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On the Euler characteristics for quandles

Ryoya Kai and Hiroshi Tamaru
Abstract

A quandle is an algebraic system whose axioms generalize the algebraic structure of the point symmetries of symmetric spaces. In this paper, we give a definition of Euler characteristics for quandles. In particular, the quandle Euler characteristic of a compact connected Riemannian symmetric space coincides with the topological Euler characteristic. Additionally, we calculate the Euler characteristics of some finite quandles, including generalized Alexander quandles, core quandles, discrete spheres, and discrete tori. Furthermore, we prove several properties of quandle Euler characteristics, which suggest that they share similar properties with topological Euler characteristics.

1 Introduction

The Euler characteristic for a topological space is one of the classical and important topological invariants. In general, the Euler characteristics can be defined for topological spaces using Betti numbers or cell complexes. Hopf and Samelson [Hopf-1941-SatzüberWirkungsräumeGeschlossener] developed a method for calculating the Euler characteristics of homogeneous spaces of compact Lie groups. A symmetric space is a space with a point symmetry at each point. A compact connected symmetric space is a homogeneous space under the action of the compact Lie group generated by these point symmetries. In conclusion, the Euler characteristic of a compact connected Riemannian symmetric space can be computed using the point symmetries.

A quandle is an algebraic system introduced in knot theory [5], that consists of a pair of a non-empty set XX and a map s:XMap(X,X)s:X\to\mathrm{Map}(X,X) satisfying certain axioms. These axioms align well with the local moves of knot diagrams, known as Reidemeister moves. Recently, quandles have played important roles in many branches of mathematics. For example, symmetric spaces can be viewed as quandles via their point symmetries. In other words, a quandle can be considered as a generalization of an algebraic system that focuses specially on point symmetries in a symmetric space. In particular, quandles can be regarded as a discretization of symmetric spaces, and there have been several recent studies from this view point (for instance, see [1, 6, 4]).

A quandle structure gives rise to certain canonical groups, which act on the quandle in a manner compatible with the point symmetries sx:=s(x):XXs_{x}:=s(x):X\to X. The following group, which plays a key role in this study, is defined by Joyce [5, §5] as the transvection group.

Definition 1.1 ([5], [3]).

The group defined by

Dis(X)=sxsy1x,yXGrp\mathrm{Dis}(X)=\langle s_{x}\circ s_{y}^{-1}\mid x,y\in X\rangle_{\mathrm{Grp}}

is called the displacement group of a quandle XX.

In this paper, we define the quandle Euler characteristic using the action of the displacement group as follows:

Definition 1.2.

Let XX be a quandle. Then the quandle Euler characteristic χQdle(X)\chi^{\mathrm{Qdle}}(X) is defined by

χQdle(X):=inf{#Fix(g,X)gDis(X)},\chi^{\mathrm{Qdle}}(X):=\inf\{\#\mathrm{Fix}(g,X)\mid g\in\mathrm{Dis}(X)\},

where Fix(g,X)\mathrm{Fix}(g,X) denotes the set of fixed points of the action of gg on XX.

By definition, the quandle Euler characteristic satisfies χQdle(X)0\chi^{\mathrm{Qdle}}(X)\in\mathbb{Z}_{\geq 0}, which aligns with the property of the topological Euler characteristics for compact homogeneous spaces. Furthermore, the following theorem explains why we refer to the number defined above as the quandle Euler characteristic.

Theorem 1.3 (Theorem 3.4).

For a compact connected Riemannian symmetric space, the quandle Euler characteristic is equal to the topological Euler characteristic.

In this paper, we prove several properties of quandle Euler characteristics, which indicate that they share similarities with topological Euler characteristics. In Section 4, we determine the quandle Euler characteristics of some particular examples of quandles.

First examples we consider are generalized Alexander quandles. A generalized Alexander quandle, denoted by GAlex(G,σ)\mathrm{GAlex}(G,\sigma), is defined as a group GG whose quandle structure is given by a group automorphism σ\sigma of GG. The class of generalized Alexander quandles is important in quandle theory, as any homogeneous quandle can be realized as a quotient of some generalized Alexander quandle. Note that any homogeneous manifold can be also expressed as a quotient of a Lie group. Therefore, in the theory of quandles, generalized Alexander quandles can be viewed as counterparts of Lie groups. The following theorem determines the quandle Euler characteristics of generalized Alexander quandles.

Theorem 1.4 (Theorem 4.1).

If σ\sigma is a non-trivial group automorphism of a group GG, then the quandle Euler characteristic of the generalized Alexander quandle GAlex(G,σ)\mathrm{GAlex}(G,\sigma) is equal to 0.

The second examples are core quandles, which are groups with quandle structures derived from the map taking the inverse element. This provides a natural quandle structure for a group from the viewpoint of symmetric spaces. In fact, a symmetric space structure of a Lie group is usually given by the core quandle structure. Similar to the case of generalized Alexander quandles, we determine the quandle Euler characteristics of core quandles, which are analogous to the topological Euler characteristics of non-trivial compact connected Lie groups that are equal to 0.

Theorem 1.5 (Theorem 4.3).

The quandle Euler characteristic of a non-trivial core quandle is equal to 0.

The third examples consist of discrete subquandles within compact Riemannian symmetric spaces. A typical example is the discrete nn-sphere, denoted by DSnDS^{n}, which is defined as a particular finite subquandle of the standard nn-sphere SnS^{n}. The following theorem suggests that the quandle Euler characteristics of certain finite objects approximate the topological Euler characteristics of continuous objects.

Theorem 1.6 (Theorem 4.6).

For any positive integer nn, the quandle Euler characteristic of the discrete nn-sphere DSnDS^{n} satisfies χQdle(DSn)=χTop(Sn)\chi^{\mathrm{Qdle}}(DS^{n})=\chi^{\mathrm{Top}}(S^{n}), that is,

χQdle(DSn)={0if n is odd,2if n is even.\chi^{\mathrm{Qdle}}(DS^{n})=\begin{cases*}0&if $n$ is odd,\\ 2&if $n$ is even.\end{cases*}

We also consider the discrete torus DTunDT^{n}_{u}, which is a discrete subquandle of a flat torus Tn=(S1)nT^{n}=(S^{1})^{n} parametrized by u=(m1,,mn)(>0)nu=(m_{1},\dots,m_{n})\in(\mathbb{Z}_{>0})^{n}. Recall that the topological Euler characteristic of a flat torus is equal to 0. Similar to discrete spheres, the quandle Euler characteristics of discrete tori approximate the topological Euler characteristics of flat tori.

Theorem 1.7 (Corollary 5.4).

For any positive integer nn and any u=(m1,,mn)(>0)nu=(m_{1},\dots,m_{n})\in(\mathbb{Z}_{>0})^{n} with mi>2m_{i}>2 for all ii, the quandle Euler characteristics of the discrete torus DTunDT^{n}_{u} satisfies χQdle(DTun)=χTop(Tn)=0\chi^{\mathrm{Qdle}}(DT^{n}_{u})=\chi^{\mathrm{Top}}(T^{n})=0.

In Section 5, we study some general properties of quandle Euler characteristics. As a corollary of the Künneth theorem, it is known that the topological Euler characteristic of the product of CW complexes is equal to the product of the topological Euler characteristics of each components (cf. [11]). Note that the direct product of quandles can be defined naturally. We prove a similar statement for the quandle Euler characteristic of the direct product:

Theorem 1.8 (Theorem 5.2).

The quandle Euler characteristic of the direct product of quandles (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}) satisfies χQdle(X1×X2)=χQdle(X1)χQdle(X2)\chi^{\mathrm{Qdle}}(X_{1}\times X_{2})=\chi^{\mathrm{Qdle}}(X_{1})\cdot\chi^{\mathrm{Qdle}}(X_{2}).

For two quandles, one can naturally define a quandle structure on the disjoint union set, which is called the interaction-free union of quandles. In the category of topological spaces, the Euler characteristic of a disjoint union of spaces is equal to the sum of the Euler characteristics of the components, since the homology group of the disjoint union is isomorphic to the direct sum of the homology groups of the individual components. We present an inequality concerning quandle Euler characteristics that mirrors this property:

Theorem 1.9 (Theorem 5.6).

Let (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}) be quandles. Then, the quandle Euler characteristic of the interaction-free union X1freeX2X_{1}\sqcup^{\mathrm{free}}X_{2} satisfies

χQdle(X1freeX2)χQdle(X1)+χQdle(X2).\chi^{\mathrm{Qdle}}(X_{1}\sqcup^{\mathrm{free}}X_{2})\leq\chi^{\mathrm{Qdle}}(X_{1})+\chi^{\mathrm{Qdle}}(X_{2}).

