ), by definition. If we can prove that π is surjective then the last part of the
theorem will follow from the first isomorphism theorem.
To prove that π is surjective, we must show that each automorphism π of πΏ
over πΎ extends to an automorphism π of π:
πO
π
/π
O
πΏ`
π
/πΏ
>
πΎ
The argument is similar to the second half of the proof of Proposition 7.1.9. By
Theorem 7.1.5, π is the splitting field of some π ∈ πΎ [π‘]. Then π is also the
splittting field of π over πΏ. Also, π∗ π = π since π is a homomorphism over πΎ and
104
π is a polynomial over πΎ. So by Proposition 6.2.11(i), there is an automorphism
π of π extending π, as required.
β‘
Example 7.1.16 Take π : πΏ : πΎ to be
Q π, π : Q(π) : Q,
√3
where π = 2 and π = π 2ππ/3 . As you will recognize by now, Q(π, π) is the splitting
field of π‘ 3 − 2 over Q, so it is a finite normal extension of Q by Theorem 7.1.5.
Also, Q(π) is the splitting field of π‘ 2 +π‘ +1 over Q, so it too is a normal extension
of Q. Part (i) of Theorem 7.1.15 implies that every element of GalQ (π‘ 3 −2) restricts
to an automorphism of Q(π).
Part (ii) implies that
Gal Q π, π : Q(π) P Gal Q π, π : Q
and that
Gal Q π, π : Q
Gal(Q(π) : Q).
Gal Q π, π : Q(π)
(7.1)
What does this say explicitly? We showed in Example 7.1.14 that Gal(Q(π, π) :
Q) π3 . That is, each element of the Galois group permutes the three roots
π, ππ, π2 π
of π‘ 3 −2, and all six permutations are realized by some element of the Galois group.
An element of Gal(Q(π, π) : Q) that fixes π is determined by which of the three
roots π is mapped to, so Gal(Q(π, π) : Q(π)) π΄3 . Finally, Gal(Q(π) : Q) πΆ2
by Example 7.1.13. So in this case, the isomorphism (7.1) states that
π3
πΆ2 .
π΄3
Exercise 7.1.17 Draw a diagram showing the three roots of π‘ 3 − 2 and
the elements of π» = Gal(Q(π, π) : Q(π)) acting on them. There is
a simple geometric description of the elements of Gal(Q(π, π) : Q)
that belong to the subgroup π». What is it?
7.2
Separability
Theorem 6.2.13 implies that | Gal(π : πΎ)| ≤ [π : πΎ] whenever π : πΎ is a
splitting field extension. Why is this an inequality, not an equality? The answer
105
can be traced back to the proof of Proposition 6.2.11 on extension of isomorphisms.
There, we had an irreducible polynomial called π∗ π, and we wrote π for the number
of distinct roots of π∗ π in its splitting field. Ultimately, the source of the inequality
was the fact that π ≤ deg(π∗ π).
But is this last inequality actually an equality? That is, does an irreducible
polynomial of degree π always have π distinct roots in its splitting field? Certainly
it has π roots when counted with multiplicity. But there will be fewer than π
distinct roots if any of the roots are repeated (have multiplicity ≥ 2). The question
is whether this can ever happen.
Formally, for a polynomial π (π‘) ∈ πΎ [π‘] and a root πΌ of π in some extension
π of πΎ, we say that πΌ is a repeated root if (π‘ − πΌ) 2 | π (π‘) in π [π‘].
Exercise 7.2.1 Try to find an example of an irreducible polynomial
of degree π with fewer than π distinct roots in its splitting field. Or
if you can’t, see if you can prove that this is impossible over Q: that
is, an irreducible over Q has no repeated roots in C. Both are quite
hard, but ten minutes spent trying may help you to appreciate what’s
to come.
Definition 7.2.2 An irreducible polynomial over a field is separable if it has no
repeated roots in its splitting field.
Equivalently, an irreducible polynomial π ∈ πΎ [π‘] is separable if it splits into
distinct linear factors in SFπΎ ( π ):
π (π‘) = π(π‘ − πΌ1 ) · · · (π‘ − πΌπ )
for some π ∈ πΎ and distinct πΌ1 , . . . , πΌπ ∈ SFπΎ ( π ). Put another way, an irreducible
π is separable if and only if it has deg( π ) distinct roots in its splitting field.
Example 7.2.3 π‘ 3 − 2 ∈ Q[π‘] is separable, since it has 3 distinct roots in C, hence
in its splitting field.
Example 7.2.4 This is an example of an irreducible polynomial that’s inseparable.
It’s a little bit complicated, but it’s the simplest example there is.
Let π be a prime number. We will consider the field πΎ = F π (π’) of rational
expressions over F π in an indeterminate (variable symbol) π’. Put π (π‘) = π‘ π − π’ ∈
πΎ [π‘]. We will show that π is an inseparable irreducible polynomial.
By definition, π has at least one root πΌ in its splitting field. But the roots of π
are the πth roots of π’, and in fields of characteristic π, each element has at most
one πth root (Corollary 2.3.22(i)). So πΌ is the only root of π in SFπΎ ( π ), despite π
having degree π > 1. Alternatively, we can argue like this:
π (π‘) = π‘ π − π’ = π‘ π − πΌ π = (π‘ − πΌ) π ,
106
where the last step comes from the Frobenius map of SFπΎ ( π ) being a homomorphism (Proposition 2.3.20(i)).
We now show that π is irreducible over πΎ. Suppose it is reducible. The unique
factorization of π into irreducible polynomials over SFπΎ ( π ) is π (π‘) = (π‘ − πΌ) π , so
any nontrivial factorization of π in πΎ [π‘] is of the form
π (π‘) = (π‘ − πΌ) π (π‘ − πΌ) π−π
where 0 < π < π and both factors belong to πΎ [π‘]. The coefficient of π‘ π−1 in (π‘ − πΌ) π
is −ππΌ, so −ππΌ ∈ πΎ. But π is invertible in πΎ, so πΌ ∈ πΎ. Hence π’ has a πth root in
πΎ = F π (π’), contradicting Exercise 3.1.13.
Warning 7.2.5 Definition 7.2.2 is only a definition of separability
for irreducible polynomials. There is a definition of separability for
arbitrary polynomials, but it’s not simply Definition 7.2.2 with the
word ‘irreducible’ deleted. We won’t need it, but here it is: an
arbitrary polynomial is called separable if each of its irreducible factors
is separable. So π‘ 2 is separable, even though it has a repeated root.
In real analysis, we can test whether a root is repeated by asking whether the
derivative is 0 there:
Over an arbitrary field, there’s no general definition of the derivative of a function, as there’s no meaningful notion of limit. But even without limits, we can
differentiate polynomials in the following sense.
Íπ
Definition 7.2.6 Let πΎ be a field and let π (π‘) = π=0
ππ π‘ π ∈ πΎ [π‘]. The formal
derivative of π is
π
∑οΈ
(π· π )(π‘) =
πππ π‘ π−1 ∈ πΎ [π‘].
π=1
We use π· π rather than π ′ to remind ourselves not to take the familiar properties
of differentiation for granted. Nevertheless, the usual basic laws hold:
Lemma 7.2.7 Let πΎ be a field. Then
π· ( π + π) = π· π + π·π,
π· ( π π) = π · π·π + π· π · π,
for all π , π ∈ πΎ [π‘] and π ∈ πΎ.
π·π = 0
β‘
107
Exercise 7.2.8 Check one or two of the properties in Lemma 7.2.7.
The real analysis test for repetition of roots has an algebraic analogue:
Lemma 7.2.9 Let π be a nonzero polynomial over a field πΎ. The following are
equivalent:
i. π has a repeated root in SFπΎ ( π );
ii. π and π· π have a common root in SFπΎ ( π );
iii. π and π· π have a nonconstant common factor in πΎ [π‘].
Proof (i)⇒(ii): suppose that π has a repeated root πΌ in SFπΎ ( π ). Then π (π‘) =
(π‘ − πΌ) 2 π(π‘) for some π(π‘) ∈ (SFπΎ ( π )) [π‘]. Hence
(π· π )(π‘) = (π‘ − πΌ) 2π(π‘) + (π‘ − πΌ) · (π·π)(π‘) ,
so πΌ is a common root of π and π· π in SFπΎ ( π ).
(ii)⇒(iii): suppose that π and π· π have a common root πΌ in SFπΎ ( π ). Then πΌ
is algebraic over πΎ (since π ≠ 0), and the minimal polynomial of πΌ over πΎ is then
a nonconstant common factor of π and π· π in πΎ [π‘].
(iii)⇒(ii): if π and π· π have a nonconstant common factor π then π splits in
SFπΎ ( π ), and any root of π in SFπΎ ( π ) is a common root of π and π· π .
(ii)⇒(i): suppose that π and π· π have a common root πΌ ∈ SFπΎ ( π ). Then
π (π‘) = (π‘ − πΌ)π(π‘) for some π ∈ (SFπΎ ( π )) [π‘], giving
(π· π )(π‘) = π(π‘) + (π‘ − πΌ) · (π·π)(π‘).
But (π· π )(πΌ) = 0, so π(πΌ) = 0, so π(π‘) = (π‘ − πΌ)β(π‘) for some β ∈ (SFπΎ ( π )) [π‘].
Hence π (π‘) = (π‘ − πΌ) 2 β(π‘), and πΌ is a repeated root of π in its splitting field. β‘
The point of Lemma 7.2.9 is that condition (iii) allows us to test for repetition
of roots in SFπΎ ( π ) without ever leaving πΎ [π‘], or even knowing what SFπΎ ( π ) is.
Proposition 7.2.10 Let π be an irreducible polynomial over a field. Then π is
inseparable if and only if π· π = 0.
Proof This follows from (i) ⇐⇒ (iii) in Lemma 7.2.9. Since π is irreducible,
π and π· π have a nonconstant common factor if and only if π divides π· π ; but
deg(π· π ) < deg( π ), so π | π· π if and only if π· π = 0.
β‘
Corollary 7.2.11 Let πΎ be a field.
108
i. If char πΎ = 0 then every irreducible polynomial over πΎ is separable.
ii. If char πΎ = π > 0 then an irreducible polynomial π ∈ πΎ [π‘] is inseparable if
and only if
π (π‘) = π 0 + π 1 π‘ π + · · · + ππ π‘ π π
for some π 0 , . . . , ππ ∈ πΎ.
In other words, the only irreducible polynomials that are inseparable are the
polynomials in π‘ π in characteristic π. Inevitably, Example 7.2.4 is of this form.
Í
Proof Let π (π‘) = ππ π‘ π be an irreducible polynomial. Then π is inseparable if
and only if π· π = 0, if and only if πππ = 0 for all π ≥ 1. If char πΎ = 0, this implies
that ππ = 0 for all π ≥ 1, so π is constant, which contradicts π being irreducible. If
char πΎ = π, then πππ = 0 for all π ≥ 1 is equivalent to ππ = 0 whenever π β€ π.
β‘
Remark 7.2.12 In the final chapter we will show that every irreducible polynomial
over a finite field is separable. So, it is only over infinite fields of characteristic π
that you have to worry about inseparability.
We now build up to showing that | Gal(π : πΎ)| = [π : πΎ] whenever π : πΎ
is a finite normal extension in which the minimal polynomial of every element of
π is separable. First, some terminology:
Definition 7.2.13 Let π : πΎ be an algebraic extension. An element of π is
separable over πΎ if its minimal polynomial over πΎ is separable. The extension
π : πΎ is separable if every element of π is separable over πΎ.
Examples 7.2.14
i. Every algebraic extension of fields of characteristic 0 is
separable, by Corollary 7.2.11.
ii. Every algebraic extension of a finite field is separable, by Remark 7.2.12.
iii. The splitting field of π‘ π − π’ over F π (π’) is inseparable. Indeed, the element
denoted by πΌ in Example 7.2.4 is inseparable over F π (π’), since its minimal
polynomial is the inseparable polynomial π‘ π − π’.
Exercise 7.2.15 Let π : πΏ : πΎ be field extensions. Show that if
π : πΎ is algebraic then so are π : πΏ and πΏ : πΎ.
Lemma 7.2.16 Let π : πΏ : πΎ be field extensions, with π : πΎ algebraic. If π : πΎ
is separable then so are π : πΏ and πΏ : πΎ.
109
Proof Both π : πΏ and πΏ : πΎ are algebraic by Exercise 7.2.15, so it does make
sense to ask whether they are separable. (We only defined what it means for an
algebraic extension to be separable.) That πΏ : πΎ is separable is immediate from the
definition. To show that π : πΏ is separable, let πΌ ∈ π. Write π πΏ and π πΎ for the
minimal polynomials of πΌ over πΏ and πΎ, respectively. Then π πΎ is an annihilating
polynomial of πΌ over πΏ, so π πΏ | π πΎ in πΏ [π‘]. Since π : πΎ is separable, π πΎ
splits into distinct linear factors in SFπΎ (π πΎ ). Since π πΏ | π πΎ , so does π πΏ . Hence
π πΏ ∈ πΏ [π‘] is separable, so πΌ is separable over πΏ.
