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On extensive amenability of algebras

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Abstract

For a module MM over a cocommutative Hopf algebra A\mathscr A, we define extensive amenability by amenability of its symmetric algebra as a module over Sym⁡(M)#A\operatorname{Sym}(M)\#\mathscr A. Using the author's coalgebraic rounding and quotient theorems, we prove that nonzero extensively amenable modules are amenable, that every module over an amenable Hopf algebra is extensively amenable, and that extensive amenability is preserved and reflected by short exact sequences. For permutation modules this definition agrees, over every field, with extensive amenability of group actions. A final section gives the modifications for exterior algebras and establishes the comparison between the two definitions in several cases.

Amenability of groups developed into a thriving and fundamental notion in part because of the variety of equivalent definitions of the notion: almost-invariant sets, invariant functionals, subexponential decay of return probabilities, triviality of a suitable Poisson boundary, etc., see [2]. The equivalences between the definitions lead both to useful applications and a powerful method of proof of (non)amenability for diverse examples and constructions. For example, an extension of groups is amenable if and only if both subgroup and quotient are amenable, and the implications are of varying difficulty depending on the definition used.

It turned out that it is much more convenient to study more generally the amenability of GG-sets; most notions and results extend, and one may define amenability of a group either as amenability of the regular GG-set GG or equivalently as amenability of all non-empty GG-sets. Remarkably however, amenability does not propagate through extensions: if f:X↠Yf:X\twoheadrightarrow Y is a map of GG-sets, then it is not true that GXG X is amenable if and only if GYG Y and all the fibre actions Gy(f−1(y))G_y(f^{-1}(y)) are amenable.

This led Juschenko, Matte Bon, Monod and de la Salle to introduce extensive amenability, a stronger property of GG-sets, which also characterizes amenable groups and does propagate through extensions [6 Proposition 2.4].

To define amenability of associative algebras, we have essentially only one definition at our disposal:

Definition (Elek [4]). Let A\mathcal A be an algebra over a field k\mathbb{k}. The left A\mathcal A-module MM is amenable if for every ϵ>0\epsilon>0 and every finite S⊆AS\subseteq\mathcal A there is a finite F⊆MF\subseteq M with

dim⁡((F+SF)/F)<ϵdim⁡F.\dim\left((F+SF)/F\right)<\epsilon\dim F.

(Here and throughout, “finite” means “finite-dimensional” when applied to vector spaces. The strict inclusion ‘⊂\subset’ prevents F=0F=0.)

The case in which A\mathcal A is a cocommutative Hopf algebra is of particular interest, covering both group rings and universal enveloppes of Lie algebras, and we restrict ourselves to this case in this article. Note that the 00 module is never amenable. The regular module A\mathcal{A} is amenable if and only if every nonzero A\mathcal{A}-module is amenable, by Corollary 1.2 below; in this case, A\mathcal{A} itself is called amenable. In a previous article, I prove that amenability is preserved by Hopf quotients, Hopf subalgebras, and cleft extensions, see [3 Theorems 1.9, 2.2 and 2.5].

One soon discovers that there is little structure on amenable modules over non-amenable Hopf algebras; for example, a direct sum of an amenable and a non-amenable module is amenable, so amenability need not pass to submodules or quotients. I propose the following definition, to recover preservation under exact sequences (see Theorem E):

Definition A. Let MM be a left A\mathcal{A}-module. It is extensively amenable if the symmetric algebra Sym⁡(M)\operatorname{Sym}(M) is amenable when viewed as a Sym⁡(M)#A\operatorname{Sym}(M)\#\mathcal{A}-module.

Here Sym⁡(M)\operatorname{Sym}(M) is a Hopf algebra with each m∈Mm \in M primitive, and Sym⁡(M)#A\operatorname{Sym}(M)\#\mathcal{A}, which from now on will be written M≀AM \wr\mathcal{A}, is Sym⁡(M)⊗A\operatorname{Sym}(M) \otimes\mathcal{A} qua coalgebra, with multiplication and action

(r#a)(s#b)=∑r(a(1)s)#a(2)b,(r#a)⋅s=r(as).(r \# a)(s \# b) = \sum r(a_{(1)}s) \# a_{(2)}b,\qquad(r \# a)\cdot s = r(as).

The induced action makes Sym⁡(M)\operatorname{Sym}(M) an A\mathcal{A}-module algebra and coalgebra, and M≀AM \wr\mathcal{A} is a cocommutative Hopf algebra.

The zero module is extensively amenable, since Sym⁡(0)=k\operatorname{Sym}(0)=k, although it is not amenable. More generally,

Proposition B. Every locally finite A\mathcal{A}-module (namely, a module in which every finite subspace is contained in a finite submodule) is extensively amenable.

Proof. For given finite S≤M≀AS \leq M \wr\mathcal{A}, choose a finite A\mathcal{A}-submodule V≤MV \leq M containing all variables in SS’s polynomial coefficients. Set q=dim⁡Vq=\dim V, and bound the degrees of those coefficients by dd. The A\mathcal{A}-action preserves polynomial degree. For En=Sym⁡≤n(V)E_n=\operatorname{Sym}^{\leq n}(V), the expanded space is contained in Sym⁡≤n+d(V)\operatorname{Sym}^{\leq n+d}(V), so its expansion ratio is at most

(n+d+qq)/(n+qq)⟶1.\binom{n+d+q}{q}\bigg/\binom{n+q}{q} \longrightarrow1.

The main results of this article are:

Theorem C (= Theorem 2.1). Every nonzero extensively amenable A\mathcal{A}-module is amenable.

Theorem D (= Theorem 2.2). Every module over an amenable cocommutative Hopf algebra is extensively amenable. In particular, its regular module is extensively amenable.

Theorem E (= Theorem 3.1). For every exact sequence of A\mathcal{A}-modules

0⟶M⟶N⟶P⟶0,0 \longrightarrow M \longrightarrow N \longrightarrow P \longrightarrow0,

NN is extensively amenable if and only if MM and PP are extensively amenable.

The following proves, in the case of extensive amenability, the corresponding result [1 Theorem 1.4] for usual amenability:

Theorem F (= Theorem 4.1). For every field kk and every GG-set XX, the permutation k[G]k[G]-module k[X]k[X] is extensively amenable if and only if G↷XG \curvearrowright X is extensively amenable.

In fact, there is quite a broad flexibility in the definition of extensive amenability of GG-sets. One may replace the functor (Z/2)(X)(\mathbb{Z}/2)^{(X)} by B(X)B^{(X)} for any nontrivial amenable group BB, or by Sym⁡fin(X)\operatorname{Sym}_{\mathrm{fin}}(X), the group of finitely supported permutations of XX, see [6 Theorem 1.3 and Examples 3.1–3.2].

