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Extending free group action on surfaces

Jesús Emilio Domínguez and Carlos Segovia Universidad Autonoma de Sinaloa, México. e-mail: jedguez@gmail.comInstituto de Matemáticas UNAM-Oaxaca, México. e-mail: csegovia@matem.unam.mx
Abstract

The present work introduces new perspectives in order to extend finite group actions from surfaces to 3-manifolds. We consider the Schur multiplier associated to a finite group GG in terms of principal GG-bordisms in dimension two, called GG-cobordisms. We are interested in the question of when a free action of a finite group on a closed oriented surface extends to a non-necessarily free action on a 3-manifold. We show the answer to this question is affirmative for abelian, dihedral, symmetric and alternating groups. As an application of our methods, we show that every non-necessarily free action of abelian groups (under certain conditions) and dihedral groups on a closed oriented surface extends to 33-dimensional handlebody.

Introduction

Let ΩnSO(G)\Omega_{n}^{SO}(G) be the free GG-bordism group in dimension nn from Conner-Floyd [CF64] and denote by Ωn+1SO,free(G)\Omega_{n+1}^{SO,\partial free}(G), the GG-bordism group of (n+1)(n+1)-dimensional manifolds with a non necessarily free GG-action which restricts to a free action over the boundary. We are interested in knowing what the image of the following map is

Ωn+1SO,free(G)ΩnSO(G).\Omega_{n+1}^{SO,\partial free}(G)\longrightarrow\Omega_{n}^{SO}(G)\,. (1)

For n=2n=2, the group Ω2SO(G)\Omega_{2}^{SO}(G) has been studied extensively with the name of the Schur multiplier [Kar87] (denoted by (G)\mathcal{M}(G)). When this group vanishes, the map (1) is surjective, such is the case for cyclic groups, groups of deficiency zero, see [Kar87]. For free actions of abelian groups and dihedral groups, the extension was given by Reni-Zimmermann [RZ96] and Hidalgo [Hid94]. Obstructions for the surjectivity of the map (1) are constructed by Samperton [Sam20], considering the quotient by the homology classes represented by tori.

Our approach considers the elements of the group Ω2SO(G)\Omega_{2}^{SO}(G) represented by what we call GG-cobordisms in dimension two. These are diffeomorphism classes of principal GG-bundles over (closed) surfaces [GS16]. We say that a GG-cobordism is extendable if it has a representative given by a principal GG-bundle over a surface SS, which is the boundary of a 33-dimensional manifold MM with an action of GG.

For GG a finite abelian group, we show that every GG-cobordism over a closed surface is extendable, see Theorem 9. For this, we decompose any GG-cobordism into small pieces given by GG-cobordisms over a closed surface of genus one, which are extendable, as we will see in Proposition 7.

For the dihedral group D2nD_{2n}, we focus in the case n=2kn=2k since the Schur multiplier (D2n)\mathcal{M}(D_{2n}) vanishes for n=2k+1n=2k+1. Similar to the abelian case, we decompose every D2nD_{2n}-cobordism into a finite product of the generator with base space of genus one, which is induced by a reflection and the rotation by 180 degrees, see Corollary 16.

For the symmetric group SnS_{n}, the Schur multiplier is non-trivial for n>3n>3 and in that case it is equal to 2\mathbb{Z}_{2}. In Proposition 18, we prove that there is a generator with base space of genus one, which is induced by any two disjoint transpositions. A similar argument works for the alternating group AnA_{n}, where for n=6,7n=6,7, we use the Sylow theory of the Schur multiplier that is shown in Proposition 14.

In summary, we have the following result.

Theorem 1.

For GG a finite abelian group or G{D2n,Sn,An}G\in\{D_{2n},S_{n},A_{n}\}, every GG-cobordism over a closed oriented surface is extendable.

We have the following applications for extending non-necessarily free actions over surfaces to 3-dimensional handlebodies:

  • i)

    In Theorem 23, the actions of abelian groups have two types of fixed points, which are the ones induced by hyperelliptic involutions and pairs of ramification points with complementary monodromies (signature >2>2). An unfolding process is performed by first considering the quotient by the hyperelliptic involutions and after some modifications, we reduce the problem to the extension of free actions.

  • ii)

    In Theorem 24, the actions of dihedral groups reduce to a finite product of an specific generator. We extend the action for this generator and for the surfaces realized by the products.

These results were proven before by different methods, by Reni-Zimmermann [RZ96] and Hidalgo [Hid94].

This article is organized as follows. In Section 1, we review the concept of GG-cobordism and the Schur multiplier, as well as the relations between them. In Section 2, we give explicit generators for the Schur multiplier of the dihedral, the symmetric and the alternating groups. Finally, in Section 3 we construct the extensions of the free actions on closed oriented surfaces for the dihedral, symmetric and alternating groups. Additionally, for non necessarily free actions on closed oriented surfaces of abelian groups (under certain conditions) and dihedral groups, we construct the extensions given by 3-dimensional handlebodies.

Acknowledgements: the first author thanks the Academia Mexicana de Ciencias for the opportunity of participating in the Scientific Research Summer of 2020. The second author is supported by cátedras CONACYT and Proyecto CONACYT ciencias básicas 2016, No. 284621. We would like to thank Bernardo Uribe and Eric Samperton for their helpful conversations.

1 Preliminaries

In this section we review in detail the definitions and properties of the theory of GG-cobordisms introduced in [GS16, Seg12]. In addition, we discuss some important facts about the Schur multiplier.

1.1 GG-cobordisms

Throughout the article, GG denotes a finite group and 1G1\in G the neutral element. Also, we consider right actions of the group GG, and all the surfaces are oriented.

Definition 2.

