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arXiv:2606.06299v2 [math.GT] 08 Jun 2026

Smooth stable isotopy of topologically isotopic surfaces

Daniel Galvin Address: Department of Mathematics, University of Texas at Austin, USA Email address: daniel.galvin@austin.utexas.edu , Patrick Orson Address: Mathematics Department, California Polytechnic State University, USA Email address: porson@calpoly.edu and Mark Powell Address: School of Mathematics and Statistics, University of Glasgow, United Kingdom Email address: mark.powell@glasgow.ac.uk
Abstract.

A stabilisation of a 44-manifold XX is the connected sum of XX with some number of copies of S2×S2S^{2}\times S^{2}. If two smooth surfaces in a 44-manifold are topologically isotopic, we investigate whether they must moreover be smoothly isotopic in some stabilisation of XX. We prove this result holds whenever the surfaces are trivial in the /2\mathbb{Z}/2-homology of XX. We also produce a large class of fundamental groups of the ambient 44-manifold for which the result holds; this class includes free products of classical knot groups and, in particular, free groups.

Key words and phrases: 
4-manifolds, topologically isotopic surfaces, external stable isotopy
1991 Mathematics Subject Classification
57K40. 57N35.

1. Introduction

A stabilisation of a smooth, compact, connected, orientable 44-manifold XX is the effect of taking the connected sum of XX with some number of copies of S2×S2S^{2}\times S^{2}. Topological results about 44-manifolds sometimes become true smoothly, after stabilisation. In the most famous instance, results of Wall [25, 26] in the simply-connected case and Gompf [13], generally, show that homeomorphic closed, orientable, smooth 44-manifolds are stably diffeomorphic.

In some cases, a similar phenomenon is known to occur for isotopy classes of self-maps of a 44-manifold. Given g1g\geq 1 and a diffeomorphism f:XXf\colon X\to X, one may assume after isotopy that ff fixes a 44-ball, use that to form the connected sum X#g(S2×S2)X\#g(S^{2}\times S^{2}), then extend ff by the identity, to get a diffeomorphism of this stabilisation of XX. We call this a stabilisation of ff. When XX is closed and simply-connected, Kreck [16] and Quinn [20] (cf. [8]) showed that topologically isotopic diffeomorphisms of XX are stably smoothly isotopic. Results of Krannich–Kupers [15] and Gabai [9] combine to extend this to the case of free fundamental group, and Orson–Powell–Randal-Williams [17] further extend this to a larger class of fundamental groups. It remains open whether this result holds for every compact 44-manifold.

Here is a natural variant of the stabilisation question for embedded surfaces.

Question 1.1.

If two smooth surfaces Σ1,Σ2X\Sigma_{1},\Sigma_{2}\subseteq X are topologically isotopic, are they necessarily smoothly isotopic in some stabilisation of XX?

The first named author provided a positive answer in the case that π1(X)\pi_{1}(X) is trivial [11]*Theorem 1.2. Our main result gives a positive answer for some cases in which XX is not simply-connected. The question remains open, in general.

Let XX be a smooth, orientable, compact 44-manifold and write π:=π1(X)\pi:=\pi_{1}(X). Suppose Σ1,Σ2X\Sigma_{1},\Sigma_{2}\subseteq X are smooth, compact, proper surfaces with Σ1=Σ2\partial\Sigma_{1}=\partial\Sigma_{2}.

Theorem A.

Suppose at least one of the following holds.

  1. (i)

    For every connected component Σ1j\Sigma_{1}^{j} of Σ1\Sigma_{1}, and for every xH2(X,/2)x\in H_{2}(X;\mathbb{Z}/2), we have that λ/2(x,[Σ1j])=0/2\lambda^{\mathbb{Z}/2}(x,[\Sigma_{1}^{j}])=0\in\mathbb{Z}/2.

  2. (ii)

    The component I2:H2(π,(2))L6(π)(2)I_{2}\colon H_{2}(\pi;\mathbb{Z}_{(2)})\to L_{6}(\mathbb{Z}\pi)_{(2)} of the algebraic assembly map is zero, there is no 2-torsion in H1(π,)H_{1}(\pi;\mathbb{Z}), and Wh2(π)=0\Wh_{2}(\pi)=0.

Then if Σ1\Sigma_{1} and Σ2\Sigma_{2} are topologically isotopic rel. boundary, they are smoothly isotopic rel. boundary in some stabilisation of XX.

In A, we are not assuming XX is closed, and we are not assuming the surfaces are orientable. Observe that in (i), even if Σ1j\Sigma_{1}^{j} is closed, we can still consider it as a homology class in H2(X,X,/2)H_{2}(X,\partial X;\mathbb{Z}/2). We write

λ/2:H2(X,/2)×H2(X,X,/2)/2\lambda^{\mathbb{Z}/2}\colon H_{2}(X;\mathbb{Z}/2)\times H_{2}(X,\partial X;\mathbb{Z}/2)\to\mathbb{Z}/2

for the /2\mathbb{Z}/2-intersection pairing of XX. Note that the condition in (i) holds automatically if each connected component of Σ1\Sigma_{1} is trivial in H2(X,X,/2)H_{2}(X,\partial X;\mathbb{Z}/2).