Other functorial constructions VectorSpace →\to AmenableAlgebra may be used in place of the symmetric algebra, provided they carry a compatible induced A\mathcal{A}-action and Hopf structure. I have not gone into the general theory which is beyond my non-AI brain, but contented myself with the exterior algebra, interpreted as a Hopf superalgebra, and call MM ∧\wedge-extensively amenable when ⋀M\bigwedge M is amenable under multiplication and the induced A\mathcal{A}-action. We regard A\mathcal{A} as purely even and MM as purely odd in the Hopf superalgebra ⋀M#A\bigwedge M \mathrel{\#} \mathcal{A}.

I have managed to prove that all the above main results remain valid for ∧\wedge-extensive amenability, but not that MM is extensively amenable if and only if it is ∧\wedge-extensively amenable, in contrast with the group case.

Acknowledgments to humans and AI. I am grateful to Mikael de la Salle for numerous stimulating discussions on this topic. My definition of extensive amenability for algebras is directly inspired from the group case.

ChatGPT 5.6 Sol was used to assist with drafting, editing, checking parts of this manuscript, and exploratory formal verification. All mathematical content was reviewed, checked, and substantially revised by the author, who is responsible for the final text.

The main results have been formalized in Lean/Mathlib and are available at

https://github.com/laurentbartholdi/hopfamenability

Two transfer lemmas

In equations “dim((F+SF)/F)<ϵdim⁡F((F+SF)/F)<\epsilon\dim F”, we refer to SS as a testing space and FF as a Følner space. By the fundamental theorem of coalgebras, finite testing spaces in a Hopf algebra may be enlarged to finite subcoalgebras containing 11. We use this reduction below.

The following is the tensor-space form of the argument proving [3 Theorem 1.9]. We record the slight strengthening needed below.

Lemma 1.1 (Tensor-factor extraction). Let H\mathcal{H} be a cocommutative Hopf algebra, let U,VU,V be left H\mathcal{H}-modules, and give U⊗VU\otimes V the diagonal H\mathcal{H}-action. If F≤HF\leq\mathcal{H} is a finite subcoalgebra containing 11, then for every nonzero finite E≤U⊗VE\leq U\otimes V there is a nonzero finite V0≤VV_0\leq V such that

dim⁡FV0dim⁡V0≤dim⁡FEdim⁡E.\frac{\dim FV_0}{\dim V_0}\leq\frac{\dim FE}{\dim E}.

Consequently, if U⊗VU\otimes V contains an amenable H\mathcal{H}-submodule, then VV is amenable.

Proof. Put E+=FEE^+=FE and choose a finite subspace W≤VW\leq V containing all second tensor coefficients of EE and E+E^+. For Z=E,E+Z=E,E^+ put rZ(L)=dim⁡(Z∩(U⊗L))r_Z(L)=\dim(Z\cap(U\otimes L)). The functions rZr_Z are monotone and supermodular on the subspace lattice of WW. For t>0t>0, let Ct(Z)C_t(Z) be the largest maximizer of rZ(L)−tdim⁡Lr_Z(L)-t\dim L, which exists by [3 Lemma 1.2]. These are also maximizers over all finite subspaces of VV: replacing LL by L∩WL\cap W leaves its rank unchanged and cannot increase its dimension.

First suppose that FF has a complete subcoalgebra flag 0=F0<⋯<Fs=F0=F_0<\cdots<F_s=F. We claim that FCt(E)⊆Ct(E+)FC_t(E)\subseteq C_t(E^+). Write C=Ct(E)C=C_t(E), C+=Ct(E+)C^+=C_t(E^+), and suppose inductively that Fi−1C⊆C+F_{i-1}C\subseteq C^+. For a∈Fi∖Fi−1a\in F_i\setminus F_{i-1}, there is a group-like g∈Fig\in F_i, by the codimension-one argument in [3 Proposition 1.8], with Δ(a)−g⊗a∈Fi⊗Fi−1\Delta(a)-g\otimes a\in F_i\otimes F_{i-1}. Set K={c∈C:ac∈C+}K=\{c\in C:ac\in C^+\}, let q:V→V/C+q:V\to V/C^+ be the quotient map, and put aˉ:C→V/C+\bar a:C\to V/C^+, aˉ(c)=q(ac)\bar a(c)=q(ac). Write δa\delta_a for the diagonal action of aa on U⊗VU\otimes V, and αg\alpha_g for the action of gg on UU. The relation for Δ(a)\Delta(a) and the inductive inclusion Fi−1C⊆C+F_{i-1}C\subseteq C^+ give

(id⁡U⊗q)δa(z)=(gU⊗aˉ)(z)(z∈U⊗C).(\operatorname{id}_U\otimes q)\delta_a(z)=(g_U\otimes\bar a)(z)\qquad(z\in U\otimes C).

Since gUg_U is invertible with inverse S(g)US(g)_U and ker⁡aˉ=K\ker\bar a=K, exactness of the tensor product gives

ker⁡(gU⊗aˉ)=U⊗K.\ker(g_U\otimes\bar a)=U\otimes K.

Moreover, δa(E)≤E+\delta_a(E)\leq E^+, because a∈Fa\in F, and the same triangular relation gives δa(U⊗C)≤U⊗(C++aC)\delta_a(U\otimes C)\leq U\otimes(C^++aC). Thus the restriction of δa\delta_a to E∩(U⊗C)E\cap(U\otimes C), followed by quotienting by E+∩(U⊗C+)E^+\cap(U\otimes C^+), has kernel exactly E∩(U⊗K)E\cap(U\otimes K). It therefore induces an injection

E∩(U⊗C)E∩(U⊗K)⟶E+∩(U⊗(C++aC))E+∩(U⊗C+).\frac{E\cap(U\otimes C)}{E\cap(U\otimes K)} \longrightarrow \frac{E^+\cap(U\otimes(C^++aC))}{E^+\cap(U\otimes C^+)}.

Maximality of CC bounds the dimension on the left below by t(dim⁡C−dim⁡K)t(\dim C-\dim K); rank-nullity identifies this with t(dim⁡(C++aC)−dim⁡C+)t(\dim(C^++aC)-\dim C^+). Hence C++aCC^++aC is also a maximizer for E+E^+, and the choice of the largest maximizer gives aC⊆C+aC\subseteq C^+.

The density/coarea identity [3 Lemma 1.2] now gives

∫0∞dim⁡Ct(E) dt=dim⁡E,∫0∞dim⁡FCt(E) dt≤dim⁡E+.\int_0^\infty\dim C_t(E)\,dt=\dim E,\qquad \int_0^\infty\dim FC_t(E)\,dt\leq\dim E^+.

Some nonzero Ct(E)C_t(E) has the asserted ratio.

For the general case, split a subcoalgebra flag after a finite field extension and descend the ratio, using [3 Lemmas 1.6 and 1.7].

Corollary 1.2. Let A\mathcal A be a commutative Hopf algebra. The regular module AA\mathcal A\mathcal A is amenable if and only if every nonzero left A\mathcal A-module is amenable.

