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Compression functions of uniform embeddings of groups into Hilbert and Banach spaces
ARZHANTSEVA, Goulnara N., DRUŢU, Cornelia, SAPIR, Mark
Abstract
We construct finitely generated groups with arbitrary prescribed Hilbert space compression alpha from the interval [0,1]. For a large class of Banach spaces E (including all uniformly convex Banach spaces), the E-compression of these groups coincides with their Hilbert space compression. Moreover, the groups that we construct have asymptotic dimension at most 3, hence they are exact. In particular, the first examples of groups that are uniformly embeddable into a Hilbert space (respectively, exact, of finite asymptotic dimension) with Hilbert space compression 0 are given. These groups are also the first examples of groups with uniformly convex Banach space compression 0.
ARZHANTSEVA, Goulnara N., DRUŢU, Cornelia, SAPIR, Mark. Compression functions of uniform embeddings of groups into Hilbert and Banach spaces. Journal für die reine und angewandte Mathematik , 2009, vol. 2009, no. 633, p. 213-235
arxiv : math/0612378
DOI : 10.1515/CRELLE.2009.066
Available at:
http://archive-ouverte.unige.ch/unige:9746
Disclaimer: layout of this document may differ from the published version.
(Walter de Gruyter BerlinNew York 2009
Compression functions of uniform embeddings of groups into Hilbert and Banach spaces
ByGoulnara Arzhantsevaat Gene`ve,Cornelia Drut¸uat Oxford, and Mark Sapirat Nashville
Abstract. We construct finitely generated groups with arbitrary prescribed Hilbert space compression aA½0;1. This answers a question of E. Guentner and G. Niblo.
For a large class of Banach spacesE(including all uniformly convex Banach spaces), the E-compression of these groups coincides with their Hilbert space compression. Moreover, the groups that we construct have asymptotic dimension at most 2, hence they are exact. In particular, the first examples of groups that are uniformly embeddable into a Hilbert space (moreover, of finite asymptotic dimension and exact) with Hilbert space compression 0 are given. These groups are also the first examples of groups with uniformly convex Banach space compression 0.
1. Introduction
1.1. Uniform embeddings. The property of uniform embeddability of groups into Hilbert spaces (and, more generally, into Banach spaces) became popular after Gromov [Gr1] suggested that this property might imply the Novikov conjecture. Indeed, following this suggestion, Yu [Yu] and later Kasparov and Yu [KY] proved that a finitely generated group uniformly embeddable into a Hilbert space, respectively into a uniformly convex Banach space, satisfies the Novikov conjecture.
This raised the question whether every finitely generated group can be embedded uniformly into a Hilbert space, or more generally, into a uniformly convex Banach space.
Gromov constructed [Gr2] finitely generatedrandomgroups whose Cayley graphs (quasi)- contain some infinite families of expanders and thus cannot be embedded uniformly into a Hilbert space (or into anylp with 1ep<y, e.g. [Roe], Ch.11.3). The recent results of V. La¤orgue [Laf ] yield a family of expanders that is not uniformly embeddable into any
This article was written while all the three authors were visitors at the Max Planck Institute in Bonn. We are grateful to the MPI for its hospitality. The research of the first author was supported by the Swiss National Science Foundation, grants PP002-68627, PP002-116899. The research of the third author was supported in part by the NSF grants DMS 0245600 and DMS 0455881 and by a BSF (USA-Israeli) grant.
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uniformly convex Banach space. Nevertheless, one cannot apply Gromov’s argument to deduce that random groups corresponding to La¤orgue’s family of graphs do not embed uniformly into any uniformly convex Banach space. Indeed, La¤orgue’s expanders are Cayley graphs of finite quotients of a non-free group, therefore there are loops of bounded size in all of them, and the graphs have bounded girth. On the other hand, Gromov’s argument succeeds only if the girth of a graph in the family of expanders is of the same order as the diameter of the graph.
1.2. Compression and compression gap.
Definition 1.1 (cf. [GuK]). Let ðX;dXÞ and ðY;dYÞ be two metric spaces and let f:X !Y be a 1-Lipschitz map. The compression of f is the supremum over all af0 such that
dY
fðuÞ;fðvÞ
fdXðu;vÞa for allu,vwith large enough dXðu;vÞ.
If E is a class of metric spaces closed under rescaling of the metric, then the E-compression of X is the supremum over all compressions of 1-Lipschitz maps X !Y, Y AE. In particular, ifEis the class of Hilbert spaces, we get theHilbert space compression ofX.
The E-compression measures the least possible distortion of distances when one tries to draw a copy ofX inside a space fromE. It is a quasi-isometry invariant ofX and it takes values in the interval ½0;1. Similar concepts of distortion have been extensively studied (mostly for finite metric spaces mapped into finite dimensional Hilbert spaces) by combina- torists for many years (see [Bou], [DL], for example).
Since any finitely generated groupG can be endowed with a word length metric and all such metrics are quasi-isometric, one can speak about theE-compression of a group G.
Guentner and Kaminker proved in [GuK] that if the Hilbert space compression of a finitely generated group G is larger than 1=2 then the reduced C-algebra of G is exact (in other words,G isexactorGsatisfies Guoliang Yu’spropertyA [Yu]).
One of the goals of this paper is to describe all possible values ofE-compression for finitely generated groups, whenEis either the class of Hilbert spaces or, more generally, the class of uniformly convex Banach spaces.
A very limited information was known about the possible values of Hilbert space compression of finitely generated groups. For example, word hyperbolic groups have Hil- bert space compression 1 [BS], and so do groups acting properly and co-compactly on a CAT(0) cube complex [CN]; co-compact lattices in arbitrary Lie groups, and all lattices in semi-simple Lie groups have Hilbert space and, moreover, Lp-compression 1 [Te]; any group that is not uniformly embeddable into a Hilbert space (such groups exist by [Gr2]) has Hilbert space compression 0, etc. (see the surveys in [AGS], [Te]). The first groups with Hilbert space compressions strictly between 0 and 1 were found in [AGS]: R. Thompson’s groupF has Hilbert space compression 1=2, the Hilbert space compression of the wreath productZoZis between 1=2 and 3=4 (later it was proved in [ANP] that it is actually 2=3), the Hilbert space compression ofZo ðZoZÞis between 0 and 1=2.
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The notion of E-compression can be generalized to the notion ofE-compression gap of a spaceX, whereEis any class of metric spaces closed under rescaling of the metric (see Definition 2.6). It measures even more accurately than the compression the best possible (least distorted) way of embedding X in a space from E. For example, it is proved in [AGS] that R. Thompson’s group F has Hilbert space compression gap ðpffiffiffix
;pffiffiffix logxÞ.
