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Computations of K- and L-Theory of Cocompact Planar Groups

WOLFGANG L ¨UCK and ROLAND STAMM

Institut f¨ur Mathematik und Informatik, Westf¨alische Wilhelms-Universtit¨at, Einsteinstr. 62, 48149 M¨unster, Germany. e-mail:{lueck,stammr}@math.uni-muenster.de

(Received: April 2000)

Abstract. The verification of the isomorphism conjectures of Baum and Connes and Farrell and Jones for certain classes of groups is used to compute the algebraicK- andL-theory and the topolo- gicalK-theory of cocompact planar groups (=cocompact N.E.C-groups) and of groupsGappearing in an extension 1 Zn G π 1 whereπ is a finite group and the conjugationπ- action onZnis free outside 0 Zn. These computations apply, for instance, to two-dimensional crystallographic groups and cocompact Fuchsian groups.

Mathematics Subject Classifications (2000): 19B28, 19D50, 19G24, 19K99.

Key words: K-theory, L-theory, planar groups.

0. Introduction

The goal of this paper is to compute the algebraic K-groupsKp(ZG) forp61, the algebraicL-groupsLp(ZG)forp∈Z(mostly after inverting 2) of the integral group ringZGand the topologicalK-groupsKp(Cr(G))forp∈Zof the reduced C-algebraCr(G)for certain infinite (discrete) groupsG. Namely, we assume that Gis either a cocompact planar group or that there is an exact sequence 1→ZnGπ → 1, whereπ is a finite group and the conjugation action ofπ onZn is free outside 0 ∈ Zn. A cocompact planar group is a discontinuous group of isometries ofS2, R2 orH2 with compact quotient. More information about these groups and the result of the explicit computations will be given in Section 4 (see Theorems 4.4 and 4.9).

For our techniques to work it is crucial to have very good information on the structure of the finite subgroups, as well as their normalizers, and the infinite virtually cyclic subgroups of cocompact planar groups. More explicitly, we use that all maximal finite subgroups are either cyclic or dihedral, and that a com- mon subgroup of any two different maximal finite subgroups has at most two elements. Furthermore, the normalizer NGM of a maximal finite subgroup M satisfies NGM = M, except if M is generated by a single reflection, in which case NGM ∼= Z×Z/2. These exceptions are responsible for the summands in- dexed byB and B00 in Theorem 4.4, whereas the other maximal finite subgroups

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correspond to the summands indexed byA. Finally, we have a complete list of the infinite virtually cyclic subgroups of a cocompact planar group; they are given as subgroups of very simple amalgams. This will allow us to reduce the computations in algebraicK- andL-theory from the family of virtually cyclic subgroups to the family of finite subgroups. All the facts about cocompact planar groups mentioned above will be recollected in Theorem 4.3 and Lemma 4.5 and 4.6.

Examples of cocompact planar groups are cocompact Fuchsian groups. Next we give the result in this comparatively easy case as an illustration.

THEOREM 0.1. LetF be a cocompact Fuchsian group with presentation F = ha1, b1, . . . , ag, bg, c1, . . . , ct |cγ11 = · · ·

=ctγt =c11· · ·ct 1[a1, b1]· · ·[ag, bg]=1i for integersg, t>0 andγi >1. Then

(a) the inclusions of the maximal subgroupsZ/γi = hciiinduce an isomorphism Mt

i=1

Whq(Z/γi)−→= Whq(F )

for q61. If the isomorphism conjecture for algebraic K-theory (see 1.9 and Theorem 1.10) holds forF also in dimensionsq>2, then this is an isomorph- ism for all q ∈ Z. (Information about Whq(Z/γi) is given in Theorem 3.2 (d);

(b) there are isomorphisms

Lq(ZF )[1/2]∼=









1+Pt

i=1

γi

2

·Z[1/2] q ≡0(4),

(2g)·Z[1/2] q ≡1(4),

1+Pt

i=1

hγi1 2

i·Z[1/2] q ≡2(4),

0 q ≡3(4),

where [r] forr ∈Rdenotes the largest integer less than or equal tor;

(c) there are isomorphisms Kq(Cr(F ))∼=

2+Pt

i=1i −1)

·Z q=0,

(2g)·Z q=1.

We will give more information about the algebraicL-theory of cocompact Fuch- sian groups without inverting 2 in Remark 4.10. The algebraicK-theory in dimen- sions 61 of cocompact Fuchsian groups has been computed in [7].

Other examples of cocompact planar groups are two-dimensional crystallo- graphic groups. Their K- andL-theory is explicitly computed in Section 5. For a two-dimensional crystallographic group Gthe algebraic K-theory ofZGin di- mensions 61 has already been determined in [32], and the topological K-theory ofCr(G)in [51].

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In Section 6 we will prove a result which is similar to that of Theorem 4.4 but applies to certain virtually Abelian groups whose classifying space for the family of finite subgroups EG = E(G,FIN) is of higher dimension. (For an infinite cocompact planar groupG, a model forEGisR2orH2with the obviousG-action, and for the groups Gappearing below,Rn with a certain G-action is a model for EG.)