The technical hypotheses on the fundamental group in A (ii) arise from an application of [17]*Corollary E. As discussed in [17]*loc.  cit., these conditions on π\pi are known to hold for free products of knot groups.

We record these observations in the following corollary to A.

Corollary 1.2.

Suppose at least one of the following holds.

  1. (i)

    For every connected component Σ1j\Sigma_{1}^{j} of Σ1\Sigma_{1}, we have that [Σ1j]=0H2(X,X,/2)[\Sigma_{1}^{j}]=0\in H_{2}(X,\partial X;\mathbb{Z}/2).

  2. (ii)

    The fundamental group π\pi is a free product of classical knot groups.

Then if Σ1\Sigma_{1} and Σ2\Sigma_{2} are topologically isotopic rel. boundary, they are smoothly isotopic rel. boundary in some stabilisation of XX.

Remark 1.3.

Cha–Kim [6] showed that given a locally flat surface ΣX\Sigma\subseteq X there exists some stabilisation of XX in which Σ\Sigma is topologically isotopic to a smooth surface. The Cha–Kim result can be viewed as a stable existence statement and A and Corollary 1.2 can be viewed as stable uniqueness counterparts, where they apply.

Outline of the proof

Here is a brief summary of the strategy for the proof, which doubles as a description of the organisation of the paper.

  • In Section 2, we begin with a homeomorphism of XX sending Σ1\Sigma_{1} to Σ2\Sigma_{2}, that is topologically isotopic rel. boundary to the identity. We show, following [11], that such a homeomorphism is always smoothable near Σ1\Sigma_{1}. Again following [11], we introduce the Casson-Sullivan obstruction to stably smoothing the homeomorphism on the exterior of Σ1\Sigma_{1}. We prove a naturality property and analyse the obstruction in our surface exterior case.

  • In Section 3, we modify the given homeomorphism to a stably smoothable one, and thus achieve a diffeomorphism sending Σ1\Sigma_{1} to Σ2\Sigma_{2} in some stabilisation of XX. This is achieved by use of the first-named author’s stable realisation of the Casson-Sullivan invariant [11].

  • In Section 4, we show that this diffeomorphism can be chosen in such a way that it is topologically pseudo-isotopic to the identity (Definition 2.4).

  • In Section 5, we consider conditions under which the topological pseudo-isotopy can be replaced by a smooth pseudo-isotopy. For this we analyse a smoothing obstruction for topological pseudo-isotopies introduced by Orson–Powell–Randal-Williams [17]. The hypotheses (i) and (ii) of A are used in this section.

  • In Section 6, we complete the proof. Following a careful analysis involving the Wh2\Wh_{2} group, we are able to appeal to a result of Singh [22] to obtain a diffeomorphism of XX sending Σ1\Sigma_{1} to Σ2\Sigma_{2}, that by a theorem of Gabai [9]*Theorem 2.5 is smoothly stably isotopic rel. boundary to the identity.

Discussion of the proof

The first named author’s proof [11]*Theorem 1.2 of our main result in the case that XX is simply connected effectively relies on the fact that diffeomorphisms of simply-connected 4-manifolds are classified up to smooth pseudo-isotopy [16, 21, 18]. Outside of the simply connected setting, such a classification is only known when π1(X)\pi_{1}(X)\cong\mathbb{Z}, topologically, by Stong–Wang [23], and smoothly, by combining [23] with [17]. Thus this proof strategy is quite limited, given the current state of knowledge.

Despite this, our main result allows many more fundamental groups. Indeed, A (i) holds for completely general finitely presented fundamental groups. So the most surprising aspect of our proof is that we are able to circumvent this lack of a pseudo-isotopy classification and achieve the outcome of Section 4: the existence of a diffeomorphism sending Σ1\Sigma_{1} to Σ2\Sigma_{2}, in some stabilisation of XX, that is topologically pseudo-isotopic to the identity.

How is this achieved? One starts with a homeomorphism of XX sending Σ1\Sigma_{1} to Σ2\Sigma_{2} that is topologically isotopic to the identity and wishes to modify the homeomorphism to smooth it to a diffeomorphism, at the expense of stabilising. The obstruction is the Casson–Sullivan invariant, and the danger is that in modifying the homeomorphism to kill this obstruction, we lose control of the topological pseudo-isotopy class of the eventual diffeomorphism, which should remain topologically pseudo-isotopic to the identity (or else we have essentially jettisoned the initial hypothesis of the proof). The key technical step to retain control is Proposition 2.13, in which we show that, to kill the Casson–Sullivan invariant, it is only necessary to modify the original homeomorphism in a neighbourhood of a union of meridians of Σ1\Sigma_{1}. As a consequence, the change can be localised to a simply connected codimension zero submanifold of X#WkX\#W_{k}, whereupon we can apply the Orson-Powell [18] topological isotopy classification for homeomorphisms of simply-connected 4-manifolds with boundary. We thus obtain a topological isotopy from the original homeomorphism, and hence also from the identity, to the one with trivial Casson–Sullivan invariant. The latter is stably topologically pseudo-isotopic to a diffeomorphism, leading to the desired stable topological pseudo-isotopy from this diffeomorphism to the identity.