This means there exists an 1-Lipschitz embedding ofF into a Hilbert space with compres- sion function ffiffiffi
px
, and every 1-Lipschitz embedding ofF into a Hilbert space has compres- sion function at most pffiffiffix
logx. This is much more precise than simply stating that the Hilbert space compression of F is 1=2. Another example: it follows from [Te] that every lattice in a semi-simple Lie group has a Hilbert space compression gap x
ffiffiffiffiffiffiffiffiffiffi logx
p log logx;x
!
and the upper bound of the gap cannot be improved. This is a much more precise statement than the statement that the Hilbert space compression of the lattice is 1.
In this paper, we show that a large class of functions appears as Hilbert space com- pression functions of graphs of bounded degree, and as upper bounds of Hilbert space compression gaps of logarithmic size of finitely generated groups. This class of functions is defined as follows. We use the notationRþfor the interval½0;yÞ.
Definition 1.2. Let C be the collection of continuous functions r:Rþ!Rþ such that for somea>0:
(1) ris increasing on½a;yÞ, and lim
x!yrðxÞ ¼y. (2) ris subadditive.
(3) The function tðxÞ ¼ x
rðxÞ is increasing, and the function tðxÞ
logxis non-decreasing on½a;yÞ.
Remark 1.3. The collection C contains all functions xa, for aAð0;1Þ, as well as functions logx, log logx, x
logbðxþ1Þ, xa
loggðxþ1ÞforaAð0;1Þ,b>1,g>0, etc.
1.3. Results of the paper. LetEbe the class of all uniformly convex Banach spaces.
Proposition 1.4(see Proposition 4.2). Letrbe a function in C. There exists a graph Pof bounded degree such thatris the Hilbert space compression function ofP,and also the E-compression function ofP.
In particular, for any aA½0;1 there exists a graph of bounded degree whose Hilbert space compression equals theE-compression,and both are equal toa.
Using the construction of the graph in Proposition 1.4, we realize every function ofC as the upper bound of a Hilbert space compression gap of logarithmic size of a finitely gen- erated group.
Theorem 1.5(see Theorem 5.5). For every functionrACthere exists a finitely gener- ated group of asymptotic dimension at most2such that for every >0, r
log1þðxþ1Þ;r
! is a Hilbert space compression gap and anE-compression gap of the group.
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In particular,for everyaA½0;1there exists a finitely generated group Gaof asymptotic dimension at most2 and with the Hilbert space compression equal to theE-compression and equal toa.
Since the groups Ga have finite asymptotic dimension, they are all exact and uni- formly embeddable1)into Hilbert spaces even when a¼0. Thus we construct the first ex- amples of groups uniformly embeddable into Hilbert spaces, moreover exact and even of finite asymptotic dimension, that have Hilbert space compression 0, and even {uniformly convex Banach space}-compression zero. Note that since the construction in [Gr2] does not immediately extend to uniformly convex Banach spaces, our groups seem to be the only existing examples of groups with {uniformly convex Banach space}-compression 0.
1.4. The plan of the proofs. The plan for proving Proposition 1.4 and Theorem 1.5 is the following. We use a family of V. La¤orgue’s expandersPk,kf1, which are Cayley graphs of finite factor-groups Mk of a lattice G of SL3ðFÞ for a local field F. La¤orgue proved [Laf ] that this family of expanders does not embed uniformly into a uniformly con- vex Banach space. Now taking any function r in C, we choose appropriate scaling con- stantslk, kf1, such that the family of rescaled metric spaces ðlkPkÞkf1 has {uniformly convex Banach space}-compression functionrand Hilbert space compression functionras well. This gives Proposition 1.4.
The group satisfying the conditions of Theorem 1.5 is constructed as a graph of groups. We use the fact that each Mk is generated by finitely many involutions, say m (that can be achieved by choosing a latticeGgenerated by involutions). One of the vertex groups of the graph of groups is the free productF of the groupsMk, other vertex groups aremcopies of the free productH¼Z=2ZZ. Edges connectF with each of themcopies ofH. The edge groups are free products of countably many copies ofZ=2Z. We identify such a subgroup in H with a subgroup of F generated by involutions, one involution from the generating set of each factor Mk. As a result, the groupG is finitely generated, and each finite subgroup Mk in G is distorted by a scaling constant close to lk. Hence the Cayley graph of G contains a quasi-isometric copy of the family of metric spaces ðlkPkÞkf1. This allows us to apply Proposition 1.4 and get an upper bound for a compres- sion gap. A lower bound is achieved by a careful analysis of the word metric onG.
In order to show that G has asymptotic dimension at most 2, we use a result by Dranishnikov and Smith [DS] on the asymptotic dimension of countable groups, and re- sults by Bell and Dranishnikov [BD], as well as by Bell, Dranishnikov and Keesling [BDK]
on the asymptotic dimension of groups acting on trees.
1.5. Other Banach spaces. The class of Banach spaces to which our arguments apply cannot be extended much beyond the class of uniformly convex Banach spaces; for instance it cannot be extended to reflexive strictly convex Banach spaces. Indeed, our proof is based on the fact that a family of V. La¤orgue’s expanders [Laf ] does not embed uniformly into a uniformly convex Banach space. But by a result of Brown and Guentner [BG], any count-
1) A finitely generated group G of finite asymptotic dimension has Guoliang Yu’s property A [HR], Lemma 4.2. That property is equivalent to the exactness of the reducedC-algebra ofG([Oz], [HR]) and guaran- tees uniform embeddability into a Hilbert space ([Yu], Th. 2.2).
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able graph of bounded degree can be uniformly embedded into a Hilbertian sumL lpnðNÞ for some sequence of numbers pnAð1;þyÞ, pn!y. The Banach spaceL
lpnðNÞ is re- flexive and strictly convex, but it is not uniformly convex.
Acknowledgement. The authors are grateful to A. Dranishnikov, A. Lubotzky, A. Rapinchuk, B. Remy, R. Tessera and D. Witte Morris for useful conversations and remarks.
2. Embeddings of metric spaces
Given two metric spaces ðX;dXÞ and ðY;dYÞ and a 1-Lipschitz mapf:X !Y we define thedistortionoff[HLW] as follows:
dtnðfÞ ¼max
x3y
dXðx;yÞ dY
fðxÞ;fðyÞ: ð1Þ
For a metric spaceðX;dÞand a collection of metric spacesEwe define theE-distortion of ðX;dÞ, which we denote by dtnEðX;dÞ, as the infimum over the distortions of all 1-Lipschitz maps fromX to a metric space fromE. Note that givenla positive real num- ber dtnEðX;dÞ ¼dtnEðX;ldÞprovided that the classEis closed under rescaling of the met- rics byl.