Unlike the case of topological Euler characteristics, the equality in the above theorem does not hold in general. We will provide an example that does not achieve this equality (see Example 5.7).

2 Preliminary

In this section, we review some notions of quandles and basic facts on symmetric spaces. In particular, the displacement groups play an important role. First, let us recall the definition of quandles.

Definition 2.1 ([5]).

Let XX be a non-empty set and let Map(X,X)\mathrm{Map}(X,X) be the set of all maps from XX to XX. For a map s:XMap(X,X)s:X\to\mathrm{Map}(X,X), the pair (X,s)(X,s) is called a quandle if the following three conditions hold:

  1. 1.

    sx(x)=xs_{x}(x)=x for any xXx\in X,

  2. 2.

    sx:XXs_{x}:X\to X is a bijection,

  3. 3.

    sxsy=ssx(y)sxs_{x}\circ s_{y}=s_{s_{x}(y)}\circ s_{x} for any x,yXx,y\in X.

For quandles (X,sX)(X,s^{X}) and (Y,sY)(Y,s^{Y}), a map f:XYf:X\to Y is called a quandle homomorphism if fsxX=sf(x)Yff\circ s_{x}^{X}=s_{f(x)}^{Y}\circ f holds for any xXx\in X. A bijective quandle homomorphism is called a quandle isomorphism.

Definition 2.2.

The quandle automorphism group Aut(X)\mathrm{Aut}(X) is the group consisting of all quandle isomorphisms from XX to XX. The quandle automorphism group is a group under composition, and acts on XX. A quandle XX is called homogeneous if its automorphism group acts transitively on XX.

Note that the maps sx:XXs_{x}:X\to X are quandle automorphisms.

Definition 2.3.

The subgroup of Aut(X)\mathrm{Aut}(X) generated by the set {sxxX}\{s_{x}\mid x\in X\} is called the inner automorphism group and is denoted by Inn(X)\mathrm{Inn}(X). A quandle XX is called connected if the inner automorphism group acts transitively on XX.

The following group is defined by Joyce [5, §5] as the transvection group.

Definition 2.4 ([5], [3]).

The subgroup of Inn(X)\mathrm{Inn}(X) defined by

Dis(X)=sxsy1x,yXGrp\mathrm{Dis}(X)=\langle s_{x}\circ s_{y}^{-1}\mid x,y\in X\rangle_{\mathrm{Grp}}

is called the displacement group of XX.

These groups and their actions are studied in detail in [3]. In particular, the actions of the displacement group and the inner automorphism group on a quandle have the same orbits.

According to the definition of a symmetric space given by Loos [7], its point symmetries provide a quandle structure. For this reason, the map sx:XXs_{x}:X\to X in the definition of a quandle is called the point symmetry at xx of XX. In the case of symmetric spaces, Loos [7] gave the following properties about the displacement group. These properties will be used in the latter argument.

Proposition 2.5 ([7, Chapter 2, Theorems 2.8 and 3.1]).

Let XX be a symmetric space, and suppose that XX is connected as a topological space. Then the followings hold:

  1. 1.

    The displacement group Dis(X)\mathrm{Dis}(X) is a connected Lie group.

  2. 2.

    XX is connected as a quandle, and in particular XX is a homogeneous space of Dis(X)\mathrm{Dis}(X).

At the end of this section, we see the nn-dimensional unit sphere as a typical example of symmetric spaces.

Example 2.6.

The nn-dimensional unit sphere SnS^{n} is a compact connected Riemannian symmetric space, and hence the point symmetries give rise to a quandle structure on SnS^{n}. The point symmetry sp:SnSns_{p}:S^{n}\to S^{n} at a point pSnp\in S^{n} is defined by

sp(x)=2x,ppx,s_{p}(x)=2\langle x,p\rangle p-x,

where ,\langle\cdot,\cdot\rangle is the standard inner product of n+1\mathbb{R}^{n+1}. In this case, the inner automorphism group Inn(Sn)\mathrm{Inn}(S^{n}) and the displacement group Dis(Sn)\mathrm{Dis}(S^{n}) are

Inn(Sn)\displaystyle\mathrm{Inn}(S^{n}) ={O(n+1)if n is odd,SO(n+1)if n is even,\displaystyle=\begin{cases*}\mathrm{O}(n+1)&if $n$ is odd,\\ \mathrm{SO}(n+1)&if $n$ is even,\end{cases*}
Dis(Sn)\displaystyle\mathrm{Dis}(S^{n}) =SO(n+1).\displaystyle=\mathrm{SO}(n+1).

Then, the quandle SnS^{n} is connected, since the orthogonal group O(n+1)\mathrm{O}(n+1) and the special orthogonal group SO(n+1)\mathrm{SO}(n+1) acts transitively on SnS^{n}. In particular, the displacement group is a connected Lie group for any dimension nn.

3 The quandle Euler characteristics

In this section, we define the quandle Euler characteristics by using the displacement group. We also show that this notion is a natural generalization of the topological Euler characteristics of compact connected symmetric spaces.

When a group GG acts on a set XX, we denote the set of fixed points of this action by Fix(G,X)\mathrm{Fix}(G,X). Similarly, we denote the set of fixed points of the action of an element gGg\in G by Fix(g,X)\mathrm{Fix}(g,X). The following is the definition of the quandle Euler characteristics.

Definition 3.1.

Let XX be a quandle. Then the quandle Euler characteristic χQdle(X)\chi^{\mathrm{Qdle}}(X) is defined by

χQdle(X):=inf{#Fix(g,X)gDis(X)}.\chi^{\mathrm{Qdle}}(X):=\inf\{\#\mathrm{Fix}(g,X)\mid g\in\mathrm{Dis}(X)\}.

In order to calculate the quandle Euler characteristic of a given quandle XX, one needs to know the displacement group Dis(X)\mathrm{Dis}(X). Since the displacement group of a trivial quandle is the trivial group, we have the following result.

Example 3.2.

The Euler characteristic of a trivial quandle is equal to its cardinality.

The definition of the quandle Euler characteristic involves a group action. This concept is inspired by a classical result from Hopf and Samelson [Hopf-1941-SatzüberWirkungsräumeGeschlossener]. Let GG be a compact connected Lie group and TT a maximal torus of GG. Then, there exists an element g0Tg_{0}\in T such that the topological closure in GG of the group generated by g0g_{0} is equal to TT. Such an element g0Tg_{0}\in T is called a generator of TT. Hopf and Samelson provided a formula for the topological Euler characteristic of a compact connected homogeneous space in terms of a maximal torus and its generator.

Proposition 3.3 ([Hopf-1941-SatzüberWirkungsräumeGeschlossener], see also [Püttmann-2002-HomogeneityRankAtomsActions]).

Let MM be a homogeneous space of a compact connected Lie group GG. Let us consider a maximal torus TT of GG, and let g0Tg_{0}\in T be a generator of TT. Then, the topological Euler characteristic χTop(M)\chi^{\mathrm{Top}}(M) satisfies

χTop(M)=#Fix(T,M)=#Fix(g0,M).\chi^{\mathrm{Top}}(M)=\#\mathrm{Fix}(T,M)=\#\mathrm{Fix}(g_{0},M).

Using this proposition, one can show that the notion of quandle Euler characteristics is a generalization of the notion of topological Euler characteristics of compact connected Riemannian symmetric spaces. Recall that a Riemannian symmetric space is a quandle by the point symmetries, and each point symmetry is an isometry.

Theorem 3.4.

For a compact connected Riemannian symmetric space, the quandle Euler characteristic is equal to the topological Euler characteristic.

Proof.

Let XX be a compact connected Riemannian symmetric space. By Proposition 2.5, the displacement group G:=Dis(X)G:=\mathrm{Dis}(X) is a connected Lie group, and acts transitively on XX. Since each point symmetry is an isometry, the displacement group G:=Dis(X)G:=\mathrm{Dis}(X) is a subgroup of the isometry group Isom(X)\mathrm{Isom}(X) of XX. Since XX is a compact Riemannian symmetric space, the isometry group is compact [8, §5], and in particular, GG is compact. Let TT be a maximal torus in GG and let g0g_{0} be a generator of TT. Since χTop(X)=#Fix(g0,X)\chi^{\mathrm{Top}}(X)=\#\mathrm{Fix}(g_{0},X) by Proposition 3.3, we have

χTop(X)infgGFix(g,X)=χQdle(X).\chi^{\mathrm{Top}}(X)\geq\inf_{g\in G}\mathrm{Fix}(g,X)=\chi^{\mathrm{Qdle}}(X).

