Hindawi Publishing Corporation International Journal of Mathematics and Mathematical Sciences Volume 2013, Article ID 983607, 8 pages http://dx.doi.org/10.1155/2013/983607 Research Article Perpendicularity in an Abelian Group Pentti Haukkanen,1 Mika Mattila,1 Jorma K. Merikoski,1 and Timo Tossavainen2 1 2 School of Information Sciences, University of Tampere, 33014, Finland School of Applied Educational Science and Teacher Education, University of Eastern Finland, P.O. Box 86, 57101 Savonlinna, Finland Correspondence should be addressed to Pentti Haukkanen; pentti.haukkanen@uta.fi Received 12 January 2013; Accepted 19 March 2013 Academic Editor: Petru Jebelean Copyright © 2013 Pentti Haukkanen et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We give a set of axioms to establish a perpendicularity relation in an Abelian group and then study the existence of perpendicularities in (Zπ , +) and (Q+ , ⋅) and in certain other groups. Our approach provides a justification for the use of the symbol ⊥ denoting relative primeness in number theory and extends the domain of this convention to some degree. Related to that, we also consider parallelism from an axiomatic perspective. 1. Introduction In [1, page 115], Graham et al. made the following suggestion: When gcd(π, π) = 1, the integers π and π have no prime factors in common and we say that they are relatively prime. This concept is so important in practice, we ought to have a special notation for it; but alas, number theorists have not agreed on a very good one yet. Therefore we cry: hear us, o mathematicians of the world! let us not wait any longer! we can make many formulas clearer by adopting a new notation now! let us agree to write “π ⊥ π”, and to say “π is prime to π,” if π and π are relatively prime. Like perpendicular lines do not have a common direction, perpendicular numbers do not have common factors. In fact, this cry had been answered even before it was made. Namely, in studying π-groups (i.e., groups with a lattice structure), Birkhoff [2, page 295] defines that two positive elements π and π of an π-group are disjoint if π ∧ π = 0 and uses the notation π ⊥ π for disjoint elements. He also remarks that disjointness specializes to relative primeness in the π-group of positive integers. A motivation for the present paper is to study how justified ultimately it is to use the symbol of perpendicularity to denote relative primeness. Does this practice rely only on the analogy between having no common direction and having no common factor or is there a deeper linkage to entitle this convention? This question leads us to ask which properties essentially establish the notion of perpendicularity in the algebraic context and what the most suitable algebraic context for the axiomatization of perpendicularity actually is; we have recently studied the axioms of perpendicularity from an elementary geometric point of view [3]. In an inner product space, perpendicularity obviously traces back to the inner product being zero. However, certain features of this perpendicularity can be shifted down to simpler algebraic structures. We will define perpendicularity in an Abelian group and examine it in Section 2. In Section 3, we will focus on perpendicularity in (Zπ , +). Davis [4] defined perpendicularity in an Abelian group differently. In Section 4, we will introduce his approach and compare it with ours. Thereafter, we will consider divisibility in (Q+ , ⋅) in Section 5 and parallelism in an Abelian group in Section 6. We will conclude our paper with a brief discussion and a supplement to the suggestion cited previously. 