THEOREM 0.2. Let 1 → ZnGπ1 be a group extension for a finite groupπ such that the conjugation action ofπ onZn is free, i.e. the only element inπ with a fixed point inZn different from zero is the identity element inπ. Let {Mα | αA} be a complete system of representatives of conjugacy classes of maximal finite subgroups ofG. Then

(a) the natural map induced by the inclusions of subgroups M

αA

Whq(Mα)→Whq(G)

is an isomorphism forq61, andKq(ZG)is trivial forq6 −2.

If the isomorphism conjecture in algebraicK-theory (see 1.9 and Theorem 1.10) holds also forq>2, then the map above is an isomorphism for allq ∈Z;

(b) there are short exact sequences

0 → M

αA

eLq(ZMα)[1/2]Lq(ZG)[1/2]

Hq(G\EG;L(Z))[1/2]→0,

where L(Z)is theL-theory spectrum associated to the ringZ,H(−;L(Z)) is the associated homology theory and the first map is induced by the various inclusionsMαG.

If we invert 2|π|, this sequence splits and we obtain isomorphisms M

αA

eLq(ZMα) 1

2|π|

!

Hq\Tn;L(Z)) 1

2|π|

−→= Lq(ZG) 1

2|π|

, where theπ-action onTnis induced by the conjugation action ofπonZn; (c) there are short exact sequences

0→M

αA

Keq(Cr(Mα))Kq(Cr(G))Kq(G\EG)→0,

whereKq(G\EG)is the topological complexK-homology ofG\EGand the first map is induced by the various inclusionsMαG.

If we invert|π|, this sequence splits and we obtain isomorphisms M

αA

Keq(Cr(Mα)) 1

|π|

!

Kq\Tn) 1

|π|

−→= Kq(Cr(G)) 1

|π|

.

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We will present more detailed information on the L-theory (without inverting 2) of groups as in Theorem 0.2 in Remark 6.4. Furthermore, we can generalize the methods of Theorem 0.1 and 0.2 to yield similar results for groups which are given as extensions of the form 1→ZnGπ →1, whereπ ∼=D2mis a dihedral group of order 2msuch that the subgroupZ/macts freely onZn. See Remark 6.5 for more information on this.

Our computations use the isomorphism conjectures inK-andL-theory due to Farrell and Jones and to Baum and Connes which are known to be true for the groups we consider here. We exploit the unified treatment of these conjectures of [15]. Thus the computation is reduced to the investigation of the homology of certain spaces over the orbit category with coefficients in K- and L-spectra over the orbit category which will be carried out by homological methods, mainly Mayer–Vietoris sequences. There are various spectral sequences to compute these homology groups but they turn out to be too complicated even for the relatively elementary groups we consider here. It seems to be very hard to compute theseK- and L-groups integrally (or after inverting 2) for more general groups even if one assumes in theK-theory case that one does know theK-theory of integral group rings of finite subgroups. Rationally these computations can be done via Chern characters and lead to rather general and explicit formulas, since the existence of the Chern characters guarantees that the relevant spectral sequences collapses [27]. The integral computations of K- and L-groups presented here exploit the explicit knowledge and special properties of the virtually cyclic and finite sub- groups and their normalizers of the groups under consideration (see Lemma 4.5 and Lemma 6.3).

The paper is organized as follows:

(1) Review of the isomorphism conjectures inK- andL-theory.

(2) Preliminaries about spaces over the orbit category.

(3) Preliminary computations of K- and L-groups of finite groups.

(4) Cocompact planar groups.

(5) Two-dimensional crystallographic groups.

(6) Extensions of finite groups with a free Abelian group references.

1. Review of the Isomorphism Conjectures inKKK- andLLL-Theory

We want to review the isomorphism conjectures inK- andL-theory as far as we will need here. Since we want to do this in the language of spaces and spectra over a category we give some basic facts about these notions. More information can be found for instance in [15, 18].

Given a (discrete) group G, a familyF of subgroups is a set of subgroups of G closed under taking subgroups and conjugates. Our main examples for famil- ies will be the families TR,FIN, VC and ALL, respectively, consisting of the trivial subgroup, finite subgroups, virtually cyclic subgroups and all subgroups,

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respectively. Recall thatGis virtually cyclic ifGis finite or containsZas subgroup of finite index. The orbit categoryOr(G,F)ofGwith respect toFhas as objects homogeneous spaces G/H with HF and as morphismsG-maps. If F is the familyALLof all subgroups, we abbreviateOr(G,ALL)byOr(G).

A contravariant (pointed)Or(G)-space is a contravariant functor fromOr(G) to the category of (pointed) spaces. A morphism between contravariant (pointed) Or(G)-spaces is a natural transformation. A G-space X defines a contravariant Or(G)-space by assigning toG/H itsH-fixed point setXH =mapG(G/H, X). A covariantOr(G)-spectrum is a covariant functor from the categoryOr(G)into the category Spectra of spectra. An object E in Spectra is a sequence of spaces (En)n∈Z together with structure maps σn: 6EnEn+1 for each n ∈ Z. A map f : EF of spectra is a sequence(fn: EnFn)n∈Z of maps satisfying fn+1◦σnE = σnF6fn for all n∈ Z. Theqth homotopy group πq(E)of a spectrum E forq ∈ Zis the colimit colimn→∞πq+n(En)with respect to the obvious maps πq+n(En)πq+n+1(En+1)induced by the structure mapsσnand the suspension homomorphisms. Next we review our main examples of covariantOr(G)-spectra.

