Lecture #1 MATH 321: Real Variables II University of British Columbia Lecture #1: Instructor: Scribe: January 7, 2008 Dr. Joel Feldman Peter Wong From Last Time: Surely we had a merry Christmas and a happy New Year. Annoucements • Office = MATH 221 (Directly above the Mathematics Department Office.) • Email = feldman@math.ubc.ca • Text = “Baby Rudin” – Principles of Mathematical Analysis 3/e by Walter Rudin • Course Website = “http://www.math.ubc.ca/∼feldman/m321/” • Topics: – Riemann-Stieltjes integral (§6) – Sequences & Series of functions (§7) – Power Series, Special Functions, Fourier Series (§8) – Another topic to be determined. • Grading: (1) A midterm on Wed. Feb 27 (25%) y = f(x) (2) Weekly problem sets due each Wednesday (25%) (t 3, f(t 3)) (3) Exam (50%) (4) Grades will probably be scaled (up, usually) Integration (Rudin §6) Recall the definition of Rb a f (x) dx from first-year calculus. a = x0 Step 1: Slice up [a, b]. x1 x 2 t3 . . . x n-1 x n= b x Definition. A partition of [a, b] is a finite set of points P = {x0 , x1 , . . . , xn } such that a = x0 < x1 < x2 < · · · < xn−1 < xn = b. Step 2: Pick a representation value of f for each subinterval. Definition. A choice T for the partition P is a finite set of points t1 , . . . , tn obeying xi−1 ≤ ti ≤ xi for each 1 ≤ i ≤ n. We shall use f (ti ) as an approximate value of f on [xi−1 , xi ]. Step 3: Compute an approximate value of Rb a f (x) dx. Definition. A Riemann partial sum is a sum of the form n X f (ti )[xi − xi−1 ] = S(P, T, f, x). i=1 Step 4: Make the partition finer. Definition. A partition P 0 is finer than the partition P if P 0 ⊃ P . 2 MATH 321: Lecture #1 Step 5: Hope the sums converge as the partition gets finer and finer. Definition. A function f : [a, b] → R is said to be Riemann-integrable on [a, b] (denoted f ∈ R on [a, b]) if there is a number I ∈ R such that ∀ε > 0, ∃Pε such that for each partition P ⊃ Pε : |S(P, T, f, x) − I| < ε for all choices T compatible with P . If so, we write lim S(P, T, f, x) = I = P Z b f (x)dx. a Generalization of this definition Let α : [a, b] → R and replace xi − xi−1 by α(xi ) − α(xi−1 ). The Riemann-Stieltjes partial sum is S(P, T, f, α) = n X f (ti )[α(xi ) − α(xi−1 )] i=1 Definition. A function f : [a, b] → R is said to be Riemann-Stieltjes integrable with respect to α on [a, b] (denoted by f ∈ R(α) on [a, b]) if there is a number I ∈ R such that ∀ε > 0, ∃Pε such that for each partition P ⊃ Pε : |S(P, T, f, α) − I| < ε for all choices T compatible with P . If so, we write lim S(P, T, f, α) = I = P Z a b f (x) dα(x) = Z b f dα. a [Examples and application shortly]. Remark. 1. The Riemann-Stieltjes integral reduces to the Riemann integral when α(x) = x. 2. We shall eventually prove that (a) α monotonic, f continuous =⇒ f ∈ R(α). (b) α continuous, f monotonic =⇒ f ∈ R(α). (From (a) and Integration by Parts) (c) α strictly monotone, f unbounded on [a, b] =⇒ f ∈ / R(α). (Use improper integrals.) Lecture #2 MATH 321: Real Variables II University of British Columbia Lecture #2: Instructor: Scribe: January 9, 2008 Dr. Joel Feldman Peter Wong From last time: We defined Z b f (x) dα(x) = lim S(P, T, f, α). P a Here, P = {x0 , x1 , · · · , xn } with a = x0 < x1 < x2 < · · · < xn = b, a = x0 x1 x2 ··· xn = b and T = {t1 , · · · , tn } with ti ∈ [xi−1 , xi ]. S(P, T, f, α) = n X f (ti )[α(xi ) − α(xi−1 )] i=1 and lim S(P, T, f, α) = I ⇐⇒ ∀ε > 0, ∃Pε such that P ⊃ Pε =⇒ |S(P, T, f, α) − I| < ε P And this time: Remark. (Connection between Rb f dα) and Riemann Integral) Observe that n X α(xi ) − α(xi−1 ) f (ti ) S(P, T, f, α) = (xi − xi−1 ) xi − xi−1 i=1 | {z } a ≈ α0 (ti ) We shall prove that if α has a continuous derivative, then Z b Z b f dα = f (x)α0 (x) dx a a Definition. A step function on [a, b] is a function α : [a, b] → R such that (i) α has finitely many points of discontinuity on [a, b]. Call si for 1 ≤ i ≤ n where a ≤ s1 < s2 < · · · < sn ≤ b. (ii) α is constant on each subinterval. [a, s1 ), a s1 s2 b = s3 (sj−1 , sj ), for 1 ≤ j ≤ n, (sn , b]. Theorem. Let a < b. Let α : [a, b] → R be a step function with discontinuities at s1 < · · · < sn . Then f ∈ R(α) on [a, b] and Z b n X − f (sj )[α(s+ f dα = j ) − α(sj )] a j=1 where α(s+ ) α(s+ j ) = lim α(t), t→sj t>sj α(s− j ) = lim α(t) t→sj t<sj α(s− ) s 2 MATH 321: Lecture #2 and by convention s1 = a =⇒ α(a− ) = α(a) sn = b =⇒ α(b+ ) = α(b) Proof. Write I = Pn j=1 − f (sj )[α(s+ j ) − α(sj )]. We prove that ∀ε > 0, ∃Pε such that P ⊃ Pε =⇒ |S(P, T, f, α) − I| < ε Let ε > 0. Choose Pε obeying (1) {s1 , . . . , sn } ⊂ Pε = {a = x̃0 < x̃1 < · · · < x̃m = b} (2) The mesh (or norm) of Pε is kPε k = max |x̃i − x̃i−1 | < δ 1≤i≤m where δ = min{s2 − s1 , s3 − s2 , . . . , sn − sn−1 , δ0 }, and δ0 is given by Insert (∗) here. Let P = {x0 , x1 , . . . , xp } ⊃ Pε and T = {t1 , . . . , tp } be a choice for P and consider each term in S(P, T, f, α) = p X f (ti )[α(xi ) − α(xi−1 )] i=1 Either (1) neither xi−1 nor xi is on sj . In this case, α(xi ) = α(xi−1 ), so α(xi ) − α(xi−1 ) = 0, or (2) xi = sj for some j. In this case, α(xi ) − α(xi−1 ) = α(sj ) − α(s− j ), or (3) xi−1 = sj for some j. In this case, α(xi ) − α(xi−1 ) = α(s+ j ) − α(sj ). 1 a 2 3 s1 1 2 3 s2 2 3 s3 1 b Lecture #3 MATH 321: Real Variables II University of British Columbia Lecture #3: Instructor: Scribe: January 11, 2008 Dr. Joel Feldman Peter Wong From last time: We were half-way through the proof of the Step Function Theorem. At the start of the class, we have a brief recap of the first half of the proof. Please refer to page 1 of step.pdf. Theorem. (The Step Function Theorem) Proof. (Continued from last time) S(P, T, f, α) = p X f (ti )[α(xi ) − α(xi−1 )] i=1 − + f (tij )[α(sj ) − α(sj )] + f (tij )[α(sj ) − α(sj )] = {z } | {z } j=1 | n X tij sj ti0j case 2 terms case 3 terms Each of tij and ti0j lie in an interval of P with one endpoint: sj Since ( |sj − tij | < δ kP k < δ =⇒ |sj − ti0j | < δ. We are aiming for the integral to be n X − f (sj )[α(s+ j ) − α(sj )] = n X j=1 j=1 + f (sj )[α(sj ) − α(s− j )] + f (sj )[α(sj ) − α(sj )] But n X + − S(P, T, f, α) − f (sj )[α(sj ) − α(sj )] j=1 ≤ n n o X + |f (tij ) − f (sj )||α(sj ) − α(s− j )| + |f (ti0j ) − f (sj )||α(sj ) − α(sj )| j=1 (*) for each 1 <≤ j ≤ n, f is continuous at sj implies ∃δj > 0 such that |f (sj ) − f (t)| < Pn k=1 ε |α(sk ) − α(s− k )| + |α(s+ j ) − α(sk )| for all |t − sj | < δj . Choose δ0 = min{δ1 , . . . , δn }. Since kP k ≤ kPε k < δ0 , we have n X + − S(P, T, f, α) − f (s )[α(s ) − α(s )] j j j < ε. j=1 Remarks. (Applications of the Riemann-Stieltjes integral) 1. We now have a Dirac δ-function on a hand-waving level, δ(x) is defined by (a) δ(x) < 0 for all x 6= 0 (b) δ(0) = +∞ δ(x) 2 (c) Rb a MATH 321: Lecture #3 δ(x)dx = 1 for all a < 0, b > 0. such that Z b f (x)δ(x) dx = a Z 0 b f (0)δ(x) dx, ∀a < 0, b > 0 (Not rigorous) a Notice that for x 6= 0, both integrals equal 0. We can also define the Heaviside function H(x) = such that δ(x) = H 0 (x). ( 0, x < 0 1, x ≥ 0 (Not rigorous) A more rigorous definition follows from the concept of Riemann-Stieltjes Integral: Z Z a b f (x)δ(x) dx = f (0) a b f (x)H 0 (x) dx = f (0) Z a 2. Application to Probability. (Next Lecture) b f dH = f (0)