It remains to prove the converse inequality. Let us take any gGg\in G, and we will show

χTop(X)#Fix(g,X).\chi^{\mathrm{Top}}(X)\leq\#\mathrm{Fix}(g,X).

Since GG is a compact Lie group, all maximal tori are conjugate. Hence there exists hGh\in G such that hgh1Thgh^{-1}\in T. Therefore, it satisfies

#Fix(g,X)=#Fix(hgh1,X)#Fix(T,X)=χTop(X),\#\mathrm{Fix}(g,X)=\#\mathrm{Fix}(hgh^{-1},X)\geq\#\mathrm{Fix}(T,X)=\chi^{\mathrm{Top}}(X),

which completes the proof. ∎

4 Examples of the quandle Euler characteristics

In this section, we calculate the quandle Euler characteristics of specific examples of quandles.

4.1 The generalized Alexander quandles

As the first example, we consider the generalized Alexander quandles. For a group GG and a group automorphism σAut(G)\sigma\in\mathrm{Aut}(G), the generalized Alexander quandle GAlex(G,σ)\mathrm{GAlex}(G,\sigma) is a quandle (G,s)(G,s), where the map s:GMap(G,G)s:G\to\mathrm{Map}(G,G) is defined by sh(g)=hσ(h1g)s_{h}(g)=h\sigma(h^{-1}g) for g,hGg,h\in G. The inverse of a point symmetry shs_{h} is given by sh1(g)=hσ1(h1g)s_{h}^{-1}(g)=h\sigma^{-1}(h^{-1}g). Note that a generalized Alexander quandle GAlex(G,σ)\mathrm{GAlex}(G,\sigma) is trivial if and only if the automorphism σ\sigma is trivial. The next theorem determines the quandle Euler characteristics of generalized Alexander quandles.

Theorem 4.1.

If σ\sigma is a non-trivial group automorphism of a group GG, then the quandle Euler characteristic of the generalized Alexander quandle GAlex(G,σ)\mathrm{GAlex}(G,\sigma) is equal to 0.

Proof.

Since σ\sigma is non-trivial, there exists gGg\in G such that σ(g)g\sigma(g)\neq g. Consider sgs11Dis(GAlex(G,σ))s_{g}\circ s_{1}^{-1}\in\mathrm{Dis}(\mathrm{GAlex}(G,\sigma)) for gGg\in G, where 11 is the identity of GG. It is enough to show that sgs1s_{g}\circ s_{1} has no fixed points. For any xGx\in G, one has

sgs11(x)=sg(σ1(x))=gσ(g1σ1(x))=gσ(g)1x.\displaystyle s_{g}\circ s_{1}^{-1}(x)=s_{g}(\sigma^{-1}(x))=g\sigma(g^{-1}\sigma^{-1}(x))=g\sigma(g)^{-1}x.

Since σ(g)g\sigma(g)\neq g, we have gσ(g)11g\sigma(g)^{-1}\neq 1, and thus sgs11(x)xs_{g}\circ s_{1}^{-1}(x)\neq x. This yields that sgs11s_{g}\circ s_{1}^{-1} has no fixed points, which completes the proof. ∎

A generalized Alexander quandle is called an Alexander quandle (or an affine quandle) if it is defined by an abelian group GG. Recall that the dihedral quandle RnR_{n} is a typical example of Alexander quandles.

Example 4.2.

The dihedral quandle RnR_{n} is a quandle isomorphic to GAlex(/n,σ)\mathrm{GAlex}(\mathbb{Z}/n\mathbb{Z},\sigma), where σ:/n/n\sigma:\mathbb{Z}/n\mathbb{Z}\to\mathbb{Z}/n\mathbb{Z} is the group automorphism defined by σ(a)=a\sigma(a)=-a. The dihedral quandles can be realized as discrete subquandles of the circle S1S^{1} (see Figure 1). Note that RnR_{n} is non-trivial if n>2n>2. Hence, for any integer n>2n>2, it follows from Theorem 4.1 that

χQdle(Rn)=χTop(S1)=0.\chi^{\mathrm{Qdle}}(R_{n})=\chi^{\mathrm{Top}}(S^{1})=0.
Refer to caption
Figure 1: The dihedral quandle R5R_{5} realized as a discrete subquandle of S1S^{1}.

4.2 The core quandles

In this subsection, we consider the core quandles. For a group GG, the core quandle Core(G)\mathrm{Core}(G) is a quandle (G,s)(G,s), where the map s:GMap(G,G)s:G\to\mathrm{Map}(G,G) is defined by sh(g)=hg1hs_{h}(g)=hg^{-1}h for g,hGg,h\in G. In particular, each point symmetry is an involution. Note that the core quandle Core(G)\mathrm{Core}(G) is trivial if and only if the order of any element in GG is less than or equal to 22; in other words, the group GG is isomorphic to a direct product of some copies of /2\mathbb{Z}/2\mathbb{Z}. Recall that any Lie group has a symmetric space structure given by the core quandle structure. The next theorem is an analogy of the fact that the Euler characteristic of a non-trivial compact connected Lie group is 0.

Theorem 4.3.

The quandle Euler characteristic of a non-trivial core quandle is equal to 0.

Proof.

Let GG be a group. If GG is abelian, the quandle Core(G)\mathrm{Core}(G) is isomorphic to the Alexander quandle GAlex(G,σ)\mathrm{GAlex}(G,\sigma), where the group automorphism σ:GG\sigma:G\to G is given by σ(g)=g1\sigma(g)=g^{-1} for gGg\in G. Since the quandle is non-trivial, the quandle Euler characteristic is equal to 0 by Theorem 4.1.

Let us assume that GG is not abelian. Then, there exist g,hGg,h\in G such that [g,h]:=ghg1h11[g,h]:=ghg^{-1}h^{-1}\neq 1, where 11 denotes the identity element. Consider the elements g1:=sg1h1s11,g2:=shsg11Dis(Core(G))g_{1}:=s_{g^{-1}h^{-1}}\circ s_{1}^{-1},g_{2}:=s_{h}\circ s_{g^{-1}}^{-1}\in\mathrm{Dis}(\mathrm{Core}(G)). For any xCore(G)x\in\mathrm{Core}(G), we have

g1(x)=sg1h1s11(x)=sg1h1(x1)=g1h1xg1h1,\displaystyle g_{1}(x)=s_{g^{-1}h^{-1}}\circ s_{1}^{-1}(x)=s_{g^{-1}h^{-1}}(x^{-1})=g^{-1}h^{-1}xg^{-1}h^{-1},
g2(x)=shsg11(x)=sh(g1x1g1)=hgxgh.\displaystyle g_{2}(x)=s_{h}\circ s_{g^{-1}}^{-1}(x)=s_{h}(g^{-1}x^{-1}g^{-1})=hgxgh.

Hence, the map φ:=g1g2Dis(X)\varphi:=g_{1}\circ g_{2}\in\mathrm{Dis}(X) satisfies

φ(x)=g1g2(x)=g1(hgxgh)=g1h1(hgxgh)g1h1=x[g,h].\displaystyle\varphi(x)=g_{1}\circ g_{2}(x)=g_{1}(hgxgh)=g^{-1}h^{-1}(hgxgh)g^{-1}h^{-1}=x[g,h].

Since [g,h]1[g,h]\neq 1, we have φ(x)x\varphi(x)\neq x. Therefore, the map φ\varphi has no fixed points, which completes the proof. ∎

4.3 Discrete spheres

In this subsection, we determine the Euler characteristics of discrete spheres, which are defined as particular finite subquandles in spheres. Recall that the nn-dimensional unit sphere SnS^{n} is a Riemannian symmetric space. See Example 2.6.

Definition 4.4.

Let {ei}\{e_{i}\} be the standard basis of n+1\mathbb{R}^{n+1}. Then the subset DSn:={±e1,,±en+1}DS^{n}:=\{\pm e_{1},\dots,\pm e_{n+1}\} is called the discrete nn-sphere.

As in [1, Example 2.4], it is easy to show that DSnDS^{n} is a subquandle in SnS^{n}. In fact, the point symmetries satisfy

sei=sei,sei(±ei)=±ei,sei(±ej)=ej(for ij).\displaystyle s_{e_{i}}=s_{-e_{i}},\qquad s_{e_{i}}(\pm e_{i})=\pm e_{i},\qquad s_{e_{i}}(\pm e_{j})=\mp e_{j}\quad(\text{for }i\neq j).