LetGroupoidsbe the category of groupoids. LetGroupoidsinjbe the subcat- egory ofGroupoidswhich has the same objects asGroupoidsand as morphisms covariant functors F: G0G1 which are faithful, i.e., for any two objects x, y inG0the induced map morG0(x, y)−→morG1(F (x), F (y))is injective. A leftG- set S defines a groupoid GG(S), where Ob(GG(S)) = S and mor(s, t) = {g ∈ G | gs = t}for s, tS. The composition law is given by group multiplication.

Obviously a map of leftG-sets defines a functor of the associated groupoids. The categoryG(G/H )is equivalent to the groupoid associated withH which has one object andHas set of morphisms, and henceG(G/H )can serve as a substitute for the subgroupH. Thus we obtain a covariant functor

GG: Or(G)→Groupoidsinj. (1.1)

In [15, section 2] covariant functors Kalg: Groupoids−→Spectra, L : Groupoids−→Spectra, Ktop: Groupoidsinj −→Spectra,

are constructed using [34] and [40] in the algebraic context. (Unfortunately there is a problem in the actual construction of Ktop concerning the pairing µ in [15, page 217] which will be corrected elsewhere. This does not affect the results of this paper.) We denote their composition with GG by the same letters or by the following abbreviations and obtain covariant functors

K = KalgG : Or(G)−→Spectra, (1.2)

L = LG: Or(G)−→Spectra, (1.3)

K = KtopG : Or(G)−→Spectra. (1.4)

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Notice that πq(L(G/H )) ∼= Lq(ZH ), πq(Kalg(G/H )) ∼= Kq(ZH ) and πq(Ktop (G/H )) ∼= Kq(Cr(H )), where Cr(H ) is the reduced C-algebra of the group H and Kq(Cr(H )) denotes its topological K-theory. Functoriality for a G-map G/HG/K, g0H 7→g0g1Kcorresponds under this isomorphism to induction with respect to the injective homomorphismHKgiven byh7→ghg1.

If∗denotes the trivial groupoid consisting of one morphism, there is for any groupoid G the canonical projection pr : G → ∗. Denote by eL(G) the homo- topy fiber of the map of spectra L(pr): L(G)L(). Thus we obtain covariant functors

eK=eKalgG : Or(G)−→Spectra, (1.5) eL=eLG: Or(G)−→Spectra, (1.6) eK=eKtopG : Or(G,FIN)−→Spectra. (1.7) Notice that we have defined eKtopG only for Or(G,FIN). The problem is that pr : G → ∗ is not a morphism in Groupoidsinj. However, if we replace the reduced C-algebra by the maximal C-algebra, then Ktop is indeed a functor on Groupoids, and for amenable groups such as all finite groups and virtually Abelian groups the natural map from the maximal to the reduced C-algebra is an isomorphism [33, Theorem 7.3.9 on page 243]. Notice that we only needKe = eKtopG : Or(G,FIN) −→ Spectrasince it will be only applied in context with Or(G)-spacesXfor whichX(G/H )is empty for infiniteH.

The homology HqG(X;E)of a contravariant Or(G)-space X with coefficients in the covariant Or(G)-spectrum E is defined for q ∈ Zin [15, section 4] using Or(G)-CW-approximations. The above homology groups are functorial inX and E. We get from [15, Lemma 4.4]

LEMMA 1.1. HpG(X, A;E) is an unreduced homology theory on pairs of con- travariant Or(G)-spaces which satisfy the WHE-axiom and the disjoint union axiom.

To be more precise, homology theory means that homotopic maps of pairs of contravariant Or(G)-spaces induce the same maps on the homology groups, that there are long exact sequences of pairs(X, A), and that for any commutative diagram of contravariantOr(G)-spaces

X0 i2

i1 //X1 j1

x2

j2 //X

the map (j2, i1): (X2, X0) −→ (X, X1) induces an isomorphism on homology, provided that the evaluation of the diagram at any objectG/H yields a pushout of

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spaces with a cofibration of spaces as upper horizontal arrow. We will frequently use the associated long exact Mayer–Vietoris sequence

· · · −→δ HpG(X0;E)HpG(X1;E)HpG(X2;E)HpG(X;E)

−→ HpG1(X0;E)→ · · · .

The disjoint union axiom says that for an arbitrary disjoint union the obvious map from the direct sum of the homology groups of the various summands to the homology of the disjoint union is an isomorphism. The WHE-axiom requires that a weak homotopy equivalence of contravariantOr(G)-spaces induces an isomorph- ism on homology, where a mapf: XY ofOr(G)-spaces or spectra is calledn- connected resp. a weak homotopy equivalence, if the mapf (G/H ): X(G/H )Y (G/H )isn-connected resp. a weak homotopy equivalence for every objectG/H. In order to guarantee the WHE-axiom,Or(G)-CW-approximations are used in the definitions. Notice, however, that we will almost everywhere do calculations with theOr(G)-spaceXitself and not with itsOr(G)-CW-approximations, which will be quite convenient since the Or(G)-spaces X we will deal with will very often be very simple. Namely, we will consider theOr(G)-spaces?G,F associated to a family F, which assigns to an object G/H the space ∗ consisting of one point if H belongs to F and the empty set ∅ otherwise. For these spaces it will be comparatively easy to check whether the necessary conditions are satisfied for the square above to get a Mayer–Vietoris sequence.