Proof. The reverse implication follows by taking the regular module. Conversely, suppose that A\mathcal A is amenable and let M≠0M\ne0. The linear isomorphism

T:A⊗M→A⊗M,a⊗m↦∑a(1)⊗a(2)m,T:\mathcal A\otimes M\to\mathcal A\otimes M,\qquad a\otimes m\mapsto\sum a_{(1)}\otimes a_{(2)}m,

with inverse a⊗m↦∑a(1)⊗S(a(2))ma\otimes m\mapsto\sum a_{(1)}\otimes S(a_{(2)})m, intertwines the action on the first factor with the diagonal action. For any fixed 0≠m∈M0\ne m\in M, the diagonal module therefore contains the amenable submodule T(A⊗km)≃AAT(\mathcal A\otimes km)\simeq\mathcal A\mathcal A. Lemma 1.1 makes MM amenable.

For commutative Hopf algebras H≤B\mathcal H\leq\mathcal B, let Q=B/BKQ=\mathcal B/\mathcal B\mathcal K be the quotient left B\mathcal B-module coalgebra, with quotient map qq. The left QQ-coaction on B\mathcal B is ρ=(q⊗id⁡)ΔB:B→Q⊗B\rho=(q\otimes\operatorname{id})\Delta_{\mathcal B}:\mathcal B\to Q\otimes\mathcal B.

Lemma 1.3 (Normal-basis induction). Let H≤B\mathcal H\leq\mathcal B be cocommutative Hopf algebras. Suppose there is a linear section σ:Q→B\sigma:Q\to\mathcal B of qq for which

Θ:Q⊗H→B,c⊗k↦σ(c)k\Theta:Q\otimes\mathcal H\to\mathcal B,\qquad c\otimes k\mapsto\sigma(c)k

is a right H\mathcal H-module and left QQ-comodule isomorphism, where the source coaction is ΔQ⊗id⁡\Delta_Q\otimes\operatorname{id}. If QQ is amenable over B\mathcal B and VV is amenable over H\mathcal H, then B⊗V\mathcal B\otimes V is amenable over B\mathcal B.

Proof. Let F≤BF\leq\mathcal B be a finite subcoalgebra containing 11, and fix 0<δ0<\delta. By [3 Theorem 1.1], choose a nonzero finite subcoalgebra C≤QC\leq Q with dim⁡FC<(1+δ)dim⁡C\dim FC<(1+\delta)\dim C, and put D=FCD=FC. Collinearity and the module-coalgebra identity give

ρ(Fσ(C))≤D⊗B.(1)\rho(F\sigma(C))\leq D\otimes\mathcal B. \tag*{(1)}

Applying id⁡Q⊗Θ−1\operatorname{id}_{Q} \otimes\Theta^{-1} and using QQ-colinearity of Θ\Theta, we obtain

(ΔQ⊗id⁡K)Θ−1(Fσ(C))≤D⊗Q⊗K,(\Delta_{Q} \otimes\operatorname{id}_{\mathcal{K}})\Theta^{-1}(F\sigma(C)) \le D \otimes Q \otimes\mathcal{K},

and applying Θ(id⁡Q⊗εQ⊗id⁡K)\Theta(\operatorname{id}_{Q}\otimes\varepsilon_{Q}\otimes\operatorname{id}_{\mathcal{K}}) yields Fσ(C)≤Θ(D⊗K)F\sigma(C) \le\Theta(D\otimes\mathcal{K}). Consequently there is a finite T≤KT\le\mathcal{K}, containing 11, such that Fσ(C)≤σ(D)TF\sigma(C)\le\sigma(D)T. Choose a finite E≤VE\le V with dim⁡TE<(1+δ)dim⁡E\dim TE<(1+\delta)\dim E. The induced vector-space identification B⊗KV≅Q⊗V\mathcal{B}\otimes_{\mathcal{K}}V\cong Q\otimes V then gives, for W=C⊗EW=C\otimes E,

FW≤D⊗TE,dim⁡FWdim⁡W<(1+δ)2.FW\le D\otimes TE,\qquad\frac{\dim FW}{\dim W}<(1+\delta)^2.

Let δ\delta tend to zero. □\square

Amenability and extensively amenable modules

Theorem 2.1. Every nonzero extensively amenable A\mathcal{A}-module is amenable.

Proof. Let MM be a nonzero extensively amenable A\mathcal{A}-module and let

d:Sym⁡(M)→Sym⁡(M)⊗M,d(m)=1⊗md:\operatorname{Sym}(M)\to\operatorname{Sym}(M)\otimes M,\qquad d(m)=1\otimes m

be the universal derivation. It is A\mathcal{A}-linear for the diagonal action and by the Leibniz identity satisfies

d(m1⋯mk)=∑i=1km1⋯mi^⋯mk⊗mi.d(m_1\cdots m_k)=\sum_{i=1}^{k}m_1\cdots\widehat{m_i}\cdots m_k\otimes m_i.

Fix a finite F≤AF\le\mathcal{A} containing 11, a nonzero m∈Mm\in M, and η>0\eta>0. Extensive amenability gives a finite E≤Sym⁡(M)E\le\operatorname{Sym}(M) such that

Z=FE+F(mE) satisfies dim⁡Z<(1+η)dim⁡E.Z=FE+F(mE)\text{ satisfies }\dim Z<(1+\eta)\dim E.

Put E′=E+mEE'=E+mE and V=d(E′)V=d(E'). The map

E→V⊕V,u↦(d(u),d(mu))E\to V\oplus V,\qquad u\mapsto(d(u),d(mu))

is injective: if both coordinates vanish, the Leibniz identity gives u⊗m=0u\otimes m=0, hence u=0u=0. Thus dim⁡E≤2dim⁡V\dim E\le2\dim V. Since dd is A\mathcal{A}-linear, d(FE′)=FVd(FE')=FV, so dd induces a surjection FE′/E′↠FV/VFE'/E'\twoheadrightarrow FV/V. As FE′=ZFE'=Z and E≤E′E\le E', we have

dim⁡FV−dim⁡V≤dim⁡FE′−dim⁡E′<ηdim⁡E≤2ηdim⁡V.\dim FV-\dim V\le\dim FE'-\dim E'<\eta\dim E\le2\eta\dim V.

Hence Sym⁡(M)⊗M\operatorname{Sym}(M)\otimes M is amenable. Lemma 1.1 extracts Følner spaces in MM. □\square

Theorem 2.2. Every module over an amenable cocommutative Hopf algebra is extensively amenable. In particular, its regular module is extensively amenable.