Let Σ\Sigma and Σ\Sigma^{\prime} be dd-dimensional closed, oriented smooth manifolds. A cobordism between Σ\Sigma and Σ\Sigma^{\prime} is a (d+1)(d+1)-dimensional oriented smooth manifold MM, with boundary diffeomorphic to ΣΣ\Sigma\sqcup-\Sigma^{\prime}, where Σ-\Sigma^{\prime} is Σ\Sigma^{\prime} with the reverse orientation. Two cobordisms MM and MM^{\prime} are equivalent if there exists a diffeomorphism ϕ:MM\phi:M\longrightarrow M^{\prime} such that we have the commutative diagram

M\textstyle{M\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ϕ\scriptstyle{\phi}Σ\textstyle{\Sigma\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Σ\textstyle{\Sigma^{\prime}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}M\textstyle{M^{\prime}}.\textstyle{\,.} (2)
Definition 3.

A principal GG-bundle over a topological space XX, consists of a fiber bundle π:EX\pi:E\rightarrow X where the group GG acts freely and transitively over each fiber.

Example 1.1.

In dimension one, for every gGg\in G, we construct the principal GG-bundle PgS1P_{g}\rightarrow S^{1} obtained by attaching the ends of [0,1]×G[0,1]\times G via multiplication by gg, i.e., (0,h)(0,h) is identified with (1,gh)(1,gh) for every hGh\in G. This construction Pg=[0,1]×G/gP_{g}=[0,1]\times G/\sim_{g} projects to the circle by restriction to the first coordinate, and the action Pg×GPgP_{g}\times G\rightarrow P_{g} is defined by right multiplication on the second coordinate. Any principal GG-bundle over the circle is isomorphic to some PgP_{g}, and PgP_{g} is isomorphic to PhP_{h} if and only if hh is conjugate to gg.

Throughout the paper, we refer to the element gGg\in G as the monodromy associated to the corresponding principal GG-bundle PgP_{g}. In the case of the neutral element of the group GG, we say that the monodromy is trivial.

Definition 4.

Let ξ:PΣ\xi:P\rightarrow\Sigma and ξ:PΣ\xi^{\prime}:P^{\prime}\rightarrow\Sigma^{\prime} be principal GG-bundles. A GG-cobordism between ξ\xi and ξ\xi^{\prime} is a principal GG-bundle ϵ:QM\epsilon:Q\rightarrow M, with diffeomorphisms for the boundaries MSS\partial M\cong S\sqcup-S^{\prime} and QPP\partial Q\cong P\sqcup-P^{\prime}, which match with the projections and the restriction of the action. Two GG-cobordisms ϵ:QM\epsilon:Q\rightarrow M and ϵ:QM{\epsilon}^{\prime}:Q^{\prime}\rightarrow M^{\prime} define the same class if MM and M{M}^{\prime} are equivalent as cobordisms by a diffeomorphism ϕ:MM\phi:M\rightarrow{M}^{\prime}, QQ and QQ^{\prime} are equivalent as cobordisms by a GG-equivariant diffeomorphism ψ:QQ\psi:Q\longrightarrow Q^{\prime}, and in addition, we have the commutative diagram

Q\textstyle{Q\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ψ\scriptstyle{\psi}ϵ\scriptstyle{\epsilon}Q\textstyle{Q^{\prime}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ϵ\scriptstyle{\epsilon^{\prime}}M\textstyle{M\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ϕ\scriptstyle{\phi}M.\textstyle{M^{\prime}\,.} (3)
Example 1.2.
  1. 1.

    A GG-cobordism from PgP_{g} to PhP_{h} (g,hGg,h\in G) with base space the cylinder, is given by an element kGk\in G such that h=kgk1h=kgk^{-1}.

  2. 2.

    A GG-cobordism with entry the disjoint union PgPhP_{g}\sqcup P_{h} and exit PghP_{gh}, with base space the pair of pants, is a G-deformation retract111By a GG-deformation retract we mean that the homotopy is by means of principal GG-bundles. of a principal G-bundle over the wedge S1S1S^{1}\vee S^{1}.

  3. 3.

    There is only one GG-cobordism over the disk and every representative is a trivial bundle.

  4. 4.

    Take as base space a two dimensional handlebody of genus nn with one boundary circle. A GG-cobordism depends on elements gi,kiGg_{i},k_{i}\in G, for 1in1\leq i\leq n, with monodromy for the boundary circle given by the product i=1n[ki,gi]\prod_{i=1}^{n}[k_{i},g_{i}].

In Figure 1, we have pictures for the GG-cobordisms over the cylinder, the pair of pants and the disc. For these pictures, we draw from left to right the direction for our cobordisms. Also, every circle is labelled with the correspondent monodromy and for every cylinder we write inside the element of the group with which we do the conjugation.

Refer to caption
Figure 1: GG-cobordism over the cylinder, the pair of pants and the disc.

In the left side of Figure 2, we have a GG-cobordism over a genus one handlebody. Additionally, in the right side, we represent an equivalent manner to see this GG-cobordism.

Refer to caption
Figure 2: Two equivalent GG-cobordisms over a handle of genus one.

If a GG-cobordism over a closed connected surface is cut along a simple closed separating curve222A simple closed curve in a surface is separating if the cut surface is not connected., the monodromy of the resulting curve lies inside the commutator group, as shown in the following proposition.

Proposition 5.

For a GG-cobordism over a closed connected surface SS, the monodromy of every embedded simple closed separating curve in SS lies in the commutator group [G,G][G,G].

Definition 6.

A GG-cobordism of dimension two, over a closed surface, is extendable if for some representative principal GG-bundle PSP\rightarrow S, with the action α:P×GP\alpha:P\times G\rightarrow P, there exits a 33-dimensional manifold MM with boundary M=P\partial M=P, with an action of GG of the form α¯:M×GM\overline{\alpha}:M\times G\rightarrow M, which extends α\alpha, i.e., we have the commutative diagram

P×G\textstyle{P\times G\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}α\scriptstyle{\alpha}P\textstyle{P\ignorespaces\ignorespaces\ignorespaces\ignorespaces}M×G\textstyle{M\times G\ignorespaces\ignorespaces\ignorespaces\ignorespaces}α¯\scriptstyle{\overline{\alpha}}M.\textstyle{M\,.} (4)
Proposition 7.

