This paper develops a theory for positive scalar curvature metrics on manifolds with certain singularities and applies it to construct such metrics on specific nonspin, atoral manifolds with odd order abelian fundamental groups, solving a longstanding conjecture.
Contribution
It introduces a new homology invariance principle for positive scalar curvature on singular manifolds and constructs metrics on a new class of nonspin, atoral manifolds with finite fundamental groups.
Findings
01
Constructed positive scalar curvature metrics on nonspin, atoral manifolds with odd order abelian fundamental groups
02
Proved the Gromov-Lawson-Rosenberg conjecture for this class of manifolds
03
Developed a homology invariance principle for manifolds with Baas-Sullivan singularities
Abstract
We introduce Riemannian metrics of positive scalar curvature on manifolds with Baas-Sullivan singularities, prove a corresponding homology invariance principle and discuss admissible products. Using this theory we construct positive scalar curvature metrics on closed smooth manifolds of dimension at least five which have odd order abelian fundamental groups, are nonspin and atoral. This solves the Gromov-Lawson-Rosenberg conjecture for a new class of manifolds with finite fundamental groups.
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Full text
Positive scalar curvature on manifolds with odd order abelian fundamental groups
Bernhard Hanke
Institut für Mathematik, Universität Augsburg, D-86135 Augsburg, Germany
We introduce Riemannian metrics of positive scalar curvature on manifolds with Baas-Sullivan singularities, prove a corresponding homology invariance principle and discuss admissible products.
Using this theory we construct positive scalar curvature metrics on closed smooth manifolds of dimension at least five which have odd order abelian fundamental groups, are nonspin and atoral.
This solves the Gromov-Lawson-Rosenberg conjecture for a new class of manifolds with finite fundamental groups.
Key words and phrases:
Manifolds with Baas-Sullivan singularities, positive scalar curvature, admissible products, group homology, Brown-Peterson homology
We will show the following existence result for positive scalar curvature metrics.
Theorem 1.1**.**
Let M be a closed connected smooth manifold of dimension at least 5 with odd order abelian fundamental group.
Assume that M is nonspin and p-atoral for all primes p dividing the order of π1(M).
Then M admits a Riemannian metric of positive scalar curvature.
For the notion of p-atorality see Definition 1.3.
For example, a closed connected oriented manifold M whose fundamental group is generated by fewer than dim(M) elements is p-atoral for all odd primes p, see Remark 1.4(v).
Theorem 1.1 contributes to the Gromov-Lawson-Rosenberg conjecture concerning the existence of positive scalar curvature metrics on closed smooth manifolds, see Rosenberg [Ros_Surv]*Conjecture 1.22.
It solves Problem 5.11 of Botvinnik and Rosenberg [BR1] for odd p.
For finite fundamental groups of odd order the Gromov-Lawson-Rosenberg conjecture can be formulated in the following concise way, see Rosenberg [Ros]*Conjecture 1.2.
Conjecture 1.2**.**
Let M be a closed connected smooth manifold with finite fundamental group of odd order.
If the universal cover of M admits a positive scalar curvature metric, then M admits a positive scalar curvature metric.
Connected manifolds with odd order fundamental groups are orientable, and they are spin if and only if their universal covers are spin.
Furthermore simply connected closed nonspin manifolds of dimension at least 5 admit positive scalar curvature metrics by Gromov and Lawson [GL]*Corollary C.
Hence, if Conjecture 1.2 holds, then each closed connected nonspin smooth manifold of dimension at least 5 with fundamental group of odd order admits a positive scalar curvature metric, thus strengthening Theorem 1.1.
Conjecture 1.2 holds in dimensions 1 and 2, and it holds in dimension 3 by the geometrization theorem.
In dimension 4 it is false – see Hanke, Kotschick and Wehrheim [HKW] – hence this case must be excluded.
In dimensions larger than or equal to 5 it holds for p-atoral manifolds whose fundamental groups are elementary abelian p-groups, where p is an odd prime.
This result is due to Botvinnik and Rosenberg [BR1, BR2] and the author [Ha15], who discovered and corrected a gap in the original argument in [BR1, BR2].
By Kwasik and Schultz [Kwasik]*Theorem 1.8, which can be generalized to the nonspin case, Conjecture 1.2 holds for manifolds of dimension larger than or equal to 5 whose fundamental groups have periodic cohomology.
Conjecture 1.2 is false without assuming that π1(M) is of odd order, see the remarks after [Ros]*Theorem 1.3.
Both this fact and the failure of the conjecture in dimension 4 illustrate that the metric obtained from π1(M)-averaging a positive scalar curvature metric on the universal cover of M is in general not of positive scalar curvature.
Conjecture 1.2 remains open in general in dimensions larger than 4.
Definition 1.3**.**
Let X be a topological space and let p be a prime.
A homology class h∈Hd(X;Z) is called p-toral, if there exist ℓ∈N, ℓ≥1, and classes c1,…,cd∈H1(X;Z/pℓ) such that
[TABLE]
Otherwise h is called p-atoral.
A closed oriented manifold M of dimension d is called p-atoral or p-toral, respectively, if the fundamental class [M]∈Hd(M;Z) has the corresponding property.
Remark 1.4**.**
(i)
The d-torus Td=(S1×⋯×S1)d for d≥1 is p-toral for all p, and so are all closed manifolds which are oriented bordant, over the classifying space B(Z/p)d, to the canonical map Td=BZd→B(Z/p)d.
2. (ii)
The p-atoral homology classes form a subgroup of Hd(X;Z).
3. (iii)
A closed connected oriented manifold Md is p-toral if and only if ϕ∗([M])∈Hd(Bπ1(M);Z) is p-toral, where ϕ:M→Bπ1(M) is the classifying map of the universal cover of M.
This uses the fact that ϕ∗:H1(Bπ1(M);Z/pℓ)→H1(M;Z/pℓ) is an isomorphism for all ℓ≥1.
4. (iv)
Let Md be closed connected oriented with finite abelian fundamental group π1(M).
Let ψ:M→M be a connected cover corresponding to a Sylow p-subgroup of π1(M).
Then M is p-toral, if and only if M is p-toral.
This follows from the relation
[TABLE]
and from the fact that ψ∗:H1(M;Z/pℓ)→H1(M;Z/pℓ) is an isomorphism for all ℓ≥1 by our assumption on π1(M).
5. (v)
Let Md be closed connected oriented and let p be an odd prime.
Furthermore assume that π1(M) is generated by fewer than d elements.
This implies that the abelianization of π1(M) is a product of fewer than d cyclic groups.
Then M is p-atoral since for ℓ≥1 the cohomology group H1(M;Z/pℓ) is generated by fewer than d elements and each element in H1(M;Z/pℓ) has square zero for odd p.
6. (vi)
In contrast the orientable real projective space RP2m−1 is 2-toral for all m≥1.
7. (vii)
One may speculate that p-toral manifolds for odd p do not admit positive scalar curvature metrics.
This would yield counterexamples to Conjecture 1.2.
In the spirit of other existence results for positive scalar curvature metrics on high dimensional manifolds the proof of Theorem 1.1 is based on the propagation of positive scalar curvature metrics along surgeries of codimension at least three; see Gromov and Lawson [GL] and Schoen and Yau [SY].
In the paper at hand this technique is combined with the realization of singular homology classes by manifolds with Baas-Sullivan singularities [baas1].
To this end we introduce and discuss the concept of positive scalar curvature metrics on manifolds with Baas-Sullivan singularities in Sections 3 and 4, which includes the discussion of admissible products.
In some particular cases positive scalar curvature metrics on simply connected manifolds with Baas-Sullivan singularities were studied by Botvinnik [Bot01].
The main steps of the proof of Theorem 1.1 are as follows.
Let Ω∗SO denote the oriented bordism ring and fix a family Q=(Q4i)i≥1 of closed oriented manifolds of dimension 4i whose bordism classes form a set of polynomial generators of Ω∗SO/torsion, and each of which is equipped with a metric of positive scalar curvature.
Such families exist by the results in [GL].
By [baas1], after inverting 2 oriented bordism with singularities in Q is naturally isomorphic to singular homology; see Section 2.
Given a topological space X we will define a subgroup H∗Q,+(X;Z)⊂H∗(X;Z), called the positive homology of X with respect to Q, see Definition 3.12.
Elements in this group are represented by maps from Baas–Sullivan manifolds admitting positive scalar curvature metrics to X.
In particular positive homology classes need not be representable by smooth manifolds.
An important ingredient for the proof of Theorem 1.1 is the following homology invariance principle, which we show at the end of Section 3.
Theorem 1.5**.**
Let M be a closed connected oriented smooth manifold of dimension d≥5 with odd order fundamental group and which is nonspin.
Let ϕ:M→Bπ1(M) be the classifying map.
Then M admits a metric of positive scalar curvature if and only if ϕ∗([M])∈HdQ,+(Bπ1(M);Z).
It hence remains to show that under the conditions of Theorem 1.1 we have ϕ∗([M])∈HdQ,+(Bπ1(M);Z) for some orientation [M] of M.
For this goal we first study the positive homology H∗Q,+(BΓ;Z) for finite abelian p-groups Γ.
In this case the homology of BΓ can inductively be computed by an exact Künneth sequence (with α≥1)
[TABLE]
The cross product can be realized by admissible products of manifolds with Baas-Sullivan singularities, and the same is true for the torsion product, which is related to a homological Toda bracket.
The construction of admissible products and Toda brackets for Baas-Sullivan manifolds with positive scalar curvature is non-trivial and will be developed in Sections 4 and 5 of our paper.
By a variant of the well known “shrinking one factor” argument (see Proposition 4.7) the cross product of two homology classes is positive, if one of the factors is positive.
However we can in general show positivity of Toda brackets only if both of the factors are positive; compare Corollary 5.5.
This does not cover Toda brackets involving homology classes of degree one (represented by circles), even though these Toda brackets are p-atoral.
Although we can show the positivity of many Toda brackets involving degree one classes by a systematic use of group homomorphisms in Proposition 6.7, there are some Toda brackets whose positivity remains obscure; see Question 6.10.
In order to bypass this issue we use the fact that the homology class ϕ∗([M])∈Hd(Bπ1(M);Z) is of a restricted type, since M is assumed to be a smooth manifold.
This fact is explored in the following result.
Theorem 1.6**.**
Let p be an odd prime and let Γ be a finite abelian p-group.
Then all p-atoral classes in the image of Ω∗SO(BΓ)→H∗(BΓ;Z) are positive.
The proof of Theorem 1.6 will be provided in Section 8.
As a preparation we investigate the (ordinary) homology of abelian p-groups Γ in Section 6.
For Γ=(Z/pα)n and p-atoral homology classes not divisible by p the proof of Theorem 1.6 is especially difficult and relies on the fact that these homology classes can be represented by generalized products of Z/pα-lens spaces modulo elements divisible by p.
We refer to Section 7 for further details.
Now let M be a manifold as in Theorem 1.1.
Let p be an (odd) prime dividing the order of π1(M), let M→M be the connected cover corresponding to the inclusion of a Sylow p-subgroup Γ⊂π1(M) and let ϕ:M→BΓ be the classifying map.
By Remark 1.4(iv) the manifold M is p-atoral, and by construction ϕ∗([M])∈Hd(BΓ) lies in the image of ΩdSO(BΓ)→Hd(BΓ).
Using Theorem 1.6 the class ϕ∗([M])∈Hd(BΓ) is positive.
Hence also the class
[TABLE]
is positive, where [π1(M):Γ] denotes the index of Γ in π1(M) and ψ:BΓ→Bπ1(M) is induced by the subgroup inclusion Γ⊂π1(M).
By the Chinese remainder theorem we find αp∈Z, where p runs through the primes dividing the order of π1(M), such that 1=∑pαp⋅[π1(M):Γp] where Γp⊂π1(M) denotes some Sylow p-subgroup.
Hence
We conjecture that Theorem 1.1 also holds for spin manifolds with vanishing α-invariants.
A proof should be based on real connective K-homology instead of ordinary homology; compare Rosenberg and Stolz [RS].
However our homological computations do not carry over to this case in an obvious way.
Hence we leave the spin analogue of Theorem 1.1 for later investigation.