Notice in the sequel that for any covariantOr(G)-spectrum E there is a canon- ical isomorphism

HqG(?G,ALL;E)−→= πq(E(G/G)),

which comes from the fact that?G,ALLis anOr(G)-CW-complex. The isomorph- ism conjecture for a groupG, a family of subgroupsFand anOr(G)-spectrum E says that the map induced by the inclusion?G,F?G,ALL

HqG(?G,F;E)HqG(?G,ALL;E)=πq(E(G/G)) (1.8) is an isomorphism for all q ∈ Z. The philosophy is to compute the groups of interest πq(E(G/G)) by the values of E(G/H ) on the groups in HF. The isomorphism conjectures of Farrell and Jones for algebraicK-theory andL-theory are the special cases where E is given by the Or(G)-spectra K and L of (1.2) and (1.3) andF is the familyVCof virtually cyclic subgroups of G. The Baum–

Connes conjecture is the special case where E is given by theOr(G)-spectra Ktop of (1.4) andFis the familyFIN of finite subgroups ofG. The Farrell and Jones isomorphism conjecture and the Baum–Connes conjecture provide tools to com- puteπq(Kalg(G/G))=Kq(ZG),πq(L(G/G))=Lq(ZG)andπq(Ktop(G/G))= Kq(Cr(G)) in terms of data given by the virtually cyclic subgroups or the finite

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subgroups ofG. IfGis torsion free, these conjectures predict that forq ∈Z Whq(G)∼=0,

Lq(ZG)∼=Hq(BG;L(Z)), Kq(Cr(G))∼=Kq(BG),

whereHq(BG;L(Z)) is the homology of the classifying space BGwith respect to the L-theory spectrum associated to the ring Z, Kq(BG) is the topological complexK-homology ofBGand Whq(G)denotes the reduced negative or zeroth K-group Keq(ZG) for q60, the ordinary Whitehead group Wh(G) for q = 1 and Waldhausen’s definition for q>1 in terms of the fiber of the assembly map BG+K(Z)K(ZG).

We mention that the assembly map appearing in the original conjectures of Farrell and Jones and of Baum and Connes are different from the one presented here. Their identification is discussed in [15, page 239, page 247–248] and based on [11] and [39, Proposition 8.4 on page 421].

THEOREM 1.2. LetGbe a planar group with compact orbit space or a virtually finitely generated Abelian group. Then the assembly maps

HqG(?G,VC;Kalg)HqG(?G,ALL;Kalg)=Kq(ZG) forq61,

HqG(?G,FIN;L)[1/2]HqG(?G,ALL;L)[1/2]=Lq(ZG)[1/2] forq∈Z, HqG(?G,FIN;Ktop)HqG(?G,ALL;Ktop)=Kq(Cr(G)) forq ∈Z, are isomorphisms. The first map is surjective forq =2.

Here and in the sequel A[1/m] for an integer m>1 means AZ Z[1/m]

for Z[1/m] = {a ·mb ∈ Q | a, b ∈ Z}. Thus A[1/m] is obtained from A by inverting m. The claim for algebraic K- and L-theory is a consequence of the results of [18, Proposition 2.3, Proposition 2.4 and Remark 2.1.3], [50] and Theorem 2.3. Since we will invert 2 in (almost) all our L-theory calculations we do not have to distinguish between the various decorations of L-groups such as Lh,Ls orL−∞ as they differ by 2-torsion because of the Rothenberg sequences.

The Baum–Connes-conjecture has been proven for a very large class of groups including virtually finitely generated Abelian groups and cocompact planar groups [21, Theorem 1.12].

2. Preliminaries About Spaces Over the Orbit Category

In this section we prove some facts about spaces over the orbit category and their homology which will be needed later.

Given a homomorphism of groups i: HG, there is an induced functor I = I (i): Or(H ) → Or(G) sendingH /K toG×i H /K = G/ i(K). Given a

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(covariant or contravariant) Or(G)-space Y, we obtain a (covariant or contravari- ant)Or(H )-spaceIY called the restriction ofY withI by the compositionYI. Given a covariantOr(H )-spaceX, its inductionIXis the covariantOr(G)-space defined in [15, Definition 1.8]. Its value at the objectG/KofOr(G)is the quotient space

a

H /LOr(H )

X(H /L)×mapG(G/K, G/ i(L))/,

where∼is the equivalence relation generated by(X(φ)(x), ψ)(x, I (φ)ψ)for aH-mapφ: H /LH /L0, aG-mapψ: G/KG(i(L))andxX(H /L0).

There is an adjunction homeomorphism for an Or(G)-space X and an Or(G)- spaceY (see [15, Lemma 1.9])

homOr(G)(IX, Y )−→= homOr(H )(X, IY ). (2.1) In the sequel we use the identification of the Weyl group WGH =NGH /H with the automorphism group autG(G/H, G/H ) which sends gHNGH /H to the G-mapRg−1: G/HG/H g0H 7→ g0g1H. Notice that autG(G/H, G/H ) = mapG(G/H, G/H )holds for finiteHbut not in general (see [26, Example 1.32 on page 22]).