Any GG-cobordism over a closed surface of genus one is extendable.

Proof.

Consider a principal GG-bundle representing the given GG-cobordism over the closed surface of genus one. It is enough to prove the case in which the total space of the bundle is a connected space. Moreover, the action of GG over the total space can be modified by an isotopy resulting in an action which depends completely on a pair of monodromies (g,k)(g,k), which are associated to two curves in the torus that intersect once. Denote by PgP_{g} and PkP_{k} the two principal GG-bundles associated to these two curves. It follows that the action of GG over the total space is given by the product of the total spaces PgP_{g} and PkP_{k}. Because of the assumptions, at least one of PgP_{g} or PkP_{k} is a connected space, let us assume that it is PgP_{g}. The extension of the action of GG is through the 3-dimensional handlebody constructed as follows. First, consider the disc DD as the union (S1×(0,1]){0}(S^{1}\times(0,1])\cup\{0\}, where 0 is the center. For each circle S1×{r}S^{1}\times\{r\}, with r(0,1]r\in(0,1], we take as monodromy the element gg so that the principal GG-bundle is PgP_{g}, and we take the center 0 as fixed point. Thus, over the disc we have the rotation by 2π/|g|2\pi/|g|, with |g||g| the order of gGg\in G. Taking the product of this disc together with the induced principal GG-bundle PkP_{k}, we obtain the extension which makes the GG-cobordism extendable. ∎

Remark: 8.

We want to emphasize why the construction given in the previous proposition does not work for closed surfaces with genus >1>1. The reason is that the set of fixed points should be a smooth submanifold, which we can not assure for genus >1>1, since we have points where three lines meet.

Now, we apply the previous results to abelian groups.

Theorem 9.

For GG a finite abelian group, any GG-cobordism is extendable.

Proof.

Consider a GG-cobordism over a connected closed surface. By Proposition 5, we can write this GG-cobordism as a connected sum of GG-cobordisms with base space of genus one. This connected sum is done for the total space along trivial bundles over a circle. Since the connected sum is in the same bordism class as the disjoint union, we are decomposing this GG-cobordism as a disjoint union of GG-cobordisms with base space a closed surface of genus one. Because of Proposition 7, any GG-cobordism over a closed surface of genus one is extendable, so the theorem follows. ∎

1.2 The Schur multiplier

The study of this theory began in 1904 by Isaai Schur in order to study the projective representations of groups. Nowadays, the Schur multiplier represents three different isomorphic groups given by the second free bordism group Ω2SO(G)\Omega_{2}^{SO}(G), the second homology group H2(G,)H_{2}(G,\mathbb{Z}) and the second cohomology group H2(G,)H^{2}(G,\mathbb{C}^{*}).

Definition 10.

Let G,G\langle G,G\rangle be the free group on all pairs x,y\langle x,y\rangle, with x,yGx,y\in G. There is a natural homomorphism of G,G\langle G,G\rangle onto the commutator group [G,G][G,G], which sends x,y\langle x,y\rangle into [x,y][x,y]. Consider the kernel Z(G)Z(G) of this homomorphism and the normal subgroup B(G)B(G) of G,G\langle G,G\rangle generated by the relations

x,x\displaystyle\left<x,x\right> 1,\displaystyle\sim 1\,, (5)
x,y\displaystyle\left<x,y\right> y,x1,\displaystyle\sim\left<y,x\right>^{-1}\,, (6)
xy,z\displaystyle\left<xy,z\right> y,zxx,z,\displaystyle\sim\left<y,z\right>^{x}\left<x,z\right>\,, (7)
y,zx\displaystyle\left<y,z\right>^{x} x,[y,z]y,z,\displaystyle\sim\left<x,[y,z]\right>\left<y,z\right>\,, (8)

where x,y,zGx,y,z\in G and y,zx=yx,zx=xyx1,xzx1\langle y,z\rangle^{x}=\langle y^{x},z^{x}\rangle=\langle xyx^{-1},xzx^{-1}\rangle. The Schur multiplier is defined as the quotient group

(G):=Z(G)B(G).\mathcal{M}(G):=\frac{Z(G)}{B(G)}\,. (9)

Miller [Mil52] shows that the quotient Z(G)/B(G)Z(G)/B(G) is canonically isomorphic to the Hopf’s integral formula

(G)R[F,F][F,R],\mathcal{M}(G)\cong\frac{R\cap[F,F]}{[F,R]}\,, (10)

where G=F|RG=\langle\,F\,|\,R\,\rangle. Moreover, in [Mil52] there are some consequent relations, which we enumerate in the following theorem.

Theorem 11 ([Mil52]).

The following relations can be deduced from (5)-(8):

x,yz\displaystyle\left<x,yz\right> x,yx,zy,\displaystyle\sim\left<x,y\right>\left<x,z\right>^{y}\,, (11)
x,ya,b\displaystyle\left<x,y\right>^{\left<a,b\right>} x,y[a,b],\displaystyle\sim\left<x,y\right>^{[a,b]}\,, (12)
[x,y,a,b]\displaystyle\left[\left<x,y\right>,\left<a,b\right>\right] [x,y],[a,b],\displaystyle\sim\left<[x,y],[a,b]\right>\,, (13)
b,ba0,b0\displaystyle\left<b,b^{\prime}\right>\left<a_{0},b_{0}\right> [b,b],a0a0,[b,b]b0b,b,\displaystyle\sim\left<[b,b^{\prime}],a_{0}\right>\left<a_{0},[b,b^{\prime}]b_{0}\right>\left<b,b^{\prime}\right>\,, (14)
b,ba0,b0\displaystyle\left<b,b^{\prime}\right>\left<a_{0},b_{0}\right> [b,b]b0,a0a0,[b,b]b,b,\displaystyle\sim\left<[b,b^{\prime}]b_{0},a_{0}\right>\left<a_{0},[b,b^{\prime}]\right>\left<b,b^{\prime}\right>\,, (15)
b,ba,a\displaystyle\left<b,b^{\prime}\right>\left<a,a^{\prime}\right> [b,b],[a,a]a,ab,b,\displaystyle\sim\left<[b,b^{\prime}],[a,a^{\prime}]\right>\left<a,a^{\prime}\right>\left<b,b^{\prime}\right>\,, (16)
xn,xs\displaystyle\left<x^{n},x^{s}\right> 1n=0,±1,;s=0,±1,,\displaystyle\sim 1\hskip 28.45274ptn=0,\pm 1,\cdots;s=0,\pm 1,\cdots\,, (17)

for x,y,z,a,b,a,b,a0,b0Gx,y,z,a,b,a^{\prime},b^{\prime},a_{0},b_{0}\in G.