Acknowledgments. This project was initiated when I was visiting the University of Notre Dame some years ago.
To Stephan Stolz I owe the idea to study positive scalar curvature metrics on manifolds with Baas-Sullivan singularities for proving Theorem 1.1.
Substantial parts of this research were carried out at the MPI Bonn and the Courant Institute of Mathematical Sciences (NYU).
The hospitality of the named institutions is gratefully acknowledged.
I appreciate a number of helpful suggestions by an anonymous referee, which led to a significant improvement of the manuscript.
Many thanks also go to John Bourke from the MSP production team.
This research has been supported by the Special Priority Programme SPP 2026 Geometry at Infinity funded by the DFG.
2. Review of manifolds with Baas-Sullivan singularities
We recall some terminology, following mainly [Bunke]*Section 3.3, and fix some notation.
Smooth d-dimensional manifolds with cornersV are modeled on subsets N(k,U)=U×[0,1)k⊂Rd for 0≤k≤d, where U⊂Rd−k is open, with smooth transition maps of the form (x,t1,…,tk)↦(x′,tσ(1),…,tσ(k)) for some permutation σ.
For a precise definition we refer to [Bunke]*Definition 3.14. and the subsequent discussion.
In particular, manifolds with corners are equipped with preferred local collar structures.
111Some authors use different conventions, compare, for instance, [Joyce]*Definition 2.2 .
The subset U×{0}⊂N(k,U) defines the points of codimension k in N(k,U).
Let V be a d-dimensional manifold with corners.
Every point x∈Vd has a codimension0≤c(x)≤d, defined with respect to any local chart around x.
This induces a decomposition of V into smooth (in general non-compact) connected submanifolds of V, called strata, of various codimensions.
Each stratum admits a canonical completion (by adding boundary points to local models), which is itself a manifold with corners, see [Bunke]*Definition 3.17.
The union of strata of codimension at least 1 in V is denoted by ∂V.
As usual we require by definition that each x∈V lies in the closure of exactly c(x) codimension-1 strata of V.
In this case the completions of strata coincide with their respective closures in V (note that this is not true for the 1-gon, for example), which are called connected faces of V.
Manifolds with Baas-Sullivan singularities were introduced in [baas1].
Let us recall some features of the theory which are relevant for our discussion.
A decomposed manifold is a manifold V with corners together with a decomposition
[TABLE]
for some n∈N, where each ∂iV is a disjoint union of connected codimension-1 faces of V which is globally collared in V and each connected codimension-1 face of V is contained in exactly one ∂iV, see [baas1]*Definition 2.1.
Each ∂iV has an induced structure of a decomposed manifold by setting ∂j(∂iV)=∂iV∩∂jV for j=i, and ∂j(∂jV)=∅ for 0≤j≤n, compare [baas1]*page 283.
Definition 2.1**.**
We call the decomposed manifold ∂0V the boundary of V.
If V is compact and ∂0V=∅, then V is called closed.
Similar to [baas1]Definition 2.2 we fix a family of closed smooth manifolds P=(P0=∗,P1,P2,…), called singularity types.
For n∈N we set Pn=(P0,…,Pn).
By definition, a Pn-manifold* is a family of decomposed manifolds
[TABLE]
where ∂A(ω)=∂0A(ω)∪⋯∪∂nA(ω), with ∂iA(ω)=∅ for i∈ω, together with isomorphisms ∂iA(ω)≅A(ω,i)×Pi of decomposed manifolds for i∈{0,…,n}∖ω.
222Some authors use the “Bockstein” notation βωA instead of A(ω).
Here we set ∂j(A(ω,i)×Pi):=∂jA(ω,i)×Pi for 0≤j≤n and we write A(ω,i) instead of A(ω∪{i}).
We also use the shorthand A for the decomposed manifold A(∅).
By definition the following compatibility condition is required to hold.
Condition 2.2**.**
For all i,j∈/ω with i=j the isomorphisms
[TABLE]
coincide after composing one of them with the interchange map Pj×Pi→Pi×Pj.
Note that each Pn-manifold A can be regarded as a Pn+1-manifold in a canonical way by setting ∂n+1A:=∅.
For a Pn-manifold A we define the union of singular strata of A as
[TABLE]
so that, obviously, ∂A=∂0A∪Sing(A) and Sing(∂0A)=∂0A∩Sing(A).
There is a bordism theory Ω∗Pn(−), which we call bordism with singularities in Pn – compare [baas1]*page 284 ff., where this theory is denoted by M(Pn)∗(−).
Given a pair of topological spaces (X,Y⊂X) elements in ΩdPn(X,Y) are by definition represented by continuous maps f:Ad→X, where (see [baas1]*Definitions 2.2. and 2.3.)
(i)
A is a compact d-dimensional Pn-manifold;
2. (ii)
on local models U×[0,1)k the map f factors through the projections
[TABLE]
3. (iii)
for all i∈{1,…,n} the restriction f∣∂iA factors as
[TABLE]
4. (iv)
f(∂0A)⊂Y.
Definition 2.3**.**
A continuous map f:Ad→X with properties (ii) and (iii) is called compatible with the singularity structure of Ad.
Definition 2.4**.**
The homology theory obtained in the limit n→∞ is called bordism with singularities in P and denoted by Ω∗P(−).
There is a straightforward generalization to bordism with tangential structures.
In this paper we will be working with oriented bordism with singularitiesΩ∗SO,Pn(−) with n≥0 or Ω∗SO,P(−), where we assume that
•
all singularity types Pi are even dimensional;
•
all Pi and A(ω) are oriented;
•
for i∈/ω and with respect to the induced orientation on ∂iA(ω) (determined by the outward normal) the given isomorphism ∂iA(ω)≅A(ω,i)×Pi is orientation preserving, if an even number of elements in ω are larger than i, and orientation reversing otherwise.
In a similar way one may define spin bordism with singularitiesΩ∗Spin,P(−), but this theory will not be considered in this paper.
Construction 2.5**.**
For n≥0 we shall define natural transformations of homology theories
[TABLE]
Let (X,Y) be a pair of topological spaces and let f:Ad→X represent an element in ΩdSO,Pn(X,Y) with a connected oriented compact Pn-manifold A.
Let A′ be obtained from A by passing to the quotient space resulting from the identifications (x,p)∼(x,p′) on ∂iA=A(i)×Pi for i=1,…,n, x∈A(i) and p,p′∈Pi.
Intuitively this process may be regarded as “coning off” the singularity types P1,…,Pn in A and thereby introducing genuine singularities.
It is shown by a straightforward computation that Hd(A′,(∂0A)′;Z)≅Z (recall dimPi≥2 for i≥1), with a preferred generator [A′,(∂0A)′] corresponding to the given orientation of A.
By assumption f factors through a map f′:(A′,(∂0A)′)→(X,Y), and we define
[TABLE]
Passing to the limit n→∞ we also obtain a natural transformation
[TABLE]
By [Nov60] the oriented bordism ring Ω∗SO modulo torsion is a polynomial ring.
There are closed oriented manifolds Q1,Q2,… with dimQi=4i such that
[TABLE]
where [Qi]∈Ω4iSO denotes the bordism class represented by Qi.
Since Ω∗SO contains no odd torsion [milnorcomplex] the sequence ([Qi])i≥1 is a regular sequence in Ω∗SO⊗Z[1/2].
Setting Q:=(Q0=∗,Q1,Q2,…) we arrive at the following fundamental result from [baas1].
Proposition 2.6**.**
For all (X,Y) the natural transformation u defined in (1) induces an isomorphism
[TABLE]
Corollary 2.7**.**
Let Γ be a finite group of odd order.
Then the map
[TABLE]
is surjective.
Proof.
This holds in degree [math], when source and target of u are equal to Z.
Let d≥1.
Since Γ is of odd order the homology group Hd(BΓ;Z) is abelian of odd order.
Hence for any m0≥0 and any x∈Hd(BΓ;Z) there exists m≥m0 with 2m⋅x=x.
The claim is hence implied by Proposition 2.6 by clearing denominators.
∎
In other words: Each homology class in H∗(BΓ;Z) is represented by a Qn-manifold for some n (which has to be larger than [math] in general, compare Example 7.6).
Next we will introduce and study the notion of positive scalar curvature metrics on these objects.
3. Positive scalar curvature on manifolds with Baas-Sullivan singularities
Definition 3.1**.**
An admissible Riemannian metric on a manifold with corners Vd is a smooth Riemannian metric g on V which on each local model U×[0,1)k restricts to a product metric gU⊕η.
Here and in the following η denotes the standard Euclidean metric and gU is some Riemannian metric on U⊂Rd−k.
Definition 3.2**.**
A family of Riemannian singularity types is a family of singularity types P=(P0=∗,P1,P2,…) together with Riemannian metrics hi on Pi for i≥1.
We call a family of Riemannian singularity types positive if each metric hi for i≥1 is of positive scalar curvature.
Definition 3.3**.**
Let P be a family of Riemannian singularity types and let A be a Pn-manifold, possibly with boundary.
An admissible metric g on A=A(∅) is called P-compatible if for each ω⊂{1,…,n} there is an admissible metric g(ω) on A(ω) such that g=g(∅) and the metric g(ω) restricts to the product metric g(ω,i)⊕hi on ∂iA(ω)≅A(ω,i)×Pi for i∈{1,…,n}∖ω.
Lemma 3.4**.**
Each Pn-manifold admits a P-compatible metric.
Proof.
Use downward induction on the cardinality of ω⊂{1,…,n}, starting with ∣ω∣=n.
∎
Construction 3.5** (Scaling P-compatible metrics).**
Let P be a family of Riemannian singularity types and let A be a Pn-manifold together with a P-compatible metric g.
For λ>0 the scaled metric λ⋅g is not P-compatible unless λ=1.
The following construction will resolve this issue.
We fix, once and for all, a smooth cut-off function ϕ:[0,1]→[0,1] equal to [math] on [0,1/3] and equal to 1 near 1.
Let λ>0 and δ≥3 real numbers.
For ω⊂{1,…,n}, say ω=(i1,…,ik) with 1≤i1<⋯<ik≤n, we obtain a k-parameter family (gt)t=(ti1,…,tik)∈[0,δ]k of Riemannian metrics on ∂i1⋯∂ikA≅A(ω)×Pi1×⋯×Pik where
[TABLE]
We abbreviate Pω:=Pi1×⋯×Pik.
With the Euclidean metric η on [0,δ]k we obtain a smooth Riemannian metric gω,λ,δ on A(ω)×Pω×[0,δ]k defined by
[TABLE]
Choose some monotonically increasing diffeomorphism χ:[0,1]→[0,δ] which has derivative λ near 1 and denote the induced diffeomorphisms [0,1]k→[0,δ]k by χ as well.
For ω⊂{1,…,n}, if ∣ω∣=k, then we replace the metric λ⋅(g(ω)⊕⨁i∈ωhi⊕η) on the local model A(ω)×Pω×[0,1)k⊂A by the metric gω,λ,δ pulled back along the diffeomorphism id×id×χ:A(ω)×Pω×[0,1)k→A(ω)×Pω×[0,δ)k.
Continuing with increasing k=0,…,n this construction results in a smooth metric on A.
Furthermore, by the choice of ϕ and since δ≥3, there are induced local corner models on A with respect to which this metric is P-compatible.
This new metric on A is denoted by g(λ,δ) and is called the (λ,δ)-scaling of g.
The diffeomorphism χ and hence the metric g(λ,δ) can be assumed to depend smoothly on λ and δ.
Note that g(λ,δ)(ω)=g(ω)(λ,δ) for ω⊂{1,…,n}.
For n=2 and δ=3 the situation is illustrated in Figure 1, where the shaded region indicates the collar near Sing(A) for the scaled metric g(λ,δ).
Definition 3.6**.**
Let P be a family of Riemannian singularity types, let A be a Pn-manifold and let g be a P-compatible metric on A.
We say that g is singularity-positive, if for all 1≤i≤n the product metric g(i)⊕hi on ∂iA=A(i)×Pi is of positive scalar curvature.
Proposition 3.7**.**
Let P be positive, let A be a compact Pn-manifold, and let g be a P-compatible metric on A.
