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Morse quasiflats I

  • Jingyin Huang ORCID logo , Bruce Kleiner EMAIL logo und Stephan Stadler
Veröffentlicht/Copyright: 6. Januar 2022

Abstract

This is the first in a series of papers concerned with Morse quasiflats, which are a generalization of Morse quasigeodesics to arbitrary dimension. In this paper we introduce a number of alternative definitions, and under appropriate assumptions on the ambient space we show that they are equivalent and quasi-isometry invariant; we also give a variety of examples. The second paper proves that Morse quasiflats are asymptotically conical and have canonically defined Tits boundaries; it also gives some first applications.

Funding statement: The first author thanks the Max-Planck Institute for Mathematics at Bonn, where part of this work was done. The second author was supported by NSF grants DMS-1711556 and DMS-2005553 and a Simons Collaboration grant. The third author was supported by DFG grant SPP 2026.

A Some properties of quasiflats

A.1 Lipschitz quasiflats and quasi-retractions

Definition A.1.

Let KX be a closed subset. A map π:XK is called a λ-quasi-retraction if it is λ-Lipschitz and the restriction π|K has displacement at most λ.

Lemma A.2.

Let X be a length space and Φ:EnX an L-Lipschitz (L,A)-quasiflat with image Q. Then there exist a constant L¯ depending only on L and A, a metric space X¯, an L¯-bilipschitz embedding XX¯ and an L-Lipschitz retraction X¯X with the following additional properties: X¯ contains a L¯-bilipschitz flat Q¯ such that dH(Q,Q¯)<L and dH(X,X¯)<L.

Proof.

We glue 𝔼n×[0,L] to X along 𝔼n×{L} via Φ. The resulting space equipped with the induced length metric is denoted by X¯. We define Q¯=𝔼n×{0}, viewed as a subset of X¯. Note that for x,yQ¯, dX¯(x,y)<2L implies dX¯(x,y)=d𝔼n(x,y). Moreover, if d𝔼n(x,y)2L(2L+A), then dX¯(x,y)12Ld𝔼n(x,y). Hence for points x,y𝔼n with 2L<d𝔼n(x,y)<2L(2L+A) there holds dX¯(x,y)12L+Ad𝔼n(x,y) and the canonical embedding 𝔼n𝔼n×{0}X¯ is (2L+A)-bilipschitz. The remaining statements follow immediately from the construction. ∎

Corollary A.3.

Let X be a length space and Φ:EnX an L-Lipschitz (L,A)-quasiflat with image Q. Then there exist constants λ1 and λ2 which depend only on L,A and n, and a λ1-Lipschitz quasiretraction π:XQ such that d(x,π(x))λ2 for any xQ. Moreover, λ20 as A0.

Proof.

Choose a thickening X¯ as in Lemma A.2 and denote by Q¯X¯ the bilipschitz flat close to Q. By McShane’s extension lemma we obtain a Lipschitz retraction X¯Q¯, where the Lipschitz constant is controlled by L,A,n. Composing with the natural projection X¯X we obtain the required map since Q is at distance L from Q¯. ∎

The following lemma is a consequence of Section 3.4.

Lemma A.4.

Let X be a metric space with an L-Lipschitz bicombing and let QX an n-dimensional (L,A)-quasiflat with λ-Lipschitz quasiretraction π:XQ. Let σ𝐈n(X) and let S=spt(σ). Suppose that h:[0,1]×SX is the homotopy from S to π(S) induced by the bicombing on X. Let ρ=supxS{d(x,π(x))}. Then there exists a constant C>0 depending only on L,L,A and n such that

𝐌(h#(0,1×σ))Cλnρ𝐌(σ).

Corollary A.5.

Let Q,π,λ1,λ2 be as in Corollary A.3. Suppose X has L-Lipschitz bicombing. Let σ𝐈n(X) such that S=spt(σ)N2ρ(Q)Nρ(Q). Suppose that the map h:[0,1]×SX is the homotopy from S to π(S) induced by the bicombing on X. Suppose ρ>λ2. Then there exists a constant C>0 depending only on L,L,A and n such that

𝐌(h#(0,1×σ))Cλnρ𝐌(σ).