Remark on a special case

As mentioned above, the case of Theorem A when π1(X)={1}\pi_{1}(X)=\{1\} was first proved in [11]*Theorem 1.2. In the further special case of π1(XΣi)={1}\pi_{1}(X\setminus\Sigma_{i})=\{1\} (which implies π1(X)=1\pi_{1}(X)=1), there is an alternative proof that uses work of Gompf [13], Boyer [3], Saeki [21], and Quinn [20] (with the correction in [8]). We detail this proof in Appendix A, for the interested reader.

The existence of such an alternative proof, based on existing results, was suggested in the introduction of [2], where it was asserted that the combination of work of Wall [25], Perron [19], and Quinn [20] would show homologous 22-spheres with simply-connected complement are topologically isotopic, and become smoothly isotopic in some stabilisation. Such a proof was again suggested, this time for general surfaces, in the introduction of [1]. Here it was asserted that the result would follow from Perron [19] and Quinn [20]. In neither case were any details given. In Remark A.2, we discuss that we do not believe such a proof would work using these citations, particularly without applying the results of Boyer [3] and Saeki [21].

Conventions

The following conventions and notation are used throughout.

  • For the remainder of the article, fix a smooth, orientable, compact 44-manifold XX, and denote π:=π1(X)\pi:=\pi_{1}(X).

  • A compact submanifold ΣX\Sigma\subseteq X is proper if the inclusion map ι:ΣX\iota\colon\Sigma\to X satisfies ι1(X)=Σ\iota^{-1}(\partial X)=\partial\Sigma. Note this adjective is meaningful when either of Σ\partial\Sigma and X\partial X are empty.

  • The symbol ν\nu applied to a subset CXC\subseteq X of a topological space means any open neighbourhood. If CXC\subseteq X is moreover a submanifold, we will use νC\nu C to specifically mean an open tubular neighbourhood and ν¯C\overline{\nu}C to denote a closed tubular neighbourhood. If C=XC=\partial X, then νC\nu C and ν¯C\overline{\nu}C denote open and closed boundary collars, respectively.

  • For the remainder of the article, fix Σ1,Σ2X\Sigma_{1},\Sigma_{2}\subseteq X smooth, proper surfaces with Σ1=Σ2\partial\Sigma_{1}=\partial\Sigma_{2}. The surfaces are permitted to be nonorientable. For i=1,2i=1,2, denote the surface exterior by Xi:=XνΣiX_{i}:=X\setminus\nu\Sigma_{i}.

  • Given a space AA and subspace BAB\subseteq A, a homotopy Ψ:A×IA\Psi\colon A\times I\to A is rel. BB if Ψ(x,t)=Ψ(x,0)\Psi(x,t)=\Psi(x,0) for all xBx\in B and tIt\in I.

  • We denote the connected sum of nn copies of S2×S2S^{2}\times S^{2} by Wn=n(S2×S2)W_{n}=n(S^{2}\times S^{2}).

Acknowledgements

We thank the Centre de Recherche Mathématiques at the Université de Montréal for hospitality during the 2025 thematic programme on ‘Topological and Geometric structures in low dimensions’, during which part of this paper was written. MP was a CRM-Simons Visiting Professor during this programme, and is grateful for the associated support. DG thanks the Max Planck Institute for Mathematics for support. Part of this research was also done while MP and DG were visiting the MPIM in Bonn. We warmly thank Simona Veselá for very helpful discussions about the result in the appendix.

2. The Casson-Sullivan invariant for a homeomorphism of surface exteriors

In this section we recall the Casson-Sullivan invariant; this is the relative Kirby-Siebenmann invariant of a homeomorphism [14] and is an obstruction to smoothing the homeomorphism. The terminology “Casson-Sullivan invariant” arose from the importance of this, as a triangulation obstruction, to the Manifold Hauptvermutung [5, 24]. In the context of 44-manifolds, the invariant was investigated by the first-named author in [11]. We discuss some elementary properties and then analyse the Casson-Sullivan invariant for a homeomorphism between surface exteriors that restricts to a diffeomorphism on the boundary.

2.1. The Casson-Sullivan invariant

We begin by recalling the general definition of the Casson-Sullivan invariant for 44-manifolds, and recap some elementary naturality properties.