LEMMA 2.1. Let G be a group with subgroups H, LG. Let {Hα|α ∈ A}

be a complete system of representatives of L-conjugacy classes of subgroups of L which are G-conjugated to H. To every index αAchoose an isomorphism µα: G/HG/Hα. LetI =I (L)be the functor induced by the inclusionL ,G. Then we have forKL:

(a) The following map is a natural equivalence of functorsOr(L)→Sets T (L/K): a

αA

mapL(L/Hα, L/K)×

×WLHαWGHα −→mapG(G/H, G/K) [φ, ψ]7→(IdG×Lφ)ψµα,

(b) There is a homeomorphism, natural inX, a

αA

X(L/Hα)×WLHα WGHα −→IX(G/H ) for every contravariant Or(L)-spaceX,

(c) There is a natural isomorphism HqG(IX;E)−→= HqL(X;E)

for E one of the spectra associated toGandLin (1.2)–(1.7),

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(d) The map from {gL\G/NGH | gH g1L} to the set of L-conjugacy classes of subgroups of LbeingG-conjugated toH which sendsLgNGH to (gH g−1)Lis bijective.

Proof. (a), (b) and (d) are elementary consequences of the definitions. (c) fol- lows from the facts that induction with I: Or(L) → Or(G) sends an Or(L)- CW-approximation to anOr(G)-CW-approximation and that the canonical map ELIEGis an equivalence ofOr(L)-spectra together with the adjunction (2.1) and [15, Lemma 4.6].

Sometimes we can use smaller families than VC such as the family FIN of finite subgroups as explained in the next result. Notice that forn= ∞andm=1 it is just [18, Theorem A.10].

DEFINITION 2.2. LetGbe a group, and letF be a family of subgroups ofG. For a subgroupHofG, we defineHFto be the family of subgroups ofH given as {H ∩K|KF}.

THEOREM 2.3. LetFG be families of subgroups of the group G. Letm>1 andnbe integers. Suppose for everyHGthat the assembly map

HqH(?H,H∩F;I (H )E)[1/m]HqH(?H,ALL;I (H )E)[1/m]

is an isomorphism forq6n. Then the relative assembly map HqG(?G,F;E)[1/m]HqG(?G,G;E)[1/m]

is an isomorphism forq6n.

Proof. In the sequel we use the identification HpG(?G,F;E)=πq(hocolim

Or(G,F) E)

as explained in [15, section 3]. By assumption the map πq

hocolim

Or(H,H∩F)I (H )E

[1/m]→πq(E(G/H ))[1/m]

is an isomorphism for q6n and HG. A standard spectral sequence argu- ment applied to the Atiyah–Hirzebruch spectral sequence [15, Theorem 4.7] or the Bousfield–Kan spectral sequence [9, XXII 5.7 on page 339] shows that the induced map

πq

hocolim

Or(G,G) hocolim

Or(H,H∩F)I (H )E

[1/m]→πq(hocolim

Or(G,G) E)[1/m]

is an isomorphism forq6n. There is an equivalence of categories

Or(G,F)(G/H )−→= Or(H, H ∩F) (G/FG/H )7→H /F,

where Or(G,F)(G/H ) denotes the category of objects over G/H. For E0(G/FG/H ):=E(G/F )we get an isomorphism

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πq

hocolim

G/HOr(G,G) hocolim

Or(H,H∩F)I (H )E ∼=πq

hocolim

G/HOr(G,G) hocolim

Or(G,F)G/HE0

. By [24, Theorem 2.4] the homotopy colimits commute, hence there is an isomor- phism forq6n

πq

hocolim

Or(G,G) E

[1/m] ∼= πq

hocolim

G/HOr(G,G) hocolim

Or(H,H∩F)I (H )E

[1/m]

∼= πq

hocolim

G/H∈Or(G,G) hocolim

Or(H,H∩F)I (H )E

[1/m]

∼= πq

hocolim

G/H∈Or(G,G) hocolim

Or(G,F)G/HE0

[1/m]

∼= πq

hocolim

G/H∈Or(G,F) hocolim

Or(G,G)G/HE0

[1/m]

∼= πq

hocolim

Or(G,F) E

[1/m].

Recall that a classifying space E(G,F) for a family F of subgroups ofG is a G-CW-complex whoseH-fixed point set is contractible if HF and empty otherwise. Such aG-space is unique up toG-homotopy. In particularE(G,TR)is a model forEG. We abbreviateEG=E(G,FIN)for the familyFIN of finite subgroups.

For the reader’s convenience we briefly sketch a different more geometric proof of Theorem 2.3. Namely, given a model forE(G,G), one can construct a model for E(G,F)by replacing each cellG/H×DninE(G,G)byG×HE(H, H∩F)×Dn and then use Mayer–Vietoris sequences. Notice that the assumption in Theorem 2.3 implies that for eachHGthe projection induces an isomorphism

HqH(?H,H∩F;I (H )E)[1/m] =HpG(G×H E(H, HF);E)[1/m]

=

−→HpG(G/H;E)[1/m]=HqH(?H,ALL;I (H )E)[1/m],

where we interpret aG-space as aOr(G)-space by assigning toG/Lits L-fixed point set.

The next result follows from the definitions of Whq(G)in [47, Definition 15.6 on page 228 and Proposition 15.7 on page 229], from the definition ofHG(X, A;E) in [15, Section 4] and from [15, Lemma 7.6].

