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Strategy of proof: From Farrell-Jones to flow spaces (Lecture III)

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Strategy of proof: From Farrell-Jones to flow spaces (Lecture III)

Wolfgang Lück Bonn Germany

email wolfgang.lueck@him.uni-bonn.de http://www.him.uni-bonn.de/lueck/

Göttingen, June 23, 2011

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Outline

We first indicate how a proof of the Farrell-Jones Conjecture can be achieved if one has appropriateflow spaces.

We give a idea ofcontrolled topologyand how to achieve control by flow spaces

We briefly explain some basics concerningcoverings.

We state and explain anaxiomatic approachto the proof which works for hyperbolic groups.

We discuss that the existence of an appropriate flow space together with an appropriateflow estimateleads to a proof of the Farrell-Jones Conjecture for hyperbolic groups.

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Controlled Topology

The assembly map can be thought of anapproximationof the algebraicK- orL-theoryby a homology theory.

The basic feature between the left and right side of the assembly map is that for the left side one hasexcisionwhich is not present on the right side.

In general excision is available if one can makerepresenting cycles small.

A best illustration for this is the proof of excision for simplicial or singular homology which is based on thesubdivisionwhose effect is to make the support of cycles arbitrary small.

The first big step in the proof of the Farrell-Jones Conjecture is to interpret the assembly map as aforget controlmap.

Then the basic idea of proof is obvious: Find a procedure to make the support of a representing cocycle as small as possible without changing its class, i.e.,gain control.

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The next two results are prototypes of this idea.

Theorem (Controlledh-Cobordism Theorem,Ferry (1977)) Let M be a compact Riemannian manifold of dimension≥5. Then there exists an=M >0, such that every-controlled h-cobordism over M is trivial.

Theorem (α-approximation theorem,Ferry (1979))

If M is a closed topological manifold of dimension≥5andαis an open cover of M, then there is an open coverβ of M with the following property:

If N is a topological manifold of the same dimension and f:N →M is a properβ-homotopy equivalence, then f isα-close to a

homeomorphism.

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One basic idea is to pass togeometric modulesby remembering the position a basis.

For instance, if we have a simplicial complexX, each basis element of the simplicial chain complex has a position inX, namely the barycenter of the simplex. Similar, one may assign to a handlebody a position in the underlying manifold.

Given a metric spaceX, letC(X,R)be the following category:

Objects are collections{Mx}={Mx |x ∈X}, where eachMx is a finitely generated freeR-module and the support is requited to be locally finite.

Morphisms{fx,y}:{Mx} → {Ny}are given by collection of R-morphismsfx,y:Mx →Ny respecting certain finiteness conditions so that the composition can be defined by the usual formula for the multiplication of matrices.

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IfX comes with aG-action, thenGacts onC(X;R)and we can consider theG-fixed point setC(X,R)G. Denote byT(X;G)the full subcategory ofC(X;R)G where we additionally require that the support of a module is cocompact.

ObviouslyT(G;R) =C(G,R)G is the category of finitely generated freeRG-modules and hence

πn K(T(G;R))

=Kn(RG).

IfX aG-space, then the projection induces an equivalence of categoriesT(G×X;R)→ T(G;R). It induces forn∈Za homotopy equivalence after takingK-theory

πn K(T(G×X;R))−=→Kn(RG).

Imposing appropriatecontrol conditionsonT(G×X;R), leads to a subcategoryT (G×X;R)with the property that

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Theforget control map

πn K(Tc(G×EVCYC(G);R))

→πn K(T(G×EVCYC(G);R)) can be identified with the assembly map appearing in the K-theoretic Farrell-Jones Conjecture.

The control conditions say, very roughly speaking, that for morphisms{(fx,y}the set{dX(x,y)|(fx,y 6=0}is small.

Suppose thatG=π1(M)for a closed Riemannian manifold with negative sectional curvature.

The idea is to use the geodesic flow on the universal covering to gain the necessary control.