Then there exists λ≥1 and δ0≥3 such that for all δ≥δ0 the metric g(λ,δ) is singularity positive.
Proof.
Since the metrics h1,…,hn are of positive scalar curvature and A is compact we find some λ≫1 such that the metric λ⋅g(i)⊕hi on ∂iA=A(i)×Pi is of positive scalar curvature for all 1≤i≤n.
By the additivity of scalar curvature in Riemannian products and since λ≥1 the metric gt in (2) is of positive scalar curvature whenever tij≤δ/3 for some 1≤j≤k.
For ω⊂{1,…,n} with ∣ω∣=k, we obtain Riemannian submersions
[TABLE]
whose fibers are equipped with the metrics gt.
By the O’Neill formula for the scalar curvature in Riemannian submersions [Besse]*(9.37), we find δ0≥3 such that for all δ≥δ0 the metric gω,λ,δ is of positive scalar curvature on the subset
We need the following variation of Definition 3.6.
Definition 3.8**.**
Let P be a family of Riemannian singularity types, let A be a Pn-manifold and let g be a P-compatible metric on A.
We say that g is positive, if for all ω⊂{1,…,n} (including ω=∅) the metric g(ω) on A(ω) is of positive scalar curvature.
This condition, which is stronger than just requiring the metric g on A to be of positive scalar curvature, will become important in the proof of the next proposition.
Note that positive metrics are singularity positive in the sense of Definition 3.6.
Proposition 3.9**.**
Let P be a family of singularity types and A be a compact Pn-manifold together with a P-compatible positive metric g.
Let Λ⊂(0,∞) be a compact subset and let s>0.
(i)
Let P be positive.
Then there exists δ0≥3 such that for all λ∈Λ and δ≥δ0 the scaled metric g(λ,δ) is positive.
2. (ii)
There exists 0<λ0≤1 such that for all 0<λ≤λ0 there exists δ0≥3 such that for all δ≥δ0 and ω⊂{1,…,n} we have scalg(λ,δ)(ω)>s.
Proof.
For ω⊂{1,…,n} the metric g(ω) is of positive scalar curvature by assumption and hence (2) implies, assuming positivity of P in case (a):
(a)
For all λ∈Λ and t∈[0,δ]k we have scalgt>0.
2. (b)
There exists 0<λ0≤1 such that for all 0<λ≤λ0 and t∈[0,δ]k we have scalgt>s.
Using the O’Neill formula and the compactness of Λ this implies, on A=A(∅):
(a)
There exists δ0≥3 such that for λ∈Λ and δ≥δ0 we have scalg(λ,δ)(∅)>0.
2. (b)
There exists 0<λ0≤1 such that for all 0<λ≤λ0 there exists δ0≥3 such that for all δ≥δ0 we have scalg(λ,δ)(∅)>s.
Now, for any θ⊂{1,…,n}, a similar argument applies to A(θ) instead of A=A(∅) so that we can pass to the maximum of the resulting constants δ0 in (a), and to the minimum of the resulting constants λ0 and the maximum of the resulting constants δ0 in (b), in order to prove the required lower estimates of scalar curvatures on all A(θ).
∎
Corollary 3.10**.**
Let P be positive, let A be a compact Pn-manifold, and let g be a P-compatible metric on A.
Furthermore, let C⊂∂0A be a union of components of ∂0A and assume that the restriction of g to C is positive (in the sense of Definition 3.8).
Then there exists λ≥1 and δ0≥3 such that for all δ≥δ0 the scaled metric g(λ,δ) is singularity positive and still restricts to a positive metric on C.
Proof.
Let λ and δ0 be chosen as in Proposition 3.7.
The claim follows from Proposition 3.9(i) applied to A:=C and Λ:={λ}, possibly after passing to some larger δ0.
∎
We can now show the following bordism principle.
Proposition 3.11**.**
Let P be a positive family of singularity types and let V be a compact Pn-manifold with dimV≥6.
Assume that the boundary ∂0V decomposes as a disjoint union ∂0V=A⊔M, where A is a closed Pn-manifold equipped with a P-compatible positive metric, and M is a closed smooth manifold.
Furthermore assume that the inclusion M↪V is a 2-equivalence.
Then M carries a Riemannian metric of positive scalar curvature.
Proof.
By Corollary 3.10 we find a P-compatible singularity-positive metric g on V which restricts to a positive metric on A⊂∂0V.
For 1≤ℓ≤k≤n+1 we consider the face
[TABLE]
Each ∂ℓ[0,1]k can be identified with [0,1]k−1 in a canonical way and ∂ℓ[0,1]k is equipped with a collar of width 0.1 equal to
[TABLE]
For 1≤k≤n+1 we fix smooth hypersurfaces Hk−1⊂[0,1]k homeomorphic to compact (k−1)-balls subject to the following conditions:
•
H0={1/2}⊂[0,1].
•
Hk−1 is invariant under permutations
[TABLE]
•
For 2≤k≤n+1 the hypersurface Hk−1 is of product form in the collar neighborhood of width 0.1 of each codimension 1 face ∂ℓ[0,1]k⊂[0,1]k for 1≤ℓ≤k, and meets this face in Hk−2;
•
the metric γk−1 on Hk−1 induced from the Euclidean metric η on [0,1]k is of nonnegative scalar curvature.
One explicit construction of Hk−1 is by attaching a C1-collar of width 1/5 to the shifted spherical segment (4/5,…,4/5)−{t∈[0,1]k∣∥t∥=3/10}⊂[0,1]k and smoothing.
Replacing U×[0,1)k by U×Hk−1 in local models of V for increasing 1≤k≤n+1 we obtain a smooth hypersurface ∂W⊂V contained in the collar neighborhood of ∂V, where we recall that ∂V is the set of points of codimension at least 1 in V.
(We write Hk−1 for Hk−1∩[0,1)k.)
The hypersurface ∂W is the boundary of a smooth embedded codimension zero submanifold W of V, which we may think of V with “smoothened corners”.
We obtain a decomposition ∂W=C0⊔C1 where C0 and C1 are disjoint smooth submanifolds of ∂W with C1=M.
Furthermore C1↪W is a 2-equivalence.
We claim that the smooth manifold C0 carries a Riemannian metric of positive scalar curvature, such that Theorem 3.11 follows from the usual bordism principle for positive scalar curvature metrics, see [Stolz]*Extension Theorem 3.3.
By assumption the induced metrics on the local models V(ω)×∏i∈ωPi×[0,1)k of V for ω⊂{0,…,n}, ω∩{1,…,n}=∅ with ∣ω∣=k are of product form g(ω)⊕⨁i∈ωhi⊕η (here we set h0=0) and of positive scalar curvature, as g is singularity-positive.
Furthermore the metric g is of positive scalar curvature in the collar neighborhood A×P0×[0,1)=A×[0,1), as g restricts to a positive metric on A.
Since the metrics γk−1 on Hk−1 have nonnegative scalar curvature this implies that the restricted metrics g(ω)⊕⨁i∈ωhi⊕γk−1 are of positive scalar curvature on V(ω)×∏i∈ωPi×Hk−1 for these ω as well as on A×H0=A×{1/2}.
Altogether we obtain a positive scalar curvature metric on C0 as required.
∎
Let Q:=(Q0=∗,Q1,Q2,…) be a family of singularity types as in Proposition 2.6.
For i≥1 we can assume that Qi is equipped with a positive scalar curvature metric hi – compare [GL] – such that Q is a positive family of singularity types in the sense of Definition 3.2.
Definition 3.12**.**
Let X be a topological space.
A homology class h∈Hd(X;Z) is called positive with respect to Q, if there is a bordism class [f:Ad→X]∈ΩdSO,Q(X) with the following properties:
•
A admits a Q-compatible positive metric (see Definition 3.8).
•
u([f:Ad→X])=h, where u:ΩdSO,Q(X)→Hd(X;Z) is as defined in Construction 2.5.
The subgroup of all positive homology classes with respect to Q is denoted by HdQ,+(X;Z).
Note that a priori the subgroup of positive homology classes depends on the choice of the metrics hi, and that
positive homology is functorial in that a map X→Y of topological spaces induces a map H∗Q,+(X;Z)→H∗Q,+(Y;Z).
Proof of Theorem 1.5.
First assume that M is equipped with a positive scalar curvature metric g.
Regarding M as a Baas-Sullivan manifold with no singular strata, g is a positive metric on M in the sense of Definition 3.8.
Hence ϕ∗([M])∈HdQ,+(Bπ1(M);Z) as required.
For the other implication assume ϕ∗([M])∈HdQ,+(Bπ1(M);Z).
We write ϕ∗([M])=u([f:Ad→Bπ1(M)]) where A is equipped with a Q-compatible positive metric.
Using an inclusion ∗→Bπ1(M) the manifold M represents a class
[TABLE]
Then β:=[ϕ:M→Bπ1(M)]−[M]∈Ω~dSO(Bπ1(M)), the reduced oriented bordism group of Bπ1(M).
Since Ω~dSO(Bπ1(M)) is a finite abelian group of odd order by assumption on π1(M) and by the Atiyah-Hirzebruch spectral sequence, we find, for each m0≥0, an m≥m0 with 2m⋅β=β.
Each element in the kernel of the map
[TABLE]
in Corollary 2.7 is 2-power torsion by Proposition 2.6, and hence, using d>0, there is some m0≥0 with
[TABLE]
Hence there is an m≥m0 with
[TABLE]
Since d≥5 we can represent [M]∈ΩdSO by a closed oriented smooth d-manifold N with a positive scalar curvature metric by [GL]*Corollary C.
By (3) there exists a compact connected oriented Q-bordism V→Bπ1(M) between M⊔N→Bπ1(M) and ∐2m(f:A→Bπ1(M)).
Here N denotes N with the reversed orientation.
We can assume that the inclusion M↪V is a 2-equivalence by applying surgeries to the interior of V.
For this we observe that the induced homomorphism π1(V)→π1(Bπ1(M)) is surjective and has finitely generated kernel since π1(V) is finitely generated and π1(M) is finite by assumption.
This kernel can hence be killed by surgeries along finitely many embedded circles in the interior of V with trivial normal bundles, thus achieving π1(M)≅π1(V).
Since now π1(V) is finite and V is compact, π2(V) is finitely generated and so is the cokernel of π2(M)→π2(V).
Moreover each element in this cokernel can be represented by an embedded 2-sphere in the interior of V with trivial normal bundle, the universal cover of M being nonspin since M is nonspin and π1(M) is of odd order.
We can hence apply finitely many surgeries to the interior of V to make π2(M)→π2(V) surjective, thus achieving our goal.
Now the assertion of Theorem 1.5 follows from Proposition 3.11.
Remark 3.13**.**
The language developed in this section allows an alternative approach to the results in [F].
4. Admissible products
The cartesian product of two manifolds A and B with corners carries an induced structure of a manifold with corners.
However, the construction of the product of Pn-manifolds as a Pn-manifold is more involved.
In order to illustrate the issue let A and B be smooth manifolds with boundaries diffeomorphic to the closed manifold P1.
This induces the structure of P1-manifolds on A and B where A(1)=B(1)={∗}.
We obtain ∂(A×B)=(P1×B)∪(A×P1), but this does not induce the structure of a P1-manifold on A×B (even after straightening the π/2-angle at ∂A×∂B), since the P1-factors on the two pieces of ∂(A×B) correspond to different P1-factors in the intersection (P1×B)∩(A×P1)=P1×P1.
Therefore an additional construction is required, which, roughly speaking, interchanges these two factors at the glueing region.
This problem was discussed in [Bot92, Mironov, Morava, Shimada], resulting in an obstruction of order at most 2 if P1 is of even dimension.
In the following we present an explicit geometric construction, which somewhat differs from the mentioned sources and is well adapted to our purpose.
We will work in an oriented setting and in particular assume that all singularity types Pi for i≥1 are even dimensional.
In the following we fix n≥0.
Let A and B be Pn-manifolds with decompositions
[TABLE]
This includes the case that ∂iA=∅ or ∂iB=∅ for some i=0,…,n.
In particular, A or B are allowed to be smooth manifolds without singular strata.
In the remainder of the construction we fix a two dimensional compact hexagonal manifold X with corners, see the dark grey region in Figure 2.