For i=1,2i=1,2, let MiM_{i} be a smooth 44-manifold and let CiMiC_{i}\subseteq M_{i} be a closed subset. Suppose

F:(M1,C1)C0(M2,C1)F\colon(M_{1},C_{1})\xrightarrow{\cong_{C^{0}}}(M_{2},C_{1})

is a homeomorphism of pairs that restricts to a diffeomorphism

F|νC1:νC1CνC2F|_{\nu C_{1}}\colon\nu C_{1}\xrightarrow{\cong_{C^{\infty}}}\nu C_{2}

for some open neighbourhood νC1\nu C_{1} of C1M1C_{1}\subseteq M_{1}. Let σi\sigma_{i} denote the smooth structure on MiM_{i}. Consider M1×IM_{1}\times I and endow (M1×[0,ε))(νC1×I)(M_{1}\times[0,\varepsilon))\cup(\nu C_{1}\times I) with the smooth structure (σ1×std[0,ε))(σ1×stdI)(\sigma_{1}\times\mathrm{std}_{[0,\varepsilon)})\cup(\sigma_{1}\times\mathrm{std}_{I}). Endow M1×(1ε,1]M_{1}\times(1-\varepsilon,1] with the pullback smooth structure Fσ2×std(1ε,1]F^{*}\sigma_{2}\times\mathrm{std}_{(1-\varepsilon,1]}. As FF restricts to a diffeomorphism on νC1\nu C_{1} these structures are compatible on the overlap; we denote by Σ\Sigma the resulting smooth manifold (M1×[0,ε)(1ε,1])(νC1×I)(M_{1}\times[0,\varepsilon)\cup(1-\varepsilon,1])\cup(\nu C_{1}\times I). This smooth structure extends to all of M1×IM_{1}\times I if and only if the Kirby-Siebenmann obstruction

ks(M1×I,Σ)H4(M1×I,Σ,/2)\mathrm{ks}(M_{1}\times I,\Sigma)\in H^{4}(M_{1}\times I,\Sigma;\mathbb{Z}/2)

vanishes. Excision and the long exact sequence of the triple (M1×I,Σ,Σ(M1×[0,ε))CLOSE(M_{1}\times I,\Sigma,\Sigma\setminus(M_{1}\times[0,\varepsilon)) yield isomorphisms

(1) H3(M1,C1,/2)H3(Σ,Σ(M1×[0,ε)),/2)H4(M1×I,Σ,/2).H^{3}(M_{1},C_{1};\mathbb{Z}/2)\cong H^{3}(\Sigma,\Sigma\setminus(M_{1}\times[0,\varepsilon));\mathbb{Z}/2)\xrightarrow{\cong}H^{4}(M_{1}\times I,\Sigma;\mathbb{Z}/2).

We explain the two isomorphisms.

  • For the first map, we consider the maps of pairs

    (M1,C1)(M1×[0,ε)(C1×I),C1×[ε,1])(Σ,Σ(M1×[0,ε))CLOSE.(M_{1},C_{1})\leftarrow(M_{1}\times[0,\varepsilon)\cup(C_{1}\times I),C_{1}\times[\varepsilon,1])\to(\Sigma,\Sigma\setminus(M_{1}\times[0,\varepsilon)).

    The leftwards map is by definition projection, and is a homotopy equivalence of pairs. The rightwards map is an inclusion of pairs, and corresponds to excising (M1C1)×(1ε,1](M_{1}\setminus C_{1})\times(1-\varepsilon,1]. Thus both maps induce isomorphisms on cohomology, leading to the left isomorphism in (1).

  • The second map is an isomorphism because, in the long exact sequence of the triple, the other terms are

    Hk(M1×I,Σ(M1×[0,ε);/2)Hk(M1×I,M1;/2)=0H^{k}(M_{1}\times I,\Sigma\setminus(M_{1}\times[0,\varepsilon);\mathbb{Z}/2)\cong H^{k}(M_{1}\times I,M_{1};\mathbb{Z}/2)=0

    for k=3,4k=3,4.

Definition 2.1.

With notation as above, the Casson-Sullivan invariant of FF relative to νC1\nu C_{1} is the element

cs(F rel. νC1)H3(M1,C1,/2)\mathrm{cs}(\text{$F$ rel.~$\nu C_{1}$})\in H^{3}(M_{1},C_{1};\mathbb{Z}/2)

mapping to ks(M1×I,Σ)\mathrm{ks}(M_{1}\times I,\Sigma) under the sequence of isomorphisms (1).

In the case that the subsets CiMiC_{i}\subseteq M_{i} are submanifolds, the neighbourhoods νCi\nu C_{i} are by convention tubular neighbourhoods, and are thus unique. Similarly, if Ci=MiC_{i}=\partial M_{i} then the neighbourhoods are unique, by uniqueness of boundary collars. So in these cases the resulting Casson-Sullivan invariant is independent of the choice of open neighbourhoods, and thus we can write

cs(F rel. C1):=cs(F rel. νC1)H3(M1,C1,/2).\mathrm{cs}(\text{$F$ rel.~$C_{1}$}):=\mathrm{cs}(\text{$F$ rel.~$\nu C_{1}$})\in H^{3}(M_{1},C_{1};\mathbb{Z}/2).
Definition 2.2.