β‘
As hinted in the introduction to this section, we will prove that | Gal(π : πΎ)| =
[π : πΎ] by refining Proposition 6.2.11.
π
πO
π
πΎ
π
/ π′
O
/ πΎ ′ π∗ π
Proposition 7.2.17 Let π : πΎ → πΎ ′ be an isomorphism of fields, let 0 ≠ π ∈ πΎ [π‘],
let π be a splitting field of π over πΎ, and let π ′ be a splitting field of π∗ π over πΎ ′.
Suppose that the extension π ′ : πΎ ′ is separable. Then there are exactly [π : πΎ]
isomorphisms π : π → π ′ extending π.
Proof This is almost the same as the proof of Proposition 6.2.11, but with the
inequality π ≤ deg(π∗ π) replaced by an equality, which holds by separability. For
the inductive hypothesis to go through, we need the extension π ′ : πΎ ′ (πΌ′π ) to be
separable, and this follows from the separability of π ′ : πΎ ′ by Lemma 7.2.16. β‘
Theorem 7.2.18 | Gal(π : πΎ)| = [π : πΎ] for every finite normal separable
extension π : πΎ.
Proof By Theorem 7.1.5, π = SFπΎ ( π ) for some π ∈ πΎ [π‘]. The result follows
from Proposition 7.2.17, taking π ′ = π, πΎ ′ = πΎ, and π = idπΎ .
β‘
Examples 7.2.19
i. | GalπΎ ( π )| = [SFπΎ ( π ) : πΎ] for any nonzero polynomial
π over a field πΎ of characteristic 0.
For instance, if π (π‘) = π‘ 3 − 2 then [SFQ ( π ) : Q] = 6 by a similar argument
to Example 5.1.22, using that SFQ ( π ) contains elements of degree 2 and 3
over Q. Hence | GalQ ( π )| = 6. But GalQ ( π ) embeds into π3 by Proposition 6.3.10, so GalQ ( π ) π3 . We already proved this in Example 7.1.16,
by a different argument.
ii. Consider πΎ = F π (π’) and π = SFπΎ (π‘ π − π’). With notation as in Example 7.2.4, we have π = πΎ (πΌ), so [π : πΎ] = degπΎ (πΌ) = π. On the other
hand, | Gal(π : πΎ)| = 1 by Corollary 6.3.14. So Theorem 7.2.18 fails if we
drop the separability hypothesis.
110
Digression 7.2.20 With some effort, one can show that in any algebraic
extension π : πΎ, the separable elements form a subfield of π. (See Stewart,
Theorem 17.22.) It follows that a finite extension πΎ (πΌ1 , . . . , πΌπ ) : πΎ is
separable if and only if each πΌπ is. Hence a splitting field extension SFπΎ ( π ) :
πΎ is separable if and only if every root of π is separable in SFπΎ ( π ), which
itself is equivalent to π being separable in the sense of Warning 7.2.5.
So: SFπΎ ( π ) is separable over πΎ if and only if π is separable over πΎ. Thus,
the different meanings of ‘separable’ interact nicely.
Digression 7.2.21 It’s a stunning fact that every finite separable extension
is simple. This is called the theorem of the primitive element. For instance,
whenever πΌ1 , . . . , πΌπ are complex numbers algebraic over Q, there is some
πΌ ∈ C (a ‘primitive element’) such that
Q(πΌ). We saw one
√ Q(πΌ
√ 1 , . . . , πΌ√π ) = √
case of this in Example 4.3.14(i): Q( 2, 3) = Q( 2 + 3).
The theorem of the primitive element was at the heart of most early accounts
of Galois theory, and is used in many modern treatments too, but not this
one.
7.3
Fixed fields
Write Aut(π) for the group of automorphisms of a field π. Then Aut(π) acts
naturally on π (Example 2.1.2(ii)). Given a subset π of Aut(π), we can consider
the set Fix(π) of elements of π fixed by π (Definition 2.1.14).
Lemma 7.3.1 Fix(π) is a subfield of π, for any π ⊆ Aut(π).
Proof Fix(π) is the equalizer Eq(π ∪ {id π }), which is a subfield of π by
Lemma 2.3.8.
β‘
For this reason, we call Fix(π) the fixed field of π.
Exercise 7.3.2 Using Lemma 7.3.1, show that every automorphism
of a field is an automorphism over its prime subfield. In other words,
Aut(π) = Gal(π : πΎ) whenever π is a field with prime subfield πΎ.
Here’s the big, ingenious, result about fixed fields. It will play a crucial part in
the proof of the fundamental theorem of Galois theory.
111
Theorem 7.3.3 Let π be a field and π» a finite subgroup of Aut(π). Then
[π : Fix(π»)] ≤ |π»|.
So the smaller |π»| is, the smaller [π : Fix(π»)] must be, which means that
Fix(π») must be bigger. In other words, the smaller |π»| is, the more of π must be
fixed by π».
Proof Write π = |π»|. It is enough to prove that any π + 1 elements πΌ0 , . . . , πΌπ of
π are linearly dependent over Fix(π»).
Write
π = (π₯ 0 , . . . , π₯ π ) ∈ π π+1 : π₯ 0 π (πΌ0 ) + · · · + π₯ π π (πΌπ ) = 0 for all π ∈ π» .
The size of fixed
fields
Then π is defined by π homogeneous linear equations in π + 1 variables, so it is a
nontrivial π-linear subspace of π π+1 .
Claim: Let (π₯ 0 , . . . , π₯ π ) ∈ π and π ∈ π». Then (π(π₯ 0 ), . . . , π(π₯ π )) ∈ π.
Proof: For all π ∈ π», we have
π₯ 0 (π−1 β¦ π)(πΌ0 ) + · · · + π₯ π (π−1 β¦ π)(πΌπ ) = 0,
since π−1 β¦ π ∈ π». Applying π to both sides gives that for all π ∈ π»,
π(π₯ 0 )π (πΌ0 ) + · · · + π(π₯ π )π (πΌπ ) = 0,
proving the claim.
Define the length of a nonzero vector x = (π₯ 0 , . . . , π₯ π ) to be the unique number
β ∈ {0, . . . , π} such that π₯β ≠ 0 but π₯β+1 = · · · = π₯ π = 0. Since π is nontrivial,
we can choose an element x of π of minimal length, β. Since π is closed under
scalar multiplication by π, we may assume that π₯β = 1. Thus, x is of the form
(π₯ 0 , . . . , π₯β−1 , 1, 0, . . . , 0). Since x is a nonzero element of π of minimal length,
the only element of π of the form (π¦ 0 , . . . , π¦ β−1 , 0, 0, . . . , 0) is 0.
We now show that π₯π ∈ Fix(π») for all π. Let π ∈ π». By the claim,
(π(π₯0 ), . . . , π(π₯ π )) ∈ π. Put
y = (π(π₯0 ) − π₯ 0 , . . . , π(π₯ π ) − π₯ π ).
Since π is a linear subspace, y ∈ π. Now π(π₯π ) − π₯π = π(0) − 0 = 0 for all π > β
and π(π₯β ) − π₯β = π(1) − 1 = 0, so by the last sentence of the previous paragraph,
y = 0. In other words, π(π₯π ) = π₯π for all π. This holds for all π ∈ π», so π₯π ∈ Fix(π»)
for all π.
We have shown that π contains a nonzero vector x ∈ Fix(π») π+1 . But taking
Í
π = id in the definition of π gives π₯π πΌπ = 0. Hence πΌ0 , . . . , πΌπ are linearly
dependent over Fix(π»).
β‘
112
Example 7.3.4 Write π
: C → C for complex conjugation. Then π» = {id, π
} is
a subgroup of Aut(C), and Theorem 7.3.3 predicts that [C : Fix(π»)] ≤ 2. Since
Fix(π») = R, this is true.
Exercise 7.3.5 Find another example of Theorem 7.3.3.
Digression 7.3.6 In fact, Theorem 7.3.3 is an equality: [π : Fix(π»)] =
|π»|. This is proved directly in many Galois theory books (e.g. Stewart,
Theorem 10.5). In our approach, it will be a consequence of the fundamental
theorem of Galois theory rather than a step on the way to proving it.
The reverse inequality, [π : Fix(π»)] ≥ |π»|, is closely related to the result
called ‘linear independence of characters’. (A good reference is Lang, Algebra, 3rd edition, Theorem 4.1.) Another instance of linear independence
of characters is that the functions π₯ β¦→ π 2 ππππ₯ (π ∈ Z) on R are linearly
independent, a fundamental fact in the theory of Fourier series.
We finish by adding a further connecting strand between the concepts of normal
extension and normal subgroup, complementary to the strands in Theorem 7.1.15.
Proposition 7.3.7 Let π : πΎ be a finite normal extension and π» a normal subgroup of Gal(π : πΎ). Then Fix(π») is a normal extension of πΎ.
Proof Since every element of π» is an automorphism over πΎ, the subfield Fix(π»)
of π contains πΎ. For each π ∈ Gal(π : πΎ), we have
π Fix(π») = Fix(ππ»π−1 ) = Fix(π»),
where the first equality holds by Lemma 2.1.15 and the second because π» is normal
in Gal(π : πΎ). Hence by Theorem 7.1.15(i), Fix(π») : πΎ is a normal extension.β‘
The stage is now set for the central result of the course: the fundamental
theorem of Galois theory.
113
Chapter 8
The fundamental theorem of Galois
theory
We’ve been building up to this moment all semester. Let’s do it!
Introduction to
Week 8
8.1
Introducing the Galois correspondence
Let π : πΎ be a field extension, with πΎ viewed as a subfield of π, as usual.
An intermediate field of π : πΎ is a subfield of π containing πΎ. Write
F = {intermediate fields of π : πΎ }.
For πΏ ∈ F , we draw diagrams like this:
π
πΏ
πΎ,
with the bigger fields higher up.
Also write
G = {subgroups of Gal(π : πΎ)}.
For π» ∈ G , we draw diagrams like this:
1
π»
Gal(π : πΎ).
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Here 1 denotes the trivial subgroup and the bigger groups are lower down. It will
become clear soon why we’re using opposite conventions.
For πΏ ∈ F , the group Gal(π : πΏ) consists of all automorphisms π of π that
fix each element of πΏ. Since πΎ ⊆ πΏ, any such π certainly fixes each element of πΎ.
Hence Gal(π : πΏ) is a subgroup of Gal(π : πΎ). This process defines a function
Gal(π : −) :
F →
G
πΏ β¦→ Gal(π : πΏ).
In the expression Gal(π : −), the symbol − should be seen as a blank space into
which arguments can be inserted.
Warning 8.1.1 The group we’re associating with πΏ is Gal(π : πΏ),
not Gal(πΏ : πΎ)! Both groups matter, but only one is a subgroup of
Gal(π : πΎ), which is what we’re interested in here.
We showed just now that Gal(π : πΏ) is a subgroup of Gal(π : πΎ).
If you wanted to show that Gal(πΏ : πΎ) is (isomorphic to) a subgroup
of Gal(π : πΎ)—which it isn’t—then you’d probably do it by trying
to prove that every automorphism of πΏ over πΎ extends uniquely to π.
And that’s false. For instance, when πΏ = πΎ, the identity on πΏ typically
has many extensions to π: they’re the elements of Gal(π : πΎ).
Although Gal(πΏ : πΎ) isn’t a subgroup of Gal(π : πΎ), it is a quotient
of it, at least when both extensions are finite and normal. We saw this
in Theorem 7.1.15, and we’ll come back to it in Section 8.2.
In the other direction, for π» ∈ G , the subfield Fix(π») of π contains πΎ. Indeed,
π» ⊆ Gal(π : πΎ), and by definition, every element of Gal(π : πΎ) fixes every
element of πΎ, so Fix(π») ⊇ πΎ. Hence Fix(π») is an intermediate field of π : πΎ.
This process defines a function
Fix :
G →
F
π» β¦→ Fix(π»).
We have now defined functions
Fo
Gal(π:−)
Fix
/
G.
The fundamental theorem of Galois theory tells us how these functions behave:
how the concepts of Galois group and fixed field interact. It will bring together
most of the big results we’ve proved so far, and will assume that the extension is
finite, normal and separable. But first, let’s say the simple things that are true for
all extensions:
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π
1
πΏ2
Gal(π : πΏ 2 )
πΏ1
Gal(π : πΏ 1 )
πΎ
Gal(π : πΎ)
Figure 8.1: The function πΏ β¦→ Gal(π : πΏ) is order-reversing (Lemma 8.1.2(i)).
Lemma 8.1.2 Let π : πΎ be a field extension, and define F and G as above.
i. For πΏ 1 , πΏ 2 ∈ F ,
πΏ 1 ⊆ πΏ 2 ⇒ Gal(π : πΏ 1 ) ⊇ Gal(π : πΏ 2 )
(Figure 8.1). For π»1 , π»2 ∈ G ,
π»1 ⊆ π»2 ⇒ Fix(π»1 ) ⊇ Fix(π»2 ).
ii. For πΏ ∈ F and π» ∈ G ,
πΏ ⊆ Fix(π») ⇐⇒ π» ⊆ Gal(π : πΏ).
iii. For all πΏ ∈ F ,
πΏ ⊆ Fix(Gal(π : πΏ)).
