Research article

Two theorems on direct products of gyrogroups

  • Received: 30 October 2022 Revised: 12 December 2022 Accepted: 21 December 2022 Published: 03 January 2023
  • MSC : Primary 20N05; Secondary 20A05, 20E34

  • We extend two standard theorems on groups to gyrogroups: the direct product theorem and the cancellation theorem for direct products. Firstly, we prove that under a certain condition a gyrogroup G can be decomposed as the direct product of two subgyrogroups. Secondly, we prove that finite gyrogroups can be cancelled in direct products: if AB, then A×HB×K or H×AK×B implies HK, where A,B,H, and K are finite gyrogroups.

    Citation: Teerapong Suksumran. Two theorems on direct products of gyrogroups[J]. AIMS Mathematics, 2023, 8(3): 6278-6287. doi: 10.3934/math.2023317

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  • We extend two standard theorems on groups to gyrogroups: the direct product theorem and the cancellation theorem for direct products. Firstly, we prove that under a certain condition a gyrogroup G can be decomposed as the direct product of two subgyrogroups. Secondly, we prove that finite gyrogroups can be cancelled in direct products: if AB, then A×HB×K or H×AK×B implies HK, where A,B,H, and K are finite gyrogroups.



    Let us mention two standard theorems involving direct products of groups in abstract algebra as follows.

    Theorem 1.1. If H and K are normal subgroups of a group (written multiplicatively) that have trivial intersection, then the internal direct product HK is isomorphic to the external direct product H×K as groups.

    Theorem 1.2. Let G,H, and K be finite groups. If G×H and G×K are isomorphic as groups, then H and K are isomorphic as groups.

    Theorem 1.1 is sometimes referred to as the direct product theorem for groups (see, for instance, Theorem 9 in p. 171 of [2]). Theorem 1.2 is sometimes referred to as the cancellation theorem for direct products of finite groups (see, for instance, [5]). The latter theorem may be used for comparing external direct products of finite groups such as the uniqueness part of the fundamental theorem of finite abelian groups (see, for instance, p. 213 of [4]).

    The notion of a gyrogroup is introduced as a suitable generalization of groups. For a detailed discussion of the formation of gyrogroups, the reader is referred to [14], for instance. For algebraic aspects of gyrogroups, the reader is referred to [1,3,6,7,13], for instance. Roughly speaking, a gyrogroup is a non-associative algebraic structure that shares several properties with groups. In fact, every group may be viewed as a gyrogroup with gyroautomorphisms being the identity automorphism. Important theorems on groups can be naturally extended to gyrogroups. This motivates us to continue studying algebraic aspects of gyrogroups. In the present article, we prove the two aforementioned theorems in the case of gyrogroups.

    For the basic theory of gyrogroups, the reader is referred to [11,14]. The formal definition of a gyrogroup can be found in p. 17 of [14]. In this section, we summarize basic terminology, notation, and results in gyrogroup theory for reference.

    In the case when is a binary operation on a non-empty set G, let Aut(G) be the set of all automorphisms of (G,). Let G be a gyrogroup. Recall that G satisfies the left gyroassociative law:

    a(bc)=(ab)gyr[a,b](c) (2.1)

    for all a,b,cG, where gyr[a,b] is an automorphism in Aut(G). We remark that G has the unique two-sided identity, denoted by e. Moreover, any element a in G has the unique two-sided inverse, denoted by a. The automorphism gyr[a,b] in (2.1) is called the gyroautomorphism generated by a and b. It can be proved that G also satisfies the right gyroassociative law:

    (ab)c=a(bgyr[b,a](c)). (2.2)

    for all a,b,cG. The cooperation of G, denoted by , is defined as ab=agyr[a,b](b) for all a,bG. In addition, we define ab=a(b) and ab=a(b). Throughout the article, if X is a non-empty set, then IX denotes the identity map on X; that is, IX(x)=x for all xX.