We will briefly explain this in the case, where the universal covering is the two-dimensional hyperbolic spaceH2.

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Consider two points with coordinates(x1,y1)and(x2,y2)in the upper half plane model of two-dimensional hyperbolic space. We want to use the geodesic flow to make their distance smaller in a functorial fashion. This is achieved by letting these points flow towards the boundary at infinity along the geodesic given by the vertical line through these points, i.e., towards infinity in the y-direction.

There is a fundamental problem: ifx1=x2, then the distance of these points is unchanged. Therefore we make the following prearrangement. Suppose thaty1<y2. Then we first let the point (x1,y1)flow so that it reaches a position wherey1=y2. Inspecting the hyperbolic metric, one sees that the distance between the two points(x1, τ)and(x2, τ)goes to zero ifτ goes to infinity. This is the basic idea to gain control in the negatively curved case.

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Why is the non-positively curved case harder?

Again, consider the upper half plane, but this time equip it with the flat Riemannian metric coming from Euclidean space.

Then the same construction makes sense, but the distance between two points(x1, τ)and(x2, τ)is unchanged if we change τ.

The basic first idea is to choose a focal point far away, say f := (x1+x2)/2, τ +169356991

, and then let(x1, τ)and(x2, τ) flow along the rays emanating from them and passing through the focal pointf.

In the beginning the effect is indeed that the distance becomes smaller, but as soon as we have passed the focal point the distance grows again. Either one chooses the focal point very far away or uses the idea of moving the focal point towards infinity while the points flow.

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The problem with this idea is obvious, we must describe this process in a functorial way and carefully check all the estimates to guarantee the desired effects.

The comments above are all rather vague. At least we want to give a preciseaxiomatic approach,which works at least in the case of hyperbolic groups. The axiomatic approach for

CAT(0)-groups is more complicated and will be omitted, some of the extra difficulties will be discussed when appropriate.

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Coverings

Definition (Open covering)

Anopen coveringU of a spaceX is a collection of open subsets {Ui |i ∈I}satisfyingX =∪i∈IUi.

Thedimension dim(U)ofU is the smallest natural numbernfor which every element inX is contained in at most(n+1)members ofU.

An open coveringVis a refinement of the open coveringU if for everyU ∈ U there existsV ∈ V withV ⊆U.

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Definition (Covering dimension)

The(topological) dimensionorcovering dimension dim(X)of a space X is the smallest natural numbernfor which every open covering possesses ann-dimensional refinement. (If no suchnexists, we write dim(X) =∞.)

IfY ⊆X is closed, then dim(Y)≤dim(X).

IFX =Y ∪Z for closedY,Z ⊆X, then

dim(X) =max{dim(Y),dim(Z)}.

IfMis an-dimensional manifold, then dim(M) =n.

IfX is an-dimensionalCW-complex, then dim(X) =n.

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Definition (Nerve)

LetU be an open covering. Therealization of its nerve|U |is the following simplicial complex: The set of vertices isU itself. The vertices U0,U1, . . . ,Unspan an-simplex if and on if∩ni=0Ui 6=∅.

Points|U |are formal sumsx =P

U∈UxUU, withxU ∈[0,1]such thatP

U∈UxU =1 and the intersection of all theU withxU 6=0 is non-empty, i.e.,{U|xU6=0}.

Every simplicial complex and in particular the realization of the nerve of an open cover can be equipped with thel1-metricd|U |, i.e., the metric where the distance between pointsx =P

UxUU andy =P

UyUU is given byd1(x,y) =P

U|xU−yU|.

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Let(X,dX)be a metric space andU an open covering of finite dimensionN.

Suppose thatβ ≥1 is aLebesgue numberforU, i.e., for every x ∈X there existsU ∈ UwithBβ(x)⊆U.

There is a map

f =fU:Z → |U |, x 7→ X

U∈U

fU(x)U,

where

fU(x) = aU(x) P

V∈UaV(x);

aU(x) = d(x,Z−U) =inf{d(x,u)|u ∈/ U}.