For all π» ∈ G ,
π» ⊆ Gal(π : Fix(π»)).
Warning 8.1.3 In part (i), the functions Gal(π : −) and Fix reverse
inclusions. The bigger you make πΏ, the smaller you make Gal(π : πΏ),
because it gets harder for an automorphism to fix everything in πΏ. And
the bigger you make π», the smaller you make Fix(π»), because it gets
harder for an element of π to be fixed by everything in π». That’s why
the field and group diagrams are opposite ways up.
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Proof (i): I leave the first half as an exercise. For the second, suppose that
π»1 ⊆ π»2 , and let πΌ ∈ Fix(π»2 ). Then π (πΌ) = πΌ for all π ∈ π»2 , so π (πΌ) = πΌ for all
π ∈ π»1 , so πΌ ∈ Fix(π»1 ).
(ii): both sides are equivalent to the statement that π (πΌ) = πΌ for all π ∈ π» and
πΌ ∈ πΏ.
(iii): the first statement follows from the ⇐ direction of (ii) by taking π» =
Gal(π : πΏ), and the second follows from the ⇒ direction of (ii) by taking
πΏ = Fix(π»). (Or, they can be proved directly.)
β‘
Exercise 8.1.4 Prove the first half of Lemma 8.1.2(i).
Exercise 8.1.5 Draw a diagram like Figure 8.1 for the second half of
Lemma 8.1.2(i).
Digression 8.1.6 If you’ve done some algebraic geometry, the formal structure of Lemma 8.1.2 might seem familiar. Given a field πΎ and a natural
number π, we can form the set F of subsets of πΎ π and the set G of ideals of
πΎ [π‘1 , . . . , π‘ π ], and there are functions F β G defined by taking the annihilating ideal of a subset of πΎ π and the zero-set of an ideal of πΎ [π‘1 , . . . , π‘ π ].
The analogue of Lemma 8.1.2 holds.
In general, a pair of ordered sets F and G equipped with functions F β G
satisfying the properties in Lemma 8.1.2 is called a Galois connection. This
in turn is a special case of the category-theoretic notion of adjoint functors.
The functions
Fo
Gal(π:−)
Fix
/
G.
are called the Galois correspondence for π : πΎ. This terminology is mostly used
in the case where the functions are mutually inverse, meaning that
πΏ = Fix(Gal(π : πΏ)),
π» = Gal(π : Fix(π»))
for all πΏ ∈ F and π» ∈ G . We saw in Lemma 8.1.2(iii) that in both cases, the
left-hand side is a subset of the right-hand side. But they are not always equal:
√3
Example 8.1.7 Let π : πΎ be Q( 2) : Q. Since [π : πΎ] is 3, which is a
prime number, the tower law implies that there are no nontrivial intermediate
fields: F = {π, πΎ }. We saw in Example 6.3.3(ii) that Gal(π : πΎ) is trivial,
so G = {Gal(π : πΎ)}. Hence F has two elements and G has only one. This
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makes it impossible for there to be mutually inverse functions between F and G .
Specifically, what goes wrong is that
√3 √3 Fix Gal Q 2 : Q = Fix idQ( √3 2) = Q 2 ≠ Q.
Exercise 8.1.8 Let π be a prime number, let πΎ = F π (π’), and let π be
the splitting field of π‘ π − π’ over πΎ, as in Examples 7.2.4 and 7.2.19(ii).
Prove that Gal(π : −) and Fix are not mutually inverse.
If Gal(π : −) and Fix are mutually inverse then they set up a one-to-one
correspondence between the set F of intermediate fields of π : πΎ and the set G
of subgroups of Gal(π : πΎ). The fundamental theorem of Galois theory tells us
that this dream comes true when π : πΎ is finite, normal and separable. And it
tells us more besides.
8.2
The theorem
The moment has come.
Theorem 8.2.1 (Fundamental theorem of Galois theory) Let π : πΎ be a
finite normal separable extension. Write
F = {intermediate fields of π : πΎ },
G = {subgroups of Gal(π : πΎ)}.
i. The functions F o
Gal(π:−)
Fix
/
G are mutually inverse.
ii. | Gal(π : πΏ)| = [π : πΏ] for all πΏ ∈ F , and [π : Fix(π»)] = |π»| for
all π» ∈ G .
iii. Let πΏ ∈ F . Then
πΏ is a normal extension of πΎ
⇐⇒ Gal(π : πΏ) is a normal subgroup of Gal(π : πΎ),
and in that case,
Gal(π : πΎ)
Gal(πΏ : πΎ).
Gal(π : πΏ)
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Proof First note that for each πΏ ∈ F , the extension π : πΏ is finite and normal (by
Corollary 7.1.6) and separable (by Lemma 7.2.16). Also, the group Gal(π : πΎ)
is finite (by Theorem 7.2.18), so every subgroup is finite too.
We prove (i) and (ii) together. First let π» ∈ G . We have
|π»| ≤ | Gal(π : Fix(π»))| = [π : Fix(π»)] ≤ |π»|,
(8.1)
where the first inequality holds because π» ⊆ Gal(π : Fix(π»)) (Lemma 8.1.2(iii)),
the equality follows from Theorem 7.2.18 (since π : Fix(π») is finite, normal and
separable), and the second inequality follows from Theorem 7.3.3 (since π» is
finite). So equality holds throughout (8.1), giving
π» = Gal(π : Fix(π»)),
[π : Fix(π»)] = |π»|.
Now let πΏ ∈ F . We have
[π : Fix(Gal(π : πΏ))] = | Gal(π : πΏ)| = [π : πΏ],
where the first equality follows from the previous paragraph by taking π» = Gal(π :
πΏ), and the second follows from Theorem 7.2.18. But πΏ ⊆ Fix(Gal(π : πΏ)) by
Lemma 8.1.2(iii), so πΏ = Fix(Gal(π : πΏ)) by Workshop 3, question 3. This
completes the proof of (i) and (ii).
We have already proved most of (iii) as Theorem 7.1.15(ii). It only remains to
show that whenever πΏ is an intermediate field such that Gal(π : πΏ) is a normal
subgroup of Gal(π : πΎ), then πΏ is a normal extension of πΎ. By Proposition 7.3.7,
Fix(Gal(π : πΏ)) : πΎ is normal. But by (i), Fix(Gal(π : πΏ)) = πΏ, so πΏ : πΎ is
normal, as required.
β‘
The fundamental theorem of Galois theory is about field extensions that are
finite, normal and separable. Let’s take a moment to think about what those
conditions mean.
An extension π : πΎ is finite and normal if and only if π is the splitting field
of some polynomial over πΎ (Theorem 7.1.5). So, the theorem can be understood
as a result about splitting fields of polynomials.
Not every splitting field extension is separable (Example 7.2.14(iii)). However,
we know of two settings where separability is guaranteed. The first is fields of
characteristic zero (Example 7.2.14(i)). The most important of these is Q, which
is our focus in this chapter: we’ll consider examples in which π : πΎ is the splitting
field extension of a polynomial over πΎ = Q. The second is where the fields are
finite (Example 7.2.14(ii)). We’ll come to finite fields in the final chapter.
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Digression 8.2.2 Normality and separability are core requirements of Galois
theory, but there are extensions of the fundamental theorem (well beyond this
course) in which the finiteness condition on π : πΎ is relaxed.
The first level of relaxation replaces ‘finite’ by ‘algebraic’. Then Gal(π : πΎ)
is no longer a finite group, but it does acquire an interesting topology. One
example is where π is the algebraic closure πΎ of πΎ, and Gal(πΎ : πΎ) is called
the absolute Galois group of πΎ (at least when char πΎ = 0). It contains all
splitting fields of polynomials over πΎ, so to study it is to study all polynomials
over πΎ at once.
Going further, we can even drop the condition that the extension is algebraic.
In this realm, we need the notion of ‘transcendence degree’, which counts
how many algebraically independent elements can be found in the extension.
You may have met this if you’re taking Algebraic Geometry.
You’ll want to see some examples! Section 8.3 is devoted to a single example
of the fundamental theorem, showing every aspect of the theorem in all its glory.
I’ll give a couple of simpler examples in a moment, but before that, it’s helpful to
review some of what we did earlier:
Remark 8.2.3 When working out the details of the Galois correspondence for a
polynomial π ∈ πΎ [π‘], it’s not only the fundamental theorem that’s useful. Some
of our earlier results also come in handy, such as the following.
i. Lemmas 6.3.7 and 6.3.8 state that GalπΎ ( π ) acts faithfully on the set of roots
of π in SFπΎ ( π ). That is, an element of the Galois group can be understood
as a permutation of the roots.
ii. Corollary 6.3.14 states that | GalπΎ ( π )| divides π!, where π is the number of
distinct roots of π in its splitting field.
iii. Let πΌ and π½ be roots of π in SFπΎ ( π ). Then there is an element of the Galois
group mapping πΌ to π½ if and only if πΌ and π½ are conjugate over πΎ (have the
same minimal polynomial). This follows from Proposition 7.1.9.
iv. In particular, when π is irreducible, the action of the Galois group on the
roots is transitive (Corollary 7.1.11). See Example 7.1.13 for an illustration
of the power of this principle.
Example 8.2.4 Let π : πΎ be a normal separable extension of prime degree π. By
the fundamental theorem, | Gal(π : πΎ)| = [π : πΎ] = π. Every group of prime
order is cyclic, so Gal(π : πΎ) πΆ π . By the tower law, π : πΎ has no nontrivial
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intermediate fields, and by Lagrange’s theorem, Gal(π : πΎ) has no nontrivial
subgroups. So F = {π, πΎ } and G = {1, Gal(π : πΎ)}:
π
1
πΎ
Gal(π : πΎ)
Both π and πΎ are normal extensions of πΎ, and both 1 and Gal(π : πΎ) are normal
subgroups of Gal(π : πΎ).
√
Example 8.2.5 Let π (π‘) = (π‘ 2 + 1)(π‘ 2 − 2) ∈ Q[π‘]. Put π = SFQ ( π ) = Q( 2, π)
and πΊ = Gal(π : πΎ) = GalQ ( π ). Then π : πΎ is a finite normal separable
extension, so the fundamental theorem applies. We already calculated πΊ in a
sketchy way in Example 6.3.6(iv). Let’s do it again in full, using what we now
know.
First,
√ √ √ [π : πΎ] = Q 2, π : Q 2 Q 2 : Q = 2 × 2 = 4
(much as in Example 5.1.18).
√
Now√consider
√ how√πΊ acts on the set {± 2, ±π} of roots
√ of π . The
√ conjugacy
class of 2 is { 2, − 2}, so for each π ∈ πΊ we have π( 2) = ± 2. Similarly,
π(π) = ±π for each π ∈ πΊ. The two choices of sign determine π entirely, so
|πΊ | ≤ 4. But by the fundamental theorem, |πΊ | = [π : πΎ] = 4, so each of the four
possibilities does in fact occur. So πΊ = {id, π+− , π−+ , π−− }, where
√ √
√ √
√ √
π−+ 2 = − 2,
π−− 2 = − 2,
π+− 2 = 2,
π+− (π) = −π,
π−+ (π) = π,
π−− (π) = −π.
The only two groups of order 4 are πΆ4 and πΆ2 × πΆ2 , and each element of πΊ has
order 1 or 2, so πΊ πΆ2 × πΆ2 .
The subgroups of πΊ are
1
β¨π+− β©
β¨π−+ β©
β¨π−− β©
(8.2)
πΊ
where lines indicate inclusions. Here β¨π+− β© is the subgroup generated by π+− ,
which is {id, π+− }, and similarly for π−+ and π−− .
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What are the fixed fields of√these √
subgroups?
√ The fundamental theorem implies
that Fix(πΊ) = Q. Also, π+− ( 2) = 2, so Q( 2) ⊆ Fix(β¨π+− β©). But
√ √ √ Q 2, π : Q 2 = 2 = |β¨π+− β©| = Q 2, π : Fix(β¨π+− β©)
√
(where the last step is by the fundamental theorem), so Q( 2) = Fix(β¨π+− β©).
Let’s reflect for a moment on the argument in the last paragraph, because it’s
one you’ll need to master. We have a subgroup π» of Gal(π : πΎ) (here, π» = β¨π+− β©)
and we want to find its fixed field. We do this in three steps:
• First, √we spot some elements πΌ1 , . . . , πΌπ fixed by π». (Here, π = 1 and
πΌ1 = 2.) It follows that πΎ (πΌ1 , . . . , πΌπ ) ⊆ Fix(π»).
• Next, we check that [π : πΎ (πΌ1 , . . . , πΌπ )] = |π»|. If they’re not equal, that
means we didn’t spot enough elements fixed by π».
• Finally, we apply a standard argument:
[π : πΎ (πΌ1 , . . . , πΌπ )] = |π»| = [π : Fix(π»)]
(using the fundamental theorem), so by the tower law,
[Fix(π») : πΎ (πΌ1 , . . . , πΌπ )] =
[π : πΎ (πΌ1 , . . . , πΌπ )]
= 1,
[π : Fix(π»)]
giving Fix(π») = πΎ (πΌ1 , . . . , πΌπ ).