Remark 2.1. IfEcontains a space withnpoints at pairwise distance at least 1 from each other then for every graphX withnvertices and edge-length metric, dtnEXediamX. The notion of distortion originated in combinatorics is related to the following notion of uniform embedding with origin in functional analysis.
Definition 2.2. Given two metric spacesðX;dXÞ andðY;dYÞ, and two proper non- decreasing functions rG:Rþ!Rþ, with lim
x!yrGðxÞ ¼y, a map f:X !Y is called a ðr;rþÞ-embedding(also called auniform embeddingor acoarse embedding) if
r
dXðx1;x2Þ edY
fðx1Þ;fðx2Þ erþ
dXðx1;x2Þ ð2Þ ;
for allx1,x2inX.
IfrþðxÞ ¼Cx, i.e. iffisC-Lipschitz for some constantC >0, then the embedding is called ar-embedding.
Definition 2.3. For a family of metric spacesXi,iAI, by aðr;rþÞ-embedding(resp.
r-embedding) of the family we shall mean theðr;rþÞ-embedding (resp.r-embedding) of the wedge union ofXi.
LetðX;dXÞbe a quasi-geodesic metric space (e.g., the set of vertices of a graph). Then it is easy to see that anyðr;rþÞ-embedding ofX is also ar-embedding. The same holds for a family of quasi-geodesic metric spaces.
Convention 2.4. Since in this paper we discuss mainly embeddings of graphs, in what follows we restrict ourselves tor-embeddings, and denote the functionrsimply byr.
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Notation 2.5. For two functions f;g:D!RwhereDORwe write f fgif there exist a;b;c>0 such that fðxÞeagðbxÞ þcfor every xAD. If f fg and gff then we write f g.
Definition 2.6. Let ðX;dÞ be a metric space, and let E be a collection of metric spaces. Let f;g:Rþ!Rþ be two increasing functions such that f fg and
x!limyfðxÞ ¼ lim
x!ygðxÞ ¼y.
We say thatðf;gÞis anE-compression gap ofðX;dÞif (1) there exists an f-embedding ofX into a space fromE;
(2) for everyr-embedding ofX into a space fromE, we haverfg.
If f ¼gthen we say that f is theE-compression functionofX.
The quotient g=f is called thesize of the gap. The functions f and gare called, the lowerandupper bound of the gaprespectively.
Remark 2.7. Assume that E is closed under rescaling of the metrics.
(i) Ifais the supremum of all numbers such thatxafr andris theE-compression function ofðX;dÞthenais theE-compression ofðX;dÞ.
(ii) If fis theE-compression function of a metric spaceðX;dÞ, andais the supremum over all numbers b such that xbff then a is the compression of ðX;dÞ in the sense of Definition 1.1.
3. Embeddings of expanders
For every finite m-regular graph, the largest eigenvalue of its incidence matrix ism.
We denote byl2the second largest eigenvalue.
We start by a well known metric property of expanders.
Lemma 3.1 ([Lub], Ch. 1). Let >0 and let Gm; be the family of all m-regular graphs with l2em. Then there exist two constants k, k0 such that for any graph P in Gm; with set of vertices V, and any vertex xAV, the set fyAVjdðx;yÞfkdiamPg has cardinality at leastk0jVj.
We now recall properties of expanders related to embeddings into Hilbert spaces. We denote byHthe class of all separable Hilbert spaces.
Theorem 3.2 ([LLR], Theorem 3.2(6), [HLW], Theorem 13.8 and its proof). Let
>0and letGm; be the family of all m-regular graphs withl2em.
(i) There exist constants c>0and d >1such that for any graphPinGm; with set of vertices V
clogjVjedtnHPediamPedlogjVj:
ð3Þ
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(ii) Moreover,there exists r>0such that for every1-Lipschitz embeddingfofPinto a Hilbert space Y there exist two vertices v1and v2 in V withdðv1;v2ÞfkdiamP(wherek is the constant in Lemma3.1)and
kfðv1Þ fðv2Þker:
Remark 3.3. Thus for all expanders inGm; the canonical embedding P,! 1
ffiffiffi2 p l2ðVÞ
has optimal distortion, see Remark 2.1.
V. La¤orgue [Laf ] proved that for some smaller family of expanders one can re- place H by a large class of Banach spaces. Namely, for every prime number p and nat- ural number r>0, he defined a class of Banach spaces Ep;r¼ S
a>0
Ep;r;a satisfying the following:
(1) For any p,r, the classEp;rcontains all uniformly convex Banach spaces2)(includ- ing all Hilbert spaces, and even all spaceslq,q>1).
(2) S
r E2;r is the set of allB-convex Banach spaces.
La¤orgue’s family of expanders that does not embed uniformly into any Banach space from Ep;r is constructed as follows. Given numbers p and r as above, let F be a local field such that the cardinality of its residual field is pr. Let G be a lattice in SLð3;FÞ.
The groupG is residually finite with Kazhdan’s property (T). In fact,Gsatisfies the Banach versionof property (T) with respect to the family Ep;r ([Laf ], §3 and Proposition 4.5).
LetðGkÞkf1be a decreasing sequence of finite index normal subgroups ofGsuch that T
kf1
Gk ¼ f1g, and letMk¼G=Gk,kf1, be the sequence of quotient groups. Given a finite symmetric set of generators ofGof cardinalitymf2, we consider eachMk endowed with the induced set ofmgenerators; we denote by dkthe corresponding word metric onMkand by Pk the corresponding m-regular Cayley graph. Since G has property (T), the family ðPk;dkÞkf1is a family of expanders ([Lub], Proposition 3.3.1). Moreover, the Banach ver- sion of property (T) for G yields Proposition 3.4 below, which implies that the family ðPk;dkÞkf1 cannot be uniformly embedded into a Banach space from Ep;r (see Remark 3.6).
2) A Banach space isuniformly convexif for everyR>0 and everyd>0 there existse¼eðR;dÞ>0 such that ifx, yare two points in the ball around the origin of radiusRat distance at leastdthen their middle point 1
2ðxþyÞis in the ball around the origin of radiusRe.