LEMMA 2.4. For a groupGthere is an isomorphism

HqG(?G,ALL, ?G,TR;Kalg)=







Whq(G) q>2,

Wh(G)=Wh1(G) q =1, Ke0(ZG)=Wh0(G) q =0, Kq(ZG)=Whq(G) q6 −1, which is natural inG.

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LEMMA 2.5. The assembly map

HqOr(G)(?G,FIN;K)−→= HqOr(G)(?G,ALL;K)

is an isomorphism for any q ∈ Zif G = Zor Z/2∗Z/2, and an isomorphism forq62 ifG=Z/2×Z,Z/2×(Z/2∗Z/2),Z/4Z/2Z/4, orZ/4Z/2(Z/2)2. Proof. We begin with the case G = Z. A model forEG = E(G,FIN) is the universal covering of S1. Therefore, the source of the assembly map above reduces toKq(Z)Kq1(Z)and the assembly map itself is the restriction of the Bass–Heller–Swan isomorphism (see [4, Chapter XII], [5] and [37, Corollary to Theorem 8 on p. 114])

Kq(Z)Kq1(Z)⊕Nilq(Z)⊕Nilq(Z)Kq(Z[Z])

to the first two summands. Since the ringZis regular and hence all its Nil-groups are trivial, the assembly map is an isomorphism forG=Z.

ForG=Z/2∗Z/2=Z o Z/2 there is a model forEGwithRas underlying space such thatG\EGis the unit interval. Then the assembly map in question can be identified with the obvious map Whq(Z/2)⊕Whq(Z/2) → Whq(Z/2∗Z/2) which is bijective by a result of Waldhausen [47, Corollary 11.5 and the following remark].

By Theorem 3.2 (e) the Nil-groups ofZ[Z/2×Zl] are trivial forq62 andl>0.

So the claim follows for G= Z×Z/2 from the Bass–Heller–Swan Theorem [4, Chapter XII], [5] and [37, Corollary to Theorem 8 on p. 114].

In the remaining casesGis of the shapeG =G1Z/2G2for finite groupsGi

such that Whq(Gi)=0 forq61 (see Theorem 3.2 (div)). The claim forq6 −1 follows from [19, Theorem 2.1]. We obtain from [47, Theorem 1 on page 137] the exact sequence

Wh2(Z/2) → Wh2(G1)⊕Wh2(G2)→Wh2(G)→Wh(Z/2)

→ Wh(G1)⊕Wh(G2)→Wh(G)→Ke0(Z[Z/2])

Ke0(ZG1)Ke0(ZG2)Ke0(ZG)→0

where it is not clear a priori why the last map is surjective. This follows from the exact sequence, obtained by applying the same argument toG×Z =(G1× Z)Z/2×Z(G2×Z),

Wh(G1×Z)⊕Wh(G2×Z)→Wh(G×Z)Ke0(Z[Z/2×Z]),

the computation Ke0(Z/2×Z) = 0 from Theorem 3.2 (diii) and (e) and the fact that Ke0(ZG1)Ke0(ZG2)Ke0(ZG)is a natural direct summand in Wh(G1× Z)⊕Wh(G2×Z) → Wh(G×Z)by the Bass–Heller–Swan decomposition. In order to get the claim for q = 0,1,2, one constructs an exact sequence as above but now withHqG(?G,FIN;Kalg)instead of Whq(G), together with a map between these exact sequences, and uses the five-lemma. The last exact sequence is the

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Mayer–Vietoris sequence associated to theG-CW-model forEGwhich has one 1-cell with isotropy group Z/2 and two 0-cells with isotropy groups G1 andG2

[43, Theorem 7 on page 32 and Corollary on page 36].

LEMMA 2.6. Let G be a group and let LG be a normal subgroup such that there is an epimorphism f: GL inducing the identity onL. Denote by SUB(L)the family of subgroups ofGwhich consists of the subgroups ofL. Then there is an isomorphism

HqG(?G,SUB(L);L)Hq(B(G/L);L(ZL)),

and analogously for both versions ofK-theory and all the reduced versions ofK- andL-theory.

Proof. We only treat the case of theL-theory spectrum L, the others are com- pletely analogous. We get from the definitions and [15, section 7] an isomorphism

HqG(?G,SUB(L);L)∼=πq(E(G/L)+G/LL(G/L)),

sinceEG/Lregarded as aG-space via the projectionGG/Lis a model for the classifying spaceE(G,SUB(L))ofGfor the familySUB(L). Fromf we obtain a morphism inGroupoidsinj

f: GG(G/L)GL(L/L).

Notice that G/L = autG(G/L, G/L)acts on GG(G/L)in the obvious way and that this action induces a non-trivial action on L(GG(G/L))although it induces a trivial action on the homotopy groups. If we equipGL(L/L)with the trivialG/L- action, the map fisL-equivariant. Sincefis an equivalence of categories, the induced map πq(L(GG(G/L)))πq(L(GL(L/L))) is an isomorphism. Hence the induced map

πq(E(G/L)+G/LL(G/L))

=

−→πq(E(G/L)+G/LL(GL(L/L)))=Hq(B(G/L);L(ZL)) is an isomorphism [15, Lemma 4.6].