Note that these maps are the restrictions of some orthogonal transformations of n+1\mathbb{R}^{n+1}. Hence, we obtain an injective orthogonal representation ρ:Inn(DSn)O(n+1)\rho:\mathrm{Inn}(DS^{n})\to O(n+1) given by

ρ(sei)=diag(ε1,,εn+1),εj={1if i=j,1if ij,\rho(s_{e_{i}})=\mathrm{diag}(\varepsilon_{1},\dots,\varepsilon_{n+1}),\quad\varepsilon_{j}=\begin{cases*}1&if $i=j$,\\ -1&if $i\neq j$,\end{cases*}

where diag(ε1,,εn+1)\mathrm{diag}(\varepsilon_{1},\dots,\varepsilon_{n+1}) denotes the diagonal matrix whose (i,i)(i,i)-entry is εi\varepsilon_{i}.

Lemma 4.5.

The image ρ(Dis(DSn))\rho(\mathrm{Dis}(DS^{n})) satisfies

ρ(Dis(DSn))={A=diag(ε1,,εn+1)εi{±1},det(A)=1}.\rho(\mathrm{Dis}(DS^{n}))=\{A=\mathrm{diag}(\varepsilon_{1},\dots,\varepsilon_{n+1})\mid\varepsilon_{i}\in\{\pm 1\},\det(A)=1\}. (1)
Proof.

In this case, it is easy to see that

ρ(Inn(DSn)){diag(ε1,,εn+1)O(n+1)εi{±1}}.\displaystyle\rho(\mathrm{Inn}(DS^{n}))\subset\left\{\mathrm{diag}(\varepsilon_{1},\dots,\varepsilon_{n+1})\in O(n+1)\mid\varepsilon_{i}\in\{\pm 1\}\right\}.

Recall that S={seisej1}S=\{s_{e_{i}}\circ s_{e_{j}}^{-1}\} is a generating set of Dis(DSn)\mathrm{Dis}(DS^{n}). For iji\neq j, one can obtain the matrix expression

ρ(seisej1)=diag(ε1,,εn+1),where εk={1k{i,j},1k{i,j}.\rho(s_{e_{i}}\circ s_{e_{j}}^{-1})=\mathrm{diag}(\varepsilon_{1},\dots,\varepsilon_{n+1}),\qquad\text{where }\varepsilon_{k}=\begin{cases*}1&$k\not\in\{i,j\}$,\\ -1&$k\in\{i,j\}$.\end{cases*}

Hence, the determinant of any element in ρ(S)\rho(S) is equal to 11. Since ρ(Dis(DSn))\rho(\mathrm{Dis}(DS^{n})) is generated by ρ(S)\rho(S), this shows the inclusion ()(\subset) in the assertion. In order to prove the inverse inclusion, let us take B=diag(ε1,,εn+1)B=\mathrm{diag}(\varepsilon_{1},\dots,\varepsilon_{n+1}) in the right-hand side of the assertion. Then the number of indices ii with εi=1\varepsilon_{i}=1 is even. Therefore the matrix BB can be written as a product of elements in ρ(S)\rho(S). This completes the proof. ∎

In the following, we identify Inn(DSn)\mathrm{Inn}(DS^{n}) with ρ(Inn(DSn))\rho(\mathrm{Inn}(DS^{n})), and also Dis(DSn)\mathrm{Dis}(DS^{n}) with ρ(Dis(DSn))\rho(\mathrm{Dis}(DS^{n})). The next theorem determines the quandle Euler characteristics of the discrete spheres.

Theorem 4.6.

For any positive integer nn, it satisfies χQdle(DSn)=χTop(Sn)\chi^{\mathrm{Qdle}}(DS^{n})=\chi^{\mathrm{Top}}(S^{n}), that is,

χQdle(DSn)={0if n is odd,2if n is even.\chi^{\mathrm{Qdle}}(DS^{n})=\begin{cases*}0&if $n$ is odd,\\ 2&if $n$ is even.\end{cases*}
Proof.

Suppose that nn is odd. Then the displacement group Dis(DSn)\mathrm{Dis}(DS^{n}) contains the identity matrix In+1-I_{n+1}. The matrix In+1-I_{n+1} has no fixed points in DSnDS^{n}. Therefore we have χQdle(DSn)=0\chi^{\mathrm{Qdle}}(DS^{n})=0.

Suppose that nn is even. Then we have

A0=(100In)Dis(DSn).A_{0}=\left(\begin{matrix}1&0\\ 0&-I_{n}\end{matrix}\right)\in\mathrm{Dis}(DS^{n}).

It is clear that A0A_{0} fixes two elements ±e1\pm e_{1} in DSnDS^{n}, which shows χQdle(DSn)2\chi^{\mathrm{Qdle}}(DS^{n})\leq 2. Recall that any element gDis(DSn)g\in\mathrm{Dis}(DS^{n}) can be expressed as

g=diag(ε1,,εn+1),\displaystyle g=\mathrm{diag}(\varepsilon_{1},\dots,\varepsilon_{n+1}),

where εi{±1}\varepsilon_{i}\in\{\pm 1\} and det(g)=1\det(g)=1. Since n+1n+1 is odd and hence #{iεi=1}\#\{i\mid\varepsilon_{i}=1\} is odd, we have #{iεi=1}1\#\{i\mid\varepsilon_{i}=1\}\geq 1. Therefore, gg has at least two fixed points in DSnDS^{n}. This shows χQdle(DSn)2\chi^{\mathrm{Qdle}}(DS^{n})\geq 2, which completes the proof. ∎

4.4 Quandles obtained from weighted graphs

In this subsection, we study the quandle Euler characteristics of the quandles obtained from weighted graphs, as introduced in [10]. See also [1].

Proposition 4.7 ([10]).

Let AA be an abelian group, VV a finite set and d:V×VAd:V\times V\to A a map with d(v,v)=0d(v,v)=0 for all vVv\in V. Then the following map s:V×AMap(V×A)s:V\times A\to\mathrm{Map}(V\times A) is a quandle structure on V×AV\times A:

s(v,a)(w,b)=(w,d(v,w)+b).s_{(v,a)}(w,b)=(w,d(v,w)+b).

The constructed quandle is called the quandle obtained from (V,A,d)(V,A,d), and denoted by V×dAV\times_{d}A. Note that (V,A,d)(V,A,d) is called an AA-weighted graph, whose edges are weighted by elements in AA. More precisely, (V,A,d)(V,A,d) is an oriented graph with the vertex set VV, the edge set E={(v,w)v,wV,d(v,w)0}E=\{(v,w)\mid v,w\in V,d(v,w)\neq 0\}, and the weight of the edge (v,w)E(v,w)\in E is given by d(v,w)d(v,w). We express a weighted-edge (v,w)E(v,w)\in E by an arrow from vv to ww that is labeled by d(v,w)d(v,w).

Let us denote an nn-point set by V=Vn={v1,,vn}V=V_{n}=\{v_{1},\dots,v_{n}\} for a positive integer nn. For an AA-weighted graph (V,A,d)(V,A,d), let us define the adjacency matrix DD with respect to (V,A,d)(V,A,d) by D:=(d(vi,vj))i,j{1,,n}D:=(d(v_{i},v_{j}))_{i,j\in\{1,\dots,n\}}, and denote the ii-th row vector of DD by did_{i}.

Remark 4.8.

For any a,bAa,b\in A and any vVnv\in V_{n}, the point symmetries satisfy s(v,a)=s(v,b)s_{(v,a)}=s_{(v,b)}. In the following, we denote the point symmetry at (v,a)Vn×dA(v,a)\in V_{n}\times_{d}A by svs_{v}. Note that svis_{v_{i}} is described by did_{i}, which is the ii-th row vector of the adjacency matrix DD. Hence, svi=svjs_{v_{i}}=s_{v_{j}} as inner automorphisms of Vn×dAV_{n}\times_{d}A if and only if di=djd_{i}=d_{j}. We can regard Inn(Vn×dA)\mathrm{Inn}(V_{n}\times_{d}A) as a subgroup of AnA^{n} by the map ι:Inn(Vn×dA)An\iota:\mathrm{Inn}(V_{n}\times_{d}A)\to A^{n} defined by ι(svi)=di\iota(s_{v_{i}})=d_{i}. In the following we identify Inn(Vn×dA)\mathrm{Inn}(V_{n}\times_{d}A) with its image of ι\iota.