When F:M1M2F\colon M_{1}\to M_{2} is a homeomorphism restricting to a diffeomorphism on the boundary, we write

cs(F):=cs(F rel. M1)H3(M1,M1,/2),\mathrm{cs}(F):=\mathrm{cs}(\text{$F$ rel.~$\partial M_{1}$})\in H^{3}(M_{1},\partial M_{1};\mathbb{Z}/2),

and call this simply the Casson-Sullivan invariant of FF.

We recall our notation for connected sums of S2×S2S^{2}\times S^{2} from the conventions in Section 1.

Definition 2.3.

We denote the connected sum of nn copies of S2×S2S^{2}\times S^{2} by Wn:=n(S2×S2)W_{n}:=n(S^{2}\times S^{2}).

In order to state a key property of the Casson-Sullivan invariant, we need the following definition.

Definition 2.4.

Let CAT{Diff,Top}\mathrm{CAT}\in\{\mathrm{Diff},\mathrm{Top}\}, let M1,M2M_{1},M_{2} be compact, smooth 4-manifolds, and let F,G:M1M2F,G\colon M_{1}\to M_{2} be CAT\mathrm{CAT}-isomorphisms that agree on the boundary G|M1=F|M1G|_{\partial M_{1}}=F|_{\partial M_{1}}.

  1. (i)

    We say that FF and GG are CAT\mathrm{CAT} pseudo-isotopic if there is a CAT\mathrm{CAT}-isomorphism

    Ψ:M1×ICATM2×I\Psi\colon M_{1}\times I\xrightarrow{\cong_{\mathrm{CAT}}}M_{2}\times I

    with F=Ψ|M1×{0}F=\Psi|_{M_{1}\times\{0\}}, G=Ψ|M1×{1}G=\Psi|_{M_{1}\times\{1\}} and such that the restriction of Ψ\Psi to M1×I\partial M_{1}\times I is the product isotopy Ψ(x,t)=(F(x),t)\Psi(x,t)=(F(x),t).

  2. (ii)

    We say that FF and GG are CAT\mathrm{CAT} stably pseudo-isotopic if there exists k0k\geq 0 and there exist stabilisations F#IdWkF\#\operatorname{Id}_{W_{k}} and G#IdWkG\#\operatorname{Id}_{W_{k}} that are CAT\mathrm{CAT} pseudo-isotopic CAT\mathrm{CAT}-isomorphisms.

Remark 2.5.

Our conventions listed in Section 1 state that isotopies need not be rel. boundary, and will always be explicitly specified to be so when needed. Note, in contrast, that pseudo-isotopies are always rel. boundary, in our definition.

Here is a key property of the Casson-Sullivan invariant that we will require later; for a proof see [11]*Proposition 2.19, Proposition 2.23.

Proposition 2.6 ([7]*Theorem 8.6(2)).

Let F:M1M2F\colon M_{1}\to M_{2} be homeomorphism of compact, smooth 4-manifolds, that restricts to a diffeomorphism on the boundary. We have that cs(F)=0\mathrm{cs}(F)=0 if and only if FF is smoothly stably pseudo-isotopic to a diffeomorphism.

We will also use the following, essentially formal, naturality statement for the Casson–Sullivan invariant.

Lemma 2.7.

Let F:(M1,C1)(M2,C2)F\colon(M_{1},C_{1})\to(M_{2},C_{2}) be a homeomorphism of pairs, where for i=1,2i=1,2, MiM_{i} is a smooth 4-manifold and CiC_{i} is a closed subset. Suppose that FF restricts to a diffeomorphism on some open neighbourhoods νC1νC2\nu C_{1}\to\nu C_{2}. Let (Vi,Di)(Mi,Ci)(V_{i},D_{i})\subseteq(M_{i},C_{i}) be an inclusion of pairs where ViV_{i} is an open codimension zero submanifold and DiCiD_{i}\subseteq C_{i} is also closed. Assume that FF restricts to a homeomorphism (V1,D1)(V2,D2)(V_{1},D_{1})\to(V_{2},D_{2}). Write νD1νC1\nu D_{1}\subseteq\nu C_{1} for some open neighbourhood and νD2\nu D_{2} for its image under FF. Then under the inclusion (V1,D1)(M1,C1)(V_{1},D_{1})\subseteq(M_{1},C_{1}) we have

H3(M1,C1)H3(V1,D1);cs(F rel. νC1)cs(F|V1 rel. νD1).H^{3}(M_{1},C_{1})\to H^{3}(V_{1},D_{1});\qquad\mathrm{cs}(\text{$F$ rel.~$\nu C_{1}$})\mapsto\mathrm{cs}(\text{$F|_{V_{1}}$ rel.~$\nu D_{1}$}).
Proof.

Given F:(M1,C1)(M2,C2)F\colon(M_{1},C_{1})\to(M_{2},C_{2}), to define the Casson-Sullivan invariant cs(F rel. νC1)\mathrm{cs}(\text{$F$ rel.~$\nu C_{1}$}), at the beginning of Section 2.1, we first built a smooth structure on the open submanifold

(M1×[0,ε)(1ε])(νC1×I)M1×I.(M_{1}\times[0,\varepsilon)\cup(1-\varepsilon])\cup(\nu C_{1}\times I)\subseteq M_{1}\times I.