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Proposition 3.4 ([Laf ], Proposition 5.2). For every a>0 there exists a constant C ¼CðaÞ such that for any kf1 and any space Y from Ep;r;a a 1-Lipschitz map f:Pk!Y satisfies:
1 ðcardPkÞ2
P
x;yAPk
kfðxÞ fðyÞk2eC 1 cardPk
P
x;yneighbors
kfðxÞ fðyÞk2: ð4Þ
Corollary 3.5. (i)For everya>0there exists a constant D¼DðaÞsuch that for any kf1,
DdiamPkedtnEp;r;aPkediamPk: ð5Þ
(ii) Moreover,there exists R¼RðaÞsuch that for every1-Lipschitz embeddingfofPk
into a space Y AEp;r;a there exist two vertices v1 and v2 in Pk withdðv1;v2ÞfkdiamPk, wherekis the constant from Lemma3.1,and
kfðv1Þ fðv2ÞkeR:
ð6Þ
Proof. The second inequality in (5) follows from Remark 2.1 and from the fact that no Banach space can be covered by finitely many balls of radius 1. We prove the first in- equality in (5). LetY be an arbitrary space fromEp;r;aand letf:Pk!Y be a 1-Lipschitz map. Inequality (4) implies that
1
½dtnðfÞcardPk2 P
x;yAPk
dkðx;yÞ2eCm:
ð7Þ
Recall that each graph Pk is m-regular. Lemma 3.1 and (7) imply that Cm½dtnðfÞ2fk2k0ðdiamPkÞ2.
Now take R>1 k
ffiffiffiffiffiffiffiffi Cm k0 r
, wherek, k0 are the constants from Lemma 3.1 andC is the constant from (4). Assume that there exists a 1-Lipschitz embeddingfof Pk into a space Y AEp;r;a such that for any two vertices v1 and v2 in Pk with dkðv1;v2ÞfkdiamPk the following inequality holds:
dkðv1;v2Þ
kfðv1Þ fðv2Þk< 1
R diamPk: Inequality (4) implies that
Cm> 1 ðcardPkÞ2
P
dkðv1;v2ÞfkdiamPk
R2dkðv1;v2Þ2
½diamPk2 fR2k2k0: This contradicts the choice of R.
Therefore there exist two vertices v1 and v2 in Pk with dkðv1;v2ÞfkdiamPk and such that:
dkðv1;v2Þ
kfðv1Þ fðv2Þkf 1
RdiamPk: The last inequality implies thatkfðv1Þ fðv2ÞkeR. r
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SinceðPk;dkÞkf1is a family of expanders, it is contained in some family Gm; . Then according to Theorem 3.2, we have diamPk logjVkj.
Remark 3.6. Theorem 3.2(ii) implies that no sub-family of the family Gm; can be uniformly embedded into a Hilbert space, in the sense of Definition 2.3.
Similarly, Corollary 3.5(ii) implies that no sub-family of the family ðPkÞkf1 can be uniformly embedded into a space fromEp;r.
The construction in the following lemma was provided to us by Dave Witte- Morris.
Lemma 3.7. Let F be a nonarchimedean local field of characteristic0. There exists a lattice in the groupSLð3;FÞcontaining infinitely many noncentral involutions.
Proof. Choose an algebraic number fieldK, such that F is one of the (nonarchimedean) completions ofK, and F is totally real.
Let pbe the characteristic of the residue field ofF, and letc¼1p3. Thusc<0, butcis a square inF. ConsiderL¼K½ ffiffiffi
pc
, and denote bytthe Galois involution ofLoverK. We likewise denote by t the involution defined on the 33 matrices by applying t to each entry. LetG ¼SUð3;L;tÞ ¼ fgASLð3;LÞjtðgTÞ g¼Id3g. Then:
(a) Gis aK-form of SLð3Þ.
(b) GF ¼SLð3;FÞ.
(c) Gis compact at each real place.
Properties (a), (b), (c) can be proved using arguments similar to the ones in [Wi], Chapter 10.
LetS be the collection of all the Archimedean places ofK and the place correspond- ing toF. According to the theorem due to Borel, Harish-Chandra, Behr and Harder ([Ma],
§I.3.2), the S-integer points of G form a lattice G in SLð3;FÞ. By [Ta], any lattice in a p-adic algebraic group is co-compact, in particular it is the case for G. The latticeGobvi- ously contains noncentral diagonal matrices that are involutions.
Letsbe one of these involutions and letZðsÞbe its centralizer in SLð3;FÞ. The sub- group GXZðsÞ has infinite index in G. Otherwise, for some positive integernone would have that gnAZðsÞ for any gAG. Since ZðsÞ is an algebraic subgroup in SLð3;FÞ and since Gis Zariski dense in SLð3;FÞ, it would follow that gnAZðsÞ for any gASLð3;FÞ.
This is impossible.
For a sequence ðgnÞnAN of representatives of distinct left cosets inG=
GXZðsÞ the involutions in the sequenceðgnsg1n ÞnAN are pairwise distinct. r
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Lemma 3.8. For every prime number p and natural number r>0, there exists m¼mðp;rÞ>0and a latticeGin SLð3;FÞ such that F is a local field with residue field of cardinality pr,andGis generated by finitely many involutionss1;. . .;sm.
Proof. LetGbe a lattice of SLð3;FÞcontaining infinitely many non-central involu- tions. According to Lemma 3.7 such a lattice exists. Consider the (infinite) subgroupG0of Ggenerated by involutions. SinceG0 is a normal subgroup inG, by Margulis’ Theorem G0 has finite index inG, thus it is a lattice itself. r
Notation 3.9. Let Gbe one of the lattices from Lemma 3.8. We keep the notation given before Proposition 3.4, referring, in addition, to the generating set consisting of invo- lutions. More precisely, consider a maximal ideal I in the ring of S-integers of the global field definingG(S is the corresponding set of valuations containing all Archimedian ones) and the congruence subgroup Gk of G corresponding to the ideal Ik. Let Mk ¼G=Gk, kf1. Let Uk¼ fs1ðkÞ;. . .;smðkÞg be the image of the generating set of G in Mk (each siðkÞ is an involution). We shall denote the corresponding word metric on Mk again by dk. Since eachsiðkÞis an involution, the Cayley graphPkofMk ism-regular. LetvðkÞde- note the cardinality of the groupMk.
Remark 3.10. It is easy to see thatvðkÞ ¼ jMkjsatisfies ckc1<logvðkÞ<ckþc1
for some constantsc,c1.
4. Metric spaces with arbitrary compression functions
Let ðX;dÞ be a metric space and l>0. We denote by lX the metric space ðX;ldÞ.