Proof.

By Lemma A.4, it suffices to show d(x,π(x))Cρ for any xS. Let z be a point in Q such that ρd(x,z)=d(x,Q)2ρ. Then

d(x,π(x))d(x,z)+d(z,π(z))+d(π(z),π(x))
2ρ+λ2+λ1d(x,z)
2ρ+ρ+λ1(2ρ)
=(3+2λ1)ρ.

A.2 Proof of Proposition 5.6

Using regular cubulations at scale R, one can decompose chains in n into pieces of size R. More generally, in a metric space X we can decompose according to Lipschitz maps φ:Xn. For integral chains of compact support in X we are going to recursively define a weak surrogate of a simplicial decomposition subordinate to (the inverse image of) a given cubulation of n.

Let us choose an orientation on n. If 𝒞 is a cubulation of n, then each cube B𝒞 inherits an orientation of n. For a cube B𝒞, we define the face decomposition of B to be B=iϵiBi, where each Bi is a codimension 1 face of B and the sign ϵi=±1 is determined by our orientation.

Definition A.6.

Let 𝒞 be a regular cubulation of n at scale R and let φ:Xn be a Lipschitz map. For a constant C>0, a (C-controlled) rectifiable stratification (at scale R) of an m-cycle S𝐙m,c(X) is a collection of currents (SB)B𝒞 such that

  1. for every B𝒞(n-k) holds SB𝐈m-k,c(X) and SB is concentrated on φ-1(B) where B denotes the interior of B,

  2. for every B𝒞(n) holds SB=Sφ-1(B),

  3. for B𝒞, let B=i=1ϵiBi be the face decomposition of B, then i=1ϵiSBi is a piece decomposition of SB,

  4. B𝒞(n-k)𝐌(SB)C𝐌(S)Rk.

Note (1) and (2) imply that S=B𝒞(n)SB is a piece decomposition.

If S𝐙m,c(X) has a rectifiable stratification (SB)B𝒞, then the collection (SB)B𝒞(n-k) is called the codimension-k-skeleton, S(m-k).

Before we turn to the existence of rectifiable stratifications, we provide an auxiliary lemma.

Lemma A.7.

Let φ:XRk be a Lipschitz map and let σZk(X) be a cycle. Denote by pi:XR the composition of φ with the projection onto the i-th coordinate axis. Suppose that

  1. σ,pi,1 and σ,pi,-1 exist and are elements in 𝑰k-1(X) for all 1ik, in particular σ(pi-1{±1})=0,

  2. for any ij hold σ,pi,1+σ,pi,-1(pj-1{±1})=0.

Let B=[-1,1]kRk and Bi±=[-1,1]i-1×{±1}×[-1,1]k-i with their interior denoted by B and (Bi±). Then the face decomposition of B=i=1k(Bi+-Bi-) induces a piece decomposition

(σφ-1(B))=i=1k(σ,pi,1φ-1((Bi+))-σ,pi,-1φ-1((Bi-))).

Proof.

We will use the abbreviation σ,pi,s|-11=σ,pi,1-σ,pi,-1. We want to prove the following slightly more general statement:

(σiIpi-1{(-1,1)})=jI(σ,pj,s|-11iI{j}pi-1{(-1,1)}).

Let us introduce the characteristic functions χi:=χ|{-1<pi<1}. Then we can write

σiIpi-1{(-1,1)}=σiIχi.

We induct on the cardinality of I. The case |I|=1 is clear. Suppose I={i1,,im}. For 1jm, let Ij=I{ij}. By induction, σiI1χi is a normal current:

(σiIχi)=σiI1χi,pi1,s|-11+((σiI1χi))χi1
=σiI1χi,pi1,s|-11+jI1(σ,pj,s|-11iI1{j}χi)χi1
=σiI1χi,pi1,s|-11+jI1(σ,pj,s|-11iI{j}χi).

There are m terms in the above summation, denoted by S1,,Sm from left to right. Note that for j>1, Sj is concentrated on the set

Aj=(iIjpi-1{(-1,1)})pj-1{±1}.