For ω⊂{1,…,n} we will construct a manifold with corners A×ωB, which, intuitively speaking, is the cartesian product A×B with all codimension 2-singularities ∂iA×∂iB=(A(i)×B(i))×Pi×Pi for i∈ω resolved.
The construction runs by induction on the cardinality of ω.
For ω=∅ we set A×ωB:=A×B, the cartesian product of A and B with its induced structure of a manifold with corners.
In addition we smoothen the π/2-angle appearing at ∂0A×∂0B.
Assume that 1≤ℓ≤n and A×ωB has been constructed whenever ∣ω∣=ℓ−1.
Let ω⊂{1,…,n} with ∣ω∣=ℓ.
Choose some i∈ω and consider the collar neighborhood
[TABLE]
of the codimension-2 face ∂iA×ω∖{i}∂iB⊂A×ω∖{i}B.
The manifold A×ωB is obtained by removing this collar neighborhood from two disjoint copies of A×ω∖{i}B and gluing in the handle (∂iA×ω∖{i}∂iB)×X as indicated in Figure 2, where X is drawn in dark grey color.
The factor Pi×Pi appearing in
[TABLE]
is glued to the left hand copy of \big{(}A\times_{\omega\setminus\{i\}}B\big{)}\setminus\Big{(}\big{(}\partial_{i}A\times_{\omega\setminus\{i\}}\partial_{i}B\big{)}\times[0,1)^{2}\Big{)} by the identity map, and to the right hand copy by the interchange map (p1,p2)↦(p2,p1).
The interchange map Pi×Pi→Pi×Pi is orientation preserving, since Pi is even dimensional, and hence the manifold A×ωB carries an induced orientation.
Remark 4.1**.**
(i)
If ∂iA=∅ or ∂iB=∅, then A×ωB consists of two disjoint copies of A×ω∖{i}B.
2. (ii)
The manifold A×ωB does not depend on the choice of i∈ω, up to canonical diffeomorphism.
For i∈ω we set
[TABLE]
where the two copies on the right hand side correspond to the upper and lower thick boundary pieces in Figure 2.
Notice that
[TABLE]
and that the identification along this subspace interchanges the two factors in Pi×Pi, thus realizing our initial goal.
In particular we get an induced isomorphism
[TABLE]
where
[TABLE]
This concludes the induction step.
Definition 4.2**.**
The manifold A×~B:=A×{1,…,n}B is called the admissible product of A and B.
Proposition 4.3**.**
The admissible product A×~B carries an induced structure of a Pn-manifold.
Proof.
By construction A×~B carries the structure of a manifold with corners (with respect to appropriate local models) and is a decomposed manifold with decomposition ∂(A×~B)=∂0(A×~B)∪⋯∪∂n(A×~B), where we set
[TABLE]
(Recall the smoothening of the π/2-angle at ∂0A×∂0B at the initial stage of the inductive construction).
It remains to define the decomposed manifolds (A×~B)(ω) for ω⊂{1,…,n} in such a way that the compatibility Condition 2.2 for decomposed manifolds holds.
First we study the case when ω has two elements.
Similar computations apply to \big{(}A(i)\times_{[n]\setminus\{i\}}B(i)\big{)}(j) and \big{(}A(j)\times_{[n]\setminus\{j\}}B(j)\big{)}(i).
Defining (A×~B)(i,j) as
[TABLE]
where we glue
•
A×[n]∖{i,j}B(i,j) and A(i)×[n]∖{i,j}B(j) along (A(i)×[n]∖{i,j}B(i,j))×Pi,
•
A×[n]∖{i,j}B(i,j) and A(j)×[n]∖{i,j}B(i) along (A(j)×[n]∖{i,j}B(i,j))×Pj,
•
A(i,j)×[n]∖{i,j}B and A(j)×[n]∖{i,j}B(i) along (A(i,j)×[n]∖{i,j}B(i))×Pi,
•
A(i,j)×[n]∖{i,j}B and A(i)×[n]∖{i,j}B(j) along (A(i,j)×[n]∖{i,j}B(j))×Pj,
we hence obtain
[TABLE]
Arguing in a similar manner for arbitrary ω⊂{1,…,n} we can work with
[TABLE]
with gluings of components associated to ω′,ω′′⊂ω with ∣ω′△ω′′∣=1 (cardinality of symmetric difference) in order to identify A×~B as a Pn-manifold.
∎
Let X and Y be topological spaces, let Ad and Be be closed oriented Pn-manifolds of dimensions d and e and let α:A→X and β:B→Y be maps which are compatible with the singularity structures of A and B (see Definition 2.3).
Then the induced map α×β:A×B→X×Y is compatible with our inductive construction of A×~B and we obtain an induced map α×~β:A×~B→X×Y.
This results in a bilinear map of bordism theories
[TABLE]
(the theories Ω∗SO,Pn(−) were introduced after Definition 2.4) and this construction extends to relative bordism groups.
With the natural transformation u:Ω∗SO,Pn(−)→H∗(−) from Construction 2.5 we hence obtain the following result.
Proposition 4.4**.**
Let × denote the cross product in singular homology.
Then for all pairs of topological spaces (X,S) and (Y,T) we have a commutative diagram
[TABLE]
Remark 4.5**.**
The factor 2n appears even if A or B are without singular strata, see Remark 4.1(i).
In particular the product on Ω∗SO,Pn(−) is not unital for n≥1.
Now, choose Riemannian metrics hi on Pi∈P for i≥1.
Let A and B be Pn-manifolds and let g and h be P-compatible metrics on A and B in the sense of Definition 3.3.
Let λ,μ>0 and δ,ϵ≥9.
With this choice of δ and ϵ, the local models U×[0,1)k on A and B, equipped with the scaled metrics g(λ,δ) and h(μ,ϵ) from Construction 3.5, can be canonically extended to local models U×[0,3)k on which these scaled metrics still restrict to product metrics gU⊕η and hU⊕η, respectively, with the Euclidean metric η on [0,3)k.
We equip the hexagonal manifold X with some admissible Riemannian metric σ (see Definition 3.1) with respect to which each side has length 3.
With these data we construct a metric g(λ,δ)⊕~h(μ,ϵ) on A×~B along the inductive construction of A×~B before Definition 4.2, starting with the product metric g⊕h on A×B and working with collar factors [0,3)2 and [0,3) instead of [0,1)2 and [0,1) in Figure 2.
Here it is important that the interchange map on Pi×Pi is an isometry with respect to hi⊕hi.
By the choice of δ and ϵ and the metric σ on X we hence obtain a P-compatible metric g(λ,δ)⊕~h(μ,ϵ) on A×~B.
Definition 4.6**.**
We call g(λ,δ)⊕~h(μ,ϵ) the admissible product metric of g(λ,δ) and h(μ,ϵ).
We obtain the following version of the well known “shrinking one factor” principle.
Proposition 4.7**.**
Assume that A and B are compact and g is positive (see Definition 3.8).
Then for any μ≥1 and ϵ≥9 there exists 0<λ≤1 and δ≥9 such that for all δ′≥δ the following holds:
(i)
The metric g(λ,δ′)⊕~h(μ,ϵ) on A×~B is positive.
2. (ii)
The metric g(λ,δ′) is positive.
3. (iii)
Let C be a compact Pn-manifold, let k be a P-compatible metric on C, and let ν>0 and θ≥9 be such that the scaled metric k(ν,θ) is positive.
Then g(λ,δ′)⊕~k(ν,θ) is positive.
Proof.
Set min(scalσ):=minx∈X{scalσ(x)}∈R.
We will use a similar notation for other metrics instead of σ.
Note that min(scalσ)<0 by the Gauss-Bonnet formula, since the boundary pieces of X are totally geodesic and meet at angles π/2.
At each inductive step in the construction of A×~B we replace two collar factors [0,3)2 (with zero scalar curvature) by a factor X equipped with the metric σ.
Hence, and more generally for ω⊂{1,…,n}, we obtain with (5)
we find 0<λ≤1 and δ≥9 with the stated properties.
∎
5. Positive cross products and Toda brackets
Let X and Y be topological spaces and consider the Künneth sequence of singular homology groups
[TABLE]
In this section we study positive homology classes (see Definition 3.12) related to the homological cross product × and the Tor-term in this sequence.
Setting 5.1**.**
Let
[TABLE]
with Qn-manifolds A and B and let a∈Hd(X) and b∈He(Y) be the images of these bordism classes under the natural transformation u from Construction 2.5.
Propositions 4.4 and 4.7(i) imply the following result.
Proposition 5.2**.**
Assume that at least one of the Baas-Sullivan manifolds A or B is equipped with a Q-compatible positive metric (see Definition 3.8).
Then the class 2^{n}\cdot\big{(}a\times b\big{)}\in\operatorname{H}_{d+e}(X\times Y) is positive.
Next we discuss the Tor term in the Künneth sequence.
Let r≥2 be an integer with ra=0=rb.
Let (C∗(X),∂) and (C∗(Y),∂) be the integral chain complexes of X and Y.
We pick chains a∈Cd+1(X) and b∈Ce+1(Y) whose boundaries represent ra and rb respectively.
The cycle
[TABLE]
represents a Toda bracket coset
[TABLE]
with respect to the submodule (a×He+1(Y))⊕(Hd+1(X)×b)⊂Hd+e+1(X×Y), which is independent from the choice of a and b.
It is well known [EML]*Section 12 that such Toda brackets generate a submodule of Hd+e+1(X×Y) which maps surjectively onto Tor(H∗(X),H∗(Y))d+e.
In the following we give a bordism theoretic description of Toda brackets.
Hence, possibly after passing to some larger n, there are compact oriented Qn-manifolds V and W with boundaries ∂0V=∐2m⋅rA and ∂0W=∐2m⋅rB such that ∐2m⋅r(A→αX) and ∐2m⋅r(B→βY) can be extended to maps α:V→X and β:W→Y where α and β are compatible with the singularity structures of V and W.
By (6) and Proposition 4.4 the coset 2m+n⋅⟨a,r,b⟩⊂H∗(X×Y) is represented by
[TABLE]
Let A and B be equipped with Q-compatible positive metrics g and h.
The metrics ∐2m⋅rg on ∐2m⋅rA and ∐2m⋅rh on ∐2m⋅rB, can be extended to (not necessarily positive) Q-compatible metrics g and h on V and W (compare the proof of Lemma 3.4).
By Proposition 3.9(i) we find δ0,ϵ0≥9 such that for all δ≥δ0 and ϵ≥ϵ0 the scaled metrics g(1,δ) and h(1,ϵ) are positive.
Choose (λ,δ) for A according to Proposition 4.7 for the scaled metric h(1,ϵ0) on W, and in an analogous fashion choose (μ,ϵ) for B for the scaled metric g(1,δ0) on V.
With these choices the admissible product metrics g(1,δ0)⊕~h(μ,ϵ) on V×~B and g(λ,δ)⊕~h(1,ϵ0) on A×~W are positive by Proposition 4.7(i).
In order to glue the induced metrics on the common boundary ∐2m⋅rA×~B we need the following result.
Lemma 5.3**.**
The metrics g(1,δ0)⊕~h(μ,ϵ) and g(λ,δ)⊕~h(1,ϵ0) on A×~B are isotopic, and hence concordant, through positive Q-compatible metrics.
Proof.
Set Λ=[λ,1]⊂R and choose δ0′≥δ0,δ according to Proposition 3.9(i) for this Λ.
We find isotopies through positive Q-compatible metrics on A:
•
from g(1,δ0) to g(1,δ0′), by the choice of δ0;
•
from g(1,δ0′) to g(λ,δ0′), by the choice of δ0′;
•
from g(λ,δ0′) to g(λ,δ), by the choice of (λ,δ) and by Proposition 4.7(ii).
Hence, by the choice of (μ,ϵ), we obtain a smooth isotopy from g(1,δ0)⊕~h(μ,ϵ) to g(λ,δ)⊕~h(μ,ϵ) through positive Q-compatible metrics, see Proposition 4.7(iii).
In an analogous fashion we find a smooth isotopy from g(λ,δ)⊕~h(1,ϵ0) to g(λ,δ)⊕~h(μ,ϵ) through positive Q-compatible metrics, thus finishing the proof of Lemma 5.3.