    Let G and H be gyrogroups. A map φ from G to H is called a gyrogroup homomorphism if φ(ab)=φ(a)φ(b) for all a,bG. A bijective gyrogroup homomorphism is called a gyrogroup isomorphism. If there exists a gyrogroup isomorphism from G to H, then we say that G is isomorphic to H, denoted by GH. Let φ:GH be a gyrogroup homomorphism. The kernel of φ, denoted by kerφ, is defined by kerφ={aG:φ(a)=e}. The image of φ, denoted by imφ, is defined by imφ={bH:b=φ(a) for some aG}.

    Let G be a gyrogroup. Recall that a non-empty subset H of G is a subgyrogroup of G if H forms a gyrogroup under the operation inherited from G. If H and K are subgyrogroups of G, define HK={hk:hH,kK}. A subgyrogroup H of G is called an L-subgyrogroup if gyr[a,h](H)=H for all aG,hH. If H is an L-subgyrogroup of G and if G is finite, then the index formula holds:

    |G|=[G:H]|H|, (2.3)

    where [G:H]=|{aH:aG}| (cf. Corollary 22 of [12]). A subgyrogroup N of G is normal, denoted by NG, provided there is a gyrogroup homomorphism φ from G to a gyrogroup such that N=kerφ. If NG, then gyr[a,b](N)=N for all a,bG (see the proof of Proposition 35 of [11]). Furthermore, the set of left cosets of N in G, G/N={aN:aG}, forms a gyrogroup under the operation defined by (aN)(bN)=(ab)N for all a,bG, called the quotient gyrogroup of G by N. In this case, the map aaN, aG, defines a gyrogroup homomorphism, called the canonical projection.

    Theorem 2.1. (See Chapter 2 of [14]) Let G be a gyrogroup and let a, b, cG.

    1) ab=ac implies b=c;       (left cancellation law I)

    2) a(ab)=b;                (left cancellation law II)

    3) (ba)a=b;                (right cancellation law I)

    4) (ba)a=b.                (right cancellation law II)

    Proposition 2.1. ([12, Part 3 of Proposition 23]) If φ:GH is a gyrogroup homomorphism, then φ(gyr[a,b](c))=gyr[φ(a),φ(b)](φ(c)) for all a,b,cG.

    Proposition 2.2. ([12, Proposition 26]) Let φ:GH be a gyrogroup homomorphism and let a,bG. Then abkerφ if and only if φ(a)=φ(b).

    Let G be a gyrogroup. The set of permutations of G is denoted by Sym(G), which forms a group under composition of maps. For each aG, the left gyrotranslation La is defined by La(x)=ax, xG, which is a permutation of G (cf. Theorem 10 of [12]). Define ˆG to be the set of left gyrotranslations,

    ˆG={La:aG}, (2.4)

    and define Syme(G) to be the set of permutations of G leaving the identity e fixed,

    Syme(G)={ρSym(G):ρ(e)=e}. (2.5)

    Theorem 2.2. ([12, Theorem 11]) Let G be a gyrogroup. For each σSym(G), σ can be written uniquely as σ=Laρ, where aG and ρSyme(G).

    Let G and H be gyrogroups. As defined in [10], the direct product of G and H, denoted by G×H, is a gyrogroup with underlying set {(g,h):gG,hH} whose operation is given componentwise by

    (a,b)(c,d)=(ac,bd) (2.6)

    for all a,cG and for all b,dH.

    Proposition 2.3. Let A,B,C, and D be gyrogroups.

    1) Then A×BB×A.

    2) If AB and BC, then AC.

    3) If AC and BD, then A×BC×D.

    Proof. The map Φ defined by Φ(a,b)=(b,a), aA,bB, is a gyrogroup isomorphism from A×B to B×A. If ϕ:AB and ψ:BC are gyrogroup isomorphisms, then ψϕ is a gyrogroup isomorphism from A to C. If ϕ:AC and ψ:BD are gyrogroup isomorphisms, then the map θ defined by θ(a,b)=(ϕ(a),ψ(b)), aA,bB, is a gyrogroup isomorphism from A×B to C×D.