We claim S1 is concentrated on A1. Recall σ({pi1=±1})=0, then

σiI1χi({pi1=±1})=0

by [83, Lemma 4.7]. By induction,

(σiI1χi)=jI1σ,pj,s|-11iI1{j}χi.

Thus by assumption (2), (σiI1χi)({pi1=±1})=0. Then

σiI1χi,pi1,1=σiI1χi,pi1,1+.

As σiI1χi is concentrated on iI1pi-1{(-1,1)}, it follows from Lemma 3.3 that σiI1χi,pi1,1 is concentrated on iI1pi-1{(-1,1)}{pi1=1}. Thus S1 is concentrated on A1 as claimed.

Note that Aj1Aj2= when j1j2, so the above sum is a piece decomposition.

Now we repeat the discussion with I1 replaced by I2 to obtain another piece decomposition. By comparing these, we conclude

σiI1χi,pi1,s|-11=σ,pi1,s|-11iI{i1}χi,

which finishes the induction. ∎

Proposition A.8.

Let φ:XRn be an L-Lipschitz map. Then there exists a constant C=C(L,n)>0 such that the following holds. For any SZm(X) and R>0 there exists a regular cubulation C of Rn at scale R such that S has a C-controlled rectifiable stratification subordinate to C.

Proof.

The action of Rn on n induces a 1-Lipschitz covering map h:nT, where T is a product of n-circles of length R. For a subset I={i1,i2,,ik}{1,2,,n}, let In and TIT be the associated subspaces. Denote by pI:XI the composition of φ with the projection nI. Let πI=hpI.

First we claim there exist a point (s1,s2,,sn)T and a constant C=C(L,n) such that for any collection of mutually disjoint subsets I1,I2,,Ik of {1,,n}, we have

  1. σ:=S,πI1,sI1,πI2,sI2,πIk,sIk𝐈m-|I|(X),

  2. permuting the order of I1,,Ik in the definition of σ will result in the same current,

  3. σ=S,πI,sI, where I=i=1kIi,

  4. 𝐌(σ)C𝐌(S)R|I|.

Here |I| denotes the cardinality of I. To see the claim, note that by repeatedly applying [83, Theorem 6.5] and Fubini, we can find a full measure subset A0T such that (i), (ii) and (iii) hold. To arrange (iv), by the coarea formula, for each subset I of {1,,n}, we can find a subset AIA0 such that n(AI)(1-ϵ)n(A0) and 𝐌(σ)Cϵ𝐌(S)R|I| whenever (s1,,sn)AI. By choosing ϵ sufficiently small (depending on n), the intersection of all AI with I ranging over subsets of {1,,n} is non-empty and the claim follows.

Let 𝒞 be the cubulation (of scale R) with vertex set h-1((s1,,sn)). Let B𝒞(n-k) be a cube and let I:=IB be the smallest subset of {1,,n} such that h(B)TI, in particular |I|=n-k. We define SB=S,πI,sIφ-1(B) and SB=S,πI,sIφ-1(B). We claim that the collection (SB)B𝒞 satisfies Definition A.6.

Definition A.6 (2) holds by definition and (4) follows from item (iv). We claim SB=SB. If B is top-dimensional, then this claim follows from S(πi-1(si))=0 for any i{1,,n}. As we slice at regular point when defining iterated slices, a similar argument implies the lower-dimensional case of the claim, which implies the second half of Definition A.6 (1). Now Definition A.6 (3) follows from Lemma A.7 and properties (i)–(iii). Note that (iv) implies SB has finite mass for each B, hence SB has finite mass by (3). The first half of Definition A.6 (1) follows from (3), (i), (ii) and (iii). ∎

Now we are ready to prove Proposition 5.6.

Proof of Proposition 5.6.

We are going to use the Federer–Fleming deformation, henceforth referred to as (FFD), with respect to the cubulation 𝒞R0. By Proposition A.8, there exists a second regular cubulation 𝒞 of n at the larger scale R such that S has a rectifiable stratification (SB)B𝒞 subordinate to 𝒞.

We will write ab if aCb for a constant C depending only on L,A,m,n and c.