LetðPnÞnf1be the sequence of Cayley graphs of finite factor groupsMn,nf1, of the latticeGfrom Lemma 3.8, see Notation 3.9.
Letrbe a function inC(see Definition 1.2). For everynf1, letxnbe a fixed vertex inPn. We are going to choose appropriate scaling constants ln, nf1, so that the wedge unionP of the metric spaceslnPn, obtained by identifying all the verticesxn to the same pointx, has the required compression functionr.
Notation 4.1. Throughout this section we denote logvðnÞ by yn. According to Re- mark 3.10,cnc1< yn<cnþc1for some constantsc,c1.
We are looking for a sequence of rescaling constants lnsatisfyingln¼rðlnynÞ. This is equivalent to the fact thattðlnynÞ ¼ yn, where tðxÞ ¼ x
rðxÞ. SincetðxÞ is increasing by the definition of C, continuous and lim
x!y tðxÞ ¼ þy, t1ðxÞ exists for large enough x.
Thus, we can takeln:¼t1ðynÞ yn
.
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Proposition 4.2. LetPbe the wedge union oflnPn,nf1. Thenris both the Hilbert space compression function and theEp;r-compression function ofP(up to the equivalence re- lation).
In particular,ris the{uniformly convex Banach space}-compression function ofP.
The proof of Proposition 4.2 will show that the same conclusions hold if we replace the sequenceðlnÞnf1by any sequence of numbersðmnÞnf1satisfyingmnln.
Proof of Proposition4.2. We are going to prove thatris the Hilbert space compres- sion function ofP. The proof thatris theEp;r-compression function is essentially the same (with reference to Theorem 3.2 replaced by a reference to Corollary 3.5).
Let dtbe the canonical distance onP, and letV be the set of vertices ofP. Consider the map f from V tol2ðVÞdefined as follows. For every nf1 and everyvAVnnfxng let
fðvÞbe equal tolndv, wheredvis the Dirac function atv. Also let fðxÞ ¼0.
We prove that the following inequalities are satisfied, withdf1 the constant in The- orem 3.2(i).
1ffiffiffi
p2r dtðv;v0Þ d
ekfðvÞ fðv0Þke ffiffiffi p2
dtðv;v0Þ:
ð8Þ
Assume that v;v0APn for some n. Then kfðvÞ fðv0Þkeln
ffiffiffi2
p (when one of the vertices is xn the first term is ln). Since dtðv;v0Þfln, we get the second inequality in (8).
To prove the first inequality, recall that by Theorem 3.2 the diameter of lnPn is at mostdlnyn. Hence
r dtðv;v0Þ d
erðlnynÞ ¼lnekfðvÞ fðv0Þk:
Assume now thatvAPmnfxmgandv0APnnfxng. Then kfðvÞ fðv0Þk ¼
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi lm2 þln2 q
elmþlnedtðv;xÞ þdtðx;v0Þ ¼dtðv;v0Þ:
On the other hand kfðvÞ fðv0Þkf 1
ffiffiffi2
p ðlmþlnÞ ¼ 1 ffiffiffi2
p
kfðvÞ fðxÞk þ kfðv0Þ fðxÞk :
By the previous case, the last term is at least 1ffiffiffi
p2 r dtðv;xÞ d
þr dtðx;v0Þ d
f 1 ffiffiffi2
p r dtðv;v0Þ d
:
The latter inequality is due to the sub-additivity and the monotonicity ofr.
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This proves that rhas property (1) of the Hilbert space compression function of P, see Definition 2.6(1).
To prove property (2) of the Hilbert space compression function, let us consider an increasing functionr:Rþ!Rþ with lim
x!yrðxÞ ¼y, and a 1-Lipschitzr-embedding gof Pinto a Hilbert space. For any pair of verticesv,v0inPwe have
r
dtðv;v0Þ
ekgðvÞ gðv0Þkedtðv;v0Þ:
ð9Þ
We shall prove thatrfr.
For everynf1, for any two verticesv, v0in the same graphlnPn, the inequality (9) can be re-written as:
r
lndðv;v0Þ
ekgðvÞ gðv0Þkelndðv;v0Þ:
ð10Þ
We denote byhthe restriction ofgtolnPn, rescaled by the factor 1=ln. The sequence of inequalities (10) divided byln yields
1 ln
r
lndðv;v0Þ
ekhðvÞ hðv0Þkedðv;v0Þ:
ð11Þ
Theorem 3.2 implies that for some constants r,d and kthere exist verticesv1andv2
such that
kynedðv1;v2Þedyn and khðv1Þ hðv2Þker:
From (11) and the monotonicity ofr, we get rðklnynÞer
lndðv1;v2Þ
elnkhðv1Þ hðv2Þkerln¼rrðlnynÞ:
Denote byznthe productlnyn, also equal tot1ðynÞ, by the definition ofln. Then we get
rðkznÞerrðznÞ:
ð12Þ
We have that ynecnþc1eyn1þC1whereC1¼cþ2c1.
By property (3) of Definition 1.2, tðxÞ ¼x=rðxÞ is an increasing map defining a bijection ½a;yÞ ! ½b;yÞ. Moreover, the condition that tðxÞ=logx is non-decreasing easily implies that for some y>1, tðxÞ þ1etðyxÞ for every xfa. It follows that tðxÞ þC1etðCxÞ for every xfa, where C is a power of y depending on C1. This implies that for every yfb, t1ðyþC1ÞeCt1ðyÞ. Consequently, for n large enough, zn¼t1ðynÞet1ðyn1þC1ÞeCt1ðyn1Þ ¼zn1. We thus get
zn
zn1
eC:
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Now take any su‰ciently large x>0. Then for some n, x is between zn1 and zn. Hence (by the monotonicity ofrandr), we get:
rðkxÞerðkznÞerrðznÞerrðCzn1ÞfrðCxÞ:
Therefore,rfras required. r
One can obviously replaceP in Proposition 4.2 by a uniformly proper space (graph of bounded degree) with the same property.
The following corollary immediately follows from Proposition 4.2.
Corollary 4.3. For every numberain½0;1there exists a proper metric space(graph of bounded degree)whose Hilbert space compression and theEp;r-compression are equal toa.
Note that a¼0 can be obtained by taking, say, rðxÞ ¼logxin Proposition 4.2. To achievea¼1 take the one-vertex graph.
5. Discrete groups with arbitrary Hilbert space compressions
For every prime number pand every natural numberr>0, we denoteEp;r simply by Ein what follows. Recall thatEcontains all uniformly convex Banach spaces.
Pick a functionrAC. For simplicity we assume thatrð1Þ>0. As in Definition 1.2, we denote bytthe functionx=rðxÞ.