The connection with bordism relates the elements of Z(G)Z(G) by means of the assignment

x1,y1x2,y2xn,yn(yn,xn)(yn1,xn1)(y1,x1),\langle x_{1},y_{1}\rangle\langle x_{2},y_{2}\rangle\cdots\langle x_{n},y_{n}\rangle\longmapsto(y_{n},x_{n})(y_{n-1},x_{n-1})\cdots(y_{1},x_{1})\,, (18)

where the sequence in the right defines the generating monodromies for a GG-cobordism over a closed surface of genus nn as in Figure 3.

Refer to caption
Figure 3: The GG-cobordism associated to the sequence (yn,xn)(yn1,xn1)(y1,x1)(y_{n},x_{n})(y_{n-1},x_{n-1})\cdots(y_{1},x_{1}), with yi,xiGy_{i},x_{i}\in G and i=1n[xi,yi]=1\prod_{i=1}^{n}[x_{i},y_{i}]=1.

Indeed, the previous four relations (5), (6), (7) and (8), are interpreted in bordism as follows:

  • (i)

    For (5) and (6), we consider the GG-cobordism defined by the pairs (x,x)(x,x) and (x,y)(y,x)(x,y)(y,x), respectively. We represent these GG-cobordisms in the left side of Figure 4, respectively.

    Refer to caption
    Refer to caption
    Figure 4: The GG-cobordisms associated to the pairs (x,x)(x,x) and (x,y)(y,x)(x,y)(y,x).

    In the top of Figure 4, we apply the Dehn twist diffeomorphism and obtain that the conjugation becomes the neutral element 1G1\in G. In the bottom of Figure 4, we cut along a trivial monodromy to reduce the genus by one. Notice that the GG-cobordisms in the left side of Figure 4 are null bordant since we can cut along a trivial monodromy eliminating the hole of the handle.

  • (ii)

    For (7) and (8), we obtain a GG-cobordism, over a handlebody of genus two, where we can find a curve with trivial monodromy which reduces the genus by one. In Figure 5, we represent these identifications, respectively.

    Refer to caption
    Refer to caption
    Figure 5: Reduction of genus through the cutting along a trivial monodromy.

Now, we focus on the Sylow theory of the Schur multiplier. We use Definition 12 and Theorem 13, in order to show Proposition 14.

Definition 12.

For a subgroup HGH\subset G, there are the following induces maps:

  • i)

    the restriction map, denoted by res:(G)(H)\operatorname{res}:\mathcal{M}(G)\rightarrow\mathcal{M}(H), which associates to a GG-cobordism over a closed surface, the restriction of the action to the subgroup HH.

  • ii)

    the corestriction map, denoted by cor:(H)(G)\operatorname{cor}:\mathcal{M}(H)\rightarrow\mathcal{M}(G), which starts with a principal HH-bundle PSP\rightarrow S and associates the Borel construction P×HGP\times_{H}G produced by the quotient of the product P×GP\times G with the action of HH of the form (x,g)h=(xh,h1g)(x,g)h=(xh,h^{-1}g). The group GG has a free action over the the Borel construction by [x,g]g^=[x,gg^][x,g]\hat{g}=[x,g\hat{g}].

In general, these maps extend to non-necessarily free actions, in particular, for the GG-bordism groups Ω3SO,free(G)\Omega_{3}^{SO,\partial free}(G) of 33-dimensional manifolds with a non necessarily free GG-action which restricts to a free action over the boundary.

Theorem 13 ([Kar87]).

Let PP be a Sylow pp-subgroup of GG and let (G)\mathcal{M}(G) the pp-component of the Schur multiplier (G)\mathcal{M}(G). Then the restriction map res:(G)(P)\operatorname{res}:\mathcal{M}(G)\rightarrow\mathcal{M}(P) induces an injective homomorphism (G)p(P)\mathcal{M}(G)_{p}\rightarrow\mathcal{M}(P), and the corestriction map cor:(P)(G)\operatorname{cor}:\mathcal{M}(P)\rightarrow\mathcal{M}(G) induces a surjective homomorphism (P)(G)p\mathcal{M}(P)\rightarrow\mathcal{M}(G)_{p}.

Proposition 14.

For a finite group GG, and Syl(G)\operatorname{Syl}(G) the set of isomorphism classes of Sylow subgroups of GG, if any element QQ in Syl(G)\operatorname{Syl}(G) satisfies that any QQ-cobordism is extendable, then any GG-cobordism is extendable.

Proof.

For n=|G|n=|G| and n=pkmn=p^{k}m with pmp\not|m, consider an element f(G)pf\in\mathcal{M}(G)_{p}, hence the composition

F:=corres:(G)p(G)p,F:=\operatorname{cor}\circ\operatorname{res}:\mathcal{M}(G)_{p}\longrightarrow\mathcal{M}(G)_{p}\,, (19)

is given by ffmf\longmapsto f^{m}, which is an automorphism of (G)p\mathcal{M}(G)_{p}. By the assumptions, the restriction res(f)\operatorname{res}(f) is extendable by a 33-manifold MM with an action of QQ, therefore, applying the corestriction we obtain that fmf^{m} is extendable by the 33-manifold cor(M)\operatorname{cor}(M). Similarly, we can start with F1(f)F^{-1}(f) and we get that ff is extendable and the proposition follows. ∎

2 Generators for the Schur multiplier

In this section we give explicit generators for the Schur multiplier of the dihedral, the symmetric and the alternating groups.