The strategy is similar to one you’ve met in linear algebra: to prove that two
subspaces of a vector space are equal, show that one is a subspace of the other and
that they have the same dimension.
Similar arguments apply to π−+ and π−− , so the fixed fields of the groups in
diagram (8.2) are
√ Q 2, π
Q
√ 2
Q(π)
Q
√ 2π
(8.3)
Q
√
Equivalently, the groups in (8.2)
are
the
Galois
groups
of
Q(
2, π) over the fields
√
in (8.3). For instance, Gal(Q( 2, π) : Q(π)) = β¨π−+ β©.
Since the overall Galois group πΊ πΆ2 × πΆ2 is abelian, every subgroup is
normal. Hence all the extensions in diagram (8.3) are normal too.
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Exercise 8.2.6 In this particular example, one can also see more
directly that all the extensions in (8.3) are normal. How?
Like any big theorem, the fundamental theorem of Galois theory has some
important corollaries. Here’s one.
Corollary 8.2.7 Let π : πΎ be a finite normal separable extension. Then for every
πΌ ∈ π \ πΎ, there is some automorphism π of π over πΎ such that π(πΌ) ≠ πΌ.
Proof Theorem 8.2.1(i) implies that Fix(Gal(π : πΎ)) = πΎ. Now πΌ ∉ πΎ, so
πΌ ∉ Fix(Gal(π : πΎ)), which is what had to be proved.
β‘
Example 8.2.8 For any π ∈ Q[π‘] and irrational πΌ ∈ SFQ ( π ), there is some
π ∈ GalQ ( π ) that does not fix πΌ. This is clear if πΌ ∉ R, as we can take π to be
complex conjugation restricted to SFQ ( π ). But it is not so obvious otherwise.
8.3
A specific example
Chapter 13 of Stewart’s book opens with these words:
The extension that we discuss is a favourite with writers on Galois
theory, because of its archetypal quality. A simpler example would
be too small to illustrate the theory adequately, and anything more
complicated would be unwieldy. The example is the Galois group of
the splitting field of π‘ 4 − 2 over Q.
We go through the same example here. My presentation of it is different from
Stewart’s, so you can consult his book if anything that follows is unclear.
Write π (π‘) = π‘ 4 − 2 ∈ Q[π‘], which is irreducible by Eisenstein’s criterion.
Write πΊ = GalQ ( π ).
Splitting field Write π for the unique real positive root of π . Then the roots of
π are ±π and ±ππ (Figure 8.2). So SFQ ( π ) = Q(π, ππ) = Q(π, π). We have
[Q(π, π) : Q] = [Q(π, π) : Q(π)] [Q(π) : Q] = 2 × 4 = 8,
where the first factor is 2 because Q(π) ⊆ R and the second factor is 4 because π
is the minimal polynomial of π over Q (being irreducible). By the fundamental
theorem, |πΊ | = 8.
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π
ππ
−π
π
π
−ππ
Figure 8.2: The roots of π , and the effects on them of π, π
∈ GalQ ( π ).
Galois group We now look for the 8 elements of the Galois group. We’ll use
the principle that if π, π ∈ πΊ with π(π) = π (π) and π(π) = π (π) then π = π (by
Lemma 4.3.6).
Complex conjugation on C restricts to a nontrivial automorphism π
of Q(π, π)
over Q, giving an element π
∈ πΊ of order 2.
I now claim that πΊ has an element π satisfying π(π) = ππ and π(π) = π. In that
case, π will act on the roots of π as follows:
π β¦→ ππ β¦→ −π β¦→ −ππ β¦→ π
(Figure 8.2). This element π will have order 4.
Proof of claim: since π is irreducible, πΊ acts transitively on the roots of π in
SFQ ( π ), so there is some π ∈ πΊ such that π(π) = ππ. The conjugacy class of π
over Q is {±π}, so π(π) = ±π. If π(π) = π then we can take π = π. If π(π) = −π then
(π β¦ π
)(π) = π(π) = ππ,
(π β¦ π
)(π) = π(−π) = −π(π) = π,
so we can take π = π β¦ π
.
(From now on, I will usually omit the β¦ sign and write things like ππ
instead. Of
course, juxtaposition is also used to mean multiplication, as in ππ. But confusion
shouldn’t arise: automorphisms are composed and numbers are multiplied.)
Figure 8.2 might make us wonder if πΊ is the dihedral group π· 4 , the symmetry
group of the square. We will see that it is.
Warning 8.3.1 The symmetry group of a regular π-sided polygon has
2π elements: π rotations and π reflections. Some authors call it π· π
and others call it π· 2π . I will call it π· π , as in the Group Theory course.
If πΊ π· 4 , we should have π
π = π −1 π
. (This is one of the defining equations
of the dihedral group; you saw it in Example 3.2.12 of Group Theory.) Let’s check
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π∈πΊ
π(π)
π(π)
π(ππ)
order
id
π
π2
3
π = π −1
π
π
π = π −1 π
π
π 2 = π 2 π
π
π −1 = ππ
π
ππ
−π
−ππ
π
−ππ
−π
ππ
π
π
π
π
−π
−π
−π
−π
ππ
−π
−ππ
π
−ππ
−π
ππ
π
1
4
2
4
2
2
2
2
geometric description
(see Warning 8.3.2)
identity
rotation by π/2
rotation by π
rotation by −π/2
reflection in real axis
reflection in axis through 1 − π
reflection in imaginary axis
reflection in axis through 1 + π
Figure 8.3: The Galois group of π‘ 4 − 2 over Q.
this. We have
π
π(π) = ππ = −ππ,
π −1 π
(π) = π −1 (π) = −ππ,
π
π(π) = π
(π) = −π,
π −1 π
(π) = π −1 (−π) = −π,
so π
π and π −1 π
are equal on π and π, so π
π = π −1 π
. It follows that π
ππ = π −π π
for
all π ∈ Z.
Figure 8.3 shows the effect of 8 elements of πΊ on π, π and ππ. Since no two
of them have the same effect on both π and π, they are all distinct elements of πΊ.
Since |πΊ | = 8, they are the only elements of πΊ. So πΊ π· 4 .
Warning 8.3.2 The ‘geometric description’ in Figure 8.3 applies only
to the roots, not the whole of the splitting field Q(π, π). For example,
π 2 is rotation by π on the set of roots, but it is not rotation by π on the
rest of Q(π, π): it fixes each element of Q, for instance.
Subgroups of the Galois group Since |πΊ | = 8, any nontrivial proper subgroup
of πΊ has order 2 or 4. Let’s look in turn at subgroups of order 2 and 4, also
determining which ones are normal. This is pure group theory, with no mention
of fields.
• The subgroups of order 2 are of the form β¨πβ© = {id, π} where π ∈ πΊ has
order 2. So, they are
β¨π 2 β©, β¨π
β©, β¨π
πβ©, β¨π
π 2 β©, β¨π
π −1 β©.
If you watched the video ‘What does it mean to be normal?’, you may be
able to guess which of these subgroups are normal in πΊ, the symmetry group
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of the square. It should be those that can be specified without referring to
particular vertices or edges of the square. So, just the first should be normal.
Let’s check.
We know that π
π 2 = π 2 π
, so π 2 commutes with both π
and π, which generate
πΊ. Hence π 2 is in the centre of πΊ (commutes with everything in πΊ). It
follows that β¨π 2 β© is a normal subgroup of πΊ. On the other hand, for each
π ∈ Z, the subgroup β¨π
ππ β© is not normal, since
π(π
ππ ) π −1 = (ππ
) ππ−1 = (π
π −1 ) ππ−1 = π
ππ−2 ∉ β¨π
ππ β©.
• The subgroups of πΊ of order 4 are isomorphic to either πΆ4 or πΆ2 × πΆ2 , since
these are the only groups of order 4.
The only elements of πΊ of order 4 are π ±1 , so the only subgroup of πΊ
isomorphic to πΆ4 is β¨πβ© = {id, π, π 2 , π 3 = π −1 }.
Now consider subgroups π» of πΊ isomorphic to πΆ2 × πΆ2 .
Exercise 8.3.3 Show that every such π» must contain π 2 . (Hint:
think geometrically.)
We have π 2 ∈ π», and both other nonidentity elements of π» have order 2, so
they are of the form π
ππ for some π ∈ Z. The two such subgroups π» are
β¨π
, π 2 β© = {id, π
, π 2 , π
π 2 },
β¨π
π, π 2 β© = {id, π
π, π 2 , π
π −1 }.
Finally, any subgroup of index 2 of any group is normal, so all the subgroups
of πΊ of order 4 are normal.
Hence the subgroup structure of πΊ π· 4 is as follows, where a box around a
subgroup means that it is normal in πΊ.
order 1
1
β¨π
β©
β¨π
, π 2 β© πΆ2 × πΆ2
β¨π
π 2 β©
β¨π 2 β©
β¨π
πβ©
β¨πβ© πΆ4
πΊ = β¨π
, πβ© π· 4
126
β¨π
π −1 β©
order 2
β¨π
π, π 2 β© πΆ2 × πΆ2
order 4
order 8
Fixed fields We now find Fix(π») for each π» ∈ G , again considering the subgroups of orders 2 and 4 in turn. We’ll use the same three-step strategy as in
Example 8.2.5.
• Order 2: take Fixβ¨π
β© (officially Fix(β¨π
β©), but let’s drop the brackets). We
have π
(π) = π, so π ∈ Fixβ¨π
β©, so Q(π) ⊆ Fixβ¨π
β©. But [Q(π, π) : Q(π)] = 2,
and by the fundamental theorem, [Q(π, π) : Fixβ¨π
β©] = |β¨π
β©| = 2, so Fixβ¨π
β© =
Q(π).
Finding fixed fields
The same argument shows that for any π ∈ πΊ of order 2, if we can spot
some πΌ ∈ Q(π, π) such that π(πΌ) = πΌ and [Q(π, π) : Q(πΌ)] ≤ 2, then
Fixβ¨πβ© = Q(πΌ). For π = π
π 2 , we can take πΌ = ππ (by Figure 8.3). We have
degQ (ππ) = 4 since ππ is a root of π , so [Q(ππ) : Q] = 4, or equivalently,
[Q(π, π) : Q(ππ)] = 2. Hence Fixβ¨π
π 2 β© = Q(ππ).
Exercise 8.3.4 I took a small liberty in the sentence beginning
‘The same argument’, because it included an inequality but the
previous argument didn’t. Prove the statement made in that sentence.
It is maybe not so easy to spot an πΌ for π
π, but the geometric description
in Figure 8.3 suggests taking πΌ = π (1 − π). And indeed, one can check that
π
π fixes π (1 − π). One can also check that π (1 − π) is not the root of any
nonzero quadratic over Q, so degQ (π (1 − π)) is ≥ 4 (since it divides 8), so
[Q(π, π) : Q(π (1 − π))] ≤ 8/4 = 2. Hence Fixβ¨π
πβ© = Q(π (1 − π)). Similarly,
Fixβ¨π
π −1 β© = Q(π (1 + π)).
Finally,
π 2 (π 2 ) = (π 2 (π)) 2 = (−π) 2 = π 2 ,
π 2 (π) = π,
so Q(π 2 , π) ⊆ Fixβ¨π 2 β©. But [Q(π, π) : Q(π 2 , π)] = 2, so Fixβ¨π 2 β© = Q(π 2 , π).
• Order 4: for π» = β¨π
, π 2 β©, note that π 2 is fixed by both π
and π 2 , so
π 2 ∈ Fix(π»), so Q(π 2 ) ⊆ Fix(π»). But π 2 ∉ Q, so [Q(π 2 ) : Q] ≥ 2, so
[Q(π, π) : Q(π 2 )] ≤ 4. The fundamental theorem guarantees that
[Q(π, π) : Fix(π»)] = |π»| = 4,
so Fix(π») = Q(π 2 ).
The same argument applies to the other two subgroups π» of order 4: if
we can spot an element πΌ ∈ Q(π, π) \ Q fixed by the generators of π», then
Fix(π») = Q(πΌ). This gives Fixβ¨πβ© = Q(π) and Fixβ¨π
π, π 2 β© = Q(π 2π).
127
In summary, the fixed fields of the subgroups of πΊ are as follows.
degree 1
Q(π, π)
Q(π)
Q(π 2 )
Q(ππ)
Q(π 2 , π)
Q(π (1 − π))
Q(π)
Q(π (1 + π))
degree 2
Q(π 2π)
degree 4
degree 8
Q
On the right, ‘degree’ means the degree of Q(π, π) over the subfield concerned,
not the degree over Q. The fundamental theorem implies that the Galois group of
Q(π, π) over each intermediate field is the subgroup of πΊ in the same position in
the earlier diagram. For example, Gal(Q(π, π) : Q(π 2 , π)) = β¨π 2 β©. It also implies
that the intermediate fields that are normal over Q are the boxed ones.
Quotients
Finally, the fundamental theorem tells us that
Gal(Q(π, π) : Q)
Gal(πΏ : Q)
Gal(Q(π, π) : πΏ)
whenever πΏ is an intermediate field normal over Q.
For πΏ = Q(π 2 , π), this gives
πΊ/β¨π 2 β© Gal(Q(π 2 , π) : Q).