LetðMk;dkÞkf1 be the sequence of finite groups defined as above, for fixed pand r, see Lemma 3.8 and Notation 3.9. Recall that dk is the word metric associated to the gen- erating setUk¼ fs1ðkÞ;. . .;smðkÞgconsisting ofm¼mðp;rÞinvolutions, and that vðkÞ is the cardinality ofMk.
Notation 5.1. We denote byj jkthe length function onMk associated toUk. Notation 5.2. Let us fix three sequences of numbers:ðlkÞkf1,ðmkÞkf1, andðmkÞkf1. For kf1, we set lk such that r
lklogvðkÞ
¼lk; equivalently lk¼t1
logvðkÞ logvðkÞ withvðkÞas above. Without loss of generality we assume (by taking a suitable subsequence ofMk) that for everykf1,lkþ1lkf4.
For every kf2, let mk be the integer part of lk1
2 , and let m1¼0. Then we put mk¼2mkþ1 for everykf1.
According to our choice, for everykf2
mkelk<mkþ2:
ð13Þ
We are now ready to construct our group.
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LetF be the free product of the groupsMk,kf1.
For everyiAf1;. . .;mg, consider a copyHi of the free productZ=2ZZ, where the generator of theZ=2Z-factor ofHi is denoted bysi, while the generator of theZ-factor of Hi is denoted byti.
Notation 5.3. We denote byj jHi the length function onHi relative to the generat- ing set fsi;tig. For every kAZ, we denote the element tiksitki in Hi by sðkÞi . Note that jsðkÞi jHi ¼2kþ1, and thatHi is the semidirect product ofhsðkÞi ;kAZiandhtii.
LetG be the fundamental group of the following graph of groups (see [Ser], Ch. 5.1, for the definition). The vertex groups areF andH1;. . .;Hm, the only edges of the graph are
ðF;HiÞ, i¼1;. . .;m. The edge groupsFXHi are free products
kf1ðZ=2ZÞk of countably many groups of order 2, where thek-th factorðZ=2ZÞkis identified withhsiðkÞi<MkinF and withhsðmi kÞiinHi.
Notation 5.4. We denote by dG and by j jG the word metric and respectively the length function onGassociated to the generating setU ¼ fs1ð1Þ;. . .;smð1Þ;t1;. . .;tmg.
Theorem 5.5. With the notation above and the terminology in Definition2.6,the fol- lowing hold:
(I) The group G has as a Hilbert space compression gap, and an E-compression gap ðpffiffiffir
;rÞ.
(II) The group G has as a Hilbert space compression gap,and an E-compression gap r
log1þðxÞ;r
!
,for every >0. Hence the Hilbert space compression and theE-compression of G are equal to the supremum over all the non-negative numbersasuch that xafr.
(III) The asymptotic dimension of G is at most2.
We start our proof by describing the length functionj jG.
By the standard properties of amalgamated products ([LS77], Ch. IV, Th. 2.6), the free productF ¼
kf1Mk and the groupsHi,i Af1;2;. . .;mg, are naturally embedded into G. Moreover, the subgroupT ¼hti;1eiemiis free of rankmand a retract ofG, so its length function coincides withj jG restricted toT.
Definition 5.6. With every elementsAMk we assign theweightwtðsÞ ¼mkjsjk. With every element bAHi we assign the weight wtðbÞ ¼ jbjHi. The weight wtðWÞ of any word
W ¼s1b1. . .snbn withs1andbnpossibly trivial andnANis the sum Pn
i¼1
½wtðsiÞ þwtðbiÞ.
Let F0 be the free product of F ¼
kf1Mk and all the 2-element groupshsðkÞi iwith
kAZnfmk;kf1gand iAf1;. . .;mg. Then G is the multiple HNN extension of F0 with
free letterst1;. . .;tmshiftingsðkÞi . This is the presentation ofGused in the following lemma.
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A subword tGi 1sðkÞi tHi 1of a word in generatorssðkÞi ,ti ofG is called apinch. It can be removed and replaced bysðki G1Þ; we call this operationremoval of a pinch.
Lemma 5.7. For every kf1and gAMk,jgjG¼wtðgÞ ¼mkjgjk.
Proof. Lets¼ jgjkand letg¼si1ðkÞsi2ðkÞ. . .sisðkÞbe a shortest representation ofg as a product of generators ofMk. Then we can representgas
tim1ksi1ð1Þtmi1 ktim2ksi2ð1Þtmi2 k. . .timsksisð1Þtmis k: HencejgjGeð2mkþ1Þs¼mkjgjk.
LetW be any shortest word in the alphabetU representingginG. SincegAF, there exists a sequence of removals of pinches and subwords of the form aa1 that transfersW into a wordW0 in generators of F (i.e. letters of the formsjðlÞ) representingg. Since the weight of everysið1ÞandtGi 1is 1, the total weight of the wordW is the length ofW. The removal of a pinch does not increase the total weight, and the removal of a wordaa1de- creases it. Hence the total weight of the letters inW0 is at most jWj. On the other hand, since W0 is a word in generators of the free productF representing an element of one of the factorsMk, all letters fromW0 must belong toMk, i.e. they have the formsiðkÞwith
iAf1;. . .;mg. Therefore the total weight ofW0ismkjW0j. SinceW0representsginMk, we
have that the total weight ofW0 is at leastmkjgjk. HencejgjG ¼ jWjfmkjgjk as required.
r
The choice ofmkgiven by (13), Proposition 4.2 and the construction in its proof, and Lemma 5.7 imply the following.
Lemma 5.8. (1) The function r is the E-compression function and the Hilbert space compression function of S¼ S
kf1
Mk endowed with the restriction of the metricdG.
(2) The map f :S !l2ðSÞdefined by fð1Þ ¼0and fðsÞ ¼mkdsfor every sAMknf1g is ar-embedding ofðS;dGÞ.
Lemma 5.8 immediately implies
Lemma 5.9. The functionris an upper bound for anE-compression gap of G(in par- ticular,also for a Hilbert space compression gap of G).
Definition 5.10. We are going to use the standard normal forms of elements in the amalgamated productG(see [LS77], Ch. IV.2):
s1b1. . .snbn
ð14Þ
where:
(N0) Possiblys1¼1 orbn¼1.
(N1) si AMki andbi AHli (si,bi are calledsyllables).
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(N2) If bi ¼1, i<n, thensi and siþ1 are not in the same Mk; if si¼1, i>1, then bi1,bi are not in the sameHk.