Proof. The commutative Hopf algebra Sym⁡(M)\operatorname{Sym}(M) is amenable [3 Theorem 2.4]. The split cleft extension

k⟶Sym⁡(M)⟶M≀A⟶A⟶k\mathbb{k}\longrightarrow\operatorname{Sym}(M)\longrightarrow M\wr\mathcal{A}\longrightarrow\mathcal{A}\longrightarrow\mathbb{k}

therefore makes M≀AM\wr\mathcal{A} amenable by [3 Theorem 2.5]. Its nonzero module Sym⁡(M)\operatorname{Sym}(M) is amenable by Corollary 1.2. □\square

Exact sequences

We first recall an elementary filtered-space observation. For compatible increasing exhaustive filtrations (Rn)n≥−1(R_n)_{n\geq-1} and (Vn)n≥−1(V_n)_{n\geq-1} on an algebra RR and an RR-module VV, with R−1=V−1=0R_{-1}=V_{-1}=0, amenability of VV implies amenability of gr⁡V\operatorname{gr} V over gr⁡R\operatorname{gr} R. Indeed, lift a finite homogeneous subspace F‾≤gr⁡R\overline{F}\leq\operatorname{gr} R to F≤RF\leq R, take a Følner space EE, and put E′=E+FEE'=E+FE. Then

gr⁡E+F‾gr⁡E≤gr⁡E′,dim⁡gr⁡E=dim⁡E,dim⁡gr⁡E′=dim⁡E′.\operatorname{gr} E+\overline{F}\operatorname{gr} E\leq\operatorname{gr} E',\qquad\dim\operatorname{gr} E=\dim E,\qquad\dim\operatorname{gr} E'=\dim E'.

This is the leading-symbol argument of [3 Lemma 7.2]; the exhaustive nonnegative filtration ensures that the induced filtrations on finite spaces preserve dimension. The same argument applies to decreasing filtrations V=V0≥V1≥⋯V=V_0\geq V_1\geq\cdots with ⋂nVn=0\bigcap_n V_n=0: their intersections with any finite-dimensional space eventually vanish. In particular, for an already graded algebra and module one may take homogeneous Følner spaces, after enlarging the finite testing space to a homogeneous one.

Theorem 3.1. For every exact sequence of A\mathcal{A}-modules

0⟶M⟶N⟶P⟶0,0\longrightarrow M\longrightarrow N\longrightarrow P\longrightarrow0,

NN is extensively amenable if and only if both MM and PP are extensively amenable.

Proof. Suppose first that NN is extensively amenable. Give NN the two-step filtration 0≤M≤N0\leq M\leq N, giving MM weight zero and N/M≅PN/M\cong P in degree 1. Then gr⁡N≅M⊕P\operatorname{gr}N\cong M\oplus P, and the induced multiplicative filtrations satisfy

gr⁡Sym⁡(N)≅Sym⁡(M⊕P),gr⁡(N≀A)≅Sym⁡(M⊕P)#A.\operatorname{gr}\operatorname{Sym}(N)\cong\operatorname{Sym}(M\oplus P),\qquad\operatorname{gr}(N\wr\mathcal{A})\cong\operatorname{Sym}(M\oplus P)\mathbin{\#}\mathcal{A}.

The preceding observation proves that M⊕PM\oplus P is extensively amenable. The two projections of M⊕PM\oplus P induce surjective counital module-coalgebra maps to Sym⁡(M)\operatorname{Sym}(M) and Sym⁡(P)\operatorname{Sym}(P). The quotient theorem [3 Theorem 1.9], with the actions factored through M≀AM\wr\mathcal{A} and P≀AP\wr\mathcal{A}, proves both conclusions.

Conversely, take B=N≀A\mathcal{B}=N\wr\mathcal{A}, K=M≀A\mathcal{K}=M\wr\mathcal{A}, and Q=B/Bker⁡εK≅Sym⁡(P)\mathcal{Q}=\mathcal{B}/\mathcal{B}\ker\varepsilon_{\mathcal{K}}\cong\operatorname{Sym}(P), with quotient map qq and coaction ρ=(q⊗id⁡)ΔB\rho=(q\otimes\operatorname{id})\Delta_{\mathcal{B}}. A vector-space section P→NP\to N induces an algebra and coalgebra section σ:Sym⁡(P)→Sym⁡(N)≤B\sigma:\operatorname{Sym}(P)\to\operatorname{Sym}(N)\leq\mathcal{B}. Multiplication gives

Θ:Sym⁡(P)⊗K→ ≅ B,p⊗k↦σ(p)k.\Theta:\operatorname{Sym}(P)\otimes\mathcal{K}\xrightarrow{\ \cong\ }\mathcal{B},\qquad p\otimes k\mapsto\sigma(p)k.

It is a right K\mathcal{K}-module isomorphism by the polynomial normal form, and is colinear because ρ(σ(p))=∑σ(p(1))⊗σ(p(2))\rho(\sigma(p))=\sum\sigma(p_{(1)})\otimes\sigma(p_{(2)}) and q(bk)=q(b)ε(k)q(bk)=q(b)\varepsilon(k). The B\mathcal{B}-action on Sym⁡(P)\operatorname{Sym}(P) factors through P≀AP\wr\mathcal{A}, so B(Sym⁡(P))\mathcal{B}(\operatorname{Sym}(P)) is amenable. Apply Lemma 1.3 to the amenable K\mathcal{K}-module Sym⁡(M)\operatorname{Sym}(M). The action map

B⊗KSym⁡(M)⟶Sym⁡(N),(r#a)⊗s↦r(a⋅s),\mathcal{B}\otimes_{\mathcal{K}}\operatorname{Sym}(M)\longrightarrow\operatorname{Sym}(N),\qquad(r\mathbin{\#}a)\otimes s\mapsto r(a\cdot s),

identifies these modules, proving that NN is extensively amenable. □

Corollary 3.2. Extensive amenability passes to submodules and quotients, is closed under extensions and direct sums, and is local on directed unions of A\mathcal{A}-submodules.

Proof. The first assertions and the finite direct-sum assertion follow from Theorem 3.1. If M=⋃iMiM=\bigcup_i M_i is directed and every MiM_i is extensively amenable, the coefficients of any finite subspace of M≀AM\wr\mathcal{A} lie in some Sym⁡(Mi)\operatorname{Sym}(M_i); a Følner space there works in Sym⁡(M)\operatorname{Sym}(M). The converse follows by submodule permanence. Arbitrary direct sums are directed unions of finite ones. □

Group actions and permutation modules

Juschenko, Matte Bon, Monod and de la Salle call a GG-set XX extensively amenable if there is a GG-invariant mean on the collection Pf(X)\mathcal{P}_{f}(X) of finite subsets of XX giving mass one to {B:T⊆B}\{B : T \subseteq B\} for every finite T⊆XT \subseteq X, see [6 Definition 1.1] or [2 Definition 9.1]. We immediately pass to an equivalent definition, see [6 Theorem 1.3]: with L=Z(X)L = \mathbb{Z}^{(X)}, XX is extensively amenable if and only if the affine action L⋊G↷LL \rtimes G \curvearrowright L is amenable.