In this proof we will denote that smooth manifold by ΣCM1×I\Sigma_{C}\subseteq M_{1}\times I. Following the similar construction for F|V1:(V1,D1)(V2,D2)F|_{V_{1}}\colon(V_{1},D_{1})\to(V_{2},D_{2}), we obtain a smooth structure on the open submanifold

(V1×[0,ε)(1ε])(νD1×I)V1×I,(V_{1}\times[0,\varepsilon)\cup(1-\varepsilon])\cup(\nu D_{1}\times I)\subseteq V_{1}\times I,

which we denote by ΣDV1×I\Sigma_{D}\subseteq V_{1}\times I. We thus have inclusions of open submanifolds

ΣD{\lx@inpgf@ignorespaces\Sigma_{D}}V1×I{\lx@inpgf@ignorespaces V_{1}\times I}ΣC{\lx@inpgf@ignorespaces\Sigma_{C}}M1×I{\lx@inpgf@ignorespaces M_{1}\times I}

As the relative Kirby-Siebenmann invariant is natural under such maps [14]*Essay IV, Theorem 10.1, this induces

H4(M1×I,ΣC)H4(V1×I,ΣD);ks(M1×I,ΣC)ks(V1×I,ΣD).H^{4}(M_{1}\times I,\Sigma_{C})\to H^{4}(V_{1}\times I,\Sigma_{D});\qquad\mathrm{ks}(M_{1}\times I,\Sigma_{C})\mapsto\mathrm{ks}(V_{1}\times I,\Sigma_{D}).

Finally, the isomorphisms described in (1) induce the corresponding isomorphisms for the pair (V1×I,ΣD)(V_{1}\times I,\Sigma_{D}), upon restriction, so that the following commutes

H3(V1,D1,/2){\lx@inpgf@ignorespaces H^{3}(V_{1},D_{1};\mathbb{Z}/2)}H3(ΣD,ΣD(V1×[0,ε)),/2){\lx@inpgf@ignorespaces H^{3}(\Sigma_{D},\Sigma_{D}\setminus(V_{1}\times[0,\varepsilon));\mathbb{Z}/2)}H4(V1×I,ΣD,/2){\lx@inpgf@ignorespaces H^{4}(V_{1}\times I,\Sigma_{D};\mathbb{Z}/2)}H3(M1,C1,/2){\lx@inpgf@ignorespaces H^{3}(M_{1},C_{1};\mathbb{Z}/2)}H3(ΣC,ΣC(M1×[0,ε)),/2){\lx@inpgf@ignorespaces H^{3}(\Sigma_{C},\Sigma_{C}\setminus(M_{1}\times[0,\varepsilon));\mathbb{Z}/2)}H4(M1×I,ΣC,/2){\lx@inpgf@ignorespaces H^{4}(M_{1}\times I,\Sigma_{C};\mathbb{Z}/2)}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}

Thus under the inclusion (V1,D1)(M1,C1)(V_{1},D_{1})\subseteq(M_{1},C_{1}) we have

H3(M1,C1)H3(V1,D1);cs(F rel. νC1)cs(F|V1 rel. νD1),H^{3}(M_{1},C_{1})\to H^{3}(V_{1},D_{1});\qquad\mathrm{cs}(\text{$F$ rel.~$\nu C_{1}$})\mapsto\mathrm{cs}(\text{$F|_{V_{1}}$ rel.~$\nu D_{1}$}),

which completes the proof. ∎

2.2. Casson-Sullivan for the surface exteriors

Recall that XX is a fixed smooth, orientable, compact 44-manifold and Σ1,Σ2X\Sigma_{1},\Sigma_{2}\subseteq X are smooth, proper surfaces with Σ1=Σ2\partial\Sigma_{1}=\partial\Sigma_{2}.

Definition 2.8.

We say a homeomorphism of pairs

F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2)\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2})

is smooth near Σ1\Sigma_{1} if the restriction

F^|ν¯Σ1:ν¯Σ1Cν¯Σ2\widehat{F}|_{\overline{\nu}\Sigma_{1}}\colon\overline{\nu}\Sigma_{1}\xrightarrow{\cong_{C^{\infty}}}\overline{\nu}\Sigma_{2}

is a diffeomorphism sending Σ1\Sigma_{1} to Σ2\Sigma_{2}.

Notation 2.9.

Given a homeomorphism that is smooth near Σ1\Sigma_{1}

F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2),\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}),

for i=1,2i=1,2, write

F:X1X2,where F:=F^|X1F\colon X_{1}\to X_{2},\quad\text{where~$F:=\widehat{F}|_{X_{1}}$}

(recall that Xi:=XνΣiX_{i}:=X\setminus\nu\Sigma_{i}). Note that F|X1F|_{\partial X_{1}} is a diffeomorphism.