One can get from one normal form to another by sequences of operations as fol- lows:
(r1) Replacingsibi with
siskðpÞ skðpÞbi
(left insertion).
(r2) Replacingbisiþ1with
biskðpÞ
skðpÞsiþ1
(right insertion).
(r3) Replacing two-syllable words with syllables from the same factor by the one- syllable word, their product.
One can easily check that this collection of moves is confluent, so one does not need the inverse of rule (r3).
Choose one representative for each left coset ofMk=hsiðkÞiand one representative in each left coset ofHi=hsiðkÞi, the representative ofhsiðkÞiis 1. LetMbe the set of all these representatives. We consider only the normal forms (14) in which all the si and bi (except possibly for the last non-identity syllable) are inM. We shall call these normal formsgood.
Every element ofG has a unique good normal form.
Lemma 5.11. Let V ¼s1b1s2. . .snbnbe the good normal form of an element g in the amalgamated product G. Then the lengthjgjG is betweenwtðVÞ=3andwtðVÞ,i.e.
Pn
i¼1
mkijsijkiþPn
i¼1
jbijH
li fjgjGf1
3 Pn
i¼1
mkijsijki þPn
i¼1
jbijH
li
ð15Þ :
For every normal form V0of g,the length of g is betweenwtðV0Þ=9andwtðV0Þ.
Proof. The first inequality in (15) follows from Lemma 5.7 and it holds for every normal form.
Consider a shortest wordW in the generators ofG representingg. Making moves of type (r3), we rewrite W in a normal form W0 without increasing its weight (note that a removal of pinches can be seen as a succession of two (r3)-type moves). We have that jgjG¼wtðWÞfwtðW0ÞfjgjG; the last inequality holds because any word of the form (14) and of weightl is equal inG to a word of length lin the generators in U and their inverses. It follows that wtðW0Þ ¼ jgjG. By doing insertion moves (r1) and (r2), we can rewrite the normal form W0 into the good normal form V of g. Note that each syllable is multiplied by at most two involutions during the process. The weight of each of these involutions does not exceed the weight of the syllables si, siþ1 involved in the moves.
Hence the total weight of the word cannot more than triple during the process. Hence wtðVÞe3 wtðW0Þ ¼3jgjG which proves the second inequality in (15).
The second statement is proved in a similar fashion: one needs to analyze the proce- dure of getting the good normal form from any normal form, and then use the first part of the lemma. r
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Definition 5.12. Lets1b1. . .snbnbe the good normal form ofg. Represent eachbias the shortest wordwðbiÞin the alphabet of generatorsfsli;tligof the corresponding subgroup Hli. Then the words1wðb1Þ. . .snwðbnÞin the alphabet S
kf1
MkWfsi;ti;iAf1;2;. . .;mgg is called theextended normal formofg.
The unicity of the good normal form and of each word wðbiÞimplies that every ele- ment inG has a unique extended normal form.
Definition 5.13. For every pair of elementsgandhinGwith extended normal forms g¼s1wðb1Þ. . .slwðblÞand h¼s10wðb10Þ. . .sn0wðbn0Þ let pðg;hÞ ¼ pðh;gÞ be the longest com- mon prefix of these words, of lengthiðg;hÞ. Thus
g1pðg;hÞfðg;hÞqðg;hÞ and h1pðg;hÞfðh;gÞqðh;gÞ
where the words fðg;hÞqðg;hÞ, fðh;gÞqðh;gÞ have di¤erent first syllables fðg;hÞ and fðh;gÞ respectively. Here the syllables are either in some Mk, kf1, or they are in ftG11;tG21;. . .;tGm1g.
Note that pðg;hÞ,qðg;hÞ,qðh;gÞare extended normal forms; fðg;hÞ(resp. fðh;gÞ) is either an element inMk for somekf1 or it is infsi;tGi 1gfor some iAf1;2;. . .;mg.
Definition 5.14. Lets1wðb1Þ. . .snwðbnÞ be the extended normal form ofg. Then for everyi let g½ibe thei-th letter of the extended normal form, letgg^i be the prefix ending in g½i, and letgibe the su‰x starting withg½i of the extended normal form.
Lemma 5.15. For every g;hAG,the distancedGðg;hÞis in the interval½A=9;Awhere A is equal to
(S) mkdk
fðg;hÞ;fðh;gÞ þwt
qðg;hÞ þwt
qðh;gÞ
if fðg;hÞ;fðh;gÞAMk,or (B) wt
fðg;hÞqðg;hÞ þwt
fðh;gÞqðh;gÞ
otherwise.
Proof. In Case (S), qðg;hÞ1
fðg;hÞ1fðh;gÞ
qðh;gÞ becomes a normal form for g1h if we combine all neighbor letters from the same Hk into one syllable, and fðg;hÞ1fðh;gÞ into one syllable. In Case (B), qðg;hÞ1fðg;hÞ1fðh;gÞqðh;gÞ becomes a normal form forg1hafter a similar procedure. Then one can use Lemma 5.11. r
For every element g in G whose extended normal form has the last syllable in Y, where Y ¼Mk for some kf1 or Y ¼ fsi;tGi 1g for some iAf1;. . .;mg, we consider a copyfgof a 1-Lipschitz embedding ofY into a Hilbert spaceHgwith optimal distortion:
either the embedding from Remark 3.3 rescaled by the factormkifY ¼Mk(i.e. the embed- ding sending all non-trivial elements inMk in pairwise orthogonal vectors of length mk) or the embedding defined by any choice of an orthonormal basis in a copy ofR2 otherwise.
Note that sincem1¼1 this is coherent with the identification ofsi AHi withsið1ÞAM1. LetHbe the Hilbertian sum of all Hg. Consider the following map from G intoH:
for everygAG let
cðgÞ:¼P
i
fgg^iðg½iÞ:
ð16Þ
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We use the mapcto prove the following.
Lemma 5.16. The group G has as a Hilbert space and anE-compression gapðpffiffiffir
;rÞ.
Proof. In view of Lemma 5.9, it su‰ces to show thatcis apffiffiffir
-embedding to finish the proof.
Let g;hAG. Then, by (16), since any two elements of H of the form fgg^iðg½iÞ, f^hhjðh½jÞeither coincide or are orthogonal to each other, we have:
kcðgÞ cðhÞk2¼fpðg;hÞfðg;hÞ
fðg;hÞ2þfpðg;hÞfðh;gÞ
fðh;gÞ2
þ P
j>iðg;hÞþ1
kfgg^jðg½jÞk2þ P
j>iðg;hÞþ1
kf^hhjðh½jÞk2eCdGðg;hÞ2
for some constant C (by Lemma 5.15 and the fact that all embeddings fare 1-Lipschitz).