In case A\mathcal{A} is a group ring k[G]k[G], our wreath product M≀A=Sym⁡(M)#AM \wr\mathcal{A} = \operatorname{Sym}(M) \# \mathcal{A} is also known as the crossed product algebra Sym⁡(M)⋊G\operatorname{Sym}(M) \rtimes G.

Theorem 4.1. For every field kk and every GG-set XX, the permutation k[G]k[G]-module k[X]k[X] is extensively amenable if and only if G↷XG \curvearrowright X is extensively amenable.

Proof. Set L=Z(X)L = \mathbb{Z}^{(X)} and R=k[L]R = k[L], and write uxu_x for the standard generators of LL and zx=ux−1z_x = u_x - 1. Let ϖ=ker⁡(ϵ:R→k)\varpi= \ker(\epsilon: R \to k) be the augmentation ideal, and filter RR by ϖn\varpi^n. The classical description of the augmentation filtration of a free abelian group gives

⋂n≥0ϖn=0,gr⁡ϖR=Sym⁡k(k⊗ZL)≃Sym⁡(k[X]),\bigcap_{n \ge0} \varpi^n = 0, \qquad\operatorname{gr}_{\varpi} R = \operatorname{Sym}_{k}(k \otimes_{\mathbb{Z}} L) \simeq\operatorname{Sym}(k[X]),

see [7 Chapter VI and Corollary VIII.8.2]. The isomorphism sends xx to the initial form of ux−1u_x - 1, so is GG-equivariant. Since GG preserves ϖ\varpi, the compatible filtration (R#k[G])n=ϖn#k[G](R \# k[G])_n = \varpi^n \# k[G] gives

gr⁡(R#k[G])≃Sym⁡(k[X])#k[G].(2)\operatorname{gr}(R \# k[G]) \simeq\operatorname{Sym}(k[X]) \# k[G]. \tag*{(2)}

Here R#k[G]≃k[L⋊G]R \# k[G] \simeq k[L \rtimes G], and RR is the permutation module of the affine action L⋊G↷LL \rtimes G \curvearrowright L. By the preceding criterion and the permutation-module equivalence [3 §3], it suffices to prove that Sym⁡(k[X])\operatorname{Sym}(k[X]) is amenable under Sym⁡(k[X])#k[G]\operatorname{Sym}(k[X]) \# k[G] if and only if RR is amenable under R#k[G]R \# k[G].

Suppose first that Sym⁡(k[X])\operatorname{Sym}(k[X]) is amenable under k[X]≀k[G]k[X] \wr k[G]. The GG-equivariant map

Sym⁡(k[X])⟶R,x↦zx\operatorname{Sym}(k[X]) \longrightarrow R, \qquad x \mapsto z_x

identifies the symmetric algebra with the polynomial subalgebra k[zx:x∈X]k[z_x : x \in X]; these are also the canonical lifts of the generators in gr⁡ϖR≃Sym⁡(k[X])\operatorname{gr}_{\varpi} R \simeq\operatorname{Sym}(k[X]). If EE is a Følner space in Sym⁡(k[X])\operatorname{Sym}(k[X]), let E~\widetilde{E} be its image in RR. For g∈Gg \in G the expansion ratios of EE and E~\widetilde{E} agree, while E~+uxE~=E~+zxE~\widetilde{E} + u_x\widetilde{E} = \widetilde{E} + z_x\widetilde{E} shows that multiplication by uxu_x has the same boundary as multiplication by zxz_x.

For any finite-dimensional subspace WW and invertible linear operators a,ba,b on its ambient space, put bW(a)=dim⁡(W+aW)−dim⁡Wb_W(a) = \dim(W + aW) - \dim W. Then

bW(ab)≤bW(a)+bW(b),bW(a−1)=bW(a).(3)b_W(ab) \leq b_W(a) + b_W(b), \qquad b_W(a^{-1}) = b_W(a). \tag*{(3)}

The first inequality follows by enlarging W+abWW + abW to W+aW+abWW + aW + abW; the additional dimension beyond W+aWW + aW is at most dim⁡((aW+abW)/aW)=dim⁡((W+bW)/W)=bW(b)\dim((aW + abW)/aW) = \dim((W + bW)/W) = b_W(b); the second follows by applying aa to W+a−1WW + a^{-1}W. Given a finite subset of L⋊GL \rtimes G, express its elements as words in finitely many ux±1u_x^{\pm1} and elements of GG. Choose EE simultaneously Følner for the corresponding variables xx and group operators, with error small compared with the sum of the word lengths. By (4.2) and

dim⁡(W+∑jajW)−dim⁡W≤∑jbW(aj),\dim\left(W + \sum_j a_jW\right) - \dim W \leq\sum_j b_W(a_j),

the image E~\widetilde{E} is Følner for the prescribed finite subset. Thus RR is amenable under R#k[G]R \# k[G], so the affine action is amenable and G↷XG \curvearrowright X is extensively amenable.

Conversely, suppose that RR is amenable under R#k[G]R \#_{\mathbb{k}}[G]. The separated-filtration argument preceding Theorem 3.1 proves that amenability is preserved on the associated graded, so k[X]\mathbb{k}[X] is extensively amenable by (4.1). □

By the lamp-functor theorem [6 Theorem 1.3], or its action-valued form [2 Proposition 9.5], these conditions are also equivalent to amenability of the affine actions

L(X)⋊G↷L(X)L^{(X)} \rtimes G \curvearrowright L^{(X)}

for L=Z/2L = \mathbb{Z}/2, L=ZL = \mathbb{Z}, or L=(k,+)L = (\mathbb{k},+). We used L=ZL = \mathbb{Z} in the proof above, and will consider L=Z/2L = \mathbb{Z}/2 in § 5.

The exterior algebra version

We consider a variant of the definition of extensive amenability: let us call the A\mathcal{A}-module MM Λ\Lambda-extensively amenable if the exterior algebra ⋀M\bigwedge M is amenable under multiplication and the induced A\mathcal{A}-action. The results above have exterior analogues, but outside characteristic two one must retain the supercoalgebra signs. We give the required modifications.

Superalgebras and the coalgebra arguments

Regard A\mathcal{A} as purely even and MM as purely odd. We work in supervector spaces, with the conventions

(u⊗v)(u′⊗v′)=(−1)∣v∣∣u′∣uu′⊗vv′,τ(u⊗v)=(−1)∣u∣∣v∣v⊗u.(u \otimes v)(u' \otimes v') = (-1)^{|v||u'|}uu' \otimes vv', \qquad\tau(u \otimes v) = (-1)^{|u||v|}v \otimes u.