2.1 Dihedral group

For n3n\geq 3, the dihedral group is the group of symmetries of the nn-regular polygon (with D2=2D_{2}=\mathbb{Z}_{2}, D4=2×2D_{4}=\mathbb{Z}_{2}\times\mathbb{Z}_{2}), and presentation

D2n=a,b:a2=1,b2=1,(ab)n=1,D_{2n}=\langle a,b:a^{2}=1,b^{2}=1,(ab)^{n}=1\rangle\,, (20)

where c:=abc:=ab is the rotation of 2π/n2\pi/n. The Schur multiplier has the form

(D2n)={0n=2k+1,2n=2k.\mathcal{M}(D_{2n})=\left\{\begin{array}[]{cl}0&n=2k+1\,,\\ \mathbb{Z}_{2}&n=2k\,.\end{array}\right. (21)

In order to find a generator we show the following.

Proposition 15.

We obtain the following identifications:

  • (i)

    ci,cj1\langle c^{i},c^{j}\rangle\sim 1,

  • (ii)

    ci,acjc,ai\left<c^{i},ac^{j}\right>\sim\langle c,a\rangle^{i},

  • (iii)

    aci,cjc,aj\left<ac^{i},c^{j}\right>\sim\langle c,a\rangle^{-j}, and

  • (iv)

    aci,acjc,aji\left<ac^{i},ac^{j}\right>\sim\langle c,a\rangle^{j-i}.

Proof.

The relation (i) follows by (17). The use of (7), (17) and (11) implies

ci,acjci,aci,cjaci,a,\displaystyle\left<c^{i},ac^{j}\right>\sim\left<c^{i},a\right>\left<c^{i},c^{j}\right>^{a}\sim\left<c^{i},a\right>\,, (22)
ci,acj=cci1,acjci1,acjcc,acjci1,ac,a.\displaystyle\left<c^{i},ac^{j}\right>=\left<cc^{i-1},ac^{j}\right>\sim\left<c^{i-1},ac^{j}\right>^{c}\left<c,ac^{j}\right>\sim\left<c^{i-1},a\right>\left<c,a\right>\,. (23)

Therefore, we obtain the relation

ci,ac,ac,ac,ai,\left<c^{i},a\right>\sim\underbrace{\left<c,a\right>\left<c,a\right>\cdots\left<c,a\right>}_{i}\,, (24)

which implies (ii). By (6) we obtain (iii) as follows

aci,cjcj,aci1c,aj.\left<ac^{i},c^{j}\right>\sim\left<c^{j},ac^{i}\right>^{-1}\sim\left<c,a\right>^{-j}\,. (25)

Finally, we use (11) and (5),

aci,acjci,acjaa,acjc1,aia,cja,\left<ac^{i},ac^{j}\right>\sim\left<c^{i},ac^{j}\right>^{a}\left<a,ac^{j}\right>\sim\left<c^{-1},a\right>^{i}\left<a,c^{j}\right>^{a}\,, (26)

and by (6) we obtain (iv). ∎

Corollary 16.

For n=2kn=2k, the generator of the group (D2n)\mathcal{M}(D_{2n}) is represented by the element ck,a\langle c^{k},a\rangle.

2.2 Symmetric group

The symmetric group SnS_{n} is composed of permutation of the set [n]={1,,n}[n]=\{1,\cdots,n\}. This group is generated by the transpositions (ij)(ij) with i,j[n]i,j\in[n]. The Schur multiplier is given as follows

(Sn)={0n3,2n4.\mathcal{M}(S_{n})=\left\{\begin{array}[]{cl}0&n\leq 3\,,\\ \mathbb{Z}_{2}&n\geq 4\,.\end{array}\right. (27)
Lemma 17.

Let k[n]k\in[n], and σ1,τ1σr,τr\langle\sigma_{1},\tau_{1}\rangle\cdots\langle\sigma_{r},\tau_{r}\rangle be a sequence with σi,τi,Sn\sigma_{i},\tau_{i},\in S_{n}, for i{1,,r}i\in\{1,\cdots,r\}. There exist a positive number 0sr0\leq s\leq r and the following elements:

  • (i)

    ai,biSna_{i},b_{i}\in S_{n}, with 0is0\leq i\leq s, such that all ai,bia_{i},b_{i} fix kk, and

  • (ii)

    cj,djSnc_{j},d_{j}\in S_{n}, with 0jrs0\leq j\leq r-s, such that for each jj, at least one of cj,djc_{j},d_{j} does not fix kk,

with the relation

σ1,τ1σr,τra1,b1as,bsc1,d1crs,crs.\langle\sigma_{1},\tau_{1}\rangle\cdots\langle\sigma_{r},\tau_{r}\rangle\sim\langle a_{1},b_{1}\rangle\cdots\langle a_{s},b_{s}\rangle\langle c_{1},d_{1}\rangle\cdots\langle c_{r-s},c_{r-s}\rangle\,. (28)

Moreover, ss is the amount of pairs σi,τi\langle\sigma_{i},\tau_{i}\rangle such that both σi\sigma_{i} and τi\tau_{i} fix kk.

Proof.

It suffices to note that for pairs a,b\langle a,b\rangle and x,y\langle x,y\rangle, with a,b,x,ySna,b,x,y\in S_{n}, such that aa and bb fix kk there is the relation

x,ya,b\displaystyle\left<x,y\right>\left<a,b\right> a,bb,ax,ya,b\displaystyle\sim\left<a,b\right>\left<b,a\right>\left<x,y\right>\left<a,b\right>
a,bx[b,a],y[b,a],\displaystyle\sim\left<a,b\right>\left<x^{[b,a]},y^{[b,a]}\right>\,,

where we have used (12). An iterative application of this process, allows us to put all terms fixing kk to the left in the sequence. ∎

Proposition 18.