∎
We obtain the following counterpart of Proposition 5.2.
Proposition 5.4**.**
We work in Setting 5.1 and assume in addition that both of the Baas-Sullivan manifolds A and B are equipped with Q-compatible positive metrics.
Let r≥2 be such that ra=0=rb.
Then for each element x∈⟨a,r,b⟩⊂Hd+e+1(X×Y) there exists ℓ≥0 such that 2ℓ⋅x is positive.
Proof.
Using the notation introduced after Proposition 5.2 the Qn-manifold
[TABLE]
in (7) carries a Q-compatible positive metric by Lemma 5.3.
Hence the class x′∈2m+n⋅⟨a,r,b⟩ represented by (V×~B)∪(A×~W)→X×Y is positive.
It is enough to show Proposition 5.4 for x∈2m+n⋅⟨a,r,b⟩.
Given such x we have x-x^{\prime}\in\big{(}a\times\operatorname{H}_{e+1}(Y)\big{)}\oplus\big{(}\operatorname{H}_{d+1}(X)\times b\big{)}\subset\operatorname{H}_{*}(X\times Y), and
by Propositions 2.6 and 5.2 and since a and b are positive there exists ℓ≥0 such that 2ℓ⋅(x−x′) is positive.
Using that x′ is positive we conclude that 2ℓ⋅x is positive.
∎
Let Γ1 and Γ2 be finite groups of odd order and set X=BΓ1 and Y=BΓ2.
Then each x∈H~∗(X×Y) is of odd order and hence for all m0≥0 there exists m≥m0 with 2m⋅x=x.
By Corollary 2.7 and Propositions 5.2 and 5.4 we conclude:
Corollary 5.5**.**
Let a∈Hd(BΓ1) and b∈He(BΓ2) where d,e≥0.
(i)
If either a or b is positive, then a×b is positive.
2. (ii)
Let r≥2 with ra=0=rb and let a and b be positive.
Then ⟨a,r,b⟩⊂Hd+e+1(BΓ1×BΓ2) only contains positive classes.
This result will be crucial for the computations in the next sections.
Remark 5.6**.**
One can show that the product ×~ on (relative) bordism groups Ω∗SO,Pn considered in Proposition 4.4 is graded commutative and associative.
Corollary 5.5, which is sufficient for the remainder of our paper, does not depend on these facts.
6. Homology of abelian groups
Let p be an odd prime.
Given an integer α≥1 we denote by Gα the cyclic group of order pα with generator gα and neutral element 1α.
The group operation in Gα is written multiplicatively.
We denote by ZGα the integral group ring of Gα.
Let (C(α)∗,∂∗) be the Z-graded Z-free chain complex with one generator cd in each degree d≥0 and differential
[TABLE]
This is the cellular chain complex with integer coefficients of the standard CW-model of the classifying space BGα with one cell in each non-negative dimension.
We hence recover the well known computation (see [Brown]*(II.3.1))
[TABLE]
For n≥1 and 1≤α1≤⋯≤αn we consider the abelian p-group
[TABLE]
and obtain
[TABLE]
where C∗(i)=C(αi)∗, i=1,…,n, refers to the ith cyclic factor in the group Γ.
Sometimes we will work with the reduced chain complex C~(α)∗:=C(α)∗/⟨c0⟩ of C(α)∗.
Note the canonical direct sum decomposition C(α)∗=C~(α)∗⊕⟨c0⟩ of chain complexes and the isomorphism H~∗(BΓ)≅H∗(C~(α1)∗⊗⋯⊗C~(αn)∗), where BΓ=BGα1∧⋯∧BGαn is the smash product of pointed classifying spaces.
In general we obtain a direct sum decomposition of chain complexes
[TABLE]
where the summand for k=0 is equal to ⟨c0⊗⋯⊗c0⟩⊂C(α1)∗⊗⋯⊗C(αn)∗, by definition.
For analyzing H∗(C(α1)∗⊗⋯⊗C(αn)∗) it is hence important to provide convenient generators of H∗(C~(αi1)∗⊗⋯⊗C~(αik)∗), for 1≤k≤n and 1≤i1<…<ik≤n.
In Proposition 6.2 we will do this for H∗(C~(α1)∗⊗⋯⊗C~(αn)∗), the other cases are analogous.
We first we write down cycle representatives of iterated Toda brackets.
Construction 6.1**.**
Let k≥1, let 1≤β1≤⋯≤βk and let m1,…,mk be positive integers.
We define a cycle in C~(β1)∗⊗⋯⊗C~(βk)∗ of degree 2m1+⋯+2mk−1 by
[TABLE]
Clearly the corresponding homology class satisfies pβ1⋅[T(c2m1−1(1),…,c2mk−1(k))]=0.
For k=1 we have T(c2m1−1(1))=c2m1−1(1), and for k≥2 we obtain iterated Toda brackets.
More precisely, setting hi:=[c2mi−1(i)]∈H2mi−1(C~(βi)∗) for i=1,…,k, we obtain
[TABLE]
We can now construct specific generators of H∗(C~(α1)∗⊗⋯⊗C~(αn)∗).
Let 1≤j≤n, let 1≤i1<⋯<ij≤n and let m1,…,mj be positive integers.
Let (s1,…,sn−j) with 1≤s1<⋯<sn−j≤n be the unique family complementary to (i1,…,ij) (this family is empty for j=n) and let d1,…,dn−j be further positive integers.
Suppressing a signed permutation of tensor factors we obtain a cycle
[TABLE]
In the following we will call cycles of this sort special.
Proposition 6.2**.**
H∗(C~(α1)∗⊗⋯⊗C~(αn)∗)* is generated by special cycles with i1=1.*
Proof.
We apply induction on n.
In the induction step we set C∗n:=C~∗(1)⊗⋯⊗C~∗(n) and consider the exact Künneth sequence
[TABLE]
By the induction hypothesis, the construction of Tor(H∗(C∗n),H∗(C~∗(n+1))) and the assumption that α1≤αn+1, Toda brackets of the form
[TABLE]
map to a generating set of Tor(H∗(C∗n),H∗(C~∗(n+1))).
This Toda bracket contains [T(c(1),…,c(ij),c(n+1))⊗c(s1)⊗⋯⊗c(sn−j)] (up to sign), and hence special cycles T(c(1),…,c(ij),c(n+1))⊗c(s1)⊗⋯⊗c(sn−j) map to a generating set of Tor(H∗(C∗n),H∗(C~∗(n+1))).
The image of the left-hand map in the Künneth sequence satisfies the claim by the induction assumption.
∎
Example 6.3**.**
Let n=3 and α1=1, α2=2 and α3=3.
Then
[TABLE]
Proposition 6.2 can be illustrated in this case by computing T(c1(2),c1(3))⊗c1(1) as
[TABLE]
Next we will derive some explicit formulas for maps in group homology induced by group homomorphisms.
We consider the homological chain complex in non-negative degrees
[TABLE]
where the differentials are given by multiplication with τα:=gα−1α and να:=∑i=0pα−1(gα)i, respectively.
With the augmentation map εα:ZGα→Z induced by the group homomorphism Gα→{1} we obtain an exact sequence
[TABLE]
In other words (F(α)∗,∂∗) is a ZGα-free resolution of the ZGα-module Z, see [Brown]*(I.6.3).
Note the canonical isomorphism of chain complexes C(α)∗=F(α)∗⊗ZGαZ.
Let α,β,λ∈N>0 with pβ∣λ⋅pα, and consider the group homomorphism
[TABLE]
Then each ZGβ-module can be regarded as a ZGα-module via the ring map
[TABLE]
With this convention the assignments (using \lambda\cdot p^{\alpha-\beta}\in\mathbb{N}_{{\color[rgb]{0,0,0}\definecolor[named]{pgfstrokecolor}{rgb}{0,0,0}\pgfsys@color@gray@stroke{0}\pgfsys@color@gray@fill{0}>0}})
[TABLE]
uniquely extend to ZGα-linear maps ZGα→ZGβ and an explicit computation
[TABLE]
and similar to obtain ϕ2m(τα⋅1α)=τβ⋅ϕ2m+1(1α), shows that we obtain an augmentation preserving map of ZGα-linear chain complexes
[TABLE]
After applying the functor −⊗ZGαZ we obtain the following result.
Proposition 6.4**.**
The induced chain map ϕ∗:C(α)∗→C(β)∗ is given by
[TABLE]
Note that the map induced in homology by ϕ∗ can be identified with the map
[TABLE]
compare [Brown]*(II.6.1).
Lemma 6.5**.**
Consider the diagonal map Δ:Gα→Gα×Gα, g↦(g,g).
Then the induced map in homology Δ∗:H∗(C(α)∗)→H∗(C(α)∗⊗C(α)∗) satisfies
[TABLE]
Proof.
Obviously ∑i=02m+1ci⊗c2m+1−i is a cycle in C(α)∗⊗C(α)∗.
It is enough to show Lemma 6.5 after passing to coefficients Z/pα.
Using the Künneth isomorphism H∗(BGα×BGα;Z/pα)≅H∗(BGα;Z/pα)⊗H∗(BGα;Z/pα) the claim now follows from the well known ring structure of H∗(BGα;Z/pα).
∎
Definition 6.6**.**
A cycle c∈C(α1)∗⊗⋯⊗C(αn)∗ is called positive, if the homology class [c]∈H∗(BΓ) is positive with respect to Q in the sense of Definition 3.12.
Obviously the cycles c2m−1∈C(α)2m−1 are positive for m≥2 since these can be represented by classifying maps of lens spaces S2m−1/(Z/pα)→BGα.
Furthermore the tensor product of two cycles, one of which is positive, is itself positive by Corollary 5.5(i), and for m1,m2≥2 the cycle T(c2m1−1,c2m2−1)∈C(α1)∗⊗C(α2)∗ is positive by Corollary 5.5(ii).
We will now identify some more positive cycles in C(α1)∗⊗C(α2)∗.
Proposition 6.7**.**
For m≥2 the following cycles in C(α1)∗⊗C(α2)∗ are positive:
(i)
p⋅T(c1,c2m−1)* and p⋅T(c2m−1,c1),*
2. (ii)
T(c1,c2m−1)* and T(c2m−1,c1), if α1<α2.*
Proof.
Given γ∈N>0 we consider the group homomorphism ϕγ:Gα1→Gα2 defined by gα1↦(gα2)γ⋅(pα2−α1) and the resulting homomorphism
[TABLE]
We claim that for m≥1 the image of (fγ)∗([c2m+1]) in H∗(C~(α1)∗⊗C~(α2)∗) is equal to
[TABLE]
This follows from Lemma 6.5 and Proposition 6.4 (with α=α1, β=α2, λ=γ⋅pα2−α1), which gives us
For m≥2 we have p∣(pm−p), but p2∤(pm−p).
Together with (9) and the fact that c2m+1 and T(c2s−1,c2t−1) for s,t≥2 are positive, this implies that suitable linear combinations of (f1)∗([c2m+1]) and (fp)∗([c2m+1]), which define positive classes in H2m+1(C(α1)∗⊗C(α2)∗), map to p⋅[T(c2m−1,c1)] and to p⋅[T(c1,c2m−1)] in H∗(C~(α1)∗⊗C~(α2)∗).
Since all cycles in C(α1)2m+1⊗C(α2)0 and C(α1)0⊗C(α2)2m+1 are positive this finishes the proof of part (i).
For part (ii) let α1<α2, consider the group homomorphism ϕ:Gα2→Gα1 defined by gα2↦gα1 and the resulting homomorphism
[TABLE]
We claim that for m≥1 the image of f∗([c2m+1]) in H∗(C~(α1)∗⊗C~(α2)∗) is equal to
[TABLE]
We argue similarly as before, observing that by Proposition 6.4 (with λ=1) we get
[TABLE]
Equation (10) together with part (i) implies that for m≥2 there is a positive cycle in C(α1)∗⊗C(α2)∗ that maps to [T(c1,c2m−1)]∈H∗(C~(α1)∗⊗C~(α2)∗).
Similar as before this implies that the cycle T(c1,c2m−1)∈C(α1)∗⊗C(α2)∗ is positive.