Remark 4.9.

It was proved in [10] that the inner automorphism group Inn(V×dA)\mathrm{Inn}(V\times_{d}A) is abelian, and every finite homogeneous quandle with abelian inner automorphism group can be constructed in this way. An AA-weighted graph (V,A,d)(V,A,d) is said to be homogeneous if there exists a graph isomorphism f:(V,E)(V,E)f:(V,E)\to(V,E) such that d(f(v),f(w))=d(v,w)d(f(v),f(w))=d(v,w) for any v,wVv,w\in V. If an AA-weighted graph (V,A,d)(V,A,d) is homogeneous, then Vn×dAV_{n}\times_{d}A is a homogeneous quandle [10, Theorem A].

Example 4.10.

The discrete sphere DSnDS^{n} is isomorphic to the quandle Vn+1×d(/2)V_{n+1}\times_{d}(\mathbb{Z}/2\mathbb{Z}), where the map d:Vn+1×Vn+1(/2)d:V_{n+1}\times V_{n+1}\to(\mathbb{Z}/2\mathbb{Z}) is defined by

d(v,w)={1if vw,0if v=w.d(v,w)=\begin{cases*}1&if $v\neq w$,\\ 0&if $v=w$.\end{cases*}

The corresponding AA-weighted graph is a perfect graph with n+1n+1 vertexes, all of whose edges are weighted by 1/21\in\mathbb{Z}/2\mathbb{Z}. In the case n=3n=3, the corresponding AA-weighted graph is described in Figure 2, and the corresponding adjacency matrix DD is

D=(0111101111011110).D=\begin{pmatrix}0&1&1&1\\ 1&0&1&1\\ 1&1&0&1\\ 1&1&1&0\\ \end{pmatrix}.
Refer to caption
Figure 2: The AA-weighted graph corresponding to the discrete sphere DS3DS^{3}

The next proposition is useful for calculating the displacement group and the quandle Euler characteristic of the quandle V×dAV\times_{d}A.

Proposition 4.11.

Let Vn×dAV_{n}\times_{d}A be the quandle obtained from an AA-weighted graph (V,A,d)(V,A,d), and did_{i} be the ii-th row vector of the adjacency matrix DD. Then we have the following:

(1)(1)

Dis(Vn×dA)={i=0n1ki(didi+1)Anki}\mathrm{Dis}(V_{n}\times_{d}A)=\left\{\sum_{i=0}^{n-1}k_{i}(d_{i}-d_{i+1})\in A^{n}\mid k_{i}\in\mathbb{Z}\right\},

(2)(2)

χQdle(Vn×dA)=#Ainf{#{iai=0}(a1,,an)Dis(Vn×dA)}\chi^{\mathrm{Qdle}}(V_{n}\times_{d}A)=\#A\cdot\inf\left\{\#\{i\mid a_{i}=0\}\mid(a_{1},\dots,a_{n})\in\mathrm{Dis}(V_{n}\times_{d}A)\right\}.

Proof.

We show (1)(1). Recall that the displacement group G:=Dis(Vn×dA)G:=\mathrm{Dis}(V_{n}\times_{d}A) is generated by

{svisvj1vi,vjVn}={didji,j{1,n}}.\{s_{v_{i}}\circ s_{v_{j}}^{-1}\mid v_{i},v_{j}\in V_{n}\}=\{d_{i}-d_{j}\mid i,j\in\{1,\dots n\}\}.

Since (didj)=(djdi)(d_{i}-d_{j})=-(d_{j}-d_{i}) for any i,ji,j, and didj=k=ij(dkdk+1)d_{i}-d_{j}=\sum_{k=i}^{j}(d_{k}-d_{k+1}) for j>ij>i, we can replace the generating set to {didi+1i{1,,n1}}\{d_{i}-d_{i+1}\mid i\in\{1,\dots,n-1\}\}. Therefore we obtain the assertion.

We show (2)(2). An element a=(a1,,an)Dis(Vn×dA)a=(a_{1},\dots,a_{n})\in\mathrm{Dis}(V_{n}\times_{d}A) acts on Vn×dAV_{n}\times_{d}A by a(vi,b)=(vi,b+ai)a\cdot(v_{i},b)=(v_{i},b+a_{i}). Hence the element (vi,b)Vn×dA(v_{i},b)\in V_{n}\times_{d}A is fixed by aa if and only if ai=0a_{i}=0. Note that if there exists an element (vi,b0)Vn×dA(v_{i},b_{0})\in V_{n}\times_{d}A fixed by aa, then for any bAb\in A, every element (vi,b)Vn×dA(v_{i},b)\in V_{n}\times_{d}A is fixed by aa. Hence the number #A#{iai=0}\#A\cdot\#\{i\mid a_{i}=0\} is equal to the number of elements fixed by aa. This completes the proof. ∎

Now we calculate quandle Euler characteristics of a concrete example of (V,A,d)(V,A,d). This example will be used to construct a quandle satisfying particular inequality (see Theorem 5.6 and Example 5.7).

Proposition 4.12.

Let nn be a positive integer with n>1n>1, and consider Vn={v1,,vn}V_{n}=\{v_{1},\dots,v_{n}\}. Let us define a map d:Vn×Vn/2d:V_{n}\times V_{n}\to\mathbb{Z}/2\mathbb{Z} by

d(vi,vj)={1if ij=1 in /n,0otherwise.d(v_{i},v_{j})=\begin{cases*}1&if $i-j=1$ in $\mathbb{Z}/n\mathbb{Z}$,\\ 0&otherwise.\end{cases*}

Then Cn:=V×d(/2)C_{n}:=V\times_{d}(\mathbb{Z}/2\mathbb{Z}) is a non-trivial homogeneous quandle and the quandle Euler characteristic is given by

χQdle(Cn)={2if n is odd,0if n is even.\chi^{\mathrm{Qdle}}(C_{n})=\begin{cases*}2&if $n$ is odd,\\ 0&if $n$ is even.\end{cases*}
Refer to caption
Figure 3: The AA-weighted graph corresponding to the quandle C3C_{3}.
Proof.

Since d0d\neq 0 and the weighted graph (Vn,/2,d)(V_{n},\mathbb{Z}/2\mathbb{Z},d) is homogeneous, the quandle CnC_{n} is non-trivial and homogeneous. In this case, the ii-th row vector of the adjacency matrix is given by

di=ei1T,d_{i}=e_{i-1}^{T},

where T denotes the transpose. By Proposition 4.11 (1)(1), we have

Dis(Cn)={(a1,,an)(/2)nak/2,k=1nak=0}.\mathrm{Dis}(C_{n})=\left\{(a_{1},\dots,a_{n})\in(\mathbb{Z}/2\mathbb{Z})^{n}\mid a_{k}\in\mathbb{Z}/2\mathbb{Z},\,\textstyle{\sum_{k=1}^{n}}a_{k}=0\right\}.

If nn is even, then (1,,1)Dis(Cn)(1,\dots,1)\in\mathrm{Dis}(C_{n}) has no fixed points, and hence the quandle Euler characteristic is equal to 0. If nn is odd, then (1,,1,0)Dis(Cn)(1,\dots,1,0)\in\mathrm{Dis}(C_{n}) and any element in Dis(Cn)\mathrm{Dis}(C_{n}) has at least one entry that is 0. Hence the Euler characteristic is equal to #(/2)=2\#(\mathbb{Z}/2\mathbb{Z})=2 by Proposition 4.11 (2)(2). This completes the proof. ∎

The next proposition shows that, given positive integer n>1n>1, there exists a non-trivial quandle whose Euler characteristic is equal to nn.

Proposition 4.13.

Let n>1n>1 be a positive integer, and consider V2={v1,v2}V_{2}=\{v_{1},v_{2}\}. Let us define a map d:V2×V2/nd:V_{2}\times V_{2}\to\mathbb{Z}/n\mathbb{Z} by

d(vi,vj)={1if (i,j)=(1,2),0otherwise.d(v_{i},v_{j})=\begin{cases*}1&if $(i,j)=(1,2)$,\\ 0&otherwise.\end{cases*}

Then Bn:=V×d/nB_{n}:=V\times_{d}\mathbb{Z}/n\mathbb{Z} is a non-trivial quandle and the quandle Euler characteristic is given by

χQdle(Bn)=n.\chi^{\mathrm{Qdle}}(B_{n})=n.
Refer to caption
Figure 4: The AA-weighted graph corresponding to the quandle BnB_{n}.
Proof.