2. Axioms and Properties of Perpendicularity Throughout this paper, πΊ = (πΊ, +) is an Abelian group so that πΊ =ΜΈ {0}. Unless otherwise stated, ⊥ is a binary relation in πΊ satisfying (A1) ∀π ∈ πΊ : ∃π ∈ πΊ : π ⊥ π, (A2) ∀π ∈ πΊ \ {0} : π ⊥ π, (A3) ∀π, π ∈ πΊ : π ⊥ π ⇒ π ⊥ π, 2 International Journal of Mathematics and Mathematical Sciences (A4) ∀π, π, π ∈ πΊ : π ⊥ π ∧ π ⊥ π ⇒ π ⊥ (π + π), (A5) ∀π, π ∈ πΊ : π ⊥ π ⇒ π ⊥ −π. We call ⊥ a perpendicularity in πΊ. This concept can be defined also in weaker structures by changing these axioms appropriately. For example, if πΊ is an Abelian monoid, then we simply omit (A5). Since the trivial perpendicularity π₯ ⊥ π¦ ⇐⇒ π₯ = 0 ∨ π¦ = 0 (1) Proof. For the first part, assume that π, π ∈ πΊ satisfy π ⊥ π, and let the order of π be π. Then π ⊥ (π − 1)π by (A4). But (π − 1)π = −π and (A5) follows. For the second part, let π ∈ πΊ have infinite order. Then the subgroup {0, ±π, ±2π, . . .} is isomorphic to Z. The relation ⊥ defined by π₯ ⊥ π¦ ⇐⇒ (∃π, ] ∈ Z : π₯ = ππ ∧ π¦ = ]π ∧ π] < 0) ∨π₯=0∨π¦=0 (2) satisfies (A1)–(A4) but not (A5). always exists, we are mainly interested in nontrivial perpendicularities. We call ⊥ maximal if it is not a subrelation of any other perpendicularity in πΊ. There always exists a maximal perpendicularity. This is obvious if πΊ is finite and, otherwise, it follows from Zorn’s lemma. Proposition 1 records some elementary properties of perpendicularity; we leave the proof for the reader. Proposition 1. Perpendicularity ⊥ has the following properties: (a) ∀π ∈ πΊ : π ⊥ 0, (b) ∀π ∈ πΊ \ {0} : π ⊥ − π, (c) ∀π, π1 , . . . , ππ ∈ πΊ, πΎ1 , . . . , πΎπ ∈ Z : π ⊥ π1 , . . . , ππ ⇒ π ⊥ (πΎ1 π1 + ⋅ ⋅ ⋅ + πΎπ ππ ), (d) ∀π, π ∈ πΊ, π, ] ∈ Z : π ⊥ π ⇒ ππ ⊥ ]π. The following characterization is useful in proving that a given relation is perpendicularity. Proposition 2. A binary relation ⊥ in πΊ is perpendicularity if and only if it satisfies (A1) and (A2) and (A6) ∀π, π, π ∈ πΊ : π ⊥ π ∧ π ⊥ π ⇒ (π − π) ⊥ π. Proof. The “only if ”-part is trivial. To prove the “if ”-part, we first show that our assumptions imply Proposition 1(a). Let π ∈ πΊ. By (A1), there is π ∈ πΊ such that π ⊥ π. Putting π := π in (A6) implies 0 ⊥ π; in particular 0 ⊥ 0. Further, (A6) with π := 0, π := π and π := 0 gives (π − 0) ⊥ 0, that is, π ⊥ 0. Now we can verify the remaining axioms. (A3) Assume π ⊥ π. Apply (A6) with π := 0; then π ⊥ π. (A5) Assume π ⊥ π. Apply (A6) with π := 0 and π := π. Then (−π) ⊥ π, and so, by (A3), π ⊥ −π. (A4) Assume π ⊥ π and π ⊥ π; then π ⊥ −π by (A5). Now (A6) with π := −π implies (π − (−π)) ⊥ π, that is, (π + π) ⊥ π. Hence, by (A3), π ⊥ (π + π). Is there a simple condition under which (A5) follows from (A1)–(A4)? The answer is positive. Proposition 3. If all elements of πΊ have finite order and if ⊥ satisfies (A1)–(A4), then it satisfies (A5). If πΊ has at least one element of infinite order, then there exists a relation ⊥ which satisfies (A1)–(A4) but not (A5). If 0 =ΜΈ π΄ ⊆ πΊ, we define the perpendicular complement or ⊥-complement of π΄ as follows: π΄⊥ = {π¦ ∈ πΊ | π¦ ⊥ π΄} = β π΅. πΊ⊇π΅⊥π΄ (3) Here π¦ ⊥ π΄ means that π¦ ⊥ π₯ for all π₯ ∈ π΄, and π΅ ⊥ π΄ means that π¦ ⊥ π΄ for all π¦ ∈ π΅. Thus π΄⊥ is the maximal set perpendicular to π΄. In particular, πΊ⊥ = {0} and {0}⊥ = πΊ. We also define 0⊥ = πΊ. Proposition 4. If π΄ ⊆ πΊ, then π΄⊥ is a subgroup of πΊ. If πΊ is cyclic, then π΄⊥ is cyclic. Proof. The first part follows by applying the subgroup test and Proposition 2. The second part follows from the fact that any subgroup of a cyclic group is cyclic. The next theorem tells when πΊ has a nontrivial perpendicularity. Theorem 5. The following conditions are equivalent: (a) πΊ has a nontrivial perpendicularity ⊥, (b) πΊ has nontrivial cyclic subgroups π» and πΎ satisfying π» ∩ πΎ = {0}, (c) πΊ has nontrivial subgroups π» and πΎ satisfying π» ∩ πΎ = {0}. Proof. (a)⇒(b). Since ⊥ is