By (9) applied to γ=1 and the positivity of c2m+1 and T(c2s−1,c2t−1) for s,t≥2 there is a positive cycle in C(α1)∗⊗C(α2)∗ that maps to
[TABLE]
and hence (since T(c1,c2m−1) has already been verified as positive) a positive cycle that maps to [T(c2m−1,c1)]∈H∗(C~(α1)∗⊗C~(α2)∗).
Similar as before this implies that T(c2m−1,c1)∈C(α1)∗⊗C(α2)∗ is positive, finishing the proof of part (ii).
∎
We also need to consider iterated Toda brackets of degree one cycles.
Lemma 6.8**.**
Let 1≤α1≤α2≤α3.
[TABLE]
are positive.
Proof.
First let α:=α1=α2=α3.
The diagonal map Δ:Gα→(Gα)3, g↦(g,g,g), satisfies
[TABLE]
where D contains all triples (d1,d2,d3) with 0≤di≤5, ∑di=5 and precisely one odd di.
This follows from the ring structure of H∗(BGα;Z/pα) and the assumption that p is odd.
For 1≤i<j≤3 let Δ(i,j):Gα→(Gα)3 denote the diagonal map δ:Gα→(Gα)2 composed with the embedding (Gα)2→(Gα)3 to the ith and jth factors.
Since δ∗([c5])=[∑i=05ci⊗c5−i] a direct calculation shows
[TABLE]
Since c5 is positive this implies positivity of T(c1,c1,c1)∈(C(α)∗)3.
Now let 1≤α1≤α2≤α3 and let
[TABLE]
where ϕi:Gα1→Gαi is induced by gα1↦(gαi)pαi−α1, 1≤i≤3.
By Proposition 6.4 we obtain
[TABLE]
This implies the first assertion.
The proof of the second assertion is similar.
∎
We obtain the following conclusive result on the positivity of iterated Toda bracket cycles (which may contain degree one cycles).
Proposition 6.9**.**
Let n≥2, 1≤α1≤⋯≤αn
and m1,…,mn≥1.
Then the following cycles in C(α1)∗⊗⋯⊗C(αn)∗ are positive:
(i)
p⋅T(c2m1−1(1),…,c2mn−1(n)), if α1=⋯=αn,
2. (ii)
T(c2m1−1(1),…,c2mn−1(n)), if α1<αn.
Proof.
Let 1≤i1<…<ir≤n be those indices with mij=1 (where 0≤r≤n).
Note that for all 1≤k≤n which are different from any ij the cycle c2mk−1(k) is positive.
We consider the following cases:
•
If r=0 then T(c2m1−1(1),…,c2mn−1(n)) represents an iterated Toda product of positive classes and is hence positive by Corollary 5.5(ii).
•
If r>1 then T(c1(i1),…,c1(ir)) is positive by Lemma 6.8 by grouping the cycles c1(ij) for 1≤j≤r into families of two and three, and applying the fact that Toda brackets of positive classes are positive.
Hence T(c2m1−1(1),…,c2mn−1(n)) represents an iterated Toda bracket of positive classes, and is therefore positive.
•
If r=1 let 1≤i≤n be the unique index with mi=1.
If α1<αn we find 1≤k≤n with αi=αk.
Then T(c2mi−1(i),c2mk−1(k)) (resp. T(c2mk−1(k),c2mi−1(i)) if k<i) is positive by Proposition 6.7(ii).
If α1=αn, then p⋅T(c2mi−1(i),c2mk−1(k)) is positive for any 1≤k≤n with k=i by Proposition 6.7(i).
The proof can now be finished as before.
∎
For κ≥1, γ∈N>0 and m=pκ we get γm≡γmod(p) in (9).
Hence the following problem cannot be answered with the methods developed in this section and enforces us to restrict to p-divisible cycles in Proposition 6.9(i), in general.
Question 6.10**.**
Let α,κ≥1.
Is the p-atoral (for odd p) cycle T(c1,c2pκ−1)∈C(α)∗⊗C(α)∗ positive?
7. Generalized products of lens spaces in group homology
Let p be an odd prime, let α,n≥1, and let Γ:=(Gα)n.
For our proof of Theorem 1.6 we will argue that certain p-atoral cycles such as the one in Question 6.10 are not contained in the image of Ω∗SO(BΓ)→H∗(BΓ) and can therefore be ignored.
In this section we will approach this issue, which is related to the classical Steenrod problem on the realization of homology classes by smooth manifolds, in terms of natural stable homology operations defined for any topological space X,
[TABLE]
which by construction vanish on classes coming from Ω∗SO(X).
In Proposition 7.9, the main result of this section, we will show that the vanishing of the operations ∂(κ,α), together with the vanishing of a suitable Bockstein operation, is indeed sufficient to detect elements in the image of Ω∗SO(BΓ)→H∗(BΓ;Fp), and that these elements can be represented by products of standard Z/pα-lens spaces.
Since we prefer to avoid a discussion of stable (co-)homology operations with coefficients Z/pℓ, for which we did not find a handy account in the literature, we construct the operation ∂(κ,ℓ) as a differential in the Atiyah-Hirzebruch spectral sequence of a homology theory derived from Brown-Peterson theory at the prime p, whose well known structure allows us to derive some crucial properties of ∂(κ,ℓ).
Recall that the coefficient ring for Brown-Peterson theory at the prime p is isomorphic to a polynomial ring
[TABLE]
where vi∈BP2pi−2.
As usual we set v0=p.
For κ,ℓ≥1 we define the ideal
[TABLE]
Proposition 7.1**.**
There is a multiplicative homology theory BP(κ,ℓ) with coefficient ring
[TABLE]
together with a natural transformation of multiplicative homology theories BP→BP(κ,ℓ), which on the level of coefficients induces the projection Z(p)[v1,v2,…]→Z(p)[v1,v2,…]/I(κ,ℓ).
Proof.
Recall the construction of a (homotopy) commutative ring spectrum BP representing Brown-Peterson theory for odd p in [Shimada]*Corollary 6.7, which is based on bordism theory with Baas-Sullivan singularities killing the polynomial generators xj for j=pi−1 with i≥1, of π∗(MU)(p)≅Z(p)[xj∣j≥1,deg(xj)=2j].
Here MU denotes the unitary bordism spectrum.
We construct BP(κ,ℓ) in a similar fashion as a bordism theory with Baas-Sullivan singularities, killing the regular sequence (pℓ,x1,…,(xpκ−1)2,…) in π∗(MU)(p).
It follows from [Shimada]*Theorem 6.2 (and the assumption that p is odd) that this theory is represented by a commutative ring spectrum BP(κ,ℓ).
Furthermore, by construction, there is a canonical map of ring spectra BP→BP(κ,ℓ) with the stated property on the level of coefficients.
∎
We have BP∗(κ,ℓ)≅⟨1,vκ⟩Z/pℓ, the free graded Z/pℓ-module with generators 1 in degree [math] and vκ in degree 2pκ−2, with multiplication satisfying vκ2=0.
The theory BP(κ,ℓ) may be considered as a form of extraordinary K-theory, where we have introduced the additional truncation vκ2=0 for computational purposes, compare Lemma 7.3.
Let X be a topological space and consider the Atiyah-Hirzebruch spectral sequence
[TABLE]
The term Es,t2 is non-zero precisely for t=0 and t=2pκ−2, and in these cases is canonically isomorphic to Hs(X;Z/pℓ) (depending on the choice of vκ).
In particular we have Es,t2=Es,t2pκ−1 and we define
[TABLE]
as the differential ∂2pκ−1:Es,02pκ−1→Es−2pk+1,2pκ−22pκ−1.
It is immediate from this construction that ∂(κ,ℓ) is natural in X, is stable with respect to suspensions, and is a derivation with respect to the homological cross product.
Since the natural transformation Ω∗SO(X)→H∗(X;Z/pℓ) factors through BP(κ,ℓ)(X) all classes in H∗(X;Z/pℓ) coming from Ω∗SO(X) lie in the kernel of ∂(κ,ℓ).
Remark 7.2**.**
The cohomology operation H∗(X;Fp)→H∗+2pκ−1(X;Fp) dual to ∂(κ,1) can be identified with the κth Milnor basis element Qκ∈Ap2pκ−1 in the mod(p)-Steenrod algebra.
For evaluating the operations ∂(κ,ℓ) for X=BGα we need to determine the BP(κ,ℓ)-theoretic Euler class of the fibration S1↪BGα→CP∞.
This is based on a formal group law computation.
For κ≥1 we define the ideal
[TABLE]
and set BP∗:=BP∗/I(κ).
Let xBP∈BP2(CP∞) be the standard complex orientation and recall BP∗(CP∞)≅BP∗[[xBP]].
Lemma 7.3**.**
Let α,κ≥1 and let pα:CP∞→CP∞ be the map induced by S1→S1, t↦tpα, using the identification BS1=CP∞.
Let (pα)∗:BP∗(CP∞)→BP∗(CP∞) be the induced map in BP-cohomology.
Then in BP∗[[xBP]] we obtain the equation
[TABLE]
where Rα∈pα⋅BP∗[[xBP]].
Proof.
We use induction on α.
We write x instead of xBP and carry out the following computations in BP∗[[x]].
For α=1 the p-typical formal group law of BP yields (p)∗(x)=px+vκ⋅xpκ (possibly after multiplying vκ with a unit in Z(p)).
Hence the assertion holds for α=1.
Using vκ2=0∈BP∗ we inductively obtain, for α≥1,
[TABLE]
where R_{\alpha+1}:=p\cdot R_{\alpha}+v_{\kappa}\cdot\big{(}p^{\alpha}\cdot x+p^{\alpha-1}v_{\kappa}\cdot x^{p^{\kappa}}+R_{\alpha}\big{)}^{p^{\kappa}}\in p^{\alpha+1}\cdot\widehat{\operatorname{BP}}^{*}[[x^{\operatorname{BP}}]].
∎
Convention 7.4**.**
Let x∈H2(CP∞;Z) be the complex orientation induced by xBP and for m≥0 let y2m∈H2m(CP∞;Z) be the generator dual to xm.
For any commutative ring R with unit we obtain an exact Gysin sequence
[TABLE]
where e=pα⋅x∈H2(CP∞;Z) is the Euler class of the S1-principal fiber bundle
[TABLE]
equipped with its canonical orientation induced by the inclusion S1⊂C, and τ∗ is the homological transfer in this fiber bundle.
For m≥0 we obtain specific generators c2m+1=τ2m(y2m)∈H2m+1(BGα;Z)≅Z/pα and c2m∈H2m(BGα;Z/pα)≅Z/pα with
[TABLE]
Furthermore, for 1≤ℓ≤α, these generators induce generators cd∈H∗(BGα;Z/pℓ) for d≥0.
We can and will assume that the generators
[TABLE]
of the cellular chain complex introduced at the beginning of Section 6 map to these specific generators of Hd(BGα;Z/pℓ) after passing to coefficients Z/pℓ.
Proposition 7.5**.**
Let α,κ≥1 and 1≤ℓ≤α.
Then the operation
[TABLE]
viewed as a map C(α)∗⊗Z/pℓ→C(α)∗−2pκ+1⊗Z/pℓ, is given by
[TABLE]
Proof.
Using the canonical isomorphism
[TABLE]
we may write the BP(κ,ℓ)-homology spectral sequence for the fiber bundle S1↪BGα→CP∞ as
[TABLE]
The only nonvanishing differential is given by ∂2:Es,02→Es−2,12, c↦(c∩e)⊗[S1], where c∈BPs(κ,ℓ)(CP∞), e∈(BP(κ,ℓ))2(CP∞) is the BP(κ,ℓ) theoretic Euler class of S1↪BGα→CP∞, and [S1]∈H1(S1;Z) is the given orientation class.
Note that this spectral sequence induces the BP(κ,ℓ)-theoretic Gysin sequence for the fiber bundle S1↪BGα→CP∞.
Let x∈(BP(κ,ℓ))2(CP∞) be the class induced by xBP.