Since dd is not the zero-map, BnB_{n} is non-trivial. In this case, the displacement group satisfies

Dis(Bn)={(0,k)(/n)2k/n}\mathrm{Dis}(B_{n})=\left\{(0,k)\in(\mathbb{Z}/n\mathbb{Z})^{2}\mid k\in\mathbb{Z}/n\mathbb{Z}\right\}

by Proposition 4.11. Since the first entry of any element in WW is 0, the Euler characteristic of BnB_{n} is equal to #(/n)=n\#(\mathbb{Z}/n\mathbb{Z})=n. This completes the proof. ∎

5 Properties of the quandle Euler characteristics

In this section, we prove several properties of the quandle Euler characteristics. These properties can be regarded as analogous to certain properties of topological Euler characteristics.

5.1 The direct product of quandles

Recall that the Euler characteristic of a product of CW complexes is equal to the direct product of the Euler characteristics of the individual components. In this subsection, we show that the same equality holds for the quandle Euler characteristic of the product of quandles.

For quandles (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}), we can define a quandle structure ss on the direct product X1×X2X_{1}\times X_{2} by setting s(x1,x2):=sx11×sx22s_{(x_{1},x_{2})}:=s^{1}_{x_{1}}\times s^{2}_{x_{2}}, that is

s(x1,x2)(y1,y2)=(sx11(y1),sx22(y2)).s_{(x_{1},x_{2})}(y_{1},y_{2})=(s^{1}_{x_{1}}(y_{1}),s^{2}_{x_{2}}(y_{2})).

The quandle (X1×X2,s)(X_{1}\times X_{2},s) is called the direct product of quandles (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}), and for simplicity, we denote it as X1×X2X_{1}\times X_{2}.

Lemma 5.1.

Let (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}) be quandles. Then

(1)(1)

the group homomorphism f:Inn(X1×X2)Inn(X1)×Inn(X2)f:\mathrm{Inn}(X_{1}\times X_{2})\to\mathrm{Inn}(X_{1})\times\mathrm{Inn}(X_{2}) defined by f(s(x1,x2))=(sx11,sx22)f(s_{(x_{1},x_{2})})=(s^{1}_{x_{1}},s^{2}_{x_{2}}) is injective,

(2)(2)

f(Dis(X1×X2))=Dis(X1)×Dis(X2)f(\mathrm{Dis}(X_{1}\times X_{2}))=\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2}).

Proof.

We show (1)(1), that is ker(f)={1}\ker(f)=\{1\}. Let us take gker(f)g\in\ker(f). Then there exist x1,,xnX1×X2x_{1},\dots,x_{n}\in X_{1}\times X_{2} and εi{±1}\varepsilon_{i}\in\{\pm 1\} such that g=sx1ε1sxnεng=s_{x_{1}}^{\varepsilon_{1}}\circ\cdots\circ s_{x_{n}}^{\varepsilon_{n}}. Here, it follows sxi=sxi1×sxi2s_{x_{i}}=s_{x_{i}^{1}}\times s_{x_{i}^{2}} for each xi=(xi1,xi2)X1×X2x_{i}=(x_{i}^{1},x_{i}^{2})\in X_{1}\times X_{2} by the definition of the point symmetries of the product quandle. By the definition of ff, one has

f(g)=((sx111)ε1(sxn11)εn,(sx122)ε1(sxn22)εn)=:(g1,g2)Inn(X1)×Inn(X2).f(g)=((s^{1}_{x_{1}^{1}})^{\varepsilon_{1}}\circ\cdots\circ(s^{1}_{x_{n}^{1}})^{\varepsilon_{n}},(s^{2}_{x_{1}^{2}})^{\varepsilon_{1}}\circ\cdots\circ(s^{2}_{x_{n}^{2}})^{\varepsilon_{n}})=:(g_{1},g_{2})\in\mathrm{Inn}(X_{1})\times\mathrm{Inn}(X_{2}).

Since gker(f)g\in\ker(f), we have gig_{i} is trivial for i{1,2}i\in\{1,2\}. On the other hand, it satisfies

g1×g2\displaystyle g_{1}\times g_{2} =((sx111)ε1(sxn11)εn)×((sx122)ε1(sxn22)εn)\displaystyle=\left((s^{1}_{x_{1}^{1}})^{\varepsilon_{1}}\circ\cdots\circ(s^{1}_{x_{n}^{1}})^{\varepsilon_{n}}\right)\times\left((s^{2}_{x_{1}^{2}})^{\varepsilon_{1}}\circ\cdots\circ(s^{2}_{x_{n}^{2}})^{\varepsilon_{n}}\right)
=((sx111)ε1×(sx122)ε1)((sxn11)εn×(sxn22)εn)\displaystyle=\left((s^{1}_{x_{1}^{1}})^{\varepsilon_{1}}\times(s^{2}_{x_{1}^{2}})^{\varepsilon_{1}}\right)\circ\cdots\circ\left((s^{1}_{x_{n}^{1}})^{\varepsilon_{n}}\times(s^{2}_{x_{n}^{2}})^{\varepsilon_{n}}\right)
=sx1ε1sxnεn=g.\displaystyle=s_{x_{1}}^{\varepsilon_{1}}\circ\cdots\circ s_{x_{n}}^{\varepsilon_{n}}=g.

This yields that g=1g=1. Therefore the homomorphism ff is injective as desired.

We show (2)(2). First, we demonstrate that f(Dis(X1×X2))Dis(X1)×Dis(X2)f(\mathrm{Dis}(X_{1}\times X_{2}))\subset\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2}). The left-hand side is generated by

D={(sx11(sy11)1,sx22(sy22)1)(x1,x2),(y1,y2)X1×X2}.D=\{(s^{1}_{x_{1}}\circ(s^{1}_{y_{1}})^{-1},s^{2}_{x_{2}}\circ(s^{2}_{y_{2}})^{-1})\mid(x_{1},x_{2}),(y_{1},y_{2})\in X_{1}\times X_{2}\}.

Since sxki(syki)1Dis(Xi)s_{x_{k}}^{i}\circ(s_{y_{k}}^{i})^{-1}\in\mathrm{Dis}(X_{i}), the right-hand side contains DD, which shows ()(\subset). Next, we prove the converse inclusion ()(\supset). The right-hand side Dis(X1)×Dis(X2)\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2}) is generated by

D={(sx11(sy11)1,1)x1,y1X1}{(1,sx22(sy22)1)x2,y2X2}.D^{\prime}=\{(s^{1}_{x_{1}}\circ(s^{1}_{y_{1}})^{-1},1)\mid x_{1},y_{1}\in X_{1}\}\cup\{(1,s^{2}_{x_{2}}\circ(s^{2}_{y_{2}})^{-1})\mid x_{2},y_{2}\in X_{2}\}.

The left-hand side contains DD^{\prime}. In fact, we have

(sx11,sx22)(sy11,sx22)1\displaystyle(s^{1}_{x_{1}},s^{2}_{x_{2}})\cdot(s^{1}_{y_{1}},s^{2}_{x_{2}})^{-1} =(sx11(sy11)1,1),\displaystyle=(s^{1}_{x_{1}}\circ(s^{1}_{y_{1}})^{-1},1),
(sx11,sx22)(sx11,sy22)1\displaystyle(s^{1}_{x_{1}},s^{2}_{x_{2}})\cdot(s^{1}_{x_{1}},s^{2}_{y_{2}})^{-1} =(1,sx22(sy22)1).\displaystyle=(1,s^{2}_{x_{2}}\circ(s^{2}_{y_{2}})^{-1}).

Since both belong to the left-hand side, it follows ()(\supset), which completes the proof. ∎

By this lemma, the displacement group of the direct product quandle is isomorphic to the product group of the displacement groups of the individual components. Using this property, we obtain the following result.

Theorem 5.2.

The quandle Euler characteristic of the direct product of quandles (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}) satisfies χQdle(X1×X2)=χQdle(X1)χQdle(X2)\chi^{\mathrm{Qdle}}(X_{1}\times X_{2})=\chi^{\mathrm{Qdle}}(X_{1})\cdot\chi^{\mathrm{Qdle}}(X_{2}).

Proof.