Here as usual ∣u∣|u| denotes degree. The exterior algebra ⋀M\bigwedge M is a supercommutative, supercocommutative Hopf superalgebra with Δ(m)=m⊗1+1⊗m\Delta(m) = m \otimes1 + 1 \otimes m and ε(m)=0\varepsilon(m) = 0. Every m∈Mm \in M satisfies m2=0m^2 = 0 in ⋀M\bigwedge M. Put

M≀∧A=⋀M#A,M \wr_{\wedge} \mathcal{A} = \bigwedge M \# \mathcal{A},

a Hopf superalgebra admitting ⋀M\bigwedge M as a supermodule coalgebra. Both ⋀M\bigwedge M and M≀∧AM \wr_{\wedge} \mathcal{A} are N\mathbb{N}-graded objects. Following the observation preceding Theorem 3.1, we may restrict our considerations to degree-graded Følner spaces.

We unfortunately need to reprove some of the previous results in the setting of Hopf superalgebras. We gather the required conclusions in the following lemma.

Lemma 5.1. Let H\mathcal{H} be a nonnegatively graded Hopf superalgebra, with parity given by degree modulo two and cocommutative degree-zero part. For compatibly nonnegatively graded objects and degree-preserving maps, the conclusions of [3 Theorems 1.1 and 1.9] (coalgebraic rounding and module-coalgebra quotient permanence), and Lemmas 1.1 and 1.3 hold in the superalgebra convention. In the quantitative statements the finite testing subcoalgebras and input subspaces are assumed homogeneous, and the resulting subcoalgebras or subspaces may be chosen homogeneous. The amenability conclusions hold for arbitrary finite testing spaces.

Proof. Every finite subspace of a graded coalgebra is contained in a finite graded subcoalgebra: take a finite subcoalgebra containing it and then its homogeneous hull. Indeed, if pnp_n denotes projection to degree nn, then

Δ(pnc)=∑i+j=n(pi⊗pj)Δ(c).\Delta(p_n c) = \sum_{i+j=n}(p_i \otimes p_j)\Delta(c).

Thus arbitrary finite testing spaces may be enlarged to homogeneous subcoalgebras containing 11; the filtered-space observation preceding Theorem 3.1 then supplies homogeneous Følner spaces.

Complete homogeneous subcoalgebra flags exist by coalgebra duality: let 0≠F=⨁n≥0Fn≤H0 \ne F = \bigoplus_{n \ge0} F_n \leq\mathcal{H} be a finite graded subcoalgebra, put Ω=k‾\Omega= \overline{\mathbb{k}}, and consider the ordinary convolution algebra R=(Ω⊗F)∗\mathcal{R} = (\Omega\otimes F)^*, with product

(fg)(c)=∑f(c(1))g(c(2)).(fg)(c) = \sum f(c_{(1)})g(c_{(2)}).

Give RR the grading Rn=(Ω⊗Fn)∗R_n=(\Omega\otimes F_n)^*, extending functionals by zero on the other degrees. Then RiRj⊆Ri+jR_iR_j\subseteq R_{i+j}, so R>0R_{>0} is a nilpotent two-sided ideal. Moreover, R/R>0≃R0R/R_{>0}\simeq R_0 is commutative, since F0F_0 is commutative. Thus, writing J0J_0 for the radical of R0R_0, we have

J:=rad⁡R=J0⊕R>0,R/J≃ΩrJ:=\operatorname{rad} R=J_0\oplus R_{>0},\qquad R/J\simeq\Omega^r

for some rr. In particular, JJ is homogeneous and nilpotent, while R/JR/J is concentrated in degree zero.

For every m≥0m\geq0, the radical layer Jm/Jm+1J^m/J^{m+1} is a graded bimodule over R/JR/J. Its left and right actions commute and preserve each degree; equivalently, it is a graded module over

(R/J)⊗Ω(R/J)op≃Ωr2.(R/J)\otimes_{\Omega}(R/J)^{\mathrm{op}}\simeq\Omega^{r^2}.

This algebra is split semisimple and concentrated in degree zero, so each layer is a direct sum of homogeneous one-dimensional sub-bimodules. Refining each radical layer by these summands and taking inverse images gives a complete flag of homogeneous two-sided ideals of RR. Their ordinary annihilators give, in reverse order, a complete homogeneous subcoalgebra flag in Ω⊗F\Omega\otimes F. Indeed, if II is a two-sided ideal and c∈I⊥c\in I^\perp, then Δ(c)\Delta(c) annihilates I⊗R+R⊗II\otimes R+R\otimes I, whence Δ(c)∈I⊥⊗I⊥\Delta(c)\in I^\perp\otimes I^\perp.

Finally, a homogeneous basis adapted to the flag involves only finitely many coefficients in Ω\Omega. They generate a finite extension of kk, over which the entire homogeneous subcoalgebra flag is defined.

For a homogeneous codimension-one step F′⊂F′+kaF'\subset F'+k a, write

Δ(a)−a⊗g∈F′⊗(F′+ka),Δ(a)−h⊗a∈(F′+ka)⊗F′,\Delta(a)-a\otimes g\in F'\otimes(F'+k a),\qquad\Delta(a)-h\otimes a\in(F'+k a)\otimes F',

where g,hg,h are even group-like elements. The super module-coalgebra identity is

Δ(ac)=∑(−1)∣a(2)∣∣c(1)∣a(1)c(1)⊗a(2)c(2).\Delta(ac)=\sum(-1)^{|a_{(2)}||c_{(1)}|}a_{(1)}c_{(1)}\otimes a_{(2)}c_{(2)}.

More explicitly, let CC be a finite graded subcoalgebra of an H\mathcal{H}-module coalgebra, not necessarily H\mathcal{H}-stable, and let D⊆(F′+ka)CD\subseteq(F'+ka)C be a graded subcoalgebra. Put V=D+F′CV=D+F'C and ϕ:C→(F′+ka)C/V\phi:C\to(F'+ka)C/V, c↦ac+Vc\mapsto ac+V, as in [3 Proposition 1.8]. On underlying vector spaces, using ordinary tensor products of linear operators, the first triangular relation gives (ϕ⊗g)Δ(c)=0(\phi\otimes g)\Delta(c)=0 on ker⁡ϕ\ker\phi; the second gives (hΠ[a]⊗ϕ)Δ(c)=0(h\Pi^{[a]}\otimes\phi)\Delta(c)=0, where Π(c)=(−1)∣c∣c\Pi(c)=(-1)^{|c|}c. Since gg and hΠ[a]h\Pi^{[a]} are invertible on the ambient module, their restrictions to CC are injective, and the two tensor-kernel arguments are unchanged. Their intersection shows that ker⁡ϕ\ker\phi is a graded subcoalgebra. The dimension inequalities in [3 Proposition 1.8] therefore telescope unchanged along the homogeneous flag. To remove the splitting assumption, extend scalars to a finite splitting field. The tensor-amplification and base-change arguments of [3 Lemmas 1.4–1.5] apply with a purely even field-extension factor and graded subspaces, so preserve semistability on the lattice of graded subcoalgebras. Apply the split transfer inequality to scalar extensions of the original graded data and descend it by preservation of dimensions and intersections. The density and comparison arguments of [3 Lemmas 1.2–1.3] and the proof of Theorem 1.1 then give rounding on the lattice of graded subcoalgebras over the original field; no descent of the rounded subcoalgebra is needed.