nontrivial, there exist π₯, π¦ ∈ πΊ\{0} such that π₯ ⊥ π¦. Then π» = β¨π₯β© and πΎ = β¨π¦β© apply. Here β¨πβ© stands for the cyclic group generated by π. (b)⇒(c). Trivial. (c)⇒(a). Define ⊥ by π₯ ⊥ π¦ ⇐⇒ (π₯ ∈ π» ∧ π¦ ∈ πΎ) ∨ (π₯ ∈ πΎ ∧ π¦ ∈ π») ∨ π₯ = 0 ∨ π¦ = 0. (4) Next we consider the maximal perpendicularity in some examples of groups. In Examples 6–9, the group operation is addition. Example 6. Let πΊ = Z6 . By Lagrange’s theorem [5, page 130, Theorem 2], the smallest π such that Zπ has a nontrivial perpendicularity is 6 = 2 ⋅ 3 because π must have at least two different prime factors. The nontrivial subgroups of Z6 are π» = β¨3β© = {0, 3} and πΎ = β¨2β© = {0, 2, 4}. Since πΊ = π» ⊕ πΎ, International Journal of Mathematics and Mathematical Sciences it has exactly one nontrivial perpendicularity, defined by 0 ⊥ 0, 1, 2, 3, 4, 5 and 3 ⊥ 2, 4 and vice versa. Consequently, this perpendicularity is maximal. Example 7. Let πΊ = Z2 × Z2 , the Klein four group. Denote 0 = (0, 0), π = (0, 1), π = (1, 0), π = (1, 1). The nontrivial subgroups are π΄ = {0, π}, π΅ = {0, π}, πΆ = {0, π}. So, there are three nontrivial perpendicularities obtained as follows: Choose two elements of π, π, and π. Define that they are perpendicular to each other and to 0. Define that the remaining element is perpendicular to 0 only. All perpendicularities arising in this way are clearly maximal. We also note that πΊ = π΄ ⊕ π΅ = π΅ ⊕ πΆ = πΆ ⊕ π΄. Example 8. Let πΊ = Z. For each π ≥ 2, the subgroup β¨πβ© = πZ is nontrivial and there are no other nontrivial subgroups than those found in this way. Because ππ ∈ β¨πβ©∩β¨πβ©, there is no pair of nontrivial subgroups with intersection {0}. Hence πΊ has only the trivial perpendicularity. Example 9. Let πΊ = R. Since R has infinitely many pairs of nontrivial subgroups with intersection {0}, it has infinitely many nontrivial perpendicularities. For example, let π» = Q and πΎ = {π₯√2 | π₯ ∈ Q} and define ⊥ by (4). To see that this perpendicularity is not maximal, let π»1 = {π₯√3 | π₯ ∈ Q} and πΎ1 = {π₯√5 | π₯ ∈ Q} and define ⊥σΈ by π₯⊥σΈ π¦ ⇐⇒ (π₯ ∈ π» ∧ π¦ ∈ πΎ) ∨ (π₯ ∈ πΎ ∧ π¦ ∈ π») ∨ (π₯ ∈ π»1 ∧ π¦ ∈ πΎ1 ) ∨ (π₯ ∈ πΎ1 ∧ π¦ ∈ π»1 ) (5) ∨ π₯ = 0 ∨ π¦ = 0. 3 Hence, for example, 8/9 ⊥ 7/5. In particular, for π, π ∈ Z+ , applying (9) to π/1 and π/1 yields that π ⊥ π ⇐⇒ gcd (π, π) = 1. (10) So, it seems that Graham et al. were prophetically quite right with their suggestion—and not forgetting Birkhoff either! We will discuss the perpendicularity of positive rational numbers in more detail in Section 5. 3. Perpendicularity in Zπ Studying perpendicularities requires that we know the structure of πΊ. Next we take a more thorough look at perpendicularity in Zπ . To that end, we begin by introducing a suitable notation to discuss the structure of Zπ and record two lemmas which are useful in the search for the maximal perpendicularity. We will also use the notations introduced in Theorem 11 and the following lemmas throughout the next sections. Theorem 11. If πΌ π = π1 1 ⋅ ⋅ ⋅ πππΌπ , (11) where π1 , . . . , ππ ∈ P are distinct and πΌ1 , . . . , πΌπ > 0, then Zπ = π»1 ⊕ ⋅ ⋅ ⋅ ⊕ π»π , (12) where π»π = β¨ππ β©, ππ = π πΌ , ππ π π = 1, . . . , π. (13) Then π₯ ⊥ π¦ ⇒ π₯ ⊥σΈ π¦. The decomposition (12) is unique (up to the order of subgroups). Example 10. Let πΊ = (Q+ , ⋅), where Q+ denotes the set of positive rational numbers. Every π ∈ Q+ can be uniquely expressed as Proof. The claim (12) follows from [5, page 399, Corollary 1] and from the facts that ZππΌπ ≅ π»π and π»π ∩ π»π = {0} for π all π, π = 1, . . . , π, π =ΜΈ π. Uniqueness follows from [5, page 399, Corollary 2]. π = ∏ π]π (π) , π∈P (6) where ]π (π) ∈ Z for each π ∈ P and only a finite number of them are nonzero. The symbol P stands for the