We now recall that a homeomorphism sending Σ1\Sigma_{1} to Σ2\Sigma_{2} can always be smoothed near the surfaces. For this we will use that the surfaces ΣiX\Sigma_{i}\subseteq X and their closed tubular neighbourhoods ν¯Σi\overline{\nu}\Sigma_{i} are already smooth submanifolds of XX.

Lemma 2.10.

Suppose we are given a homeomorphism

F^:XC0X\widehat{F}^{\prime}\colon X\xrightarrow{\cong_{C^{0}}}X

such that F^(Σ1)=(Σ2)\widehat{F}^{\prime}(\Sigma_{1})=(\Sigma_{2}). Then F^\widehat{F}^{\prime} is topologically isotopic rel. boundary to a homeomorphism that is smooth near Σ1\Sigma_{1}

F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2),\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}),
Proof.

This was proved in [11]*Lemma 5.3, and we refer the reader to there for full details. We provide a sketch for convenience. Smooth F^|Σ1\widehat{F}^{\prime}|_{\Sigma_{1}} using that homeomorphisms of surfaces are smoothable, and extend using isotopy extension. By uniqueness of tubular neighbourhoods [7]*Theorem 9.3, we can further isotope to a homeomorphism sending a smooth tubular neighbourhood of Σ1\Sigma_{1} to a smooth tubular neighbourhood of Σ2\Sigma_{2}, via a D2D^{2}-bundle (with SO(2)\mathrm{SO}(2) structure group) isomorphism covering a diffeomorphism. As shown in [11]*Lemma 5.3, such a bundle isomorphism can be fibrewise isotoped so as to give a diffeomorphism between the total spaces. ∎

We will need the following notation for the cornered structure of the surface exteriors.

Notation 2.11.

For i=1,2i=1,2, the exterior XiX_{i} is a manifold with corners, where

Xi=0Xi101XiXi,defined by0Xi:=XiX,\partial X_{i}=\partial_{0}X_{i}\cup_{\partial_{01}X_{i}}\partial_{1}X_{i},\qquad\text{defined by}\qquad\partial_{0}X_{i}:=\partial X_{i}\cap\partial X,

so that 1Xi\partial_{1}X_{i} is the total space of the sphere bundle of the normal bundle to Σi\Sigma_{i}. The total space of the disc bundle to Σi\Sigma_{i} is also a manifold with corners, where

ν¯Σi=0ν¯Σi101ν¯Σiν¯Σi,defined by0ν¯Σi:=ν¯ΣiX,\partial\overline{\nu}\Sigma_{i}=\partial_{0}\overline{\nu}\Sigma_{i}\cup_{\partial_{01}\overline{\nu}\Sigma_{i}}\partial_{1}\overline{\nu}\Sigma_{i},\qquad\text{defined by}\qquad\partial_{0}\overline{\nu}\Sigma_{i}:=\partial\overline{\nu}\Sigma_{i}\cap\partial X,

so that 1ν¯Σi=1Xi\partial_{1}\overline{\nu}\Sigma_{i}=\partial_{1}X_{i} and 01ν¯Σi=01Xi\partial_{01}\overline{\nu}\Sigma_{i}=\partial_{01}X_{i}. There is then a decomposition of XX into manifolds with corners

X=Xi1Xiν¯Σi,withX=0Xi0ν¯Σi.X=X_{i}\cup_{\partial_{1}X_{i}}\overline{\nu}\Sigma_{i},\qquad\text{with}\qquad\partial X=\partial_{0}X_{i}\cup\partial_{0}\overline{\nu}\Sigma_{i}.

This is depicted schematically in Figure 1.

01Xi\partial_{01}X_{i}01Xi\partial_{01}X_{i}XiX_{i}ν¯Σi\overline{\nu}\Sigma_{i}1Xi=1ν¯Σi\partial_{1}X_{i}=\partial_{1}\overline{\nu}\Sigma_{i}0Xi\partial_{0}X_{i}0ν¯Σi\partial_{0}\overline{\nu}\Sigma_{i}YY
Figure 1. Left: a schematic for the decomposition of XX as described in 2.11. Right: the closed subspace YY used in the proof of Proposition 2.13.

We now wish to analyse the Casson-Sullivan invariant of a homeomorphism F:X1X2F\colon X_{1}\to X_{2} that restricts to a diffeomorphism on the boundary.

Definition 2.12.

Given a connected component ΣijΣi\Sigma_{i}^{j}\subseteq\Sigma_{i}, a meridian to that component is a simple closed curve in 1ν¯Σij\partial_{1}\overline{\nu}\Sigma_{i}^{j} that is the boundary of a D2D^{2}-fibre in a tubular neighbourhood of Σij\Sigma_{i}^{j}. Note that by uniqueness of tubular neighbourhoods, any two such curves are homologous in H1(1ν¯Σij,/2)H_{1}(\partial_{1}\overline{\nu}\Sigma_{i}^{j};\mathbb{Z}/2).