We only prove the case mn and the m>n case is similar.

First we claim that there exists a constant C0=C0(L,A,n) and a family of currents (PB)B𝒞 such that

  1. for every B𝒞(n-k) holds PB𝐈m-k,c(n) and spt(PB)NC0(φ(spt(SB))),

  2. each PB is a cubical chain with respect to 𝒞R0,

  3. for B𝒞, let B=iϵiBi be the face decomposition of B, then PB=iϵiPBi,

  4. B𝒞(n-k)𝐌(PB)C0𝐌(S)Rk,

  5. Fill(φ#S-B𝒞(n)PB)C0𝐌(S).

We define (PB)B𝒞 inductively as follows. Let τB=φ#SB. Take SB with B𝒞(n-m). Then SB is a 0-dimensional cycle. Applying (FFD) to τB with respect to the cubulation 𝒞R0, we obtain a cubical chain PB and a homotopy hB with hB=PB-τB. Note that

𝐌(PB)𝐌(SB)and𝐌(hB)R0𝐌(SB).

Clearly

B𝒞(n-m)𝐌(PB)𝐌(S)RmandB𝒞(n-m)𝐌(hB)R0𝐌(S)Rm𝐌(S)Rm-1.

Suppose PB and hB with B𝒞(n-m+k-1) are already defined such that conditions (a)–(d) hold, hB=PB-τB and

B𝒞(n-m+k-1)𝐌(hB)𝐌(S)Rm-k.

Take B with B𝒞n-m+k. Let B=iϵiBi be the face decomposition. Define

PB=τB+iϵihBi.

Then PB=iϵiPBi. Applying FFD to PB with respect to 𝒞R0, we obtain a cubical chain PB and a homotopy hB with hB=PB-τB (note that PB is fixed when applying the radial push-out procedure of FFD to PB). Then

B𝒞(n-m+k)𝐌(PB)B𝒞(n-m+k)𝐌(τB)+B𝒞(n-m+k-1)𝐌(hB)𝐌(S)Rm-k,
B𝒞(n-m+k)𝐌(hB)R0B𝒞(n-m+k)𝐌(PB)𝐌(S)Rm-k-1(as RR0),
B𝒞(n-m+k)𝐌(PB)B𝒞(n-m+k)𝐌(PB)𝐌(S)Rm-k.

Then the claim follows.

For each PB, define TB=ι(PB), where ι is defined with respect to 𝒞R0 (see Proposition 5.2). Define

P=B𝒞(n)PBandT=B𝒞(n)TB=ι(P).

Now we construct H𝐈m+1(X) such that H=S-T.

We start with B with B𝒞(n-m). By the estimates in Definition 5.1, SB-TB is a cycle of diameter R. We apply the strong cone inequality to obtain HB such that

diam(spt(HB))Rand𝐌(HB)R(𝐌(SB)+𝐌(TB)).

Thus

B𝒞(n-m)𝐌(HB)R𝐌(S)Rm𝐌(S)Rm-1.

Suppose HB with B𝒞(n-m+k-1) are already defined such that

  1. diam(spt(HB))R,

  2. B𝒞(n-m+k-1)𝐌(HB)𝐌(S)Rm-k,

  3. HB=SB-TB-iϵiHBi, where B=iBi is the face decomposition.

Take B with B𝒞(n-m+k). Consider

σB=SB-TB-iϵiHBi.

Let Bi=ijϵijBij be the face decomposition of Bi. Then

σB=iϵiSBi-iϵiTBi-iϵi(SBi-TBi-ijϵijBij)=0

by the sign convention. Applying the strong cone inequality to σB we obtain a filling HB. As diam(spt(HBi))R for each i, we have diam(spt(σB))R, hence diam(spt(HB))R. Moreover, 𝐌(HB)R(𝐌(SB)+𝐌(TB)+Bi𝐌(HBi). Thus by Proposition A.8 and the previous claim,

B𝒞(n-m+k)𝐌(HB)RB𝒞(n-m+k)σB
RB𝒞(n-m+k)(𝐌(SB)+𝐌(TB))+RB𝒞(n-m+k-1)𝐌(HB)
𝐌(S)Rm-k-1.