We identify the group Dis(X1×X2)\mathrm{Dis}(X_{1}\times X_{2}) with Dis(X1)×Dis(X2)\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2}) by Lemma 5.1. Hence any element gDis(X1)g\in\mathrm{Dis}(X_{1}) can be written as g=(g1,g2)g=(g_{1},g_{2}) with g1Dis(X1)g_{1}\in\mathrm{Dis}(X_{1}) and g2Dis(X2)g_{2}\in\mathrm{Dis}(X_{2}). Since the action is given by (g1,g2).(x1,x2)=(g1(x1),g2(x2))(g_{1},g_{2}).(x_{1},x_{2})=(g_{1}(x_{1}),g_{2}(x_{2})), it follows that the set of fixed points satisfies

Fix((g1,g2),X1×X2)=Fix(g1,X1)×Fix(g2,X2).\mathrm{Fix}((g_{1},g_{2}),X_{1}\times X_{2})=\mathrm{Fix}(g_{1},X_{1})\times\mathrm{Fix}(g_{2},X_{2}).

Therefore, (g1,g2)(g_{1},g_{2}) attains the infimum of #Fix((g1,g2),X1×X2)\#\mathrm{Fix}((g_{1},g_{2}),X_{1}\times X_{2}) if and only if both of g1g_{1} and g2g_{2} attain the infimums of #Fix(g1,X1)\#\mathrm{Fix}(g_{1},X_{1}) and #Fix(g2,X2)\#\mathrm{Fix}(g_{2},X_{2}), respectively. This completes the proof of the desired equality. ∎

As an application of Theorem 5.2, one can calculate the quandle Euler characteristics of the discrete tori. As seen in Example 4.2, the dihedral quandles can be regarded as discrete subquandles of the circle S1S^{1}. Thus, we define the discrete tori as follows:

Definition 5.3.

For a positive integer nn and an integer vector u=(m1,,mn)(>0)nu=(m_{1},\dots,m_{n})\in(\mathbb{Z}_{>0})^{n}, the discrete torus DTunDT^{n}_{u} is defined by

DTun:=k=1nRmk.DT^{n}_{u}:=\prod_{k=1}^{n}R_{m_{k}}.

According to the classification given in [4], a flat connected finite quandle is a discrete torus. Recall that a compact connected flat Riemannian symmetric space is just a flat torus Tn=(S1)nT^{n}=(S^{1})^{n}, and its topological Euler characteristic is equal to 0. The Euler characteristic of a discrete torus has the same property:

Corollary 5.4.

For any positive integer nn and any u=(m1,,mn)(>0)nu=(m_{1},\dots,m_{n})\in(\mathbb{Z}_{>0})^{n} with mi>2m_{i}>2, the quandle Euler characteristics of the discrete torus DTunDT^{n}_{u} satisfies χQdle(DTun)=χTop(Tn)=0\chi^{\mathrm{Qdle}}(DT^{n}_{u})=\chi^{\mathrm{Top}}(T^{n})=0.

Proof.

Since mk>2m_{k}>2, any component RmkR_{m_{k}} is non-trivial. As seen in Example 4.2, the quandle Euler characteristics of RmkR_{m_{k}} is equal to 0. By applying Theorem 5.2, we have the quandle Euler characteristics of discrete torus is equal to 0, which completes of proof. ∎

5.2 The interaction-free union of quandles

Recall that the Euler characteristic of a disjoint union of topological spaces is equal to the sum of the Euler characteristics of the individual components. In this subsection, we provide a comparable inequality for the Euler characteristics of the interaction-free union of quandles.

For two quandles (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}), we can define a quandle structure ss on the disjoint union X1X2X_{1}\sqcup X_{2} by setting

sx(y)={yif {x,y}X0,X1,sxi(y)if {x,y}Xi.s_{x}(y)=\begin{cases*}y&if $\{x,y\}\not\subset X_{0},X_{1}$,\\ s_{x}^{i}(y)&if $\{x,y\}\subset X_{i}$.\end{cases*}

The quandle (X1X2,s)(X_{1}\sqcup X_{2},s) is called the interaction-free union of quandles (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}), and for simplicity, we denote it by X1freeX2X_{1}\sqcup^{\mathrm{free}}X_{2}. Note that the natural inclusion map ιi:XiX1freeX2\iota_{i}:X_{i}\to X_{1}\sqcup^{\mathrm{free}}X_{2} is an injective quandle homomorphism and induces a group homomorphism ιi:Inn(Xi)Inn(X1freeX2)\iota_{i}:\mathrm{Inn}(X_{i})\to\mathrm{Inn}(X_{1}\sqcup^{\mathrm{free}}X_{2}).

Lemma 5.5.

Let (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}) be quandles. Let us define the map ι:Inn(X1)×Inn(X2)Inn(X1freeX2)\iota:\mathrm{Inn}(X_{1})\times\mathrm{Inn}(X_{2})\to\mathrm{Inn}(X_{1}\sqcup^{\mathrm{free}}X_{2}) by ι(g1,g2)=ι1(g1)ι2(g2)\iota(g_{1},g_{2})=\iota_{1}(g_{1})\iota_{2}(g_{2}). Then,

  1. (1)(1)

    the map ι:Inn(X1)×Inn(X2)Inn(X1freeX2)\iota:\mathrm{Inn}(X_{1})\times\mathrm{Inn}(X_{2})\to\mathrm{Inn}(X_{1}\sqcup^{\mathrm{free}}X_{2}) is a group isomorphism,

  2. (2)(2)

    ι(Dis(X1)×Dis(X2))Dis(X1freeX2)\iota(\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2}))\subset\mathrm{Dis}(X_{1}\sqcup^{\mathrm{free}}X_{2}).

Proof.

We show (1)(1), that is, ι\iota is a group homomorphism and is a bijection. First, we show that ι\iota is a group homomorphism. For x1X1x_{1}\in X_{1} and x2X2x_{2}\in X_{2}, the maps sx1s_{x_{1}} and sx2s_{x_{2}} are commutative in Inn(X1freeX2)\mathrm{Inn}(X_{1}\sqcup^{\mathrm{free}}X_{2}) by the definition of the interaction-free union. Thus, an element in ι1(X1)\iota_{1}(X_{1}) and an element in ι2(X2)\iota_{2}(X_{2}) are commutative. Hence for (g1,g2),(h1,h2)Inn(X1)×Inn(X2)(g_{1},g_{2}),(h_{1},h_{2})\in\mathrm{Inn}(X_{1})\times\mathrm{Inn}(X_{2}), we have

ι((g1,g2)(h1,h2))\displaystyle\iota((g_{1},g_{2})(h_{1},h_{2})) =ι(g1h1,g2h2)\displaystyle=\iota(g_{1}h_{1},g_{2}h_{2})
=ι1(g1h1)ι2(g2h2)\displaystyle=\iota_{1}(g_{1}h_{1})\iota_{2}(g_{2}h_{2})
=ι1(g1)ι1(h1)ι2(g2)ι2(h2)\displaystyle=\iota_{1}(g_{1})\iota_{1}(h_{1})\iota_{2}(g_{2})\iota_{2}(h_{2})
=ι1(g1)ι2(g2)ι1(h1)ι2(h2)\displaystyle=\iota_{1}(g_{1})\iota_{2}(g_{2})\iota_{1}(h_{1})\iota_{2}(h_{2})
=ι(g1,g2)ι(h1,h2).\displaystyle=\iota(g_{1},g_{2})\iota(h_{1},h_{2}).

Therefore the map ι\iota is a group homomorphism. Next, we show that ι\iota is surjective. To prove this, let us consider

S:={(sx11,1)x1X1}{(1,sx22)x2X2},S:=\{(s^{1}_{x_{1}},1)\mid x_{1}\in X_{1}\}\sqcup\{(1,s^{2}_{x_{2}})\mid x_{2}\in X_{2}\},

which is a generating set of Inn(X1)×Inn(X2)\mathrm{Inn}(X_{1})\times\mathrm{Inn}(X_{2}). Note that ι(sx11,1)=sx1\iota(s_{x_{1}}^{1},1)=s_{x_{1}} and ι(1,sx22)=sx2\iota(1,s_{x_{2}}^{2})=s_{x_{2}}. Then the image ι(S)\iota(S) satisfies

ι(S)={sxInn(X1freeX2)xX1X2},\iota(S)=\{s_{x}\in\mathrm{Inn}(X_{1}\sqcup^{\mathrm{free}}X_{2})\mid x\in X_{1}\sqcup X_{2}\},

which is a generating set of Inn(X1freeX2)\mathrm{Inn}(X_{1}\sqcup^{\mathrm{free}}X_{2}). Thus, the group homomorphism ι\iota is surjective. Lastly, we show that ι\iota is injective, that is kerι={1}\ker\iota=\{1\}. Let us take (g1,g2)ker(ι)(g_{1},g_{2})\in\ker(\iota), where g1Inn(X1)g_{1}\in\mathrm{Inn}(X_{1}) and g2Inn(X2)g_{2}\in\mathrm{Inn}(X_{2}). Then the map ι(g1,g2)=ι1(g1)ι2(g2)\iota(g_{1},g_{2})=\iota_{1}(g_{1})\iota_{2}(g_{2}) acts trivially on X1freeX2X_{1}\sqcup^{\mathrm{free}}X_{2}. In particular, the element ι1(g1)=ι(g1,g2)ι2(g2)1\iota_{1}(g_{1})=\iota(g_{1},g_{2})\iota_{2}(g_{2})^{-1} acts trivially on X1X_{1}. Thus we conclude that g1g_{1} is trivial, and similarly we conclude that g2g_{2} is trivial. Therefore, we have (g1,g2)=(1,1)(g_{1},g_{2})=(1,1) as desired.