Viewing vκ∈BP2pκ−2(κ,ℓ)≅(BP(κ,ℓ))−2pκ+2 Lemma 7.3 implies
[TABLE]
Now consider the isomorphisms
[TABLE]
the first one of which is induced by the projection BGα→CP∞ and the second one by the homological transfer τ∗ for the bundle S1↪BGα→CP∞.
Under these isomorphisms the differential ∂2:Es,02→Es−2,12, c↦(c∩e)⊗[S1], corresponds to the differential
[TABLE]
in the Atiyah-Hirzebruch spectral sequence Es,t2=Hs(BGα;BPt(κ,ℓ))⟹BPs+t(κ,ℓ)(BGα).
Since this differential defines ∂(κ,ℓ), Proposition 7.5 follows.
∎
Example 7.6**.**
Let α,κ≥1 and Γ=(BGα)2.
Then in H∗(BΓ;Z/pα) we get
[TABLE]
and hence the cycle T(c1,c2pκ−1)∈C(α)∗⊗C(α)∗ appearing in Question 6.10 does not lift to Ω2pκ+1SO(BΓ).
For p=3 and α,κ=1 this reproduces the class in H7(B(Z/3)2;Z) considered in [Thom54]*page 62, which was the first example of an integral homology class that cannot be represented by a smooth manifold.
For a topological space X and ℓ≥1 we denote by β(ℓ):H∗(X;Z/pℓ)→H∗−1(X;Fp) the Bockstein operation for the exact coefficient sequence 0→Z/p→⋅pℓZ/pℓ+1→Z/pℓ→0.
Note that β(ℓ) vanishes on classes that lift to integral homology.
Definition 7.7**.**
Let ℓ≥1.
We call the submodule
[TABLE]
the almost representable homology in H∗(X;Z/pℓ).
Let α,n≥1 and Γ=(Gα)n.
It follows from Proposition 7.5 that p⋅H∗(BΓ;Z/pα) is contained in RH∗(BΓ;Z/pα).
The same holds for the image of Ω∗SO(BΓ)→H∗(BΓ;Z/pα).
In Proposition 7.9 we will show a weak converse of the last statement.
We first define specific elements in the group homology H∗(BΓ;Fp), which are represented by smooth manifolds.
Definition 7.8**.**
For m≥1 denote by L2m−1=S2m−1/(Z/pα) the standard Z/pα-lens space.
Let 1≤k≤n and let ϕ:(Gα)k→(Gα)n be some group homomorphism.
For m1,…,mk≥1 we obtain the map
[TABLE]
where Ψ is the product of classifying maps.
The class Φ∗([L2m1−1×⋯×L2mk−1])∈H∗(BΓ;Fp) is called a generalized product of lens spaces.
Obviously this element lifts to Ω∗SO(BΓ).
We can now state the main result of this section.
Proposition 7.9**.**
The image of RH∗(BΓ;Z/pα)↪H∗(BΓ;Z/pα)→H∗(BΓ;Fp) is generated by generalized products of Z/pα-lens spaces.
Remark 7.10**.**
It was observed first in [BR1]*Theorem 5.6 that generalized products of lens spaces generate the image of Ω∗SO(B(Z/p)n)→H∗(B(Z/p)n;Fp).
A complete proof of this statement was given in [Ha15].
Already for α=1 Proposition 7.9 is stronger than [BR1]*Theorem 5.6 as it is not clear a priori that all classes in RH∗(B(Z/p)n;Fp) lift to Ω∗SO(B(Z/p)n).
The proof of Proposition 7.9, which will be given at the end of this section, requires some preparation.
Our argument is mainly algebraic and in principle carried out in the reduced homology H~∗(BΓ;Fp), which is reflected in the following notation.
Let
•
C∗=H~∗(BGα;Fp) be the free Z-graded Fp-module with one generator cd in each degree d≥1;
•
(C∗)n=H~∗(BΓ;Fp) be its n-fold tensor product, with n≥0;
•
∂(κ), κ≥0, be the differential on (C∗)n of degree −2pκ+1, which acts as a derivation and satisfies
[TABLE]
•
C∗n,r:=⋂0≤κ≤rker∂(κ)⊂(C∗)n for r≥0, and C∗n,∞=⋂κ≥0ker∂(κ).
Proposition 7.11**.**
The canonical map
[TABLE]
sends RH∗(BΓ;Z/pα) onto Cn,∞.
Proof.
The Bockstein operation β(α):H∗(BGα;Z/pα)→H∗−1(BGα;Fp) is given by C(α)∗⊗Z/pα→C(α)∗−1⊗Fp, c0↦0, c2m−1↦0, and c2m↦c2m−1 for m≥1.
Hence its n-fold tensor product derivation restricts to a map (C~(α)∗⊗Z/pα)n→(C∗)n whose kernel goes onto ker∂(0)⊂(C∗)n under tensoring the domain with Fp.
For κ≥1 the computation of ∂(κ,α):H∗(BGα;Z/pα)→H∗−2pκ+1(BGα;Z/pα) in Proposition 7.5 implies that its n-fold tensor product derivation restricts to a map (C~(α)∗⊗Z/pα)n→(C~(α)∗⊗Z/pα)n whose kernel goes onto ker∂(κ)⊂(C∗)n under tensoring the domain with Fp.
From these facts Proposition 7.11 follows, using p⋅H∗(BΓ;Z/pα)⊂RH∗(BΓ;Z/pα).
∎
We will now analyse the submodule C∗n,∞⊂(C∗)n.
For this aim we define the Z-graded Fp-modules:
•
N∗:=span{c2m−1∣m≥1}=H~odd(BGα;Fp)⊂C∗;
•
L∗:=span{y2m∣m≥1}=H~even(CP∞;Fp), where y2m are free generators of degree 2m;
•
L<pk:=span{y2m∣1≤m<pk}⊂L∗ for k≥0.
Note that the canonical projection C∗→L∗, c2m↦y2m, c2m−1↦0 (which on the topological side is induced by BGα→CP∞) commutes with the differentials ∂(κ) for κ≥0, which we define as zero on L∗.
Let (N∗)n be the n-fold tensor product of N∗ for n≥0.
For every 1≤k≤n and every group homomorphism ϕ:(Gα)k→(Gα)n=Γ we obtain an induced map
[TABLE]
Definition 7.12**.**
For n≥1 we set
[TABLE]
Since the generators of N∗ are represented by Z/pα-lens spaces we have L∗n⊂C∗n,∞ by Proposition 7.11.
The crucial step for the proof of Proposition 7.9 consists in showing that here equality holds, see Proposition 7.16.
We first derive a lower bound for the size of L∗n⊂C∗n,∞.
Proposition 7.13**.**
For n≥1 the canonical projection L∗n+1→(N∗)n⊗L<pn is surjective.
Proof.
Essentially the proof for α=1 in [Ha15]*Proposition 5.3 generalizes to larger α.
For notational reasons we work with the additive group Z/pα instead of Gα.
For 0≤λ1,…,λn≤p−1 we consider the group homomorphism
[TABLE]
For all γ≥1 we have an Fp-algebra isomorphism
[TABLE]
where t1,…,tγ are indeterminates of degree 2 and s1,…,sγ are indeterminates of degree 1.
The map induced in Fp-cohomology by Bϕ(λ1,…,λn):B(Z/pα)n→B(Z/pα)n+1 satisfies
[TABLE]
for ν≥0.
This computation uses the ring structures of H∗(B(Z/pα)γ;Fp) for γ=n,n+1.
The pn×pn Vandermonde-matrix
[TABLE]
(where the subscript parametrizes the rows) with entries in Fp[t1,…,tn] has determinant
[TABLE]
applying the lexicographic order to the index set.
Hence the column vectors of V are linearly independent over Fp[t1,…,tn].
Setting N∗:=Hodd(BZ/pα;Fp) this means, in view of (14), that the map
[TABLE]
is injective.
Dualizing this statement over Fp we conclude that the map
[TABLE]
is surjective.
∎
The modules (N∗)n⊗L<pn play an important role in the determination of Cn,∞, which we will carry out in two steps.
First note that we have a canonical direct sum decomposition
[TABLE]
where (C∗)(γ)n⊂(C∗)n is generated by those elementary tensors cd1⊗⋯⊗cdn involving γ components of even degree.
For example (C∗)(0)n=(N∗)n.
Since the differentials ∂(κ) map (C∗)(γ)n to (C∗)(γ−1)n we get induced direct sum decompositions of C∗n,r for r≥0.
The next, somewhat involved, proposition takes care of the particular component
[TABLE]
for certain r.
The full structure of C∗n,∞ will afterwards be determined in Proposition 7.16.
Note that for r≥0 the differential ∂(r):(C∗)n→(C∗)n induces a map ∂(r):D∗n,r−1→(N∗)n with kernel D∗n,r.
Here and later we set D∗n,−1:=(C∗)(1)n.
Proposition 7.14**.**
For n≥0 the following holds.
(i)
The canonical projection π:D∗n+1,n−1→(N∗)n⊗L∗ is surjective and there exists a surjective map ∂(n):(N∗)n⊗L∗→(N∗)n+1 such that the following diagram commutes:
[TABLE]
2. (ii)
The projection ker(∂(n))→(N∗)n⊗L<pn is an isomorphism.
3. (iii)
D∗n+1,n(=ker(∂(n)))=D∗n+1,∞.
Proof.
We apply induction on n.
For n=0 the proposition holds as
•
D∗1,−1=L∗=(N∗)0⊗L∗ and π is an isomorphism,
•
∂(0):D∗1,−1→N∗−1 is an isomorphism and hence D∗1,0=0=(N∗)0⊗L<p0.
Now assume that n≥1 and Proposition 7.14 has been shown up to n−1.
Let c=c2d1−1⊗⋯⊗c2dn−1∈(N∗)n and let m>0.
We will show c⊗y2m∈im(π).
Let 0≤κ≤n−1.
Using the inductive assumption ((i)) we find c(κ)∈D∗κ+1,κ−1 with ∂(κ)(c(κ))=c2d1−1⊗⋯⊗c2dκ+1−1.
Setting c(κ):=c(κ)⊗c2dκ+2−1⊗⋯⊗c2dn−1 we then have c(κ)∈Ddeg(c)+2pκ−1n,κ−1 and ∂(κ)(c(κ))=c.
Using the induction assumption again several times in order to balance ∂(j)(c(κ)) for j=κ+1,…,n−1 we can arrange furthermore that ∂(j)(c(κ))=0 for κ<j≤n−1.
Summarizing we have ∂(j)(c(κ))=0 for 0≤j≤n−1 with j=κ, while ∂(κ)(c(κ))=c.
With these choices we get
[TABLE]
and π indeed sends this element to c⊗y2m∈(N∗)n⊗L∗.
This shows surjectivity of π.
If c∈D∗n+1,n−1∩ker(π), then c∈D∗n,n−1⊗N∗ by the definition of D∗n,n−1 and hence c∈D∗n,∞⊗N∗, using the inductive assumption ((iii)).
We conclude ∂(n)(c)=0, and hence ∂(n) is well defined.
Next let c∈(N∗)n and let m>0.
We claim c⊗c2m−1∈im(∂(n)), showing that ∂(n), and hence ∂(n), is surjective.
The proof is by induction on deg(c).
As in (15) we find c(κ)∈Ddeg(c)+2pκ−1n,κ−1 for 0≤κ≤n−1 with
[TABLE]
We have ∂(n)(c⊗c2m+2pn−2)=(−1)nc⊗c2m−1 and
[TABLE]
For 0≤κ≤n−1 we compute
[TABLE]
Hence ∂∗(n)(c(κ))⊗c2m+2pn−2pκ−1∈im(∂(n)) by induction on deg(c).
Altogether we see c⊗c2m−1∈im(∂(n)) as required.
The proof of (i), the most difficult part of Proposition 7.14, is now complete.
For (ii) we first observe that \dim\ker(\overline{\partial^{(n)}})_{d}=\dim\big{(}(N_{*})^{n}\otimes L_{<p^{n}}\big{)}_{d} for d≥0, since, by an elementary dimension count,
is surjective by Lemma 7.13, so that also the projection ker(∂(n))→(N∗)n⊗L<pn is surjective.
Since domain and target of this map have the same dimension in each degree this implies assertion (ii).
For assertion (iii) let c∈D∗n+1,n.