All items of the conclusions of the proposition now follow. ∎

B Neck property and coarse neck property

The purpose of this section is to provide a short cut from the neck property to coarse neck property under stronger assumptions on the ambient metric spaces, which leads to a weaker version of Theorem 9.5.

Lemma B.1.

Let (Xk,Qk,rk,pk,τk) be a sequence and D>0, ρ<1 constants such that:

  1. Xk is a complete metric space with an L-Lipschitz bicombing,

  2. QkXk is an n-dimensional (L,A)-quasiflat containing the base point pkQk,

  3. rk,

  4. for any asymptotic cone Xω arising from the rescaled sequence (1rkXk,pk), Qω has the neck property in Xω (cf. Definition 6.4) with uniform constant C,

  5. τk𝑰n(Xk), spt(τk)B(pk,rk)Nρrk(Qk) and 𝐌(τk)Drkn,

  6. σk:=τk satisfies spt(σk)N2ρrk(Qk) and 𝐌(σk)Drkn-1.

Then there exists a constant C depending only on C,L,L,A and n such that for all sufficiently large k,

Fill(σk)Cρrk𝐌(σk).

Proof.

Since Xk has a Lipschitz bicombing, we may assume that the quasiflat Qk is represented by a Lipschitz quasi-isometric embedding. Let Xk=1rkXk and Qk=1rkQk. We still use τk and σk to denote the rescaled currents. By Lemma 7.2, we can pass to a regularized sequence (τk) with τk𝐈n,c(Xk) such that τk comes with mass bounds and support control and such that τk is homologous to τk in a small tubular neighborhood of spt(τk). Moreover, we may assume that there is a compact metric space Z, a chain τ𝐈n,c(Z) and isometric embeddings ψk:spt(τk)Z such that ψk#τk converges to τ in the flat distance in (Z). We set σ=τ.

Let Xω be an ultralimit of Xk and QωXω be the ultralimit of the quasiflats Qk. We view spt(τ) with the induced metric from Z as a subset of Xω. Moreover, we may assume that the metric spaces Xk and Xω are isometrically embedded in Z by replacing Z by the metric space obtained from gluing Xω and the metric spaces Xk to Z along spt(τω) and the sets spt(τk) (see [22, Lemma I.5.24]). Also, we can assume that Z has a convex geodesic bicombing by replacing Z by (Z). By construction, inside XωZ we know τ is supported in XωNρ(Qω) and σω=τω is supported in N2ρ(Qω).

Let πk:ZQk be a Lipschitz quasi-retraction as in Corollary A.3. Then there exists L0 depending only on L and A, such that πk is L0-Lipschitz. We use FillU to denote the filling volume inside a space U. By assumption we have FillXω(σ)Cρ𝐌(σ). Since σk converges to σ with respect to flat distance in Z, we conclude FillZ(σk)2Cρ𝐌(σk) for all k large enough. Hence, for all such k it holds

FillQk(πk#σk)2L0nCρ𝐌(σk).

By Corollary A.5, there exists a constant C1=C1(L,L,A,n) such that

FillXk(σk-πk#σk)C1ρ𝐌(σk)

and the proof is complete. ∎

Corollary B.2.

Suppose X has an L-Lipschitz bicombing and QX is an (L,A) quasiflat. If for any asymptotic cone Xω of X (with base points in Q) Qω has the neck property in Xω, then Q has the coarse neck property in X.

Theorem B.3.

Let Q:RnX be an (L,A)-quasiflat in a proper metric space X with a Lipschitz bicombing. Then the following conditions are equivalent:

  1. Q is (μ,b)-rigid (cf. Definition 6.12).

  2. Q has super-Euclidean divergence (cf. Definition 6.20).

  3. Q has coarse neck property (cf. Definition 8.1).

  4. Q has coarse piece property (cf. Definition 9.1).

Proof.

The implication (2)  (3) follows from Proposition 7.4, Proposition 6.11 and Corollary B.2. The proof of (1)  (2), (3)  (4) and (4)  (1) is the same as the proof of Theorem 9.5. ∎

Here we lose the dependence of the constants in various definitions as in Theorem 9.5, as the arguments go through asymptotic cones.