set of primes. For example, if π = 8/25, then ]2 (π) = 3, ]3 (π) = 0, ]5 (π) = −2, ]7 (π) = ]11 (π) = ⋅ ⋅ ⋅ = 0. Assign now π ⊥ π ⇐⇒ ∀π ∈ P : ]π (π) = 0 ∨ ]π (π) = 0. (7) π , π’ Lemma 12. For all π, π = 1, . . . , π, π =ΜΈ π, ππ2 =ΜΈ 0, π= π , V π, π’, π, V ∈ Z+ , (8) ππ ππ = 0. π2 2πΌ1 π1 π1 π2 = gcd (π, π’) = gcd (π, V) = 1, 2πΌ = π2 2 ⋅ ⋅ ⋅ ππ2πΌπ ≡ΜΈ 0 (mod π) , π π πΌ πΌ π1 1 π2 2 πΌ (15) πΌ πΌ = π2 2 ⋅ ⋅ ⋅ πππΌπ π1 1 π3 3 ⋅ ⋅ ⋅ πππΌπ πΌ = π3 3 ⋅ ⋅ ⋅ πππΌπ π ≡ 0 then π ⊥ π ⇐⇒ gcd (ππ’, πV) = 1. (14) Proof. It is enough to consider π = 1, π = 2. Regarding π1 and π2 as integers, we have π12 = In other words, if π= Although we consider Zπ mainly as an Abelian group, it is now useful to work with Zπ as a ring. (9) and (14) follows. (mod π) , 4 International Journal of Mathematics and Mathematical Sciences Lemma 13. Let ⊥ be a perpendicularity in Zπ . Then ∀π, π, π, π ∈ Zπ : π ⊥ π σ³¨⇒ ππ ⊥ ππ. respectively. So, it is natural to define their “inner product” by (16) Proof. Let π = πΎ1, π = πΏ1, where πΎ and πΏ are integers with 0 ≤ πΎ, πΏ < π. Since ππ = (πΎ1)π = πΎ(1π) = πΎπ and, similarly, ππ = πΏπ, Proposition 1(d) implies (16). Now we are ready to introduce a perpendicularity which turns out to be maximal in Zπ . Let π₯ = π₯1 + ⋅ ⋅ ⋅ + π₯π , π¦ = π¦1 + ⋅ ⋅ ⋅ + π¦π ∈ Zπ , (17) β¨π₯, π¦β© = π₯1 π¦1 + ⋅ ⋅ ⋅ + π₯π π¦π . Proposition 15 shows that this operation coincides with the ordinary multiplication in Zπ . Proposition 15. Given π₯, π¦ ∈ Zπ , β¨π₯, π¦β© = π₯π¦. π π π π π=1 π=1 π=1 π,π=1 π =ΜΈ π π₯π¦ = (∑π₯π ) (∑π¦π ) = ∑π₯π π¦π + ∑ π₯π π¦π . (18) Proof. Let ⊥ be another perpendicularity in Zπ . Our claim is that π₯ ⊥ π¦ ⇒ π₯ ⊥0 π¦. By (12), we can express where the integers ππ , ππ ∈ πΌ ππ = π/ππ π , π = 1, . . . , π. Suppose against the claim of theorem that there exist ⊥0 π¦. Then ππ , ππ =ΜΈ 0 for some π₯, π¦ ∈ Zπ such that π₯ ⊥ π¦ but π₯ π. Reordering the indices so that π = 1 and applying (16), we have π₯π1 ⊥ π¦π1 which implies that π1 π12 ⊥ π1 π12 (20) by (14). Hence, by Proposition 1(d), π1 π1 π1 π12 ⊥ π π2 , gcd (π1 , π1 ) gcd (π1 , π1 ) 1 1 (21) lcm (π1 , π1 ) π12 ⊥ lcm (π1 , π1 ) π12 . (22) that is, Consequently, lcm (π1 , π1 ) π12 = 0 by (A2). In other words, regarding also π1 as an integer, lcm (π1 , π1 ) π12 = lcm (π1 , π1 ) ≡0 π,π=1 π =ΜΈ π ∀π₯, π¦ ∈ Zπ : π₯ ⊥ π¦ σ³¨⇒ π₯π¦ = 0. Theorem 17. The following conditions are equivalent: (a) πΌ1 = ⋅ ⋅ ⋅ = πΌπ = 1, (b) ∀π₯, π¦ ∈ Zπ : π₯π¦ = 0 ⇒ π₯ ⊥0 π¦, (c) ∀π₯ ∈ Zπ : π₯2 = 0 ⇒ π₯ = 0. Proof. (a)⇒(b). Assume that π₯ ⊥0 π¦. Express π₯ and π¦ as in (19). We can rearrange the indices so that, for some π ∈ {1, . . . , π}, 2πΌ1 ππ = 0 ∨ ππ = 0, πΌ Considering the direct sum (12) external, we can identify π₯ and π¦ in (17) with vectors (π₯1 , . . . , π₯π ) and (π¦1 , . . . , π¦π ), π = 1, . . . , π , π = π + 1, . . . , π. (29) By (25), π₯π¦ = π1 π1 π12 + ⋅ ⋅ ⋅ + ππ ππ ππ 2 . (mod π) , and π1 1 divides lcm(π1 , π1 ). However, since it divides neither π1 nor π1 , this is a contradiction. Hence, π₯ ⊥0 π¦. (28) Does the converse of Theorem 16 hold if ⊥ = ⊥0 ? And, related to Proposition 15, is β¨π₯, π¦β© = π₯π¦ a proper inner product? Namely, an inner product in a real vector space is symmetric and bilinear and it satisfies β¨π₯, π₯β© = 0 ⇒ π₯ = 0. The operation β¨π₯, π¦β© = π₯π¦ in Zπ has clearly the first and second properties but what about the third one? The answers to both questions are contained in Theorem 17. ππ , ππ =ΜΈ 0, (23) (27) Proof. If π₯ ⊥ π¦, then π₯ ⊥0 π¦ by Theorem 14. So, π₯π¦ = 0 by (18) and (25). π1 2πΌ π,π=1 π =ΜΈ π Theorem 16. Let ⊥ be a perpendicularity in Zπ . Then π2 = lcm (π1 , π1 ) π2 2 ⋅ ⋅ ⋅ ππ2πΌπ π The claim follows. (19) πΌ {0, . . . , ππ π −1} and the residue class π ∑ π₯π π¦π = ∑ ππ ππ ππ ππ = 0. Theorem 14. The