Normal subgroups
and normal
extensions
(8.4)
The left-hand side is the quotient of π· 4 by a subgroup isomorphic to πΆ2 . It has
order 4, but it has no element of order 4: for the only elements of πΊ of order 4
are π ±1 , whose images in πΊ/β¨π 2 β© have order 2. Hence πΊ/β¨π 2 β© πΆ2 × πΆ2 . On
the other hand, Q(π 2 , π) is the splitting field over Q of (π‘ 2 − 2)(π‘ 2 + 1), which by
Example 8.2.5 has Galois group πΆ2 × πΆ2 . This confirms the isomorphism (8.4).
The other three intermediate fields normal over Q, I leave to you:
Exercise 8.3.5 Choose one of Q(π 2 ), Q(π) or Q(π 2π), and do the same
for it as I just did for Q(π 2 , π).
As you’ve now seen, it can take quite some time to work through a particular example of the Galois correspondence. You’ll get practice at doing this in
workshops.
Beyond examples, there are at least two other uses of the fundamental theorem.
The first is to resolve the old question on solvability of polynomials by radicals,
which we met back in Chapter 1. The second is to work out the structure of finite
fields. We will carry out these two missions in the remaining two weeks.
128
Chapter 9
Solvability by radicals
Introduction to
Week 9
We began this course with a notorious old problem: can every polynomial be
solved by radicals? Theorem 1.3.5 gave the answer and more: not only is it
impossible to find a general formula that does it, but we can tell which specific
polynomials can be solved by radicals.
Theorem 1.3.5 states that a polynomial over Q is solvable by radicals if and only
if it has the right kind of Galois group—a solvable one. In degree 5 and higher,
there are polynomials that have the wrong kind of group. These polynomials are
not, therefore, solvable by radicals.
We’ll prove one half of this ‘if and only if’ statement: if π is solvable by
radicals then GalQ ( π ) is solvable. This is the half that’s needed to show that some
polynomials are not solvable by radicals. The proof of the other direction is in
Chapter 18 of Stewart’s book, but we won’t do it.
If you’re taking Algebraic Topology, you’ll already be familiar with the idea
that groups can be used to solve problems that seem to have nothing to do with
groups. You have a problem about some objects (such as topological spaces or
field extensions), you associate groups with those objects (maybe their fundamental
groups or their Galois groups), you translate your original problem into a problem
about groups, and you solve that instead. For example, the question of whether R2
and R3 are homeomorphic is quite difficult using only general topology; but using
algebraic topology, we can answer ‘no’ by noticing that the fundamental group of
R2 with a point removed is not isomorphic to the fundamental group of R3 with a
point removed. In much the same way, we’ll answer a difficult question about field
extensions by converting it into a question about groups.
For this chapter, you’ll need what you know about solvable groups. At a
minimum, you’ll need the definition, the fact that any quotient of a solvable group
is solvable, and the fact that π5 is not solvable.
129
9.1
Radicals
We speak of square roots, cube roots, and so on, but we also speak about roots
of polynomials. To distinguish between these two related usages, we will use the
word radical for square roots etc. (Radical comes from the Latin for root. A
radish is a root, and a change is radical if it gets to the root of the matter.)
Back in Chapter 1, I said that a complex number is called radical if ‘it can be
obtained from the rationals using only the usual arithmetic operations [addition,
subtraction, multiplication and division] and πth roots [for π ≥ 1]’. As an example,
I said that
√οΈ3 √
√2
7
1
+
2− 7
2
(9.1)
√οΈ
√οΈ
4
5 2
6+ 3
is radical, whichever square root, cube root, etc., we choose (p. 12). Let’s now
make this definition precise.
√
The first point is that the notation π π§ or π§1/π is highly dangerous:
Warning 9.1.1 Let π§ be a complex number and π ≥ 2. Then there
√
is no single number called π π§ or π§ 1/π . There are π elements πΌ of C
√
such that πΌπ = π§. So, the notation π π§ or π§1/π makes no sense if it is
intended to denote a single complex number. It is simply invalid.
When π§ belongs to the set R+ of nonnegative reals, the convention is
√
that π π§ or π§ 1/π denotes the unique πΌ ∈ R+ such that πΌπ = π§. There is
also a widespread convention that when π§ is a negative real and π is
√
odd, π π§ or π§1/π denotes the unique real πΌ such that πΌπ = π§. In these
cases, there is a sensible and systematic way of choosing one of the
πth roots of π§. But for a general π§ and π, there is not.
Complex analysis has a lot to say about different choices of πth roots.
But we don’t need to go into that. We simply treat all the πth roots of π§
on an equal footing, not attempting to pick out any of them as special.
With this warning in mind, we define the radical numbers without using no√
tation like π π§ or π§ 1/π . It is a ‘top-down’ definition, in the sense of Section 2.2.
Loosely, it says that the radical numbers form the smallest subfield of C closed
under taking square roots, cube roots, etc.
The definition of
radical number
Definition 9.1.2 Let Qrad be the smallest subfield of C such that for πΌ ∈ C,
πΌπ ∈ Qrad for some π ≥ 1 ⇒ πΌ ∈ Qrad .
A complex number is radical if it belongs to Qrad .
130
(9.2)
So any rational number is radical; any πth root of a radical number is radical;
the sum, product, difference or quotient of radical numbers is radical; and there
are no more radical numbers than can be obtained by those rules.
For the definition of Qrad to make sense, we need there to be a smallest subfield
of C with the property (9.2). This will be true as long as the intersection of any
family of subfields of C satisfying (9.2) is again a subfield of C satisfying (9.2):
for then Qrad is the intersection of all subfields of C satisfying (9.2).
Exercise 9.1.3 Check that the intersection of any family of subfields
of C satisfying (9.2) is again a subfield of C satisfying (9.2). (That any
intersection of subfields is a subfield is a fact we met back on p. 29;
the new aspect is (9.2).)
Example 9.1.4 Consider again the expression (9.1). It’s not quite as random as
it looks. I chose it so that the various radicals are covered by one of the two
conventions√οΈmentioned in Warning 9.1.1: they’re all πth roots of positive reals
√2
3√
7
2 − 7, which is an odd root of a negative real. Let π§ be the
except for
number (9.1), choosing the radicals according to those conventions.
I claim that π§ is radical, or equivalently that π§ belongs to every subfield πΎ of C
satisfying (9.2).
√οΈ5
2/3 ∈ πΎ
First, Q ⊆ πΎ since Q is the prime subfield of
C.
So
2/3
∈
πΎ,
and
so
√οΈ5
by (9.2). Also, 6 ∈ πΎ and πΎ is a field, so 6 + 2/3 ∈ πΎ. But then by (9.2) again,
the denominator of (9.1) is in πΎ. A similar argument shows that the numerator is
in πΎ. Hence π§ ∈ πΎ.
Definition 9.1.5 A nonzero polynomial over Q is solvable by radicals if all of its
complex roots are radical.
The simplest nontrivial example of a polynomial solvable by radicals is something of the form π‘ π − π, where π ∈ Q. The theorem we’re heading for is that
any polynomial solvable by radicals has solvable Galois group, and if that’s true
then the group GalQ (π‘ π − π) must be solvable. Let’s consider that group now. The
results we prove about it will form part of the proof of the big theorem.
We begin with the case π = 1.
Lemma 9.1.6 For all π ≥ 1, the group GalQ (π‘ π − 1) is abelian.
Proof Write π = π 2ππ/π . The complex roots of π‘ π − 1 are 1, π, . . . , ππ−1 , so
SFQ (π‘ π − 1) = Q(π).
Let π, π ∈ GalQ (π‘ π − 1). Since π permutes the roots of π‘ π − 1, we have
π(π) = ππ for some π ∈ Z. Similarly, π (π) = π π for some π ∈ Z. Hence
(π β¦ π)(π) = π(π π ) = π(π) π = ππ π ,
131
and similarly (π β¦ π)(π) = ππ π . So (π β¦ π)(π) = (π β¦ π)(π). Since SFQ (π‘ π − 1) =
Q(π), it follows that π β¦ π = π β¦ π.
β‘
Exercise 9.1.7 In the last sentence of that proof, how exactly does it
‘follow’?
Much more can be said about the Galois group of π‘ π − 1, and you’ll see a bit
more in workshops. But this is all we need for our purposes.
Now that we’ve considered π‘ π − 1, let’s do π‘ π − π for an arbitrary π.
Lemma 9.1.8 Let πΎ be a field and π ≥ 1. Suppose that π‘ π − 1 splits in πΎ. Then
GalπΎ (π‘ π − π) is abelian for all π ∈ πΎ.
The hypothesis that π‘ π − 1 splits in πΎ might seem so restrictive as to make
this lemma useless. For instance, it doesn’t hold in Q or even R (for π > 2).
Nevertheless, this turns out to be the key lemma in the whole story of solvability
by radicals.
Proof If π = 0 then GalπΎ (π‘ π − π) is trivial; suppose otherwise.
Choose a root π of π‘ π − π in SFπΎ (π‘ π − π). For any other root π, we have
(π/π) π = π/π = 1 (valid since π ≠ 0), and π‘ π − 1 splits in πΎ, so π/π ∈ πΎ.
It follows that SFπΎ (π‘ π − π) = πΎ (π). Moreover, given π, π ∈ GalπΎ (π‘ π − π), we
have π(π)/π ∈ πΎ (since π(π) is a root of π‘ π − π), so
π(π)
π(π)π (π)
π(π)
·π =
· π (π) =
.
(π β¦ π)(π) = π
π
π
π
Similarly, (πβ¦π)(π) = π(π)π (π)/π, so (π β¦π)(π) = (πβ¦π)(π). Since SFπΎ (π‘ π −π) =
πΎ (π), it follows that π β¦ π = π β¦ π.
β‘
Warning 9.1.9 For π ∈ Q, the Galois group of π‘ π − π over Q is
not usually abelian. For instance, we saw in Example 7.1.14 that
GalQ (π‘ 3 − 2) is the nonabelian group π3 .
Exercise 9.1.10 What does the proof of Lemma 9.1.8 tell you about
the eigenvectors and eigenvalues of the elements of GalπΎ (π‘ π − π)?
Exercise 9.1.11 Use Lemmas 9.1.6 and 9.1.8 to show that GalQ (π‘ π −π)
is solvable for all π ∈ Q.
This is harder than most of these exercises, but I recommend it as a
way of getting into the right frame of mind for the theory that’s coming
in Section 9.2.
132
Digression 9.1.12 We’re only going to do the theory of solvability by
radicals over Q. It can be done over any field, but Q has two special features.
First, Q can be embedded in an algebraically closed field that we know very
well: C. This makes some things easier. Second, char Q = 0. For fields of
characteristic π, there are extra complications (Stewart, Section 17.6).
9.2
Solvable polynomials have solvable groups
Here we’ll prove that every polynomial over Q that is solvable by radicals has
solvable Galois group.
You know by now that in Galois theory, we tend not to jump straight from
polynomials to groups. We go via the intermediate stage of field extensions, as in
the diagram
polynomial β¦−→ field extension β¦−→ group
that I first drew after the definition of GalπΎ ( π ) (p. 93). That is, we understand
polynomials through their splitting field extensions.
So it shouldn’t be a surprise that we do the same here, defining a notion of
‘solvable extension’ and showing (roughly speaking) that
solvable polynomial β¦−→ solvable extension β¦−→ solvable group.
Solvable
polynomials have
solvable groups:
a map
In other words, we’ll define ‘solvable extension’ in such a way that (i) if π ∈ Q[π‘]
is a polynomial solvable by radicals then SFQ ( π ) : Q is a solvable extension, and
(ii) if π : πΎ is a solvable extension then Gal(π : πΎ) is a solvable group. Hence
if π is solvable by radicals then GalQ ( π ) is solvable—the result we’re aiming for.
Definition 9.2.1 Let π : πΎ be a finite normal separable extension. Then π : πΎ
is solvable (or π is solvable over πΎ) if there exist π ≥ 0 and intermediate fields
πΎ = πΏ 0 ⊆ πΏ 1 ⊆ · · · ⊆ πΏπ = π
such that πΏ π : πΏ π−1 is normal and Gal(πΏ π : πΏ π−1 ) is abelian for each π ∈ {1, . . . , π }.
Exercise 9.2.2 Let π : π : πΎ be extensions, with π : π, π : πΎ and
π : πΎ all finite, normal and separable. Show that if π : π and π : πΎ
are solvable then so is π : πΎ.
We will focus on subfields of C, where separability is automatic (Example 7.2.14(i)).
133
Example 9.2.3 Let π ∈ Q and π ≥ 1. Then SFQ (π‘ π − π) : Q is a finite normal
separable extension, being a splitting field extension over Q. I claim that it is
solvable.
Proof: if π = 0 then SFQ (π‘ π − π) = Q, and Q : Q is solvable (taking π = 0 and
πΏ 0 = Q in Definition 9.2.1). Now assume that π ≠ 0. Choose a complex root π of
π‘ π − π and write π = π 2ππ/π . Then the complex roots of π‘ π − π are
π, ππ, . . . , ππ−1 π.
So SFQ (π‘ π − π) contains (ππ π)/π = ππ for all π, and so π‘ π − 1 splits in SFQ (π‘ π − π).