DEFINITION 2.7. If E is a spectrum, we denote the generalized homology of a space X which is associated to E byH(X;E). If E is the topological K-theory spectrum K=K(C), then we also writeK(X)=H(X;K).

LEMMA 2.8. LetGbe a discrete group. LetAbe a ring withZ ⊂ A⊂ Qsuch that the order of any finite subgroup ofGis invertible inA.

(a) Let H be any generalized homology theory. Then we obtain a natural iso- morphism

H(BG)ZA−→= H(G\EG)ZA.

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(b) There is a long exact sequence

· · · → Hq+1(G\EG;L(Z))HqG(?G,FIN;eL)HqG(?G,FIN;L)

Hq(G\EG;L(Z))→ · · · ,

where L(Z)is theL-theory spectrum associated to the ringZ. This sequence splits after tensoring withA, yielding isomorphisms

Hq(G\EG;L(Z))ZAHqG(?G,FIN;eL)

ZA−→= HqG(?G,FIN;L)ZA.

(c) For topological K-theory we obtain the long exact sequence

· · · → Kq+1(G\EG)HqG(?G,FIN;K)e →HqG(?G,FIN;K)

Kq(G\EG)→ · · · .

This sequence splits after tensoring withAyielding isomorphisms

Kq(G\EG)ZAHqG(?G,FIN;K)e ⊗ZA−→= HqG(?G,FIN;K)ZA.

Proof. (a) By the Atiyah–Hirzebruch spectral sequence it suffices to check the claimed isomorphism in the special case where H is the cellular homology H. The claim follows from the fact that the projection induces a homology equivalence of projective AG-chain complexes C(EG)Z AC(EG)Z A which is then an AG-chain homotopy equivalence and hence induces a chain homotopy equivalenceC(EG)ZGAC(EG)ZGA.

(b) There are natural maps ofOr(G)-spectraeLLL(Z), where L(Z)de- notes the constantOr(G)-spectrum with value L(Z)= L(). Since its evaluation at an objectG/H is a fibration of spectra, it induces a long exact sequence

· · · →HqG+1(X;L(Z))−−→δq+1 HqG(X;eL)HqG(X;L)HqG(X;L(Z))→ · · ·, for any contravariant Or(G)-space X. Notice that it suffices to check exactness for anyOr(G)-CW-complexXand hence for anyOr(G)-space of the form mapG (G/?, G/K)for any fixed object G/K inOr(G), where the claim reduces to the exactness of the long homotopy sequence associated to a fibration. We get from [15, Lemma 7.6] an identificationHqG(?G,FIN;L(Z))withHq(G\EG;L(Z))and thus the desired long exact sequence by takingX =?G,FIN.

The composition

Hq(BG;L(Z))=HqG(?G,TR;L)Hq(?G,FIN;L)Hq(G\EG;L(Z)) becomes an isomorphism after tensoring withAby assertion (a) and thus induces the splitting of the long exact sequence after tensoring withA.

The proof of (c) is analogous to that of assertion (b) taking into account that Kq(Y )=Hq(Y;Ktop(C))holds by definition.

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3. Preliminary Computations of K- and L-Groups of Finite Groups

In this section we state some computations aboutK-andL-groups for finite groups which we will use later in the computations for infinite groups.

DEFINITION 3.1. Letπbe a finite group. Byq(π ),r(π )andc(π ), we denote the number of irreducible rational, real respective complex representations ofπ. Let rC(π )be the number of isomorphisms classes of irreducible realπ-representations V which are of complex type, i.e. autRπ(V ) ∼= C. LetRO(π )resp.R(π )be the real resp. complex representation ring. For a positive integerm, we letZ/mdenote the cyclic group of orderm, andD2mis the dihedral group of order 2m.

THEOREM 3.2. For a finite groupπ, we have the following:

(a) There are isomorphismsRO(π )∼=Zr(π )andR(π )∼=Zc(π ). The numberq(π ) is the number of conjugacy classes of cyclic subgroups inπ, the numberc(π ) is the number of conjugacy classes of elements inπ and the numberr(π )is the number ofR-conjugacy classes of elements inπ, whereg1andg2inπare R-conjugated ifg1andg2org11andg2are conjugated,

(b) Kq(Cr(π ))∼=

R(π )∼=Zc(π ) q=0,

0 q=1.

In particular

K0(Cr(Z/m)) ∼= Zm K0(Cr(D2m)) ∼=

Zm/2+3 m≡0(2), Z(m1)/2+2 m≡1(2), (c) Lq(Zπ )[1/2]∼=Lq(Rπ )[1/2]∼=



Z[1/2]r(π ) q ≡0(4), Z[1/2]rC(π ) q ≡2(4),

0 q ≡1,3(4).

In particular,

L0(Z[Z/m])[1/2]∼=Z[1/2][(m+2)/2], L2(Z[Z/m])[1/2]∼=Z[1/2][(m1)/2], L0(Z[D2m])[1/2]∼=

Z[1/2]m/2+3 m≡0(2), Z[1/2](m1)/2+2 m≡1(2), L2(Z[D2m])[1/2]∼=0.

(d) (i) Kq(Zπ )=0 forq6 −2.