Thuscis a Lipschitz embedding.
To prove the lower bound, note that forg½iinHk, jg½ijG ¼ kfgg^iðg½iÞk ¼1grðjg½ijGÞ:
Also ifg½iAMk then by Lemma 5.8 (2), and by the definition offgwe may write jg½ijG¼mkjg½ijk¼ kfgg^iðg½iÞkgrðjg½ijGÞ:
Thus, in all cases,
kfgg^iðg½iÞkgrðjg½ijGÞ:
Now, in case (B), kcðgÞ cðhÞk2gr
dG
fðg;hÞ; fðh;gÞ2
þ P
j>iðg;hÞþ1
rðjg½jjGÞ2þ P
j>iðg;hÞþ1
rðjh½jjGÞ2: The fact that rðg½iÞfrð1Þ for non-identityg½i, and the subadditivity of r(plus Lemma 5.15) imply
kcðgÞ cðhÞk2gr
dGðg;hÞ
as desired. In case (S), the proof is similar, only one needs to take into account that fpðg;hÞfðg;hÞ
fðg;hÞ2þfpðg;hÞfðh;gÞ
fðh;gÞ2
¼fpðg;hÞfðg;hÞ
fðg;hÞ
fpðg;hÞfðh;gÞ
fðh;gÞ2 fr
dG
fðg;hÞ;fðh;gÞ2
: r
Lemma 5.16 gives part (I) of Theorem 5.5.
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Let us prove part (II). For simplicity, we take¼1. The reader can easily modify the proof to make it work for every >0. Thus, we are going to prove that rðxÞ
log2ðxþ1Þ is a lower bound for a Hilbert space compression gap and anE-compression gap ofG. That is, we are going to prove that there exists a rðxÞ
log2ðxþ1Þ-uniform embedding of G in a Hilbert space.
Consider the same Hilbert spaceHand the same embeddingsfgforgAG as before.
Let us define an embedding p ofG into H. Let g be given in an extended normal form.
Then we set
pðgÞ:¼P
j
kjfgg^jðg½jÞ where the coe‰cientskj are defined as follows:
kj ¼
ffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgjÞ q log
wtðgjÞ þ1 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðg½jÞ
p :
We shall need the following two elementary inequalities, the first of which is obvious.
Lemma 5.17. For every sequence of positive numbers a1;. . .;an,we have Pn
i¼1
Pn
r¼i
ar
aie
Pn
r¼1
ai
2
:
Lemma 5.18. Let a1;. . .;anbe positive real numbers with anf1. Then a1
ða1þ þanÞlog2ða1þ þanþ1Þ ð17Þ
þ a2
ða2þ þanÞlog2ða2þ þanþ1Þþ þ an
anlog2ðanþ1Þ eC for some constant C.
Proof. For everyk ¼1;. . .;ndenotesk ¼akþ þan. Then (17) can be rewritten as follows:
s1s2
s1log2ðs1þ1Þþ þ sn1sn
sn1log2ðsn1þ1Þþ 1 log2ðsnþ1Þ: ð18Þ
Since the function 1
xlog2ðxþ1Þis decreasing, one can estimate (providedbfaf1) ba
blog2ðbþ1ÞeÐb
a
dx
xlog2ðxþ1Þ e2Ðb
a
dx
ðxþ1Þlog2ðxþ1Þ¼ 2
logðaþ1Þ 2 logðbþ1Þ: Applying this inequality to (18) and usinganf1, we get (17). r
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Let g, hbe two elements in G given in their extended normal forms. Let i¼iðg;hÞ, f ¼ fðg;hÞ, f0¼ fðh;gÞ, p¼ pðg;hÞ,q¼qðg;hÞ, q0¼qðh;gÞ.
ThenpðgÞ pðhÞ ¼S1þS2þS3where
S1¼ Pi
r¼1
ffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgrÞ p log
wtðgrÞ þ1
ffiffiffiffiffiffiffiffiffiffiffiffiffi wtðhrÞ q log
wtðhrÞ þ1 0
@
1
A 1
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðg½rÞ
p fgg^rðg½rÞ;
S2¼
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgiþ1Þ p
log
wtðgiþ1Þ þ1 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðg½iþ1Þ
p fpfðfÞ
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðhiþ1Þ q
log
wtðhiþ1Þ þ1 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðh½iþ1Þ
p fpf0ðf0Þ;
S3¼ P
rfiþ2
ffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgrÞ p log
wtðgrÞ þ1 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðg½rÞ
p fgg^rðg½rÞ P
rfiþ2
ffiffiffiffiffiffiffiffiffiffiffiffiffi wtðhrÞ q log
wtðhrÞ þ1 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðh½rÞ
p f^hhrðh½rÞ:
Lemma 5.19(Upper bound). kpðgÞ pðhÞkfdGðg;hÞ,that ispis Lipschitz.
Proof. SinceGis finitely generated, it su‰ces to prove that the normkpðgÞ pðgsÞk is bounded uniformly insAUWU1 andgAG. In this case the sum S3 does not appear, andS2¼ 1
log 2fgsðsÞhas norm 1
log 2. By eventually replacinggwithgsands withs1, we can always assume thath¼gssatisfies wtðhrÞ ¼wtðgrÞ þ1 for allrei. Then
kS1k2¼ Pi
r¼1
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgrÞ þ1 p
log
wtðgrÞ þ2
ffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgrÞ p log
wtðgrÞ þ1
!2
wtðg½rÞ:
Since the functionx7!
ffiffiffix p
logðxþ1Þis increasing forxfe21 it follows that
kS1k2fPi
r¼1
½ ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgrÞ þ1
p ffiffiffiffiffiffiffiffiffiffiffiffiffi wtðgrÞ
p 2
log2
wtðgrÞ þ1 wtðg½rÞePi
r¼1
wtðg½rÞ wtðgrÞlog2
wtðgrÞ þ1: Lemma 5.18 implies now that
kS1k2¼Oð1Þ: r ð19Þ
Lemma 5.20(Lower bound). kpðgÞ pðhÞkg r
dGðg;hÞ log2
dGðg;hÞ þ1if g3h.
Proof. We can write kS3k2g P
rfiþ2
wtðgrÞ log2
wtðgrÞ þ1
wtðg½rÞr
wtðg½rÞ2
ð20Þ
þ P
rfiþ2
wtðhrÞ log2
wtðhrÞ þ1
wtðh½rÞr
wtðh½rÞ2
:
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