Hence
Q ⊆ SFQ (π‘ π − 1) ⊆ SFQ (π‘ π − π).
Now SFQ (π‘ π − 1) : Q is normal (being a splitting field extension) and has abelian
Galois group by Lemma 9.1.6. Also SFQ (π‘ π − π) : SFQ (π‘ π −1) is normal (being the
splitting field extension of π‘ π − π over SFQ (π‘ π − 1), by Lemma 6.2.14(ii)), and has
abelian Galois group by Lemma 9.1.8. So SFQ (π‘ π − π) : Q is a solvable extension,
as claimed.
The definition of solvable extension bears a striking resemblance to the definition of solvable group. Indeed:
Lemma 9.2.4 Let π : πΎ be a finite normal separable extension. Then
π : πΎ is solvable ⇐⇒ Gal(π : πΎ) is solvable.
Proof We will only need the ⇒ direction, and that is all I prove here. For the
converse, see the workshop questions.
Suppose that π : πΎ is solvable. Then there are intermediate fields
πΎ = πΏ 0 ⊆ πΏ 1 ⊆ · · · ⊆ πΏπ = π
such that each extension πΏ π : πΏ π−1 is normal with abelian Galois group. For
each π ∈ {1, . . . , π }, the extension π : πΏ π−1 is finite, normal and separable (by
Corollary 7.1.6 and Lemma 7.2.16), so we can apply the fundamental theorem of
Galois theory to it. Since πΏ π : πΏ π−1 is a normal extension, Gal(π : πΏ π ) is a normal
subgroup of Gal(π : πΏ π−1 ) and
Gal(π : πΏ π−1 )
Gal(πΏ π : πΏ π−1 ).
Gal(π : πΏ π )
By hypothesis, the right-hand side is abelian, so the left-hand side is too. So the
sequence of subgroups
Gal(π : πΎ) = Gal(π : πΏ 0 ) ⊇ Gal(π : πΏ 1 ) ⊇ · · · ⊇ Gal(π : πΏ π ) = 1
exhibits Gal(π : πΎ) as a solvable group.
134
β‘
Exercise 9.2.5 Prove the ⇐ direction of Lemma 9.2.4. It’s a very
similar argument to the proof of ⇒.
According to the story I’m telling, solvability by radicals of a polynomial
should correspond to solvability of its splitting field extension. Thus, the subfields
of C that are solvable over Q should be exactly the splitting fields SFQ ( π ) of
polynomials π that are solvable by radicals. (This is indeed true, though we won’t
entirely prove it.) Now if π , π ∈ Q[π‘] are both solvable by radicals then so is π π,
and SFQ ( π π) is a solvable extension of Q containing both SFQ ( π ) and SFQ (π).
So it should be the case that for any two subfields of C solvable over Q, there is
some larger subfield, also solvable over Q, containing both.
The following pair of lemmas proves this. They use the notion of compositum
(Definition 5.3.3).
Lemma 9.2.6 Let π : πΎ be a field extension and let πΏ and πΏ ′ be intermediate
fields.
π
πΏπΏ ′
i. If πΏ : πΎ and πΏ ′ : πΎ are finite and normal, then so is πΏπΏ ′ : πΎ.
πΏ′
πΏ
ii. If πΏ : πΎ is finite and normal, then so is πΏπΏ ′ : πΏ ′.
πΎ
iii. If πΏ : πΎ is finite and normal with abelian Galois group, then so is πΏπΏ ′ : πΏ ′.
Proof For (i), we have πΏ = SFπΎ ( π ) and πΏ ′ = SFπΎ ( π ′) for some π , π ′ ∈ πΎ [π‘].
Now πΏπΏ ′ is the subfield of π generated by πΏ ∪ πΏ ′, or equivalently by the roots of
π and π ′. So πΏπΏ ′ = SFπΎ ( π π ′), which is finite and normal over πΎ.
For (ii), we have πΏ = SFπΎ ( π ) for some π ∈ πΎ [π‘]. Then πΏπΏ ′ = SF πΏ ′ ( π )
by Lemma 6.2.14(i) (with π = πΏ and π = πΏ ′), so πΏπΏ ′ is finite and normal over
πΏ ′. Now Gal(πΏπΏ ′ : πΏ ′) = Gal πΏ ′ ( π ), which by Corollary 6.3.12 is isomorphic to
a subgroup of GalπΎ ( π ) = Gal(πΏ : πΎ). So if Gal(πΏ : πΎ) is abelian then so is
Gal(πΏπΏ ′ : πΏ ′), proving (iii).
β‘
Lemma 9.2.7 Let πΏ and π be subfields of C such that the extensions πΏ : Q and
π : Q are finite, normal and solvable. Then there is some subfield π of C such
that π : Q is finite, normal and solvable and πΏ, π ⊆ π.
Both the statement and the proof of this lemma should remind you of
Lemma 5.3.8 on ruler and compass constructions.
Proof Take subfields
Q = πΏ 0 ⊆ · · · ⊆ πΏ π = πΏ,
Q = π0 ⊆ · · · ⊆ ππ = π
135
such that πΏ π : πΏ π−1 is normal with abelian Galois group for each π, and similarly
for π π : π π−1 . There is a chain of subfields
Q = πΏ 0 ⊆ · · · ⊆ πΏ π = πΏ = πΏπ0 ⊆ · · · ⊆ πΏππ = πΏπ
(9.3)
of C. Put π = πΏπ. Certainly πΏ, π ⊆ π. We show that π : Q is finite, normal
and solvable.
That π : Q is finite and normal follows from Lemma 9.2.6(i).
To see that π : Q is solvable, we show that each successive extension in (9.3)
is normal with abelian Galois group. For those to the left of πΏ, this is immediate.
For those to the right, let π ∈ {1, . . . , π }. Since π π : π π−1 is finite and normal
with abelian Galois group, so is πΏπ π : πΏπ π−1 by Lemma 9.2.6(iii).
β‘
The set of radical numbers is a subfield of C closed under taking πth roots. So
if the story I’m telling is right, the set of complex numbers that can be reached
from Q by solvable extensions should also be a subfield of C closed under taking
πth roots. That’s an informal description of our next two results. Write
Qsol = {πΌ ∈ C : πΌ ∈ πΏ for some subfield πΏ ⊆ C that is finite, normal and solvable
over Q}.
Lemma 9.2.8 Qsol is a subfield of C.
Proof This is similar to the proof that the algebraic numbers form a subfield of
C (Proposition 5.2.7). Let πΌ, π½ ∈ Qsol . Then πΌ ∈ πΏ and π½ ∈ π for some πΏ, π
that are finite, normal and solvable over Q. By Lemma 9.2.7, πΌ, π½ ∈ π for some
π that is finite, normal and solvable over Q. Then πΌ + π½ ∈ π, so πΌ + π½ ∈ Qsol ,
and similarly πΌ · π½ ∈ Qsol . This shows that Qsol is closed under addition and
multiplication. The other parts of the proof (negatives, reciprocals, 0 and 1) are
straightforward.
β‘
Lemma 9.2.9 Let πΌ ∈ C and π ≥ 1. If πΌπ ∈ Qsol then πΌ ∈ Qsol .
The proof (below) is slightly subtle. Here’s why.
Let πΏ be a subfield of C that’s finite, normal and solvable over Q, and take
πΌ ∈ C and π ≥ 1 such that πΌπ ∈ πΏ. To find some larger π that contains πΌ itself and
is also solvable over Q, we could try putting π = SF πΏ (π‘ π − πΌπ ). But the problem
is that π : Q is not in general normal. And normality is part of the definition of
Qsol , ultimately because it’s essential if we want to use the fundamental theorem
of Galois theory. The basic problem is this:
136
Warning 9.2.10 A normal extension of a normal extension is not in
general normal, just as a normal subgroup of a normal subgroup is not
in general normal.
An example should clarify.
√
√
√4
2 =
2
and
π
=
2.
We
have
πΌ
2
∈
Q(
2), and
Example
9.2.11
Put
πΌ
=
√
the
abelian
Q( 2) : Q is finite, normal and solvable (since its Galois group is
√4
2
sol
group πΆ2 ), so πΌ ∈ Q . Hence, according to Lemma 9.2.9, πΌ = 2 should be
contained in some finite normal solvable extension π of Q.
√
How can we find such an π? We can’t take π = SFQ(√2) (π‘ 2 − 2), since this
√3
√4
is Q( 2), which is not normal over Q (for the same reason that Q( 2) isn’t).
To find a bigger π, still finite √
and solvable over Q but also normal,
we have
√
to adjoin a square root not just of 2 but also of its conjugate, − 2. This is the
crucial point: the whole idea of normality is that conjugates are treated equally.
(Normal behaviour means that anything
you do for one element, you do for all
√4
4
its conjugates.) The result is Q( 2, π) = SFQ (π‘
√4 − 2), which is indeed a finite,
solvable and normal extension of Q containing 2.
Proof of Lemma 9.2.9 Write π = πΌπ ∈ Qsol . Choose a subfield πΎ of C such that
π ∈ πΎ and πΎ : Q is finite, normal and solvable.
Step 1: enlarge πΎ to a field in which π‘ π − 1 splits. Put πΏ = SFπΎ (π‘ π − 1) ⊆ C.
Since πΎ : Q is finite and normal, πΎ = SFQ ( π ) for some nonzero π ∈ Q[π‘], and
then πΏ = SFQ (π‘ π − 1) π (π‘) . Hence πΏ : Q is finite and normal. The Galois group
of πΏ : πΎ is GalπΎ (π‘ π − 1), which is isomorphic to a subgroup of GalQ (π‘ π − 1) (by
Corollary 6.3.12), which is abelian (by Lemma 9.1.6). Hence πΏ : πΎ is a normal
extension with abelian Galois group. Also, πΎ : Q is solvable. It follows from the
definition of solvable extension that πΏ : Q is solvable.
In summary, πΏ is a subfield of C such that π ∈ πΏ and πΏ : Q is finite, normal
and solvable, and, moreover, π‘ π − 1 splits in πΏ. We now forget about πΎ.
Step 2: adjoin the πth roots of the conjugates of π. Write π ∈ Q[π‘] for the
minimal polynomial of π over Q, and put π = SF πΏ (π(π‘ π )) ⊆ C. Then πΌ ∈ π, as
π(πΌπ ) = π(π) = 0. We show that π : Q is finite, normal and solvable.
Since πΏ : Q is finite and normal, πΏ = SFQ (π) for some nonzero π ∈ Q[π‘].
Then π = SFQ (π(π‘)π(π‘ π )), so π : Q is finite and normal. Moreover, π : πΏ is
finite and normal, being a splitting field extension.
Now to show that π : Q is solvable, it is enough to show that π : πΏ is solvable,
by Exercise 9.2.2. Since πΏ : Q is normal and π ∈ Q[π‘] is the minimal polynomial
137
of π ∈ πΏ, it follows by definition of normality that π splits in πΏ, say
π(π‘) =
π
Ö
(π‘ − ππ )
π=1
(ππ ∈ πΏ). Define subfields πΏ 0 ⊆ · · · ⊆ πΏ π of C by
πΏ0 = πΏ
πΏ 1 = SF πΏ 0 (π‘ π − π 1 )
πΏ 2 = SF πΏ 1 (π‘ π − π 2 )
..
.
πΏ π = SF πΏπ −1 (π‘ π − ππ ).
Then
πΏ π = πΏ π½ ∈ π : π½π ∈ {π 1 , . . . , ππ } .
In particular, πΏ π = π. For each π ∈ {1, . . . , π }, the extension πΏ π : πΏ π−1 is finite
and normal (being a splitting field extension), and its Galois group is abelian (by
Lemma 9.1.8 and the fact that π‘ π − 1 splits in πΏ ⊆ πΏ π−1 ). So π : πΏ is solvable. β‘
Now we can relate the set Qrad of radical numbers, defined in terms of basic
arithmetic operations, to the set Qsol , defined in terms of field extensions.
Proposition 9.2.12 Qrad ⊆ Qsol . That is, every radical number is contained in
some subfield of C that is a finite, normal, solvable extension of Q.
In fact, Qrad and Qsol are equal, but we won’t prove this.
Proof By Lemmas 9.2.8 and 9.2.9, Qsol is a subfield of C such that πΌπ ∈ Qsol ⇒
πΌ ∈ Qsol . The result follows from the definition of Qrad .
β‘
This brings us to the main result of this chapter. Notice that it doesn’t mention
field extensions: it goes straight from polynomials to groups.
Theorem 9.2.13 Let 0 ≠ π ∈ Q[π‘]. If the polynomial π is solvable by radicals
then the group GalQ ( π ) is solvable.
Proof Suppose that π is solvable by radicals. Write πΌ1 , . . . , πΌπ ∈ C for its roots.
For each π, we have πΌπ ∈ Qrad (by definition of solvability by radicals), hence
πΌπ ∈ Qsol (by Proposition 9.2.12). So each of πΌ1 , . . . , πΌπ is contained in some
subfield of C that is finite, normal and solvable over Q. By Lemma 9.2.7, there is
some subfield π of C that is finite, normal and solvable over Q and contains all of
πΌ1 , . . . , πΌπ . Then Q(πΌ1 , . . . , πΌπ ) ⊆ π; that is, SFQ ( π ) ⊆ π.