(ii) The rank of Wh(π )as an Abelian group isr(π )q(π ). We have Wh(Z/m)∼=Z[m/2]+1δ(m),

whereδ(m)is the number of divisors ofmand [m/2] is the largest integer less or equal tom/2.

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(iii) We have Whq(π ) = 0 forq61 for the following finite groupsπ = {1}, Z/2,Z/3,Z/4,Z/2×Z/2,D6,D8. Iflis a prime, thenK1(Z[Z/ l]) = K1(Z[Z/ l×Z/ l])=0. We have

Whq(Z/6)∼=

0 q =0,1, Z q = −1, Whq(D12)∼=

0 q =0,1, Z q = −1.

(iv) We have

Wh2(π )=0, forπ = {1},Z/2,Z/3,Z/4,

|Wh2(Z/6)|62, Wh2(D6)=Z/2, Wh2((Z/2)2)>(Z/2)2.

The assembly mapH2(BZ/2;K(Z))K2(Z[Z/2])is an isomorphism.

(e) There are isomorphisms for an integern>0 and a prime numberlandq ∈Z Lq(Z[Zn×π])[1/2]∼=

Mn i=0

n i

·Lqi(Z[π])[1/2],

Kq(Cr(Zn×π ))∼= Mn

i=0

n i

·Kqi(Cr(π )), Kq(Z[Zn×Z/ l])

∼=Kq(Z[Z/ l])n·Kq1(Z[Z/ l])n

2

·Kq2(Z[Z/ l]), q62, Whq(Zn×Z/ l)

∼=Whq(Z/ l)n·Whq1(Z/ l)n

2

·Whq2(Z/ l) q62, Nilq(Z[Zn×Z/ l])=0, q62.

Proof. (a) is proven in [42, Theorem 7 on page 19, Corollary 2 on page 96, page 102, page 106]. (b) follows from Morita equivalence applied to C[π] ∼= Qc(π )

i=1 M(ni, ni,C)and the computationK0(C) =Zand K1(C) =0. (c) follows from [40, Proposition 22.34 on page 253]. (d) The computations of Kq(Zπ )for q6 −1 follow from [13]; thatK1(Zπ )=0 forπ =Z/ lorZ/ l×Z/ lcan also be found in [4, Theorem 10.6, p. 695]. For information about Wh(π )we refer to [31]. The vanishing ofKe0(Zπ )is proven forπ =D6in [41, Theorem 8.2] and for π =D8in [41, Theorem 6.4]. The casesπ =Z/2,Z/3,Z/4,Z/6, and(Z/2)2are in [14, Corollary 5.17]. Finally, Ke0(ZD12) =0 follows from [14, Theorem 50.29 on page 266] and the fact that QD12 as aQ-algebra splits into copies ofQ and

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matrix algebras overQ, so its maximal order has vanishing class group by Morita equivalence.

The claims about Wh2(Z/n)forn =2,3,4,6 and for Wh2((Z/2)2)are taken from [16, Proposition 5], [17, p.482] and [46, p. 218 and 221]. We getK2(ZD6)∼= 3·Z/2 from [46, Theorem 3.1]. The assembly mapH2(BZ/2;K(Z))K2(Z[Z/2]) is an isomorphism by [17, Theorem on p. 482]. Now construct a commutative diagram

H2(BZ/2;K(Z)) =- H2(BD6;K(Z))

K2(Z[Z/2])

=

? - K2(ZD6)

?

whose lower horizontal arrow is split injective and whose upper horizontal arrow is an isomorphism by the Atiyah–Hirzebruch spectral sequence. Hence the right vertical arrow is split injective and Wh2(D6)=Z/2.

(e) The claim forL-groups follows from the Shaneson splitting [44, Theorem 5.1] and for topologicalK-groups for instance from the more general Voiculescu–

Pimsner sequence [8, Theorem 10.2.1 on page 83]. The claim for the algebraic K-groups follows for q60 from [4, Theorem 10.6 on page 695]. To prove the vanishing of the Nil1- and Nil2-terms, consider the following cartesian square of rings:

Z[Z/ l×Zk] t7→exp(2π i/ l)- Z[exp(2π i/ l)][Zk]

Z[Zk]

t7→1

? -Z/ l[Zk],

?

wheretis a generator ofZ/ l. Letξ :=exp(2π i/ l). By [30, Theorem 3.3 and 6.2]

and the methods of [46, Section 1], this diagram yields a long exact Mayer Vietoris sequence

K3(Z/ l[Zk]) → K2(Z[Z/ l×Zk])→K2(Z[Zk])⊕K2(Z[ξ][Zk])

K2(Z/ l[Zk])→K1(Z[Z/ l×Zk])

K1(Z[Zk])⊕K1(Z[ξ][Zk]).

The rings Z/ l, Z[ξ] and Z are regular, so they have trivial Nil-terms in any di- mension [37, Corollary to Theorem 8 on p. 122]. Furthermore, sinceZ/ lis a field, its higher algebraic K-groups are finite [36, Theorem 8 on p. 583], and the K- groups of a Dedekind ring (such as Z[ξ]) are finitely generated [38, Theorem 1 on p. 179]. Therefore, the groupsKi(Z/ l[Zk]), Ki(Z[Zk])and Ki(Z[ξ][Zk])are finitely generated fori = 1,2,3, and hence so isKi(Z[Z/ l×Zk])fori = 1,2.

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