Assume n4n\geq 4, and take elements σi,τi,σj,τjSn\sigma_{i},\tau_{i},\sigma^{\prime}_{j},\tau^{\prime}_{j}\in S_{n}, for 1ir1\leq i\leq r and 1js1\leq j\leq s, with the same commutator, i.e.,

[σ1,τ1][σr,τr]=[σ1,τ1][σs,τs].[\sigma_{1},\tau_{1}]\cdots[\sigma_{r},\tau_{r}]=[\sigma^{\prime}_{1},\tau^{\prime}_{1}]\cdots[\sigma^{\prime}_{s},\tau^{\prime}_{s}]\,. (29)

Therefore, for the element u:=(1,2),(3,4)u:=\langle(1,2),(3,4)\rangle, there is the relation

σ1,τ1σr,τrukσ1,τ1σs,τs,\langle\sigma_{1},\tau_{1}\rangle\cdots\langle\sigma_{r},\tau_{r}\rangle\sim u^{k}\langle\sigma^{\prime}_{1},\tau^{\prime}_{1}\rangle\cdots\langle\sigma^{\prime}_{s},\tau^{\prime}_{s}\rangle\,, (30)

with k{0,1}k\in\{0,1\}.

Proof.

First, we observe that from (7) and (11), we can assume that all the elements σi,τi,σj,τjSn\sigma_{i},\tau_{i},\sigma^{\prime}_{j},\tau^{\prime}_{j}\in S_{n} are transpositions. By (8), every pair σ,τ\langle\sigma,\tau\rangle with σ\sigma and τ\tau disjoint transpositions is in the same class as the pair u:=(1,2),(3,4)u:=\left<(1,2),(3,4)\right>. Therefore, we can assume that the pairs are of the form (i,j),(j,k)\left<(i,j),(j,k)\right>, with i,ji,j and kk different numbers.

By exhaustion, the proposition follows for the symmetric group SnS_{n}, with 4n64\leq n\leq 6. We proceed by induction for n7n\geq 7 and we suppose that for k<nk<n, the generator of the Schur multiplier (Sn)\mathcal{M}(S_{n}) is given by the element u:=(1,2),(3,4)u:=\left<(1,2),(3,4)\right>. Set by mm the maximum of rr and ss, for the sequences σ1,τ1σr,τr\langle\sigma_{1},\tau_{1}\rangle\cdots\langle\sigma_{r},\tau_{r}\rangle and σ1,τ1σs,τs\langle\sigma^{\prime}_{1},\tau^{\prime}_{1}\rangle\cdots\langle\sigma^{\prime}_{s},\tau^{\prime}_{s}\rangle. For m=1m=1, the proposition follows from the triviality of (S3)\mathcal{M}(S_{3}). Suppose that our proposition follows for sequences with length l<ml<m. We consider the sequence

σ1,τ1σr,τr(σ1,τ1σs,τs)1σ1,τ1σr,τrτs,σsτ1,σ1,\langle\sigma_{1},\tau_{1}\rangle\cdots\langle\sigma_{r},\tau_{r}\rangle\left(\langle\sigma^{\prime}_{1},\tau^{\prime}_{1}\rangle\cdots\langle\sigma^{\prime}_{s},\tau^{\prime}_{s}\rangle\right)^{-1}\sim\langle\sigma_{1},\tau_{1}\rangle\cdots\langle\sigma_{r},\tau_{r}\rangle\langle\tau^{\prime}_{s},\sigma^{\prime}_{s}\rangle\cdots\langle\tau^{\prime}_{1},\sigma^{\prime}_{1}\rangle\,, (31)

which has trivial commutator and length given by M:=r+s2mM:=r+s\leq 2m. Let x{1,,n}x\in\{1,\cdots,n\} be the number that is fixed by the most terms of the sequence (31). Given that the sequences have non trivial terms, each term permutes 33 different numbers in {1,2,,n}\{1,2,\cdots,n\}. Therefore, the number xx is not fixed by at most 3(r+s)n\frac{3(r+s)}{n} terms. Given that 3(r+s)n3(2m)7<m\frac{3(r+s)}{n}\leq\frac{3(2m)}{7}<m, hence xx is not fixed by at most m1m-1 terms. By Lemma 17, we can find an equivalent sequence for (31), with the following form

α1,β1αt,βtfix number xαt+1,βt+1αM,βMdo not fix number x,\underbrace{\left<\alpha_{1},\beta_{1}\right>\cdots\left<\alpha_{t},\beta_{t}\right>}_{\text{fix number x}}\underbrace{\left<\alpha_{t+1},\beta_{t+1}\right>\cdots\left<\alpha_{M},\beta_{M}\right>}_{\text{do not fix number x}}\,, (32)

where:

  • i)

    Mt<mM-t<m;

  • ii)

    the αi,βiSn\alpha_{i},\beta_{i}\in S_{n}, with 0it0\leq i\leq t, fix xx; and

  • iii)

    the αj,βjSn\alpha_{j},\beta_{j}\in S_{n}, with t+1jMt+1\leq j\leq M, at least one does not fix xx.

Moreover, by the proof of Lemma 17, the elements αi,βi,αj,βjSn\alpha_{i},\beta_{i},\alpha^{\prime}_{j},\beta^{\prime}_{j}\in S_{n} are again transpositions. Now we consider the sequences

A:=α1,β1αt,βtA:=\left<\alpha_{1},\beta_{1}\right>\cdots\left<\alpha_{t},\beta_{t}\right> (33)

and

B:=(αt+1,βt+1αM,βM)1=βM,αMβt+1,αt+1,B:=\left(\left<\alpha_{t+1},\beta_{t+1}\right>\cdots\left<\alpha_{M},\beta_{M}\right>\right)^{-1}=\left<\beta_{M},\alpha_{M}\right>\cdots\left<\beta_{t+1},\alpha_{t+1}\right>\,, (34)

where both sequences have the same commutator. Furthermore, the sequence AA has pairs composed by elements in Sn1S_{n-1} because they fix xx. By our induction hypothesis, for nn, we conclude that the Schur multiplier (Sn1)\mathcal{M}(S_{n-1}) is generated by u=(1,2),(3,4)u=\langle(1,2),(3,4)\rangle. Therefore, AuiCA\sim u^{i}C for i{0,1}i\in\{0,1\} and CC is a sequence of pairs with elements in Sn1S_{n-1}. We can take CC to be of length <m<m, as it is has the same commutator as the chain BB of length <m<m. By the other induction hypothesis, for mm, since BB and CC have length less than mm, then there is j{0,1}j\in\{0,1\} such that BujCB\sim u^{j}C. This shows that the product of our initial sequences in (31) is equivalent to uiju^{i-j} and the proof of the proposition follows. ∎

Corollary 19.