    The main purpose of this article is to generalize Theorems 1.1 and 1.2 from groups to gyrogroups. The direct product theorem for gyrogroups proves useful in understanding the gyrogroup that arises in Cayley's theorem for gyrogroups, as we will see shortly. The cancellation theorem for gyrogroups may be used to compare direct products of finite gyrogroups, as in the case of groups.

    To prove the direct product theorem for gyrogroups, we need two preliminary lemmas involving gyroautomorphisms, which are important in their own right.

    Lemma 3.1. Let H and K be normal subgyrogroups of a gyrogroup G such that HK={e}.

    1) Then hk=kh for all hH,kK.

    2) If hH and bG, then gyr[h,b](k)=k for all kK.

    3) If kK and aG, then gyr[a,k](h)=h for all hH.

    Proof. Since HG and KG, we obtain H=kerφ and K=kerψ, where φ and ψ are homomorphisms of G to some gyrogroups. Let hH and kK. Since φ preserves the operations and φ(h)=e, it follows that

    φ(h(k(hk)))=φ(h)(φ(k)(φ(h)φ(k)))=e.

    Hence, h(k(hk))H. Similarly, ψ(h(k(hk)))=e and then h(k(hk))K. Since HK={e}, we obtain h(k(hk))=e, which implies hk=kh by the left cancellation law II. This proves Part 1.

    Let hH, bG, and kK. Since gyr[h,b](K)=K, it follows that gyr[h,b](k)=k for some kK. By Proposition 2.1, φ(k)=φ(gyr[h,b](k))=gyr[φ(h),φ(b)](φ(k))=φ(k) since φ(h)=e. By Proposition 2.2, kkH. Hence, kkHK. By assumption, kk=e, which implies k=k by the left cancellation law II. This proves Part 2. Part 3 is proved in a similar fashion to Part 2.

    Lemma 3.2. ([8, Lemma 1]) If H and K are subgyrogroups of a gyrogroup G with the property that gyr[a,b](K)K for all a,bH and HK={e}, then h1k1=h2k2, where h1,h2H,k1,k2K, implies h1=h2 and k1=k2.

    Proof. See the proof of Lemma 1 of [8].

    The following theorem gives a criterion to decompose a gyrogroup into the direct product of its subgyrogroups. This generalizes the familiar direct product theorem for groups.

    Theorem 3.1. (Direct product theorem for gyrogroups) Let G be a gyrogroup. If H and K are subgyrogroups of G such that

    (i)G=HK;

    (ii)HG and KG;

    (iii)HK={e},

    then GH×K as gyrogroups.

    Proof. Define a map ϕ by ϕ(h,k)=hk for all hH,kK. Then ϕ sends H×K to G. We show that ϕ is an isomorphism. By condition (i), ϕ is surjective. Let h1,h2H and k1,k2K. Suppose that ϕ(h1,k1)=ϕ(h2,k2). Then h1k1=h2k2. By Lemma 3.2, h1=h2 and k1=k2. This proves that ϕ is injective. Using the left and right gyroassociative laws and Lemma 3.1, we obtain

    ϕ((h1,k1)(h2,k2))=ϕ(h1h2,k1k2)=(h1h2)(k1k2)=h1(h2gyr[h2,h1](k1k2))=h1(h2(k1k2))=h1((h2k1)gyr[h2,k1](k2))=h1((h2k1)k2)=h1((k1h2)k2)=h1(k1(h2gyr[h2,k1](k2)))=h1(k1(h2k2))=(h1k1)gyr[h1,k1](h2k2)=(h1k1)(gyr[h1,k1](h2)gyr[h1,k1](k2))=(h1k1)(h2k2)=ϕ(h1,k1)ϕ(h2,k2).