C Simpler proof for the Morse lemma

In this section we provide simpler proofs of Proposition 10.4 and Proposition 10.3 under the stronger assumption of Lipschitz bicombing. Using Proposition 7.4 and Lemma 6.22, these results will be a consequence of Proposition C.1 and Proposition C.5 below, where we take 𝒳 to be the collection of all complete metric spaces with L-Lipschitz bicombing and 𝒬 to be the collection of all n-dimensional quasiflats in such metric spaces with δ-super-Euclidean divergence for some given σ.

Proposition C.1.

Let X be a collection of complete metric spaces with L-Lipschitz bicombing and let Q be a family of n-dimensional L-Lipschitz (L,A)-quasiflats in X. Take XX and let QX be an L-Lipschitz (L,A)-quasiflats (not necessarily of dimension n). Suppose that Q has asymptotically full support property with respect to the singular homology. Then there exist A0>0 and ϵ0>0 depending only on X,L,A,n and Q such that for each QQ, either dH(Q,Q)A0, or

(C.2)lim suprdH(Bp(r)Q,Bp(r)Q)rϵ0

for some (hence any) pQ.

Proof.

This follows from Lemma C.3 and Lemma C.4 below. ∎

Lemma C.3.

Let X be a metric space with a Lipschitz bicombing. Let F,FX be bilipschitz embeddings of closed convex subsets of Rm with dimF=n. Suppose F has full support in X. If F is contained in a tubular neighborhood of F and FF, then F is equal to F. In particular, their dimensions coincide.

Proof.

We only treat the case where F is non-trivial and not compact, the case of empty boundary or compact boundary is either similar or easier. After rescaling we may assume FN1(F). Then

n=dim(F)dim(F)=n.

Let π:XF be an L-Lipschitz retraction. Choose a point pFF. For large r>0, choose a relative singular cycle σrCn-1(F{p},F) such that its image avoid Bp(r) and σr represents a non-trivial class in H~n-1(F{p},F). Choose a chain βrCn-1(F) filling σr, then σr-βr represents a non-trivial class in H~n-1(F{p}). Let hr denote the singular n-chain induced by the Lipschitz bicombing such that hr=σr-σr, where σr:=π*σr. If τr is an n-chain in F filling σr-βr, then τr+hr fills σr-βr. Since F has full support, p has to lie in the image of τr+hr, and if r is large enough, even in the image of τr. Hence pF and therefore FF. But then F=F because F has full support. ∎

The next lemma is similar to [77, Divergence Lemma 4.1].

Lemma C.4.

Let X,Q,Q,Q,X be as in Proposition C.1. There exists a constant ρ>0 depending only on the constants L,A,n,X and Q with the following property. If pQ is such that d(p,Q)ρ, there exists a point qQBp(ρ2) with d(q,Q)d(p,Q)+1.

Proof.

Suppose for contradiction that there are two sequences (Qk)𝒬 and (Qk) of (L,A)-quasiflats in Xk𝒳 such that there are points pkQk with λk=d(pk,Qk) and such that

QkBpk(λk2)Nλk+1(Qk).

We pass to an asymptotic cone (Xω,pω)=ωlim(1λkXk,pk). Then d(pω,Qω)=1 and QωN1(Qω). As Qω has full support in Xω, by Lemma C.3, Qω=Qω. Contradiction. ∎

Proposition C.5.

Let X be a family of complete metric spaces with L-Lipschitz bicombing. Let D be a family of n-dimensional L-Lipschitz (L,A)-quasidisks in X such that D has asymptotic full support property with respect to the singular homology. Let D be some n-dimensional L-Lipschitz (L,A)-quasidisk. Then for every constant c there exists a constant C depending only on c,L,A,n,X and D such that for each DD, dH(D,D)<c implies dH(D,D)<C.

Proof.