Likewise, in Lemma 1.1, the leading action on U⊗VU\otimes V is hΠU[a]⊗ah\Pi^{[a]}_{U}\otimes a; its first factor is invertible. Use graded subspaces in the density argument, and descend the extracted subspace’s expansion ratio by [3 Lemma 1.7]; its coefficient filtration preserves homogeneity. This ratio descent is used only for subspaces, not for subcoalgebras. For an even counital coalgebra quotient q:C→Qq:C\to Q, the map $(\operatorname{id}\otimes q)\Delta_C:C\to C\otimes Q remains an injective H\mathcal{H}-module map with the super diagonal action, proving quotient permanence. Finally, the normal-basis proof uses only rounding, colinearity and dimensions, and is unchanged with graded spaces.

Permanence and ordinary amenability.

Theorem 5.2. Proposition B, Theorems 2.1, 2.2 and 3.1, and Corollary 3.2 remain valid with “extensively amenable” replaced by “⋀\bigwedge-extensively amenable”.

Proof. For a locally finite module, ⋀V\bigwedge V, with VV a sufficiently large finite invariant subspace, is already a finite invariant space for the given test.

For an exact sequence, the weight filtration used in Theorem 3.1 again has associated graded ⋀(M⊕P)\bigwedge(M\oplus P). (In applying Lemma 5.1, the nonnegative grading is still total exterior degree.) Quotient permanence from Lemma 5.1 gives descent to MM and PP. For ascent put B=N⋊∧A\mathcal{B}=N\rtimes_{\wedge}\mathcal{A}, K=M⋊∧A\mathcal{K}=M\rtimes_{\wedge}\mathcal{A}, and Q=⋀PQ=\bigwedge P. A linear splitting P→NP\to N induces a graded Hopf-superalgebra section σ:⋀P→⋀N⊆B\sigma:\bigwedge P\to\bigwedge N\subseteq\mathcal{B}. Exterior normal form gives the right-K\mathcal{K} isomorphism Θ(p⊗k)=σ(p)k\Theta(p\otimes k)=\sigma(p)k, and

(q⊗id⁡)ΔB(σ(p))=∑p(1)⊗σ(p(2)).(q\otimes\operatorname{id})\Delta_{\mathcal{B}}(\sigma(p))=\sum p_{(1)}\otimes\sigma(p_{(2)}).

Thus Θ\Theta is also a left-QQ comodule map. The super version of Lemma 1.3 proves ascent exactly as before. The direct-sum and directed-union arguments are unchanged.

If A\mathcal{A} is amenable, put B=M⋊∧A\mathcal{B}=M\rtimes_{\wedge}\mathcal{A} and K=⋀M\mathcal{K}=\bigwedge M. The algebra K\mathcal{K} is locally finite-dimensional and therefore amenable. The quotient B⊗Kk=A\mathcal{B}\otimes_{\mathcal{K}}k=\mathcal{A}, with its regular action, is amenable. The Hopf section A→B\mathcal{A}\to\mathcal{B} gives the right-K\mathcal{K} normal basis A⊗K→B\mathcal{A}\otimes\mathcal{K}\to\mathcal{B}; bijectivity follows from the smash-product relations and the bijective antipode of A\mathcal{A}. The super induction lemma, applied to V=KV=\mathcal{K}, makes B\mathcal{B} amenable. Its quotient module coalgebra B⊗Ak≅⋀M\mathcal{B}\otimes_{\mathcal{A}}k\cong\bigwedge M is amenable by Lemma 5.1.

It remains to pass from ⋀\bigwedge-extensive amenability of MM, for M≠0M\ne0, to ordinary amenability. Put J=⋀>0MJ=\bigwedge^{>0}M, and let π:⋀M→J\pi:\bigwedge M\to J be the A\mathcal{A}-linear projection. Fix 0≠m∈M0\ne m\in M, a finite subspace F≤AF\le\mathcal{A} containing 11, and η>0\eta>0. Choose a finite E≤⋀ME\le\bigwedge M with dim⁡(FE+F(mE))<(1+η)dim⁡E\dim(FE+F(mE))<(1+\eta)\dim E, and put E′=E+mEE'=E+mE and W=π(E′)W=\pi(E'). As in Theorem 2.1,

E⟶W⊕W,u↦(π(u),π(mu))E\longrightarrow W\oplus W,\qquad u\mapsto\bigl(\pi(u),\pi(mu)\bigr)

is injective: π(u)=0\pi(u)=0 gives u∈k1u\in k1, and then π(mu)=mu=0\pi(mu)=mu=0 forces u=0u=0. Thus dim⁡E≤2dim⁡W\dim E\le2\dim W. The quotient-surjection argument of that theorem, applied to π\pi, gives

dim⁡(FW/W)≤dim⁡(FE′/E′)<ηdim⁡E≤2ηdim⁡W.\dim(FW/W)\le\dim(FE'/E')<\eta\dim E\le2\eta\dim W.

Letting η\eta tend to zero proves amenability of JJ. The coproduct components of bidegree (n−1,1)(n-1,1) give an A\mathcal{A}-linear injection

J⟶(⋀M)⊗M,m1∧⋯∧mn⟼∑i=1n(−1)n−i(m1∧⋯mi^⋯∧mn)⊗mi.J\longrightarrow\left(\bigwedge M\right)\otimes M,\qquad m_1\wedge\cdots\wedge m_n\longmapsto\sum_{i=1}^{n}(-1)^{n-i}(m_1\wedge\cdots\widehat{m_i}\cdots\wedge m_n)\otimes m_i.

It is injective, since distinct wedge basis monomials have disjoint nonempty image supports. Apply Lemma 1.1.

Permutation modules and comparison.

Theorem 5.3. For every field kk and every GG-set XX,

k[X] is ⋀-extensively amenable⟺G⋉X is extensively amenable.k[X]\text{ is }\bigwedge\text{-extensively amenable}\quad\Longleftrightarrow\quad G\ltimes X\text{ is extensively amenable}.

Proof. Put L=(Z/2)(X)L=(\mathbb{Z}/2)^{(X)}, identified with Pf(X)\mathcal{P}_{f}(X) by support. By [6 Theorem 1.3], the action G↷XG\curvearrowright X is extensively amenable if and only if the affine action L⋊G↷LL\rtimes G\curvearrowright L is amenable.