    This proves that ϕ preserves the gyrogroup operations.

    The converse of the above theorem also holds, in the sense of the following theorem.

    Theorem 3.2. Let A and B be gyrogroups and let G=A×B. Then G contains subgyrogroups H and K such that

    (i)G=HK;

    (ii)HG and KG;

    (iii)HK={(e,e)}.

    Proof. Set H={(a,e):aA} and K={(e,b):bB}. By definition, (a,b)=(a,e)(e,b) for all aA,bB. Hence, G=HK. Let π1:A×BA and π2:A×BB be the projection maps defined by π1(a,b)=a and π2(a,b)=b for all (a,b)A×B, respectively. Then π1 and π2 are gyrogroup homomorphisms such that H=kerπ2 and K=kerπ1. This shows that HG and KG. It is clear that HK={(e,e)}.

    We give a few concrete examples to illustrate Theorem 3.1 below.

    Example 3.1. Let A be the gyrogroup Dih(G8) given in Example 5 of [8], called the dihedralized gyrogroup of G8. Let B be the gyrogroup Qgyr16 given in Example 5.2 of [9]. Then G=A×B is a finite gyrogroup of order 256. Set H={(a,(0,0)):aA} and K={((0,0),b):bB}. As in the proof of Theorem 3.2, H and K are distinct normal subgyrogroups of G such that HK contains precisely the identity of G.

    Example 3.2 Referring to the Einstein gyrogroup (B,E) in Section 3.8 of [14], we know by Theorem 12 of [12] that Sym(B) forms a gyrogroup under the operation given by

    στ=LuEv(αβ) (3.1)

    for all u,vB,α,βSym0(B)={ρSym(B):ρ(0)=0}. Using (3.1), one can check that H={Lu:uB} and K=Sym0(B) are distinct normal subgyrogroups of Sym(B) such that HK contains precisely the identity of Sym(B).

    The previous example can be generalized to arbitrary gyrogroups as follows. Recall that Cayley's theorem for gyrogroups states that every gyrogroup is isomorphic to a gyrogroup of permutations. Let G be a gyrogroup. Let σ and τ be arbitrary permutations of G. By Theorem 2.2, σ and τ have unique factorizations σ=Laα and τ=Lbβ, where a,bG and α,βSyme(G). This allows us to introduce a gyrogroup operation on Sym(G), given by

    στ=Lab(αβ). (3.2)

    Then (Sym(G),) becomes a gyrogroup containing ˆG as an isomorphic copy of G. Moreover, by the direct product theorem, (Sym(G),)ˆG×Syme(G) as gyrogroups. This leads to new insight into the gyrogroup version of Cayley's theorem.

    To prove the cancellation theorem for direct products of finite gyrogroups, we need preliminary results, which are important in their own right. We remark that this method of proof follows the same steps as in the case of finite groups. Let G and H be gyrogroups. Define Hom(G,H) to be the set of all homomorphisms from G to H,

    Hom(G,H)={φ:φ is a homomorphism from GtoH}, (3.3)

    and define IHom(G,H) to be the set of all injective homomorphisms from G to H,

    IHom(G,H)={φ:φ is an injective homomorphism from GtoH}. (3.4)

    Proposition 3.1. Let G,H, and K be gyrogroups.

    1) If HK, then there is a bijection from Hom(G,H) to Hom(G,K).

    2) There is a bijection from Hom(G,H)×Hom(G,K) to Hom(G,H×K).

    3) There is a bijection from IHom(G,H) to IHom(G/{e},H).