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Theorem (Contracting map)

If x,y ∈X satisfy dX(x,y)≤ 4(N+1)β , then we get

d|U |(f(x),f(y))≤ 12(N+1)2

β ·dX(x,y).

The largerβ is, the estimate applies more often and the stronger mapf is contracting.

The largerN is, the estimate applies less often and the weakerf is contracting. IfN =∞, there is no conclusion at all.

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Proof:

PutbV(x,y) :=aV(x)−aV(y)forV ∈ U.

|bV(x,y)| ≤dX(x,y)sincedX is a metric.

Since there are at most 2(N+1)elementsV ∈ U with bV(x,y)6=0, we get

X

V

|bV(x,y)| ≤2(N+1)d(x,y)≤ β 2. Since there isU∈ U withBβ(x)⊆U, we get

X

V

aV(x)≥aU(x)≥β.

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We compute:

fU(y)−fU(x)

= aU(y) P

V∈U aV(y) − aU(x) P

V∈UaV(x)

= aU(y)·(P

V∈UaV(x))−aU(x)·(P

V∈UaV(y) (P

V∈U aV(x))·(P

V∈UaV(y))

= aU(x)·P

VbV(x,y)−aU(x)·P

V aV(x) +aU(y)·P

VaV(x) (P

VaV(x))·(P

VaV(x)−bV(x,y))

= aU(x)·P

VbV(x,y)−bU(x,y)·P

VaV(x) (P

VaV(x))·(P

VaV(x)−bV(x,y)) .

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We estimate:

X

U

|fU(x)−fU(y)|

= X

U

aU(x)·P

VbV(x,y)−bU(x,y)·P

VaV(x) (P

VaV(x))·(P

VaV(x)−bV(x,y))

≤ X

U,aU(x)6=0

P

VbV(x,y) P

VaV(x)−bV(x,y)

+

X

U,bU(x,y)6=0

bU(x,y) P

VaV(x)−bV(x,y)

≤ 3(N+1)

P

V|bV(x,y)|

|P

VaV(x)−bV(x,y)|

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= 3(N+1)

P

V|bV(x,y)|

|P

VaV(x)−bV(x,y)|

≤ 3(N+1) 2(N+1)d(x,y)

|P

VaV(x)−bV(x,y)|

≤ 6(N+1)2d(x,y) P

VaV(x)−P

|bV(x,y)|

≤ 6(N+1)2d(x,y) β−2(N+1)d(x,y)

≤ 6(N+1)2d(x,y) β− β2

= 12(N+1)2d(x,y)

β .

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Definition (OpenF-covering)

LetF be a family of subgroups ofGand letY be aG-space. Anopen F-coveringU is an open covering ofY satisfying

U ∈ U,g ∈G =⇒ gU ∈ U;

U ∈ U,g ∈G,gU∩U 6=∅ =⇒ gU=U;

ForU∈ U the subgroupGU :={g∈G|gU =U}belongs toF.

Example

PutX =RandG=Z. Then

U = {(n,n+1)|n∈Z} ∪ {(n+1/2,n+3/2)|n∈Z};

V = {(n−1/2,n+3/2|n∈Z}, are openG-invariant coverings.

U is a openT R-covering, whereas there is noF for whichV is an

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Lemma

LetU be an openF-covering. ThenU is a simplicial complex with simplicial G-action and also a G-CW -complex such that all isotropy groups belong toF.

Definition (Weak Z-set condition)

A pair(X,X)satisfies theweakZ-set conditionif exists a homotopy H:X ×[0,1]→X, such thatH0=idX andHt(X)⊂X for everyt >0.

IfMis a manifold with boundary, then(M, ∂M)satisfies the weak Z-set condition because of the existence of a collar.