For n4n\geq 4, the generator of the group (Sn)\mathcal{M}(S_{n}) is represented by the element u:=(1,2),(3,4)u:=\langle(1,2),(3,4)\rangle.

2.3 Alternating group

The alternating group AnA_{n} is the normal subgroup of SnS_{n} with index 22. The Schur multiplier has the form

(An)={0n3,2n=4,5,6n=6,7,2n8.\mathcal{M}(A_{n})=\left\{\begin{array}[]{cl}0&n\leq 3\,,\\ \mathbb{Z}_{2}&n=4,5,\\ \mathbb{Z}_{6}&n=6,7,\\ \mathbb{Z}_{2}&n\geq 8\,.\end{array}\right. (35)
Proposition 20.

For n4n\geq 4, the element (1,2)(3,4),(1,3)(2,4)\langle(1,2)(3,4),(1,3)(2,4)\rangle is nontrivial in (An)\mathcal{M}(A_{n}).

Proof.

Because of the relations (7) and (11) in (Sn)\mathcal{M}(S_{n}), we have the following

(1,2)(3,4),(1,3)(2,4)\displaystyle\langle(1,2)(3,4),(1,3)(2,4)\rangle (3,4),(2,3)(1,4)(1,2),(1,3)(2,4)\displaystyle\sim\langle(3,4),(2,3)(1,4)\rangle\langle(1,2),(1,3)(2,4)\rangle
(3,4),(2,3)(2,4),(1,4)(1,2),(1,3)(2,3),(2,4)\displaystyle\sim\langle(3,4),(2,3)\rangle\langle(2,4),(1,4)\rangle\langle(1,2),(1,3)\rangle\langle(2,3),(2,4)\rangle

We also have from (8), (11) and (2,4),(1,4)=(2,3),(1,3)(3,4)\langle(2,4),(1,4)\rangle=\langle(2,3),(1,3)\rangle^{(3,4)} that

(2,4),(1,4)\displaystyle\langle(2,4),(1,4)\rangle (3,4),[(2,3),(1,3)](2,3),(1,3)=(3,4),(1,2)(1,3)(2,3),(1,3)\displaystyle\sim\langle(3,4),[(2,3),(1,3)]\rangle\langle(2,3),(1,3)\rangle=\langle(3,4),(1,2)(1,3)\rangle\langle(2,3),(1,3)\rangle
(3,4),(1,2)(3,4),(2,3)(2,3),(1,3)=u(3,4),(2,3)(2,3),(1,3)\displaystyle\sim\langle(3,4),(1,2)\rangle\langle(3,4),(2,3)\rangle\langle(2,3),(1,3)\rangle=u\langle(3,4),(2,3)\rangle\langle(2,3),(1,3)\rangle

As [(3,4),(2,3)]=[(2,3),(2,4)][(3,4),(2,3)]=[(2,3),(2,4)], [(2,3),(1,3)]=[(1,3),(1,2)][(2,3),(1,3)]=[(1,3),(1,2)] and (S3)=0\mathcal{M}(S_{3})=0, we have that (3,4),(2,3)(2,3),(2,4)\langle(3,4),(2,3)\rangle\sim\langle(2,3),(2,4)\rangle and (2,3),(1,3)(1,3),(1,2)\langle(2,3),(1,3)\rangle\sim\langle(1,3),(1,2)\rangle. Therefore,

(1,2)(3,4),(1,3)(2,4)\displaystyle\langle(1,2)(3,4),(1,3)(2,4)\rangle (2,3),(2,4)(2,4),(1,4)(1,2),(1,3)(2,3),(2,4)\displaystyle\sim\langle(2,3),(2,4)\rangle\langle(2,4),(1,4)\rangle\langle(1,2),(1,3)\rangle\langle(2,3),(2,4)\rangle
u(2,3),(2,4)2(1,3),(1,2)(1,2),(1,3)(2,3),(2,4)\displaystyle\sim u\langle(2,3),(2,4)\rangle^{2}\langle(1,3),(1,2)\rangle\langle(1,2),(1,3)\rangle\langle(2,3),(2,4)\rangle
u(2,3),(2,4)3u=(1,2),(3,4),\displaystyle\sim u\langle(2,3),(2,4)\rangle^{3}\sim u=\langle(1,2),(3,4)\rangle\,,

where (2,3),(2,4)3\langle(2,3),(2,4)\rangle^{3} vanishes since [(2,3),(2,4)]3=1[(2,3),(2,4)]^{3}=1 and (S3)=0\mathcal{M}(S_{3})=0. As a consequence, the element (1,2)(3,4),(1,3)(2,4)\langle(1,2)(3,4),(1,3)(2,4)\rangle is nontrivial in (Sn)\mathcal{M}(S_{n}), and hence it is also nontrivial in (An)\mathcal{M}(A_{n}) for n4n\geq 4. ∎

Corollary 21.

For n4n\geq 4 and n{6,7}n\not\in\{6,7\}, the generator of the group (An)\mathcal{M}(A_{n}) is represented by the element (1,2)(3,4),(1,3)(2,4)\langle(1,2)(3,4),(1,3)(2,4)\rangle.

3 Extending group actions on surfaces

This section contains the main applications of this work. We start with free actions of abelian, dihedral, symmetric and alternating groups and then, we show that these actions extend to actions on 3-manifolds. Finally, we see the case of non-necessarily free actions for abelian and dihedral groups.