perpendicularity ⊥0 is maximal and every other perpendicularity in Zπ is contained in it. π¦ = π1 π1 + ⋅ ⋅ ⋅ + ππ ππ , (26) But, recalling (19) and (14), is clearly a perpendicularity. π₯ = π1 π1 + ⋅ ⋅ ⋅ + ππ ππ , (25) Proof. We have where π₯π , π¦π ∈ π»π , π = 1, . . . , π. The relation ⊥0 , defined in Zπ by π₯ ⊥0 π¦ ⇐⇒ ∀π ∈ {1, . . . , π} : π₯π = 0 ∨ π¦π = 0, (24) (30) If π1 π1 π12 +⋅ ⋅ ⋅+ππ ππ ππ 2 = 0, then the integer π1 π1 π12 +⋅ ⋅ ⋅+ππ ππ ππ 2 ≡ 0 (mod π), that is, π1 π1 π2 π2 + ⋅ ⋅ ⋅ + π π π π 2 ≡0 ππ π12 (mod π = π1 ⋅ ⋅ ⋅ ππ ) . (31) International Journal of Mathematics and Mathematical Sciences However, this is impossible because none of π1 , . . . , ππ divides the left-hand side. (Namely, ππ divides every other summand except the πth one.) Therefore, π₯π¦ =ΜΈ 0 and our claim follows by contradiction. (b)⇒(c). If π₯2 = 0, then π₯ ⊥0 π₯ by (b) and π₯ = 0 by (A2). (c)⇒(a). Suppose that (a) does not hold. Then, say, πΌ1 > 1. Let π₯ = π/π1 . Since the integer π₯2 = = 2 π = π12 2πΌ π1 1 2πΌ −2 2πΌ π1 1 π2 2 ⋅ ⋅ ⋅ ππ2πΌπ π12 ⋅ ⋅ ⋅ ππ2πΌπ (32) ≡0 (mod π) , 5 He assumes that πΊ is an Abelian group, but the definition applies more generally to an Abelian monoid, too. It is easy to see that (D1)–(D4) are equivalent to (A1)–(A4). Axiom (D5) arises from introducing the concept of “disjointness” on a vector lattice; see [2, page 295], [6]. In fact, ⇔ can be replaced with ⇐ in (D5) due to the following observation. Proposition 21. Assume that ⊥ satisfies (D1)–(D3) (or, equivalently, (A1)–(A3)). Then ∀π, π ∈ πΊ : π ⊥ π ⇒ {π}⊥⊥ ∩ {π}⊥⊥ = {0} . Proof. We show first that if 0 =ΜΈ π΄ ⊆ πΊ, then 2 the residue class π₯ = 0. But π₯ =ΜΈ 0 and hence (c) does not hold. Again, our claim follows now by contradiction. Corollary 18. If and only if the conditions of Theorem 17 are satisfied, then ∀π₯, π¦ ∈ Zπ : π₯ ⊥0 π¦ ⇐⇒ π | (π₯π¦) , (33) where π₯π¦ is the product of integers π₯ and π¦. Example 19. Let πΊ = Z30 . Since 30 = 2 ⋅ 3 ⋅ 5, the decomposition (12) is Z30 = β¨ 30 30 30 β©⊕β¨ β©⊕β¨ β© 2 3 5 (36) π΄ ∩ π΄⊥ = {0} . (37) If π₯ ∈ π΄ ∩ π΄⊥ , then π₯ ⊥ π¦ for all π¦ ∈ π΄. In particular, π₯ ⊥ π₯, and hence π₯ = 0 by (D3) and (37) follows. Assume next that π ⊥ π and let π₯ ∈ {π}⊥⊥ ∩ {π}⊥⊥ . Since π₯ ⊥ {π}⊥ and π ∈ {π}⊥ , we have π₯ ⊥ π implying that π₯ ∈ {π}⊥ . Thus π₯ ∈ {π}⊥ ∩ {π}⊥⊥ . But (37) applied to π΄ = {π}⊥ implies that {π}⊥ ∩ {π}⊥⊥ = {0} and π₯ = 0 follows. How are these two perpendicularities related? We give a partial answer. Let us denote by π΄ and π· the axioms (A1)– (A5) and (D1)–(D5), respectively. (34) = {0, 15} ⊕ {0, 10, 20} ⊕ {0, 6, 12, 18, 24} . Proposition 22. If all elements of πΊ have finite order, then π· ⇒ π΄. If πΊ has at least one element of infinite order, then there exists a relation ⊥ satisfying π· but not π΄. For example, since 2 = 0 ⋅ 15 + 2 ⋅ 10 + 2 ⋅ 6 and 15 = 1 ⋅ 15 + 0 ⋅ 10 + 0 ⋅ 6, we have 2 ⊥0 15. Generally, (33) implies that π₯ ⊥0 π¦ if and only if the corresponding integers satisfy 30 | (π₯π¦). Proof. The first claim follows from Proposition 3. Concerning the second one, ⊥ defined by (2) establishes a relation satisfying π· but not (A5). Example 20. Let πΊ = Z360 . Since 360 = 23 ⋅ 32 ⋅ 5, we have Proposition 23. Assume that πΊ has elements π1 , π2 , π3 , π4 =ΜΈ 0 such that β¨ππ β© ∩ β¨ππ β© = {0} whenever π =ΜΈ π. Then there exists a relation ⊥ satisfying π΄ but not π·. Z360 = β¨ 360 360 360 β©⊕β¨ 2 β©⊕β¨ β© 23 3 5 = {45, 90, . . . , 315} ⊕ {40, 80, . . . , 320} (35) ⊕ {72, 144, . . . , 288} . For example, 5 ⊥0 72 because 5 = 1 ⋅ 45 + 8 ⋅ 40 + 0 ⋅ 72 and 72 = 0 ⋅ 45 + 0 ⋅ 40 + 1 ⋅ 72. Now (33) is only necessary for ⊥0 but not sufficient. For example, 10 ⊥0 36 due to the fact that 10 = 2 ⋅ 45 + 7 ⋅ 40 + 0 ⋅ 72 and 36 = 4 ⋅ 45 + 0 ⋅ 40 + 3 ⋅ 72. However, 360 | (10 ⋅ 36). 