    Proof. To prove Part 1, suppose that Φ:HK is an isomorphism. Define a map σ by σ(φ)=Φφ for all φHom(G,H). As the composite of gyrogroup homomorphisms is again a gyrogroup homomorphism, σ(φ) lies in Hom(G,K). Hence, σ sends Hom(G,H) to Hom(G,K). Note that Φ1 is an isomorphism from K to H. We obtain similarly that the map τ defined by τ(ψ)=Φ1ψ for all ψHom(G,K) sends Hom(G,K) to Hom(G,H). Direct computation shows that στ=IHom(G,K) and τσ=IHom(G,H). Hence, σ is bijective and σ1=τ.

    For αHom(G,H) and βHom(G,K), define a map α×β by

    α×β(g)=(α(g),β(g))for all gG.

    It is not difficult to see that α×β is a homomorphism from G to H×K. Define a map σ by σ(α,β)=α×β for all αHom(G,H),βHom(G,K). Then σ maps Hom(G,H)×Hom(G,K) to Hom(G,H×K). It is easy to see that σ is injective. Suppose that φHom(G,H×K). Let π1:H×KH and π2:H×KK be the projection maps defined by π1(h,k)=h and π2(h,k)=k for all (h,k)H×K, respectively. Then π1φHom(G,H) and π2φHom(G,K). Let gG and assume that φ(g)=(h,k) with hH, kK. Then σ(π1φ,π2φ)(g)=(π1(φ(g)),π2(φ(g)))=(h,k)=φ(g) and so σ(π1φ,π2φ)=φ. This proves that σ is surjective, which completes the proof of Part 2. The proof of Part 3 is straightforward.

    Proposition 3.2. Let G and H be gyrogroups. Then there is a bijection from Hom(G,H) to NGIHom(G/N,H).

    Proof. First, note that if NG and KG, then G/N=G/K if and only if N=K. In fact, G/N=G/K implies eN is the identity of G/K. Hence, eN=eK by the uniqueness of the identity and so N=K. It follows that IHom(G/N,H) and IHom(G/K,H) have empty intersection whenever NK.

    Set U=NGIHom(G/N,H). For each φHom(G,H), let ¯φ be the isomorphism from G/kerφ to imφ defined as in the proof of the first isomorphism theorem (cf. Theorem 28 of [12]) by the equation ¯φ(akerφ)=φ(a) for all aG. Then ¯φ is an injective homomorphism from G/kerφ to H; that is, ¯φIHom(G/kerφ,H). Define a map σ by σ(φ)=¯φ for all φHom(G,H). Then σ maps Hom(G,H) to U. For each normal subgyrogroup N of G, let πN be the canonical projection from G to G/N. For each ψU, as noted above, there is a unique normal subgyrogroup N of G such that ψIHom(G/N,H) and we can define τ(ψ)=ψπN. Then τ defines a map from U to Hom(G,H). We show that σ and τ are inverses of each other. Let φHom(G,H). Note that (τσ)(φ)=τ(¯φ)=¯φπkerφ and that (¯φπkerφ)(a)=¯φ(akerφ)=φ(a) for all aG. Hence, ¯φπkerφ=φ. This proves that τσ=IHom(G,H). Let ψU. Then ψIHom(G/N,H), where NG. Note that (στ)(ψ)=σ(ψπN)=¯ψπN. Since ker(ψπN)=N, we obtain by definition that

    ¯ψπN(aN)=¯ψπN(aker(ψπN))=(ψπN)(a)=ψ(aN)

    for all aG. Hence, ¯ψπN=ψ. This proves that στ=IU. Therefore, σ is bijective and σ1=τ.

    Suppose that G and H are finite gyrogroups. Because the union in the previous proposition is disjoint, we derive a counting formula for homomorphisms from G to H in terms of injective homomorphisms from G/N to H, where N runs over all normal subgyrogroups of G.

    Corollary 3.1. If G and H are finite gyrogroups, then

    |Hom(G,H)|=NG|IHom(G/N,H)|. (3.5)

    Proof. Since G and H are finite, Hom(G,H) is a finite set. As noted in the proof of Proposition 3.2, if NK, then IHom(G/N,H)IHom(G/K,H)=. Hence, Hom(G,H) is the disjoint union of the sets IHom(G/N,H) as N varies over all normal subgyrogroups of G. Thus, |Hom(G,H)|=|NGIHom(G/N,H)|=NG|IHom(G/N,H)|.