Since L∗n+1⊂C∗n+1,∞ Proposition 7.13 implies that there exists x∈D∗n+1,∞ such that the projection of c+x to (N∗)n⊗L<pn vanishes,
Since ∂∗(n)(c+x)=0 and ker(∂(n)) maps isomorphically to (N∗)n⊗L<pn we obtain π(c+x)=0∈(N∗)n⊗L∗.
We conclude c+x∈D∗n,n⊗N∗=D∗n,∞⊗N∗ by the induction assumption (iii).
Since D∗n,∞⊗N∗⊂D∗n+1,∞ and x∈D∗n+1,∞ assertion (iii) follows.
∎
Let c∈ker(C∗n+1,∞→(N∗)n⊗L<pn).
We decompose c=c′+c′′ where c′∈D∗n+1,∞ and c′′ is a linear combination of elementary tensors cd1⊗⋯⊗cdn+1 with [math] or at least 2 even degree components.
Obviously c^{\prime\prime}\in\ker(\mathscr{C}^{n+1,\infty}\to(N_{*})^{n}\otimes L_{*}\big{)}.
This fact and the assumption on c imply c′∈ker(D∗n+1,∞→(N∗)n⊗L<pn).
But by Proposition 7.14(ii) the projection (N∗)n⊗L∗→(N∗)n⊗L<pn induces an isomorphism π(D∗n+1,n)≅(N∗)n⊗L<pn.
Hence we must also have c′∈ker(D∗n+1,∞→(N∗)n⊗L∗).
∎
We finally obtain a precise description of C∗n,∞ and of L∗n⊂C∗n,∞ (recall Definition 7.12), showing in particular that the last inclusion is an equality.
Proposition 7.16**.**
Let Jn denote the set of families J=(J1,…,Jn), where Ji=N∗ or Ji=L<pk and k is the number of Jj for j<i with Jj=N∗.
Then the canonical map (induced by projections C∗→N∗ and C∗→L∗)
[TABLE]
is an isomorphism.
The restriction of Ψn to L∗n⊂C∗n,∞ is still surjective, and hence also an isomorphism.
In particular L∗n=C∗n,∞.
Proof.
Since source and target of Ψ1 are equal to L∗1=N∗ the assertions are clear for n=1.
By induction we assume that they hold for some n≥1.
For J=(J1,…,Jn)∈Jn let k(J) denote the number of components Ji=N∗.
Furthermore we set Ji′=C∗ for Ji=N∗ and Ji′=L<pk for Ji=L<pk.
In the induction step we first prove injectivity of Ψn+1.
Let c∈kerΨn+1.
We study the image of c under the composition of projections
[TABLE]
Note that π1 commutes with the differentials ∂(κ) for κ≥0 (with zero differentials on L<pk).
Let c′∈J1′⊗⋯⊗Jn′⊗C∗ be one component of π1(c), where J∈Jn.
By assumption the image of c′ under the map
and hence π2(c′)=0 (recall that k(J)+1 is the number of factors C∗ in J1′⊗⋯⊗Jn′⊗C∗ and that all other factors are equal to some L<pk with zero differential).
Applying this argument to all components c′ of π1(c) we conclude π2(π1(c))=0.
Let π:C∗n+1,∞→C∗n,∞⊗L∗ be the projection (recall again that C∗→L∗ commutes with all differentials ∂(κ) for κ≥0).
Since (Ψn⊗id)∘π=π2∘π1 our induction assumption (injectivity of Ψn) implies π(c)=0.
Hence c∈kerΨn⊗N∗, which is equal to [math], again by the induction assumption.
This shows that Ψn+1 is injective.
We next show that Ψn+1 maps L∗n+1⊂C∗n+1,∞ surjectively onto ⨁Jn+1J1⊗⋯⊗Jn+1, completing the induction step.
Let (J1,…,Jn+1)∈Jn+1.
We have to show J1⊗⋯⊗Jn+1⊂Ψn+1(L∗n+1).
By induction we have J1⊗⋯⊗Jn⊂Ψn(L∗n).
In particular J1⊗⋯⊗Jn⊗N∗⊂Ψn+1(L∗n⊗N∗).
Since L∗n⊗N∗⊂L∗n+1 we can hence restrict to the case Jn+1=L<pk(J), where J:=(J1,…,Jn).
For each group homomorphism ϕ:(Gα)k(J)→(Gα)k(J)+1 we obtain an induced map (N∗)k(J)→(N∗)k(J)⊗L<pk(J) (compare (13)) and hence an induced map J1⊗⋯⊗Jn→J1⊗⋯⊗Jn⊗L<pk(J) equal to the identity on factors Ji=L<pk for some k and i=1,…,n.
Using the proof of Proposition 7.13 the images of these maps for different ϕ span J1⊗⋯⊗Jn⊗L<pk(J).
Since J1⊗⋯⊗Jn⊂Ψn(L∗n) by induction we conclude J1⊗⋯⊗Jn⊗L<pk(J)⊂Ψn+1(L∗n+1) by the functoriality of group homology.
∎
Remark 7.17**.**
The formulation of Proposition 7.16 is inspired by [JW]*Theorem 5.1, also see [Ha15]*Theorem 1.2.
In contrast to these sources the algebraic argument above does not rely on the solution of a Conner-Floyd conjecture for Ω∗SO(BΓ), which seems to be inaccessible at present for α>1.
Indeed we believe that our approach may be a first step towards an algebraic proof of the Conner-Floyd conjecture (for α=1), which was resolved in [Mitchell, RW] by topological methods.
The decomposition of (C(α)∗)n from (8) (after tensoring with Z/pα, respectively Fp) is compatible with the operations β(α) and ∂(κ,α).
By induction on n it is hence sufficient to show that the image of the composition
[TABLE]
is generated by generalized products of Z/pα-lens spaces L2m1−1×⋯×L2mk−1→BΓ for 1≤k≤n.
Propositions 7.11 and 7.16 imply that the image of ψ is equal to C∗n,∞=L∗n, from which this claim follows.
∎
Let 1≤α1≤⋯≤αn, let Γ=Gα1×⋯×Gαn and let h∈H∗(BΓ;Z) be contained in the image of Ω∗SO(BΓ)→H∗(BΓ;Z).
Using the decomposition from (8) we represent h by a cycle in
[TABLE]
Proposition 8.1**.**
Let 1≤k≤n and 1≤i1<…<ik≤n.
Then the (i1,…,ik)-component of this cycle in C~(αi1)∗⊗⋯⊗C~(αik)∗⊂C(αi1)∗⊗⋯⊗C(αik)∗ is positive.
Mapping the resulting positive classes in H∗(BGαi1×⋯×BGαik;Z) to H∗(BΓ;Z) by the canonical subgroup inclusions this implies that h∈H∗(BΓ;Z) is positive, finishing the proof of Theorem 1.6.
It is enough to deal with the case k=n, the other components of h are treated in an analogous fashion.
For this aim let c∈C~(α1)∗⊗⋯⊗C~(αn)∗ represent the corresponding component of h.
Let 1≤n′≤n be maximal with αn′=α1, that is α1=⋯=αn′<αn′+1≤⋯≤αn.
We set Γ′:=(Gα1)n′, regarded as a subgroup of Γ in the obvious way.
By Proposition 6.2 we may assume that c is a linear combination of special cycles
[TABLE]
We write
[TABLE]
where c′ is a linear combination of special cycles in (C~(α1)∗)n′ and R is a linear combination of special cycles
[TABLE]
such that ij≥n′+1 or there exists 1≤μ≤n−j with sμ≥n′+1 and dμ≥2.
By Proposition 6.9(ii) and Corollary 5.5(i) the cycle R∈C~(α1)∗⊗⋯⊗C~(αn)∗⊂C(α1)∗⊗⋯⊗C(αn)∗ is positive.
For completing the proof of the positivity of c it hence remains to show that also the cycle c′∈(C~(α1)∗)n′⊂(C(α1)∗)n′ is positive.
We will argue that by the results of Section 7 the cycle c′ is positive modulo some p-divisible, p-atoral cycle, which can then be dealt with by Proposition 6.9(i).
The next lemma ensures the crucial property of c′ needed for this argument.
Lemma 8.2**.**
We have [c′]∈RH∗(BΓ′;Z/pα1).
Proof.
Since [c′] lifts to an integral class it lies in the kernel of the Bockstein operation β(α1):H∗(BΓ′;Z/pα1)→H∗(BΓ′;Fp).
In the remainder of this proof we will work with coefficients Z/pα1.
It remains to show that ∂(κ,α1)(c′)=0∈(C(α1)∗)n′ for all κ≥1.
Since by Proposition 7.5 the cycle c0 is not hit by a differential ∂(κ,α1) it is sufficient to show this vanishing property after projection to (C~(α1)∗)n′.
The class [c]∈H∗(C~(α1)∗⊗⋯⊗C~(αn)∗)≅H~∗(BΓ) is equal to the image of h under the projection BΓ→BΓ.
Since h lifts to Ω∗SO(BΓ) we conclude that ∂(κ,α1)(c)=0∈C~(α1)∗⊗⋯⊗C~(αn)∗.
(Recall that αn′+1,…,αn>α1 and we use coefficients Z/pα1.)
Since ∂(κ,α1) acts as a derivation and trivially on c1(s) for n′+1≤s≤n, the claim ∂(κ,α1)(c′)=0∈(C~(α1)∗)n′ therefore follows from the assertion
[TABLE]
In order to show this assertion let τ be one of the special cycles appearing in R.
The following computations are based on Proposition 7.5 with ℓ=α1 and α∈{α1,…,αn}.
If there exists a 1≤μ≤n−j with sμ≥n′+1 and dμ≥2, then ∂(κ,α1)(τ)∈S∗, as ∂(κ,α1) acts as a derivation and ∂(κ,α1)(c2dμ−1(sμ))=0.
We will now consider the case ij≥n′+1.
By definition
[TABLE]
We distinguish the following cases:
•
Let 1≤iγ≤n′.
Since αij>α1, hence ∂(κ,α1)(c2mj(ij))=0, we see that
[TABLE]
is a sum of elementary tensors each of which contains a component c2mj(ij).
•
Let n′+1≤iγ≤n.
Then αiγ−αi1≥1 and
[TABLE]
We conclude ∂(κ,α1)(τ)∈S∗ in the case ij≥n′+1 as well, finishing the proof of Lemma 8.2.
∎
By Lemma 8.2 and Proposition 7.9 the image of [c′] in H∗(BΓ′;Fp) is a linear combination of generalized products of Z/pα1-lens spaces L2m1−1×⋯×L2mk−1→BΓ′ for 1≤k≤n′.
The cycle R occurring in (16) is p-atoral, since each summand is of degree larger than n and p is odd.
Since also c is p-atoral we conclude that c′∈(C(α1)∗)n′ is p-atoral (here we use again that αn′+1,…,αn>α1).
We can therefore assume that in the generalized products of lens spaces appearing before the case m1=…=mk=1 does not occur.
In summary, modulo some p-atoral positive cycle (represented by a linear combination of generalized products of lens spaces) we can assume that c′ is a p-atoral cycle in (C~(α1)∗)n′⊂(C(α1)∗)n′ that maps to 0∈H∗(BΓ′;Fp).
Since H∗(BΓ′;Z)⊗Fp→H∗(BΓ′;Fp) is injective we get [c′]=p⋅[ξ] for a cycle ξ∈(C~(α1)∗)n′.
According to Proposition 6.2 we can assume that ξ is a linear combination of special cycles, and hence p⋅ξ is a linear combination of cycles
[TABLE]
Proposition 6.9(i) implies that such cycles are positive in (C(α1)∗)n′ whenever j≥2.
Since these cycles are also p-atoral for j≥2 (for p-odd) we can assume that p⋅ξ is a linear combination of cycles c2d1−1⊗⋯⊗c2dn′−1 with at least one di≥2 (by p-atorality of c′).
This shows that p⋅ξ, and hence c′ are positive.
In summary we have shown that c∈C~(α1)∗⊗⋯⊗C~(αn)∗⊂C(α1)∗⊗⋯⊗C(αn)∗ is positive, finishing the proof of Proposition 8.1 and hence of Theorem 1.6.