138
By Lemma 9.2.4, Gal(π : Q) is solvable. Now SFQ ( π ) : Q is normal, so
by the fundamental theorem of Galois theory, Gal(SFQ ( π ) : Q) is a quotient of
Gal(π : Q). But Gal(SFQ ( π ) : Q) = GalQ ( π ), and a quotient of a solvable group
is solvable, so GalQ ( π ) is solvable.
β‘
Examples 9.2.14
i. For π ∈ Q and π ≥ 1, the polynomial π‘ π − π is solvable by
radicals, so the group GalQ (π‘ π − π) is solvable. You may already have proved
this in Exercise 9.1.11. It also follows from Example 9.2.3 and Lemma 9.2.4.
ii. Let π 1 , . . . , π π ∈ Q and π1 , . . . , π π ≥ 1. Each of the polynomials π‘ ππ −ππ is
Î
solvable by radicals, so their product is too. Hence GalQ π (π‘ ππ − ππ ) is a
solvable group.
Theorem 9.2.13 is most sensational in its contrapositive form: if GalQ ( π ) is not
solvable then π is not solvable by radicals. That’s the subject of the next section.
Digression 9.2.15 The converse of Theorem 9.2.13 is also true: if GalQ ( π )
is solvable then π is solvable by radicals. You can even unwind the proof
to obtain an explicit formula for the solving the quartic by radicals (Stewart,
Chapter 18).
For this, we have to deduce properties of a field extension from assumptions
about its Galois group. A solvable group is built up from abelian groups,
and every finite abelian group is a direct sum of cyclic groups. The key
step in proving the converse of Theorem 9.2.13 has come to be known as
‘Hilbert’s Theorem 90’ (Stewart’s Theorem 18.18), which gives information
about field extensions whose Galois groups are cyclic.
Digression 9.2.16 The proof of Theorem 9.2.13 might not have ended quite
how you expected. Given my explanations earlier in the chapter, you might
justifiably have imagined we were going to show that when the polynomial
π is solvable by radicals, the extension SFQ ( π ) : Q is solvable. That’s not
what we did. We showed that SFQ ( π ) is contained in some larger subfield
π such that π : Q is solvable, then used that to prove the solvability of the
group GalQ ( π ).
But all is right with the world: SFQ ( π ) : Q is a solvable extension. Indeed, its
Galois group GalQ ( π ) is solvable, so Lemma 9.2.4 implies that SFQ ( π ) : Q
is solvable too.
9.3
An unsolvable polynomial
Here we give a specific example of a polynomial over Q that is not solvable by
radicals. By Theorem 9.2.13, our task is to construct a polynomial whose Galois
139
group is not solvable. The smallest non-solvable group is π΄5 (of order 60). Our
polynomial has Galois group π5 (of order 120), which is also non-solvable.
Finding Galois groups is hard, and we will use a whole box of tools and tricks,
from Cauchy’s theorem on groups to Rolle’s theorem on differentiable functions.
First we prove a useful general fact on the order of Galois groups.
Lemma 9.3.1 Let π be an irreducible polynomial over a field πΎ, with SFπΎ ( π ) : πΎ
separable. Then deg( π ) divides | GalπΎ ( π )|.
Proof Let πΌ be a root of π in SFπΎ ( π ). By irreducibility, deg( π ) = [πΎ (πΌ) : πΎ],
which divides [SFπΎ ( π ) : πΎ] by the tower law, which is equal to | GalπΎ ( π )| by
Theorem 7.2.18 (using separability).
β‘
Next, we need some results about the symmetric group ππ . I assume you know
that ππ is generated by the ‘adjacent transpositions’ (12), (23), . . . , (π − 1 π). This
may have been proved in Fundamentals of Pure Mathematics, and as the Group
Theory notes say (p. 58):
This is intuitively clear: suppose you have π people lined up and you
want them to switch into a different order. To put them in the order
you want them, it’s clearly enough to have people move up and down
the line; and each time a person moves one place, they switch places
with the person next to them.
Here’s a different way of generating ππ .
Lemma 9.3.2 For π ≥ 2, the symmetric group ππ is generated by (12) and
(12 . . . π).
Proof We have
(12 . . . π)(12)(12 . . . π) −1 = (23),
either by direct calculation or the general fact that π(π 1 . . . π π )π −1 =
(π(π 1 ) . . . π(π π )) for any π ∈ ππ and cycle (π 1 . . . π π ). So any subgroup π»
of ππ containing (12) and (12 . . . π) also contains (23). By the same argument, π»
also contains (34), . . . , (π − 1 π). But the adjacent transpositions generate ππ , so
π» = ππ .
β‘
Lemma 9.3.3 Let π be a prime number, and let π ∈ Q[π‘] be an irreducible
polynomial of degree π with exactly π − 2 real roots. Then GalQ ( π ) π π .
Proof Since char Q = 0 and π is irreducible, π is separable and therefore has π
distinct roots in C. By Proposition 6.3.10, the action of GalQ ( π ) on the roots of
π in C defines an isomorphism between GalQ ( π ) and a subgroup π» of π π . Since
140
Figure 9.1: The function π₯ β¦→ π₯ 5 − 6π₯ + 3.
π is irreducible, π divides | GalQ ( π )| = |π»| (by Lemma 9.3.1). So by Cauchy’s
theorem, π» has an element π of order π. Then π is a π-cycle, since these are the
only elements of π π of order π.
The complex conjugate of any root of π is also a root of π , so complex
conjugation restricts to an automorphism of SFQ ( π ) over Q. Exactly two of the
roots of π are non-real; complex conjugation transposes them and fixes the rest.
So π» contains a transposition π.
Without loss of generality, π = (12). Since π is a π-cycle, ππ (1) = 2 for
some π ∈ {1, . . . , π − 1}. Since π is prime, ππ also has order π, so it is a π-cycle.
Now without loss of generality, ππ = (123 . . . π). So (12), (12 . . . π) ∈ π», forcing
π» = π π by Lemma 9.3.2. Hence GalQ ( π ) π π .
β‘
Exercise 9.3.4 Explain why, in the last paragraph, ππ has order π.
Theorem 9.3.5 Not every polynomial over Q of degree 5 is solvable by radicals.
Proof We show that π (π‘) = π‘ 5 − 6π‘ + 3 satisfies the conditions of Lemma 9.3.3.
Then GalQ ( π ) is π5 , which is not solvable, so by Theorem 9.2.13, π is not solvable
by radicals.
Evidently deg( π ) is the prime number 5, and π is irreducible by Eisenstein’s
criterion with prime 3. It remains to prove that π has exactly 3 real roots. This is
where we use some analysis, considering π as a function R → R (Figure 9.1).
We have
lim π (π₯) = −∞,
π (0) > 0,
π₯→−∞
π (1) < 0,
lim π (π₯) = ∞,
π₯→∞
and π is continuous on R, so by the intermediate value theorem, π has√οΈat least 3
real roots. On the other hand, π ′ (π₯) = 5π₯ 4 − 6 has only 2 real roots (± 4 6/5), so
141
by Rolle’s theorem, π has at most 3 real roots. Hence π has exactly 3 real roots,
as required.
β‘
Exercise 9.3.6 Prove that for every π ≥ 5, there is some polynomial
of degree π that is not solvable by radicals.
Example 9.3.7 There are also quintics with Galois group π΄5 . These are not
solvable by radicals, since π΄5 is not a solvable group. One example, although we
won’t prove it, is π‘ 5 + 20π‘ + 16.
Digression 9.3.8 We now know that some polynomials π over Q are not
solvable by radicals, which means that not all their complex roots are radical.
Could it be that some of the roots are radical and others are not? Yes: simply
take a polynomial π that is not solvable by radicals and put π (π‘) = π‘π(π‘).
Then the roots of π are 0 (which is radical) together with the roots of π
(which are not all radical).
But what if π is irreducible? In that case, either all the roots of π are radical
or none of them are. This follows from the fact that the extension Qrad : Q is
normal, which we will not prove.
Digression 9.3.9 There are many similarities between the theory of constructibility of points by ruler and compass and the theory of solvability of
polynomials by radicals. In both cases, the challenge is to construct some
things (points in the plane or roots of polynomials) using only certain tools
(ruler and compass or a machine for taking πth roots). In both cases, there
were difficult questions of constructibility that remained open for a very long
time, and in both cases, they were solved by field theory.
The solutions have something in common too. For the geometry problem,
we used iterated quadratic extensions, and for the polynomial problem, we
used solvable extensions, which could reasonably be called iterated abelian
extensions. For the geometry problem, we showed that the coordinates of any
point constructible by ruler and compass satisfy a certain condition on their
degree over Q (Theorem 5.3.10); for the polynomial problem, we showed
that any polynomial solvable by radicals satisfies a certain condition on its
Galois group over Q. There are other similarities: compare Lemmas 5.3.8
and 9.2.7, for example, and maybe you can find more similarities still.
We have now used the fundamental theorem of Galois theory to solve a major
problem about Q. What else can we do with it?
The fundamental theorem is about separable extensions. Our two main sources
of separable extensions are:
142
• fields of characteristic 0 such as Q (Example 7.2.14(i)), which we’ve explored
extensively already;
• finite fields (Example 7.2.14(ii)), which we’ve barely touched.
In the next and final chapter, we’ll use the fundamental theorem and other results
we’ve proved to explore the world of finite fields. In contrast to the intricately
complicated world of finite groups, finite fields are almost shockingly simple.
143
Chapter 10
Finite fields
This chapter is dessert. Through this semester, we’ve developed a lot of sophisticated theory for general fields. All of it works for finite fields, but becomes much
simpler there. It’s a miniature world in which life is sweet. For example:
Introduction to
Week 10
• If we want to apply the fundamental theorem of Galois theory to a field
extension π : πΎ, we first have to ask whether it is finite, and whether it is
normal, and whether it is separable. When π and πΎ are finite fields, all
three conditions are automatic.
• There are many fields of different kinds, and to classify them all would be a
near-impossible task. But for finite fields, the classification is very simple.
We know exactly what finite fields there are.
• The Galois correspondence for arbitrary field extensions can also be complicated. But again, it’s simple when the fields are finite. Their Galois groups
are very easy (they’re all cyclic), we know what their subgroups are, and it’s
easy to describe all the subfields of any given finite field.
So although the world of finite fields is not trivial, there’s a lot about it that’s
surprisingly straightforward.
We’ve already encountered two aspects of finite fields that may seem counterintuitive. First, they always have positive characteristic, which means they satisfy
some equation like 1 + · · · + 1 = 0 (Lemma 2.3.17). Second, any element of a finite
field of characteristic π has precisely one πth root (Corollary 2.3.22(ii)), making
finite fields quite unlike C, R or Q. But the behaviour of πth roots and πth powers
is fundamental to all of finite fields’ nice properties.
144
10.1
Classification of finite fields
If you try to write down a formula for the number of groups or rings with a given
number of elements, you’ll find that it’s hard and the results are quite strange. For
instance, more than 99% of the first 50 billion groups have order 1024.
But fields turn out to be much, much easier. We’ll obtain a complete classification of finite fields in the next two pages.
The order of a finite field π is its cardinality, or number of elements, |π |.
Lemma 10.1.1 Let π be a finite field. Then char π is a prime number π, and
|π | = π π where π = [π : F π ] ≥ 1.
In particular, the order of a finite field is a prime power.
Proof By Lemmas 2.3.11 and 2.3.17, char π is a prime number π. By
Lemma 2.3.16, π has prime subfield F π . Since π is finite, 1 ≤ [π : F π ] < ∞;
write π = [π : F π ]. As a vector space over F π , then, π is π-dimensional and so
isomorphic to Fππ . But |Fππ | = |F π | π = π π , so |π | = π π .
β‘
Example 10.1.2 There is no field of order 6, since 6 is not a prime power.
Warning 10.1.3 Order and degree mean different things. For instance, if the order of a field is 9, then its degree over its prime
subfield F3 is 2.
Lemma 10.1.1 prompts two questions:
• Given a prime power π π , is there some field of order π π ?
• If so, how many are there?
To answer them, we need to use the Frobenius automorphism π of a finite field
(Proposition 2.3.20).
Exercise 10.1.4√Work out the values of the Frobenius automorphism
on the field F3 ( 2), which you first met in Exercise 4.3.18.
The answer to the first of these two questions is yes:
Lemma 10.1.5 Let π be a prime number and π ≥ 1. Then the splitting field of
π
π‘ π − π‘ over F π has order π π .
145
π
Proof Put π (π‘) = π‘ π − π‘ ∈ F π [π‘] and π = SFF π ( π ). Then π· π = −1 (since
π ≥ 1), so by (i)⇒(ii) of Lemma 7.2.9, π has no repeated roots in π. Hence π
has at least π π elements.
π
Write π for the Frobenius map of π and π π = π β¦ · · · β¦ π. Then π π (πΌ) = πΌ π
for all πΌ, so the set πΏ of roots of π in π is Fix{π π }. Since π is a homomorphism,
Lemma 7.3.1 implies that πΏ is a subfield of π. Hence by definition of splitting
field, πΏ = π; that is, every element of π is a root of π . And since deg( π ) = π π ,
it follows that π has at most π π elements.