4. Another Definition of Perpendicularity Davis [4] defined perpendicularity as a binary relation ⊥ in πΊ satisfying Proof. The relation ⊥ defined by (5) with π» = β¨π1 β©, πΎ = β¨π2 β©, π»1 = β¨π3 β©, and πΎ1 = β¨π4 β© satisfies π΄. Since {π1 }⊥⊥ ∩ {π3 }⊥⊥ = ⊥ π3 , it does not satisfy (D5). β¨π1 β© ∩ β¨π3 β© = {0} and π1 5. Divisibility in Q+ It will turn out that perpendicularity has got something to do also with divisibility in Q+ . To that end, we begin by noticing that every π ∈ Q+ can be said to be a rational divisor of every π ∈ Q+ because π = ππ for some π ∈ Q+ . So, this divisibility is trivial. In order to be able to discuss nontrivial divisibilities in Q+ , we have to consider which properties essentially establish this relation. The following three ones seem quite obvious. Let | be a relation in Q+ satisfying (D1) ∀π, π ∈ πΊ : π ⊥ π ⇒ π ⊥ π, (i) ∀π ∈ Q+ : π | π, (D2) ∀π ∈ πΊ : 0 ⊥ π, (ii) ∀π, π, π ∈ Q+ : π | π ∧ π | π ⇒ π | (ππ), (D3) ∀π ∈ πΊ : π ⊥ π ⇒ π = 0, (iii) ∀π, π, π ∈ Q+ : π | π ∧ π | π ⇒ π | π. (D4) ∀π, π, π ∈ πΊ : π ⊥ π ∧ π ⊥ π ⇒ (π + π) ⊥ π, (D5) ∀π, π ∈ πΊ : π ⊥ π ⇔ {π}⊥⊥ ∩ {π}⊥⊥ = {0}. We call | a divisibility in Q+ . In other words, divisibility is a reflexive and transitive relation (i.e., a preorder) satisfying (ii). 6 International Journal of Mathematics and Mathematical Sciences If π | π, then we say that π is a divisor of π and that π is divisible by π. If π | π, π | π and π | π ∧ π | π ⇒ π | π, then π is a greatest common divisor of π and π, denoted by gcd| (π, π). All these notions are meaningful also in any Abelian monoid. Let us recall that every π ∈ Q+ can be expressed as π = ∏ π]π (π) , π∈P (38) where ]π (π) ∈ Z for each π ∈ P, and only a finite number of them are nonzero. If ]π (π) =ΜΈ 0, then π is a prime factor of π. Consider the set π of all sequences (π2 , π3 , . . . , ππ , . . .), where the index runs through P, each ππ ∈ Z, and only a finite number of them are nonzero. The mapping π(π) = (]2 (π) , ]3 (π) , . . . , ]π (π) , . . .) (39) is an isomorphism from (Q+ , ⋅) onto (π, +) where addition is defined termwise. For example, 8 π(45) + π ( ) = (0, 2, 1, 0, 0, . . .) + (3, 0, −2, 0, 0, . . .) 25 is a divisibility, gcdπΏ (π, π) exists and is unique for all π, π ∈ Q+ , and gcdπΏ (π, π) = ∏ πmin(]π (π),]π (π)) . π∈P Assume now that π, π, π’, V ∈ Z+ so that gcd(π, π’) = gcd(π, V) = 1. An alternative expression for (45) is π π πΏ ⇐⇒ π | π ∧ π’ | V, V π’ gcdπΏ ( = (3, 2, −1, 0, 0, . . .) . (40) π∈P gcdπΏ (π, π) = gcd (45, 33) 3 = . lcm (14, 100) 700 (49) Since gcdπΏ (|π/π’|, |π/V|) = gcd(ππ’, πV), we have by (9) (50) This relation generalizes (10) and answers the cry of Graham et al. in a slightly wider context than what they, perhaps, had thought. Eugeni and Rizzi [7, Section 2] defined divisibility in Q+ by setting the relation πΎ so that π π πΎ ⇐⇒ π | π ∧ V | π’. V π’ (51) Then gcdπΎ (π, π) always exists and is unique, and (41) gcd (π, π) π π , )= . π’ V gcd (π’, V) (52) gcd (45, 33) 45 33 3 , )= = . 14 100 gcd (14, 100) 2 (53) gcdπΎ ( Since only a finite number of summands are nonzero, this sum is finite. For example, β¨45, (48) For example, if π = 45/14 = 2−1 ⋅ 32 ⋅ 51 ⋅ 7−1 and π = 33/100 = 2−2 ⋅ 31 ⋅ 5−2 ⋅ 111 , then gcdπΏ (π, π) = 2−2 ⋅ 31 ⋅ 5−2 ⋅ 7−1 = 3/700. Alternatively, Given π, π ∈ Q+ , we define their “inner product” being the Euclidean inner product of the vectors π(π) and π(π): β¨π, πβ© = β¨π(π) , π(π)β© = ∑ ]π (π) ]π (π) . gcd (π, π) π π . , )= π’ V lcm (π’, V) π ⊥1 π ⇐⇒ gcdπΏ (|π| , |π|) = 1. 