Suppose for contradiction that there are sequences Dk𝒟 and Dk of n-dimensional L-Lipschitz (L,A)-quasidisks such that dH(Dk,Dk)<c but dH(Dk,Dk). Choose points xkDk at maximal distance from Dk and set λk=d(xk,Dk). Suppose that DkXk𝒳. Consider the ultralimit (Xω,xω)=ωlim(1λkXk,xk). The ultralimits Dω and Dω of the quasidisks are bilipschitz embeddings of closed convex subsets of n which fulfill DωN1(Dω). As Dω has full support, Lemma C.3 yields Dω=Dω. This contradicts d(xω,Dω)=1. ∎

D Examples of Morse quasiflats

D.1 Examples in weakly special cube complexes

We recall the following definition from [70], which is a weak version of special cube complexes introduced in [67].

Definition D.1.

A cube complex D is weakly special if

  1. D is non-positively curved,

  2. no hyperplane of Dself-osculates or self-intersects.

Note that the notions of self-osculation and self-intersection were introduced in [67, Definition 3.1]. The key property we need about weakly special cube complexes is the following, which was proved in [70, Section 5.2].

Lemma D.2.

Let D be a compact weakly special cube complex and let G=π1(D). Let D~ be the universal cover of D. Then there exist a finite index subgroup GG, and a labeling and orientation of edges in D~ such that

  1. the labeling and orientation of edges are invariant under the G-action,

  2. if two edges of D~ are parallel, then they have the same label, and their orientation is compatible with the parallelism,

  3. if two different edges of D~ intersect at a vertex, then they have different labels.

Pick a base vertex xD~. For every edge path ω in D~ starting at x, we define L(ω) to be the word ei1ϵi1ei2ϵi2ei3ϵi3, where eij is the label of the j-th edge in ω and ϵij=±1 records the orientation of the j-th edge. Moreover, Lemma D.2 implies that if two edge paths starting at x correspond to the same word, then they are equal.

Lemma D.3.

Let G,D and D~ be as in Lemma D.2. Suppose there is a convex subcomplex WD~ which splits as a product W=W1×W2. Pick an element gG such that there exist vertices w1W1 and w2W2 such that g maps vertex (w1,w2)W to another vertex in W of form (w1,w2). Then g maps W1×{w2} to W1×{w2}. Moreover, g restricted on W1×{w2} is exactly the parallelism map between W1×{w2} and W1×{w2}.

Proof.

Let w1W1 be a vertex and ωW1 an edge path from w1 to w1. By Lemma D.2 (2) and (3), ω×{w2} and ω×{w2} correspond to the same word. Now Lemma D.2 (1) implies that g(ω×{w2}) and ω×{w2} are two edge paths which start at the same point, and correspond to the same word. Thus g(ω×{w2})=ω×{w2} and the lemma follows. ∎

Theorem D.4.

Suppose G is virtually the fundamental group of a compact weakly special cube complex. Then each highest abelian subgroup of G is a Morse quasiflat.

Proof.

We assume without loss of generality that G is the fundamental group of a compact weakly special cube complex D. Also by Lemma D.2, we assume there is a G-invariant labeling and orientation of edges in D~ satisfying the conclusion of Lemma D.2. Let AG be a highest abelian subgroup (note that A is free), and let k be the rank of A. Let ED~ be an A-invariant k-flat such that A acts on E properly and cocompactly. By sliding E and possibly replacing A by a finite index subgroup, we can assume E is not contained in any hyperplane of D~. It suffices to show E is a Morse flat in D~. By Corollary 11.5, it suffices to show E does not bound a (k+1)-half-flat in D~. We argue by contradiction and assume E bounds a (k+1)-half-flat FD~. Note that F is also not contained in a hyperplane.

Let CF (resp. CE) be the combinatorial convex hull of F (resp. E). Let (F) (resp. (E)) be the collection of hyperplanes of D~ that intersect F (resp. E). Then there is a one-to-one correspondence between hyperplanes in CF (resp. CE) and hyperplanes in (F) (resp. (E)). As no hyperplane of D~ contains E or F, we have a decomposition (F)=12, where 1 is the set of hyperplanes that intersect F in a k-half-flat, and 2 is the set of hyperplanes that intersect F in a k-flat. Note that if h1, then hF is transverse to E; if h2, then hF is parallel to E. Thus 1=(E). The decomposition (F)=(E)2 induces a product decomposition CFCE×CE.