3.1 Free actions on surfaces

Definition 22.

Consider a compact oriented surface SS with a (free) group action

α:S×GS.\alpha:S\times G\longrightarrow S\,. (36)

We say that the action is extendable if there exists a 33-manifold MM with boundary M=S\partial M=S, with an action of GG of the form α¯:M×GM\overline{\alpha}:M\times G\longrightarrow M, which extends α\alpha, i.e., we have the commutative diagram

S×G\textstyle{S\times G\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}α\scriptstyle{\alpha}S\textstyle{S\ignorespaces\ignorespaces\ignorespaces\ignorespaces}M×G\textstyle{M\times G\ignorespaces\ignorespaces\ignorespaces\ignorespaces}α¯\scriptstyle{\overline{\alpha}}M.\textstyle{M\,.} (37)
Proof of Theorem 1.

By Theorem 9 we know that any free action of a finite abelian group is extendable. For dihedral groups D2nD_{2n}, we have two cases to consider. One is for n=2k+1n=2k+1, but since (D4k+2)=0\mathcal{M}(D_{4k+2})=0, then any free action is extendable. The other is for n=2kn=2k, where by Corollary 16, the generator of the Schur multiplier is represented by a GG-cobordism over a closed surface of genus one, therefore, by Proposition 7 these free actions are extendable. Now consider free actions of the symmetric groups SnS_{n}, since (Sn)=0\mathcal{M}(S_{n})=0 for n3n\leq 3, it remains to prove the extension for n4n\geq 4. Similar as for dihedral groups, by Corollary 19 these free actions are extendable. For the alternating groups AnA_{n} the free actions are extendable for n3n\leq 3. Again, for n4n\geq 4 and n6,7n\neq 6,7, by Corollary 21 these actions are extendable. In the case of free actions of AnA_{n} for n=6,7n=6,7, we notice that the Sylow subgroups of A6A_{6} and A7A_{7} have the following isomorphic types {D8,3×3×3,5,7}\{D_{8},\mathbb{Z}_{3}\times\mathbb{Z}_{3}\times\mathbb{Z}_{3},\mathbb{Z}_{5},\mathbb{Z}_{7}\} and because of Proposition 14, we obtain that these free actions are extendable. ∎

3.2 Non-necessarily free action on surfaces

Now we consider non-necessarily free actions of finite abelian groups and dihedral groups. The extension of these actions was already given by Reni-Zimmermann [RZ96] with 33-dimensional methods and by Hidalgo [Hid94] with 22-dimensional methods.

Theorem 23.

Let GG be a finite abelian group with an action on a closed oriented surface where the fixed points are of two types:

  • (i)

    fixed points produced by hyperelliptic involutions, see Figure 6,

    Refer to caption
    Figure 6: Hyperelliptic involutions

    and

  • (ii)

    ramification points with complementary monodromies (signature >2>2).

Then the action is extendable by a 33-dimensional handlebody.

Proof.

The extension is performed in some steps. First, we consider the quotient of the surface by the hyperelliptic involutions in some order and smooth the corners with the aim to obtain a smooth closed oriented surface. The hyperelliptic involutions act in the set of ramification points with signature >2>2 and in the quotient we still have ramifications points grouped into pairs. Then we connect the complementary monodromies by cylinders in order to have a free action over a closed oriented surface. From Theorem 9, we have that this free action is extendable and by the proof of Proposition 15, this extension is by means of a 3-dimensional handlebody. Now we disconnect the complementary monodromies by cutting in each of the cylinders that we glued. Each cylinder has only one fixed point by the proof of Proposition 7. Finally, we extend the action to the original surface by an unfolding process using the hyperelliptic involutions in the reverse order in which we constructed the initial quotient surface. ∎

Theorem 24.

Every action of a dihedral group D2nD_{2n} over a closed orientable surface is extendable by a 33-dimensional handlebody.

Proof.

By Proposition 15, the extension problem reduces to a finite product of the same D2nD_{2n}-cobordism induced by the pair c,aab,ab,aa\langle c,a\rangle\sim\langle ab,a\rangle\sim\langle b,a\rangle^{a}. Thus, it is enough to solve the extension problem for the pair b,a\langle b,a\rangle and for the D2nD_{2n}-cobordism over the pair of pants with entries in [D2n,D2n]=c2[D_{2n},D_{2n}]=\langle c^{2}\rangle. The last reduces to the extension of GG-cobordisms over pair of pants where G=[D2n,D2n]G=[D_{2n},D_{2n}], which follows because the group is cyclic. For the pair b,a\langle b,a\rangle we construct a representative D2nD_{2n}-cobordism and there are two cases to consider:

  • (i)

    For n=2kn=2k, we consider the disjoint union of two spheres, where each one is the gluing of two nn-gons by the boundary. Denote by TT the operation of switching from one sphere to the other and by SS the operation of switching from one nn-gon to the other in the same sphere. The action of aa lifts to the composition Sa=aSSa=aS and the action of bb lifts to the composition Tb=bTTb=bT. We obtain n=2kn=2k fixed points over each sphere plus the north a south poles. Then for each fixed point (except the north and south pole), we remove a small disc around it and we connect the holes for opposite fixed points with a cylinder. In a similar way as for abelian groups, this action extends with the north and south pole as unique ramification points. For k=2k=2, in Figure 7, we draw an illustrator of this construction.

    Refer to caption
    Figure 7: Representative for b,a\langle b,a\rangle with n=2kn=2k (k=1k=1).
  • (ii)

    For n=2k+1n=2k+1, we consider one sphere as the gluing of two nn-gons by the boundary. Denote by SS the operation of switching from one nn-gon to the other. Thus the action of aa lifts to the composition Sa=aSSa=aS and the action of bb lifts to the composition Sb=bSSb=bS. We obtain 2n2n fixed points plus the north a south poles. Then we perform the same procedure to construct the extension of the action, as in the even case.

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