β‘
As for the second question, there is exactly one field of each prime power order.
To show this, we need a lemma.
Lemma 10.1.6 Let π be a finite field of order π. Then πΌ π = πΌ for all πΌ ∈ π.
The proof uses the same argument as in Example 2.3.21.
Proof The multiplicative group π × = π \ {0} has order π − 1, so Lagrange’s
theorem implies that πΌ π−1 = 1 for all πΌ ∈ π × . Hence πΌ π = πΌ whenever 0 ≠ πΌ ∈ π,
and clearly the equation holds for πΌ = 0 too.
β‘
Exercise 10.1.7 Verify directly that π½4 = π½ for all π½ in the 4-element
field F2 (πΌ) of Example 5.1.8.
Lemma 10.1.8 Every finite field of order π is a splitting field of π‘ π − π‘ over F π .
Proof Let π be a field of order π. By Lemma 10.1.1, π = π π for some prime π
and π ≥ 1, and char π = π. Hence π has prime subfield F π . By Lemma 10.1.6,
π
every element of π is a root of π (π‘) = π‘ π − π‘. So π has |π | distinct roots in π;
but |π | = π π = deg( π ), so π splits in π. The set of roots of π in π generates π,
since it is equal to π. Hence π is a splitting field of π .
β‘
Together, these results completely classify the finite fields.
Theorem 10.1.9 (Classification of finite fields)
i. Every finite field has
order π π for some prime π and integer π ≥ 1.
ii. For each prime π and integer π ≥ 1, there is exactly one field of order
π π , up to isomorphism. It has characteristic π and is a splitting field for
π
π‘ π − π‘ over F π .
Proof This is immediate from the results above together with the uniqueness of
splitting fields (Theorem 6.2.13(ii)).
β‘
When π > 1 is a prime power, we write Fπ for the one and only field of order π.
146
Warning 10.1.10 Fπ is not Z/β¨πβ© unless π is a prime. It can’t be,
because Z/β¨πβ© is not a field (Example 2.3.27). To my knowledge, there
is no description of Fπ simpler than the splitting field description.
We now know exactly how many finite fields there are of each order. But
generally in algebra, it’s important to think not just about the objects (such as vector
spaces, groups, modules, rings, fields, . . . ), but also the maps (homomorphisms)
between objects. So now that we’ve counted the finite fields, it’s natural to try
to count the homomorphisms between finite fields. Field homomorphisms are
injective, so this boils down to counting subfields and automorphisms. Galois
theory is very well equipped to do that! We’ll come to this in the final section. But
first, we look at another way in which finite fields are very simple.
10.2
Multiplicative structure
The multiplicative group πΎ × of a finite field πΎ is as easy as can be:
Proposition 10.2.1 For an arbitrary field πΎ, every finite subgroup of πΎ × is cyclic.
In particular, if πΎ is finite then πΎ × is cyclic.
The multiplicative
group of a finite
field is cyclic
Proof This was Theorem 5.1.13 and Corollary 5.1.14 of Group Theory.
β‘
Example 10.2.2 In examples earlier in the course, we frequently used the πth root
of unity π = π 2ππ/π ∈ C, which has the property that every other πth root of unity
is a power of π.
Can we find an analogue of π in an arbitrary field πΎ? It’s not obvious how
to generalize the formula π 2ππ/π , since the exponential is a concept from complex
analysis. But Proposition 10.2.1 solves our problem. For π ≥ 1, put
ππ (πΎ) = {πΌ ∈ πΎ : πΌπ = 1}.
Then ππ (πΎ) is a subgroup of πΎ × , and is finite since its elements are roots of π‘ π − 1.
So by Proposition 10.2.1, ππ (πΎ) is cyclic. Let π be a generator of ππ (πΎ). Then
every πth root of unity in πΎ is a power of π, which is what we were aiming for.
Note, however, that ππ (πΎ) may have fewer than π elements, or equivalently,
the order of π may be less than π. For instance, if char πΎ = π then π π (πΎ) is trivial
and π = 1, by Example 2.3.23(ii).
Exercise 10.2.3 Let πΎ be a field and let π» be a finite subgroup of πΎ ×
of order π. Prove that π» ⊆ ππ (πΎ).
147
Example 10.2.4 The group F×π is cyclic, for any prime π. This means that there
is some π ∈ {1, . . . , π − 1} such that π, π2 , . . . runs through all elements of
{1, . . . , π − 1} when taken mod π. In number theory, such an π is called a
primitive root mod π (another usage of the word ‘primitive’). For instance, you
can check that 3 is a primitive root mod 7, but 2 is not, since 23 ≡ 1 (mod 7).
Finding the primitive roots mod π is one aspect of finite fields that is not trivial.
Corollary 10.2.5 Every extension of one finite field over another is simple.
Proof Let π : πΎ be an extension with π finite. By Proposition 10.2.1, the group
π × is generated by some element πΌ ∈ π × . Then π = πΎ (πΌ).
β‘
This is yet another pleasant aspect of finite fields.
Exercise 10.2.6 In the proof of Corollary 10.2.5, once we know that
the group π × is generated by πΌ, how does it follow that π = πΎ (πΌ)?
Digression 10.2.7 In Digression 7.2.21, I mentioned the theorem of the
primitive element: every finite separable extension π : πΎ is simple. One of
the standard proofs involves splitting into two cases, according to whether
π is finite or infinite. We’ve just done the finite case.
Corollary 10.2.8 For every prime number π and integer π ≥ 1, there exists an
irreducible polynomial over F π of degree π.
Proof The field F π π has prime subfield F π . By Corollary 10.2.5, the extension
F π π : F π is simple, say F π π = F π (πΌ). The minimal polynomial of πΌ over F π is
irreducible of degree [F π (πΌ) : F π ] = [F π π : F π ] = π.
β‘
This is not obvious. For example, can you find an irreducible polynomial of
degree 100 over F31 ?
10.3
Galois groups for finite fields
Here we work out the Galois correspondence for F π π : F π .
Warning 10.3.1 The term ‘finite field extension’ means an extension π : πΎ that’s finite in the sense defined on p. 67: π is finitedimensional as a vector space over πΎ. It doesn’t mean that π and πΎ
are finite fields. But the safest policy is to avoid this term entirely.
The three hypotheses of the fundamental theorem of Galois theory are always
satisfied when both fields in the extension are finite:
148
Lemma 10.3.2 Let π : πΎ be a field extension.
i. If πΎ is finite then π : πΎ is separable.
ii. If π is also finite then π : πΎ is finite and normal.
Proof For (i), we show that every irreducible polynomial π over πΎ is separable.
Write π = char πΎ > 0, and suppose for a contradiction that π is inseparable. By
Corollary 7.2.11,
π (π‘) = π 0 + π 1 π‘ π + · · · + ππ π‘ π π
for some π 0 , . . . , ππ ∈ πΎ. For each π, there is a (unique) πth root ππ of ππ in πΎ, by
Corollary 2.3.22(ii). Then
π
π
π
π (π‘) = π 0 + π 1 π‘ π + · · · + ππ π‘ π π .
But by Proposition 2.3.20(i), the function π β¦→ π π is a homomorphism πΎ [π‘] →
πΎ [π‘], so
π (π‘) = (π 0 + π 1 π‘ + · · · + ππ π‘ π ) π .
This contradicts π being irreducible.
For (ii), suppose that π is finite. Write π = char π > 0. By Theorem 10.1.9,
π is a splitting field over F π , so by Lemma 6.2.14(ii), it is also a splitting field
over πΎ. Hence π : πΎ is finite and normal, by Theorem 7.1.5.
β‘
Part (i) fulfils the promise made in Remark 7.2.12 and Example 7.2.14(ii), and
the lemma as a whole lets us use the fundamental theorem freely in the world
of finite fields. We now work out the Galois correspondence for the extension
F π π : F π of an arbitrary finite field over its prime subfield.
Proposition 10.3.3 Let π be a prime and π ≥ 1. Then Gal(F π π : F π ) is cyclic of
order π, generated by the Frobenius automorphism of F π π .
By an earlier workshop question, Gal(F π π : F π ) is the group of all automorphisms of F π π .
Proof Write π for the Frobenius automorphism of F π π ; then π ∈ Gal(F π π : F π ).
π
First we calculate the order of π. By Lemma 10.1.6, πΌ π = πΌ for all πΌ ∈ F π π , or
π
equivalently, π π = id. If π is a positive integer such that π π = id then πΌ π = πΌ for
π
all πΌ ∈ F π π , so the polynomial π‘ π − π‘ has π π roots in F π π , so π π ≤ π π , so π ≤ π.
Hence π has order π.
On the other hand, [F π π : F π ] = π, so by the fundamental theorem of Galois
theory, | Gal(F π π : F π )| = π. The result follows.
β‘
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Exercise 10.3.4 What is the fixed field of β¨πβ© ⊆ Gal(F π π : F π )?
In Fundamentals of Pure Mathematics or Group Theory, you presumably saw
that the cyclic group of order π has exactly one subgroup of order π for each divisor
π of π. (And by Lagrange’s theorem, there are no subgroups of other orders.)
Exercise 10.3.5 Refresh your memory by proving this fact about
subgroups of cyclic groups.
In the case at hand, Gal(F π π : F π ) = β¨πβ© πΆπ , and when π | π, the unique
subgroup of order π is β¨π π/π β©.
Proposition 10.3.6 Let π be a prime and π ≥ 1. Then F π π has exactly one subfield
of order π π for each divisor π of π, and no others. It is
π
πΌ ∈ F ππ : πΌ π = πΌ .
Proof The subfields of F π π are the intermediate fields of F π π : F π , which by the
fundamental theorem of Galois theory are precisely the fixed fields Fix(π») of
subgroups π» of Gal(F π π : F π ). Any such π» is of the form β¨π π/π β© with π | π, and
π/π
Fixβ¨π π/π β© = πΌ ∈ F π π : πΌ π = πΌ .
The tower law and the fundamental theorem give
[Fixβ¨π π/π β© : F π ] =
[F π π : F π ]
[F π π : Fixβ¨π π/π β©]
=
π
|β¨π π/π β©|
=
π
,
π
so | Fixβ¨π π/π β©| = π π/π . As π runs through the divisors of π, the quotient π/π also
runs through the divisors of π, so putting π = π/π gives the result.
β‘
Warning 10.3.7 The subfields of F π π are of the form F π π where π
divides π, not π ≤ π. For instance, F8 has no subfield isomorphic to
F4 (that is, no 4-element subfield), since 8 = 23 , 4 = 22 , and 2 β€ 3.
Let π be a divisor of π. By Proposition 10.3.6, F π π has exactly one subfield
isomorphic to F π π . We can therefore speak of the extension F π π : F π π without
ambiguity. Since F π π = Fixβ¨π π β© (by Proposition 10.3.6) and β¨π π β© πΆπ/π , it
follows from the fundamental theorem that
Gal(F π π : F π π ) πΆπ/π .
(10.1)
So in working out the Galois correspondence for F π π : F π , we have accidentally derived the Galois group of a completely arbitrary extension of finite fields. Another
way to phrase (10.1) is:
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Proposition 10.3.8 Let π : πΎ be a field extension with π finite. Then Gal(π : πΎ)
is cyclic of order [π : πΎ].
β‘
In the Galois correspondence for F π π : F π , all the extensions and subgroups
involved are normal, either by Lemma 10.3.2 or because cyclic groups are abelian.
For π | π, the isomorphism
Gal(F π π : F π )
Gal(F π π : F π )
Gal(F π π : F π π )
supplied by the fundamental theorem amounts to
πΆπ
πΆπ .
πΆπ/π
Alternatively, substituting π = π/π, this is πΆπ /πΆ π πΆπ/π .
Example 10.3.9 Consider the Galois correspondence for F π12 : F π , where π is
any prime. Writing π for the Frobenius automorphism of F π12 , the subgroups of
πΊ = Gal(F π12 : F π ) are
β¨π 12 β© πΆ1 1
order 1
β¨π 6 β© πΆ2
order 2
β¨π 4 β© πΆ3
order 3
β¨π 3 β© πΆ4
β¨π 2 β© πΆ6
order 4
order 6
πΊ = β¨πβ© πΆ12
order 12
Their fixed fields are
degree 1
F π12
degree 2
F π6
degree 3
F π4
F π3
degree 4
degree 6
F π2
degree 12
Fπ
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Here, ‘degree’ means the degree of F π12 over the subfield, and (for instance) the
subfield of F π12 called F π4 is
4
πΌ ∈ F π12 : πΌ π = πΌ .
The Galois group Gal(F π12 : F π4 ) is β¨π 4 β© πΆ3 , and similarly for the other subfields.
Exercise 10.3.10 What do the diagrams of Example 10.3.9 look like
for π 8 in place of π 12 ? What about π 432 ? (Be systematic!)
Ordered sets
In the workshop, you’ll be asked to work through the Galois correspondence
for an arbitrary extension F π π : F π π of finite fields, but there’s not much more to
do: almost all the work is contained in the case π = 1 that we have just done.
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