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Theorem (Axiomatic Formulation)

Let G be a finitely generated group. LetF be a family of subgroups of G. Suppose:

There exists a G-space X such that the underlying space X is the realization of an abstract simplicial complex;

There exists a G-space X which contains X as an open G-subspace such that the underlying space of X is compact, metrizable and contractible;

The pair(X,X)satisfies the weak Z -set condition.

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Theorem (continued)

There existswide openF-coverings, i.e.:

There is N ∈N, which only depends on the G-space X , such that for everyβ ≥1there exists an openF-coverU(β)of G×X with the following two properties:

For every gG and xX there exists U∈ U(β)such that Bβ(g)× {x} ⊂U;

The dimension of the open coverU(β)is smaller than or equal to N.

Then both the K - and L-theoretic Farrell-Jones Conjecture (with coefficients) holds for(G,F).

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An obvious choice for(X,X)isX =X ={•}. But then the existence of wide open coverings impliesF =ALL.

Proof: We can chooseβ so large thatBβ(e)contains a (finite) set of generatorsS. ChooseU∈ U withBβ(e)∈U. Then we have gU∩U 6=∅and hencegU =U for allg∈S. This impliesGU =G and henceG∈ F.

In some sense we will need the spaceX to obtain some additional spaces to maneuver open sets around in order avoid two many intersections.

It is crucial thatX is compact.

In some senseN andβconflict another. The larger we takeβ, the higher is the chance that many members ofU intersect.

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IfMis a closed manifold with non-positive sectional curvature and G=π1(M), then the canonical choice forX isMe and forX its standard compactificationM =Me ∪∂M.e

IfGis a hyperbolic group, one uses forX theRips complexand forX =X ∪∂G, where∂Gis theboundaryof a hyperbolic group.

In the sequel we consider this case.

The main technical point is then the construction of the wide VCYC-coveringU(β).

This will be achieved with the help of a flow space FS(X). We will use a variant which is closely related to the construction

ofMineyev(2005).

Our main contribution to the flow space in the case of a hyperbolic group is the following flow estimate.

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Theorem (Flow space estimate)

There exists a continuous G-equivariant map j:G×X →FS(X)

such that for everyα >0there exists a numberβ =β(α)such that the following holds:

If g,h∈G with dG(g,h)≤α and x ∈X then there isτ0∈[−β, β]such that for allτ ∈R

dFSτj(g,x), φτ+τ0j(h,x))≤fα(τ).

Here fα:R→[0,∞)is a function that depends only onαand has the property thatlimτ→∞fα(τ) =0.

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Then the next big step is to construct an appropriate openVCYC- covering on the flow space FS(X)such that the desired covering onG×X is obtained by pulling back this open covering on FS(X) withΦτ◦jfor appropriateτ.

Theorem (Long thin coverings)

There exists a natural number N such that for everyβ >0there is an VCYC-coverU ofFS(X)with the following properties:

dimU ≤N;

For every x ∈X there exists U∈ U such that

Φ[−β,β](x) :={Φτ(x)|τ ∈[−β, β]} ⊆U;

G\U is finite.

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One ingredient in the proof that the existence of long thin coverings implies the existence of wide open coverings is the conclusion by a compactness argument, that there existsδ >0 such that for everyc ∈FS(X)there existsUc ∈ U with

Bδ[−β,β](x))⊆Uc, ifU is the long thin covering forβ.

Next we explain why our strategy will not work for a smaller family thanVCYCI.

Consider a subgroupH ⊆Gwhich can be written as an extension 1→F →H →Z→1 for a finite groupH. Chooseg ∈H which maps to a generator ofZ. Then there arex ∈X andt ∈(0,∞) such thatφt(x) =gx andhx =x holds for allh∈F. Ifαsatisfies t < α, thenΦ[−α,α](x)⊆Uimpliesgx ∈Uandhx ∈U for all h∈F. HencegU∩U6=∅andhU∩U6=∅for allh∈F. This impliesg∈GU andh∈GU for allh∈F. HenceGU containsH.

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