Suppose first that this affine action is amenable. Choose an order on XX and the resulting wedge basis

(eB)B∈Pf(X)(e_B)_{B\in\mathcal{P}_{f}(X)}

of ⋀k[X]\bigwedge k[X]. A finite testing space SS in ⋀k[X]#k[G]\bigwedge k[X]\# k[G] is contained in the span of finitely many elements ri#gir_i\# g_i, where each rir_i is an exterior monomial. Write Ti=supp⁡(ri)∈LT_i=\operatorname{supp}(r_i)\in L, and put hi=(Ti,gi)∈L⋊Gh_i=(T_i,g_i)\in L\rtimes G.

Choose a finite Følner set F⊆LF\subseteq L for the finitely many hih_i, and set

E=⟨eB:B∈F⟩k.E=\langle e_B:B\in F\rangle_k.

For B∈FB\in F, the vector (ri#gi)eB(r_i\#g_i)e_B is either 00, or a nonzero scalar multiple of eTi△giB=ehiBe_{T_i\triangle g_iB}=e_{h_iB}; indeed, it is nonzero precisely when Ti∩giB=∅T_i\cap g_iB=\varnothing. Hence

E+SE⊆⟨eB:B∈F∪⋃ihiF⟩k.E+SE\subseteq\left\langle e_B:B\in F\cup\bigcup_i h_iF\right\rangle_k.

Choosing FF sufficiently Følner therefore makes EE Følner for the original testing space. Thus k[X]k[X] is ⋀\bigwedge-extensively amenable.

Conversely, suppose that k[X]k[X] is ⋀\bigwedge-extensively amenable. For x∈Xx\in X, define

εx:⋀k[X]→⋀k[X],εx(v)=x∧v,\varepsilon_x:\bigwedge k[X]\to\bigwedge k[X],\qquad\varepsilon_x(v)=x\wedge v,

let p1:⋀k[X]→k[X]p_1:\bigwedge k[X]\to k[X] be projection onto degree one, and let x∗:k[X]→kx^*:k[X]\to k be the coordinate functional of xx. Define contractions by

ιx=((x∗∘p1)⊗id⁡)Δ,\iota_x=((x^*\circ p_1)\otimes\operatorname{id})\Delta,

and put

cx=εx+ιx.c_x=\varepsilon_x+\iota_x.

On the wedge basis, cx(eB)=±eB△{x}c_x(e_B)=\pm e_{B\triangle\{x\}}, so cxc_x is a signed permutation whose underlying permutation is the toggle B↦B△{x}B\mapsto B\triangle\{x\}. Likewise GG acts by signed permutations, with underlying permutation B↦gBB\mapsto gB. Let Γ≤GL⁡(⋀k[X])\Gamma\leq\operatorname{GL}(\bigwedge k[X]) be the group generated by all cxc_x and the operators induced by GG. Its underlying permutation action on Pf(X)\mathcal{P}_{f}(X) has the same image as the affine action L⋊G↷LL\rtimes G\curvearrowright L.

Let T⊆XT\subseteq X and S⊆GS\subseteq G be finite. By Lemma 5.1, there is a nonzero finite graded subcoalgebra C≤⋀k[X]C\leq\bigwedge k[X] which is arbitrarily Følner for multiplication by the x∈Tx\in T and for the g∈Sg\in S. Since CC is a subcoalgebra, every coefficient operator of its coproduct preserves CC; in particular,

ιxC⊆C.\iota_xC\subseteq C.

Consequently

cxC⊆C+xC,c_xC\subseteq C+xC,

so the same CC is arbitrarily Følner for the signed permutation operators cxc_x, x∈Tx\in T, and for g∈Sg\in S. The boundary estimates (3), applied to words in these operators, show that this monomial representation of Γ\Gamma is amenable.

Gromov’s ordering argument for linear actions [5 §3.6] applies unchanged to monomial actions: the nonzero scalar coefficients do not affect the leading coordinates. Therefore amenability of this monomial representation implies amenability of its underlying permutation action on Pf(X)\mathcal{P}_{f}(X). Since this action has the same image as L⋊G↷LL\rtimes G\curvearrowright L, the affine action is amenable. By [6 Theorem 1.3], G↷XG\curvearrowright X is extensively amenable.

In characteristic two the binary-lamp correspondence is particularly explicit:

⋀k[X]≅k[(Z/2)(X)],x↦ux−1.\bigwedge k[X] \cong k[(\mathbb{Z}/2)^{(X)}], \qquad x \mapsto u_x-1.

This is a GG-equivariant algebra isomorphism, not a Hopf isomorphism for the primitive exterior coproduct: Δ(ux−1)\Delta(u_x-1) has the additional term (ux−1)⊗(ux−1)(u_x-1)\otimes(u_x-1).

Proposition 5.4. If A\mathcal{A} is a cocommutative Hopf algebra in characteristic 2, then every extensively amenable A\mathcal{A}-module is Λ\Lambda-extensively amenable. If A\mathcal{A} is generated as an algebra by its primitive elements, the converse also holds.

Proof. The quotient Sym⁡(M)⟶Sym⁡(M)/(m2:m∈M)=⋀M\operatorname{Sym}(M)\longrightarrow\operatorname{Sym}(M)/(m^2:m\in M)=\bigwedge M is an A\mathcal{A}-equivariant Hopf map: in characteristic two, cocommutativity makes the ideal generated by squares A\mathcal{A}-stable. The module-coalgebra quotient theorem [3 Theorem 1.9] gives the first implication.

For the converse put R=Sym⁡(M)R=\operatorname{Sym}(M), let R[2]R^{[2]} be the subalgebra generated by squares, and put B=R#A\mathcal{B}=R\mathbin{\#}\mathcal{A}, K=R[2]#A\mathcal{K}=R^{[2]}\mathbin{\#}\mathcal{A}. Primitives act as derivations and annihilate every square, so A\mathcal{A} acts on R[2]R^{[2]} through its counit. The commutative Hopf algebra R[2]R^{[2]} is amenable by [3 Theorem 2.4]; since the K\mathcal{K}-action factors through its regular action, it is an amenable K\mathcal{K}-module. Moreover B⊗Kk=⋀M\mathcal{B}\otimes_{\mathcal{K}} k=\bigwedge M, which is amenable by hypothesis. Choose a basis of MM. Sending a wedge basis monomial to its squarefree polynomial gives a coalgebra section; separating even exponents from squarefree exponents gives the colinear right-K\mathcal{K} normal basis. Lemma 1.3 applied to V=R[2]V=R^{[2]} proves amenability of B⊗KR[2]≅R\mathcal{B}\otimes_{\mathcal{K}}R^{[2]}\cong R. □

Remark 5.5. Replacing squares by pp-th powers gives the analogous equivalence between the symmetric and truncated symmetric constructions in characteristic pp, for primitively generated A\mathcal{A}.

I still do not know whether the symmetric and exterior definitions are equivalent.

Institut Camille Jordan, Université de Lyon 1 and Section de Mathématiques, Université de Genève

Email address: [email protected]

References

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