    We are now in a position to prove a left cancellation law for direct products of finite gyrogroups: if G,H, and K are finite gyrogroups, then G×HG×K implies HK.

    Theorem 3.3. (Left cancellation in direct products) Let G,H, and K be finite gyrogroups. If G×HG×K, then HK.

    Proof. Suppose that G×HG×K. First, we show that

    |Hom(L,H)|=|Hom(L,K)|

    for all finite gyrogroups L. Let L be a finite gyrogroup. Note that |Hom(L,G)|0 because the trivial homomorphism t defined by t(a)=e for all aL is an element in Hom(L,G). By Part 1 and Part 2 of Proposition 3.1,

    |Hom(L,G)||Hom(L,H)|=|Hom(L,G×H)|=|Hom(L,G×K)|=|Hom(L,G)||Hom(L,K)|,

    which implies |Hom(L,H)|=|Hom(L,K)|.

    Next, we show that |IHom(L,H)|=|IHom(L,K)| for all finite gyrogroups L by induction on |L|. The case where |L|=1 is clear. Suppose that {e}NL. Since N is an L-subgyrogroup of G, we obtain that |L/N|=|L||N|<|L|. Hence, by the inductive hypothesis, |IHom(L/N,H)|=|IHom(L/N,K)|. By Part 3 of Proposition 3.1 and (3.5),

    |IHom(L,H)|=|IHom(L/{e},H)|=|Hom(L,H)|{e}NL|IHom(L/N,H)|=|Hom(L,K)|{e}NL|IHom(L/N,K)|=|IHom(L/{e},K)|=|IHom(L,K)|,

    which completes the induction.

    In the particular case when L=H, we have |IHom(H,K)|=|IHom(H,H)|1 because the identity homomorphism on H is in IHom(H,H). Hence, there is a homomorphism ϕIHom(H,K). Since |G||H|=|G×H|=|G×K|=|G||K|, it follows that |H|=|K|. Since ϕ is injective, |ϕ(H)|=|H|=|K|. Since ϕ(H)K and K is finite, ϕ(H)=K. This proves that ϕ is surjective and so ϕ becomes an isomorphism from H to K. Thus, HK.

    Corollary 3.2. (Right cancellation in direct products) Let G,H, and K be finite gyrogroups. If H×GK×G, then HK.

    Proof. This follows directly from Theorem 3.3 and Proposition 2.3.

    We may weaken the assumptions of Theorem 3.3 and Corollary 3.2, as shown in the following theorem.

    Theorem 3.4. (Cancellation in direct products) Let A,B,H, and K be finite gyrogroups such that AB. If A×HB×K or H×AK×B, then HK.

    Proof. Suppose that A×HB×K. Since AB, it follows by Part 3 of Proposition 2.3 that A×HB×H. By Part 2 of Proposition 2.3, B×HB×K. By Theorem 3.3, HK. The case where H×AK×B is proved similarly.

    We emphasize that the finiteness of gyrogroups in Theorem 3.3 is crucial. In fact, there are infinite gyrogroups (indeed, infinite groups) G,H, and K such that G×HG×K but H and K are not isomorphic. For example, let G=i=1Z, let H=Z, and let K=Z×Z, where Z is the additive group of integers. Then G×HG×K but H and K are not isomorphic.

    We prove a few theorems that involve direct products of gyrogroups, especially the direct product theorem for gyrogroups and some cancellation laws for direct products of finite gyrogroups. These results extend two well-known results in abstract algebra.

    This work was supported by the Research Group in Mathematics and Applied Mathematics, Chiang Mai University.

    The author declares no conflict of interest.



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  • This article has been cited by:

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