8 72 ) = π ( ) = π (23 ⋅ 32 ⋅ 5−1 ) 25 5 (47) and that for (46) is = (3, 2, −1, 0, 0, . . .) , π (45 ⋅ (46) 8 β© = 0 ⋅ 3 + 2 ⋅ 0 + 1 ⋅ (−2) + 0 + 0 + ⋅ ⋅ ⋅ = −2. (42) 25 For example, gcdπΎ ( Next we define |π| by setting ]π (|π|) = |]π (π)| for all π ∈ P or, equivalently, |π| = π−1 ((]2 (|π|), ]3 (|π|), ]5 (|π|), . . .)). For example, if π = 40/63 = 23 ⋅ 3−2 ⋅ 51 ⋅ 7−1 , then |π| = 23 ⋅ 32 ⋅ 51 ⋅ 71 = 2520. Letting ⊥1 be the same relation as the one defined by (7), it can be characterized now by We define now the corresponding perpendicularity by writing π ⊥1 π ⇐⇒ β¨|π| , |π|β© = 0. Summing up, we have at least three nontrivial perpendicularities in Q+ . Let us see how they relate to one another. ⊥1 versus ⊥2 . Clearly ⊥1 ⇒ ⊥2 (i.e., π₯⊥1 π¦ ⇒ π₯⊥2 π¦). The ⊥1 2/3. converse does not hold. For example, 6⊥2 2/3 but 6 ⊥1 versus ⊥ER . Clearly ⊥1 ⇒ ⊥ER . The converse does not ⊥1 3/2. hold. For example, 2/3⊥ER 3/2 but 2/3 ⊥2 versus ⊥ER . These perpendicularities are independent. ⊥ER 2/3. On the other hand, For example, 6⊥2 2/3 but 6 ⊥2 3/2. 2/3⊥ER 3/2 but 2/3 However, regarding (Z+ , ⋅) as a submonoid of (Q+ , ⋅), it is obvious that ⊥1 = ⊥2 = ⊥ER in Z+ . Moreover, in Z+ , they yield the very perpendicularity proposed by Graham et al. (43) Also the relation ⊥2 in Q+ , defined by π ⊥2 π ⇐⇒ β¨π, πβ© = 0, (44) is a perpendicularity. We will introduce one more nontrivial perpendicularity using divisibility. For that purpose, we first notice that the relation πΏ defined by ππΏπ ⇐⇒ ∀π ∈ P : ]π (π) ≤ ]π (π) (45) π ⊥ER π ⇐⇒ gcdπΎ (π, π) = 1 ⇐⇒ gcd (π, π) = gcd (π’, V) = 1. (54) International Journal of Mathematics and Mathematical Sciences 6. Parallelism Parallelism is closely related to perpendicularity. Considering different geometric contexts we notice soon that, in general, parallelism does not have any other properties except those of equivalence. However, any equivalence relation cannot be said to stand for parallelism in any reasonable way. This leads us to ask whether it is possible or not to define parallelism in Abelian groups having a perpendicularity so that it makes sense. Let πΊ have a perpendicularity ⊥ and let π, π ∈ πΊ. We say that π and π are parallel and write π β π if {π}⊥ = {π}⊥ . The relation β is clearly an equivalence. If π =ΜΈ 0, then π β¦ 0, since {0}⊥ = πΊ by Proposition 1(a) but {π}⊥ =ΜΈ πΊ by (A2). All nonzero elements are parallel if and only if ⊥ is trivial. If πΊ = Zπ and ⊥ = ⊥0 , then, recalling (19), π₯β π¦ ⇐⇒ (∀π ∈ {1, . . . , π} : ππ = 0 ⇐⇒ ππ = 0) ⊥ ⇐⇒ {π₯}⊥ = {π¦} = π»ππ ⊕ ⋅ ⋅ ⋅ ⊕ π»ππ‘ , (55) where ππ = ππ = 0 ⇔ π ∈ {π1 , . . . , ππ‘ }. For example, consider Z30 (see Example 19). Since 2 = 0 ⋅ 15 + 2 ⋅ 10 + 2 ⋅ 6 and 16 = 0 ⋅ 15 + 1 ⋅ 10 + 1 ⋅ 6, we have {2}⊥ = {16}⊥ = {0, 15}, and so 2 β 16. Now, let πΊ = Q+ and let ⊥1 , ⊥2 , and ⊥ER be as before. Denote the corresponding parallelisms by β1 , β2 , and βER , respectively. Then πβ1 π if and only if π and π have the same prime factors. Further, π/π’βER π/V if and only if π and π have the same prime factors and π’ and V have the same prime factors. Let us study how these parallelisms relate to one another. β1 versus β2 . We show that β2 ⇒ β1 . Assume first that πβ2 π. If πβ¦1 π, then there exists π0 ∈ P such that, say, ⊥2 π, and ]π0 (π) = 0 and ]π0 (π) =ΜΈ 0. But now π0 ⊥2 π and π0 ⊥2 ⊥2 so {π} =ΜΈ {π} contradicting the assumption. The converse does not hold. For example, let π = 6 and π = 12; then πβ1 π. ⊥2 π, and hence {π}⊥2 =ΜΈ {π}⊥2 . In If π₯ = 2/3, then π₯⊥2 π but π₯ other words, πβ¦2 π. β1 versus βER . Clearly βER ⇒ β1 . The converse does not hold. For example, 2/3β1 3/2 but 2/3β¦ER 3/2. β2 versus βER . We show that β2 ⇒ βER . Given π1 , . . . , ππ‘ ∈ P, denote by π(π1 , . . . , ππ‘ ) the set of such positive integers that are not divisible by any ππ , π = 1, . . . , π‘. Let π = π/π’ ∈ Q+ , gcd(π, π’) = 1. Factorize πΌ πΌ π = π1 1 ⋅ ⋅ ⋅ πβ β , π½ π½ π’ = π1 1 ⋅ ⋅ ⋅ ππ π , (56) where π1 , . . . , πβ , π1 , . . . , ππ ∈ P are distinct and πΌ1 , . . . , πΌβ , π½1 , . . ., π½π > 0. (If