Since A is highest, by [111, Theorems 2.1 and 3.6], CE and E have finite Hausdorff distance. However, FCE×CE, thus CE cannot be bounded. Pick a base vertex w1CE, then there exist a pair of vertices w2w2 of CE such that (w1,w2) and (w1,w2) are mapped to the same vertex under the covering map D~D. Thus there is an element gG such that g(w1,w2)=(w1,w2).

We claim that g commutes with any element in A. It suffices to show for any aA, ag(w1,w2)=ga(w1,w2). Since a leaves CE invariant, it follows from Lemma D.3 that a(CF)=CF, the action of a respects the product decomposition CFCE×CE and a acts by identity on the CE factor. Since g(w1,w2)=(w1,w2), Lemma D.3 implies g|CE×{w2} is the parallelism map from CE×{w2} to CE×{w2}. Thus ag(w1,w2)=ga(w1,w2).

We claim the intersection of A with the subgroup g generated by g is the identity element. Let P=CE×W be the combinatorial parallel set of CE. Then we can identify CE as a convex subcomplex of W. Since g(CE×{w2})=CE×{w2}, we have g(P)=P. By Lemma D.3, g respects the product decomposition P=CE×W and acts as identity on the CE factor. If gnA, then gn(CE)=CE. However, gn must fix CE pointwise by previous discussion. Thus n=0 since G is torsion free.

The previous two claims imply that A is contained in an abelian group of higher rank generated by g and A, and this contradiction finishes the proof. ∎

D.2 An example arising from branched covering

A truncated hyperbolic space of dimension 3 provides an example of a CAT(0) space which contains Morse-geodesics and flats of dimension at least 2. Taking products we obtain examples of CAT(0) spaces which contain Morse-flats which are not top-dimensional.

We are going to twist this example a bit to produce a smooth irreducible example.

Let M¯ be a finite volume cusped hyperbolic manifold of dimension n3. Suppose that M¯ contains a separating closed hypersurface N¯ which is totally geodesic [98], [85]. We remove the cusps of M¯ and deform the metric conformally near the boundary, leaving the metric unchanged in a neighborhood of N¯, to obtain M¯, which is negatively curved in the interior and such that each component of its boundary is a totally geodesic flat torus. The double M of M¯ contains a finite family of totally geodesic flat hypersurfaces and a closed totally geodesic hyperbolic hypersurface N. Then there exist finite coverings

β:VM×M

of any degree, branched along N×N. The pull-back metric on V is locally CAT(0) [64, Section 4.4] and can be smoothed near β-1(N×N) to a metric of non-positive sectional curvature [56].

Denote by πV:V~V and πM:M~M the universal covers of V respectively M. We obtain an induced covering map between universal covers

β~:V~M~×M~

which branches along (πM×πM)-1(N×N).

Since M~ is a space with isolated (n-1)-flats, the product space M~×M~ has isolated (2n-2)-flats. Further, a pair of geodesic in M~ yields a 2-flat in M~×M~. By the criterion in Proposition 11.3, we see that if none of these geodesics lies in one of the isolated flats, then the associated 2-flat is Morse.

Now we turn to V~. Since the top-dimensional tori in M×M are disjoint from N×N, the corresponding top-dimensional flats in M~×M~ lift to flats in V~. In particular, V~ contains flats of dimension 4. Similarly, if we take two closed geodesics in M, both of them disjoint from N and the flat hypersurfaces, then their product yields an immersed flat torus in M×M. The inverse image of this torus under (πM×πM)β~ is a discrete family of 2-flats, and each of these has to be Morse by Corollary 11.5.

Acknowledgements

We thank J. Behrstock for bringing [9] to our attention and pointing out Theorem 1.21. We also thank J. Russell for some helpful discussions. We warmly thank the referee for a careful reading and many helpful comments to improve the exposition.

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Received: 2020-06-15
Revised: 2021-10-08
Published Online: 2022-01-06
Published in Print: 2022-03-01

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