We show (2)(2). Let us consider

S:={(sx11(sy11)1,1)x1,y1X1}{(1,sx22(sy22)1)x2,y2X2},S^{\prime}:=\{(s^{1}_{x_{1}}\circ(s^{1}_{y_{1}})^{-1},1)\mid x_{1},y_{1}\in X_{1}\}\sqcup\{(1,s^{2}_{x_{2}}\circ(s^{2}_{y_{2}})^{-1})\mid x_{2},y_{2}\in X_{2}\},

which is a generating set of Dis(X1)×Dis(X2)\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2}). Then the image ι(S)\iota(S^{\prime}) is given by

ι(S)={sx1(sy1)1x1,y1X1}{sx2(sy2)1x2,y2X2},\iota(S^{\prime})=\{s_{x_{1}}\circ(s_{y_{1}})^{-1}\mid x_{1},y_{1}\in X_{1}\}\sqcup\{s_{x_{2}}\circ(s_{y_{2}})^{-1}\mid x_{2},y_{2}\in X_{2}\},

which is a subset of the group Dis(X1freeX2)\mathrm{Dis}(X_{1}\sqcup^{\mathrm{free}}X_{2}). Since the group ι(Dis(X1)×Dis(X2))\iota(\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2})) is generated by ι(S)\iota(S^{\prime}), we have (2)(2), which completes the proof. ∎

By this lemma, we can regard the product group of the displacement groups of the individual components as a subgroup of the displacement group of the interaction-free union quandle. Using this property, we obtain the following result.

Theorem 5.6.

Let (X1,s1)(X_{1},s^{1}) and (X2,s2)(X_{2},s^{2}) be quandles. Then, the quandle Euler characteristic of the interaction-free union X1freeX2X_{1}\sqcup^{\mathrm{free}}X_{2} satisfies

χQdle(X1freeX2)χQdle(X1)+χQdle(X2).\chi^{\mathrm{Qdle}}(X_{1}\sqcup^{\mathrm{free}}X_{2})\leq\chi^{\mathrm{Qdle}}(X_{1})+\chi^{\mathrm{Qdle}}(X_{2}).
Proof.

We regard Dis(X1)×Dis(X2)\mathrm{Dis}(X_{1})\times\mathrm{Dis}(X_{2}) as a subgroup of Dis(X1freeX2)\mathrm{Dis}(X_{1}\sqcup^{\mathrm{free}}X_{2}) by the map ι\iota in Lemma 5.5. For each i{1,2}i\in\{1,2\}, there exists giDis(Xi)g_{i}\in\mathrm{Dis}(X_{i}) such that

#Fix(gi,Xi)=χQdle(Xi).\#\mathrm{Fix}(g_{i},X_{i})=\chi^{\mathrm{Qdle}}(X_{i}).

Then g:=g1g2g:=g_{1}g_{2} is regarded as an element in Dis(X1freeX2)\mathrm{Dis}(X_{1}\sqcup^{\mathrm{free}}X_{2}). Since gig_{i} acts trivially on the other component, it follows that the set of fixed points satisfies

Fix(g,X1freeX2)=Fix(g1,X1)Fix(g2,X2).\mathrm{Fix}(g,X_{1}\sqcup^{\mathrm{free}}X_{2})=\mathrm{Fix}(g_{1},X_{1})\sqcup\mathrm{Fix}(g_{2},X_{2}).

This concludes that

χQdle(X1freeX2)#Fix(g,X1freeX2)=#Fix(g1,X1)+#Fix(g2,X2)=χQdle(X1)+χQdle(X2),\chi^{\mathrm{Qdle}}(X_{1}\sqcup^{\mathrm{free}}X_{2})\leq\#\mathrm{Fix}(g,X_{1}\sqcup^{\mathrm{free}}X_{2})=\#\mathrm{Fix}(g_{1},X_{1})+\#\mathrm{Fix}(g_{2},X_{2})=\chi^{\mathrm{Qdle}}(X_{1})+\chi^{\mathrm{Qdle}}(X_{2}),

which completes the proof. ∎

The following provides an example that does not satisfy the equality in Theorem 5.6. We will use a quandle obtained from a weighted graph. Note that this quandle is homogeneous, and therefore, the equality in Theorem 5.6 does not hold in general, even for homogeneous quandles.

Example 5.7.

Let C3C_{3} be the quandle in Proposition 4.12. Then we have

χQdle(C3freeC3)=0<4=χQdle(C3)+χQdle(C3).\chi^{\mathrm{Qdle}}(C_{3}\sqcup^{\mathrm{free}}C_{3})=0<4=\chi^{\mathrm{Qdle}}(C_{3})+\chi^{\mathrm{Qdle}}(C_{3}).
Proof.

Since we proved χQdle(C3)=2\chi^{\mathrm{Qdle}}(C_{3})=2 in Proposition 4.12, we have only to show that the Euler characteristic of C3freeC3C_{3}\sqcup^{\mathrm{free}}C_{3} is equal to 0. Recall that C3C_{3} is obtained from the /2\mathbb{Z}/2\mathbb{Z}-weighted graph in Figure 3. We have that C3freeC3C_{3}\sqcup^{\mathrm{free}}C_{3} coincides with the quandle obtained from the /2\mathbb{Z}/2\mathbb{Z}-weighted graph in Figure 5, which is the disjoint union of two copies of the graph of C3C_{3}. With respect to the labeling in Figure 5, the corresponding adjacency matrix DD is given by

D=(010000001000100000000010000001000100).D=\begin{pmatrix}0&1&0&0&0&0\\ 0&0&1&0&0&0\\ 1&0&0&0&0&0\\ 0&0&0&0&1&0\\ 0&0&0&0&0&1\\ 0&0&0&1&0&0\end{pmatrix}.

It follows from Proposition 4.11 that

(1,1,1,1,1,1)=(d1d2)+(d3d4)+(d5d6)Dis(C3freeC3).(1,1,1,1,1,1)=(d_{1}-d_{2})+(d_{3}-d_{4})+(d_{5}-d_{6})\in\mathrm{Dis}(C_{3}\sqcup^{\mathrm{free}}C_{3}).

Since this element has no fixed points, we have χQdle(C3freeC3)=0\chi^{\mathrm{Qdle}}(C_{3}\sqcup^{\mathrm{free}}C_{3})=0 by Proposition 4.11 (2)(2). ∎

Refer to caption
Figure 5: The AA-weighted graph corresponding to the quandle C3freeC3C_{3}\sqcup^{\mathrm{free}}C_{3}.

Acknowledgement

The authors would like to thank Hirotaka Akiyoshi, Katsunori Arai, Seiichi Kamada, Akira Kubo, Fumika Mizoguchi, Takayuki Okuda, Makoto Sakuma, and Yuta Taniguchi for helpful comments and useful discussions. The first author was supported by JST SPRING, Grant Number JPMJSP2139. The second author was supported by JSPS KAKENHI Grant Numbers JP22H01124 and JP24K21193. The authors were partly supported by MEXT Promotion of Distinctive Joint Research Center Program JPMXP00723833165.

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(R. Kai) Department of Mathematics, Graduate School of Science, Osaka Metropolitan University, 3-3-138, Sugimoto, Sumiyoshi-ku, Osaka, 558-8585, Japan

Email address: [email protected]


(H. Tamaru) Department of Mathematics, Graduate School of Science, Osaka Metropolitan University, 3-3-138, Sugimoto, Sumiyoshi-ku, Osaka, 558-8585, Japan

Email address: [email protected]