π = 1 or π’ = 1, then the corresponding “empty product” is one.) Now π π11 {π}⊥2 = { π1 π1 π ⋅ ⋅ ⋅ πββ π ⋅ ⋅ ⋅ πππ π₯ | πΌ π + ⋅ ⋅ ⋅ + πΌβ πβ + π½1 π1 π¦ 1 1 + ⋅ ⋅ ⋅ + π½π ππ = 0, π₯, π¦ ∈ π (π1 , . . . , πβ , π1 , . . . , ππ ) } . (57) 7 (The “empty sum” is zero.) Assume that π = π/V ∈ Q+ , gcd(π, V) = 1, satisfies πβ2 π, that is, {π}⊥2 = {π}⊥2 . Then, by (57), necessarily π π π = π11 ⋅ ⋅ ⋅ πββ , π π V = π1 1 ⋅ ⋅ ⋅ πππ , (58) where π1 , . . . , πβ , π1 , . . . , ππ > 0. Hence πβER π, and the claim follows. The converse is not valid. For example, 2/3βER 4/3 but 2/3β¦2 4/3. 7. Discussion This paper began with a citation by three established mathematicians and computer scientists who showed a remarkable intuition by promoting the use of the symbol of perpendicularity in number theory. Indeed, we have previously seen how this notion settles comfortably in this setting and gains new meanings at a more general level in the context of Abelian group theory. We conclude this paper with the following supplement to their proposal. Let perpendicularity and parallelism mean here ⊥1 and β1 , respectively. Consider the “direction vector” of π ∈ Q+ by (π(2), π(3), . . . , π(π), . . .), where π(π) = 0 if ]π (π) = 0 and π(π) = 1 otherwise. For example, the direction vectors of 45, 1, and 8/25 are, respectively (0, 1, 1, 0, 0, . . .), (0, 0, . . .), and (1, 0, 1, 0, 0, . . .). Now, like the directions of perpendicular lines are as different as possible, the prime factors of perpendicular (positive rational) numbers are as different as possible; that is, such numbers do not have common prime factors. In other words, the direction vectors of perpendicular numbers are as different as possible in the sense that they have no common element of value one. Like parallel lines have the same direction, parallel numbers have the same prime factors. In other words, their direction vectors are equal. Finally, we note that perpendicularity can be axiomatized in a natural way also in many other algebraic structures. Davis [8] did that in a ring. In a vector space, perpendicularity is customarily defined based on an inner product. Another possible approach is to supplement (A1)–(A5) with suitable axioms concerning the multiplication of a vector by a scalar. It might be interesting to study under which additional conditions there exists an inner product inducing this perpendicularity. Acknowledgment The authors would like to thank the referees for carefully reading the paper and kind comments. References [1] R. L. Graham, D. E. Knuth, and O. Patashnik, Concrete Mathematics: A Foundation for Computer Science, Addison-Wesley, Reading, Mass, USA, 2nd edition, 1994. [2] G. Birkhoff, Lattice Theory, American Mathematical Society, Providence, RI, USA, 3rd edition, 1993. [3] P. Haukkanen, J. K. Merikoski, and T. Tossavainen, “Axiomatizing perpendicularity and parallelism,” Journal for Geometry and Graphics, vol. 15, no. 2, pp. 129–139, 2011. 8 [4] G. Davis, “Orthogonality relations on abelian groups,” Journal of the Australian Mathematical Society. Series A, vol. 19, pp. 173– 179, 1975. [5] W. K. Nicholson, Introduction to Abstract Algebra, John Wiley & Sons, New York, NY, USA, 2nd edition, 1999. [6] A. I. Veksler, “Linear spaces with disjoint elements and their conversion into vector lattices,” LeningradskiΔ±Μ GosudarstvennyΔ±Μ PedagogicΜeskiΔ±Μ Institut imeni A. I. Gercena. UcΜenye Zapiski, vol. 328, pp. 19–43, 1967 (Russian). [7] F. Eugeni and B. Rizzi, “An incidence algebra on rational numbers,” Rendiconti di Matematica, vol. 12, no. 3-4, pp. 557– 576, 1979. [8] G. Davis, “Rings with orthogonality relations,” Bulletin of the Australian Mathematical Society, vol. 4, pp. 163–178, 1971. 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