The following technical lemma shows that the Casson-Sullivan invariant of FF is governed by the /2\mathbb{Z}/2-homology classes of meridians.

Proposition 2.13.

Suppose F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2)\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}) is a homeomorphism that is smooth near Σ1\Sigma_{1}, and that moreover F^\widehat{F} is topologically isotopic rel. boundary to a diffeomorphism. Then the class PD(cs(F))\mathrm{PD}(\mathrm{cs}(F)) is equal to j=1N[γj]\sum_{j=1}^{N}[\gamma_{j}] in H1(X1,/2)H_{1}(X_{1};\mathbb{Z}/2), for {γj}j=1N\{\gamma_{j}\}_{j=1}^{N} meridians to some collection of pairwise distinct connected components Σ1j\Sigma^{j}_{1} of Σ1\Sigma_{1}.

Proof.

Throughout this proof, /2\mathbb{Z}/2-coefficients in homology and cohomology are understood. For brevity, we write for i=1,2i=1,2

i:=iν¯Σ1,01:=01ν¯Σ1.\partial_{i}:=\partial_{i}\overline{\nu}\Sigma_{1},\quad\partial_{01}:=\partial_{01}\overline{\nu}\Sigma_{1}.

Define

Y=X1(ν¯Σ1)Y=\partial X_{1}\cup\partial(\overline{\nu}\Sigma_{1})

and take the specific open neighbourhood

νY:=ν(X1)ν((ν¯Σ1));\nu Y:=\nu(\partial X_{1})\cup\nu(\partial(\overline{\nu}\Sigma_{1}));

in other words, the union of an open boundary collar on X1\partial X_{1} and an open tubular neighbourhood of (ν¯Σ1)\partial(\overline{\nu}\Sigma_{1}). The closed subspace YY is depicted schematically in Figure 1. As F^\widehat{F} is topologically isotopic rel. boundary to a diffeomorphism, in particular it is a diffeomorphism upon restriction to X\partial X. This, together with the hypothesis that F^\widehat{F} is smooth near Σ1\Sigma_{1}, implies F^\widehat{F} may be assumed to be a diffeomorphism on νY\nu Y. This means there is a Casson-Sullivan invariant cs(F^ rel. νY)H3(X,Y)\mathrm{cs}(\text{$\widehat{F}$ rel.~$\nu Y$})\in H^{3}(X,Y).

We develop the following diagram, show that it commutes, and justify the claimed isomorphisms.

H2(Y,X){\lx@inpgf@ignorespaces H^{2}(Y,\partial X)}H3(X,Y){\lx@inpgf@ignorespaces H^{3}(X,Y)}H3(X1,X1)H3(ν¯Σ1,ν¯Σ1){\lx@inpgf@ignorespaces H^{3}(X_{1},\partial X_{1})\oplus H^{3}(\overline{\nu}\Sigma_{1},\partial\overline{\nu}\Sigma_{1})}H2(XX,XY){\lx@inpgf@ignorespaces H_{2}(X\setminus\partial X,X\setminus Y)}H1(XY){\lx@inpgf@ignorespaces H_{1}(X\setminus Y)}H1(X1X1)H1(ν¯Σ1){\lx@inpgf@ignorespaces H_{1}(X_{1}\setminus\partial X_{1})\oplus H_{1}(\overline{\nu}\Sigma_{1}\setminus\partial)}H1(101){\lx@inpgf@ignorespaces H_{1}(\partial_{1}\setminus\partial_{01})}H1(X1X)H1(ν¯Σ10){\lx@inpgf@ignorespaces H_{1}(X_{1}\setminus\partial X)\oplus H_{1}(\overline{\nu}\Sigma_{1}\setminus\partial_{0})}H1(X1)H1(ν¯Σ1){\lx@inpgf@ignorespaces H_{1}(X_{1})\oplus H_{1}(\overline{\nu}\Sigma_{1})}δ\scriptstyle{\lx@inpgf@ignorespaces\delta}PALD\scriptstyle{\lx@inpgf@ignorespaces\mathrm{PALD}}\scriptstyle{\lx@inpgf@ignorespaces\cong}PALD\scriptstyle{\lx@inpgf@ignorespaces\mathrm{PALD}}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}(PALD,PALD)\scriptstyle{\lx@inpgf@ignorespaces(\mathrm{PALD},\mathrm{PALD})}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\partial}\scriptstyle{\lx@inpgf@ignorespaces\cong}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}(k,)\scriptstyle{\lx@inpgf@ignorespaces(k_{*},\ell_{*})}\scriptstyle{\lx@inpgf@ignorespaces\cong}

In the top left square, the map δ\delta is the connecting map in the long exact sequence of the triple (X,Y,X)(X,Y,\partial X) and the map \partial is the connecting map in the long exact sequence of the triple (XX,XY,)(X\setminus\partial X,X\setminus Y,\emptyset). The downward maps denoted PALD\mathrm{PALD} are Poincaré-Alexander-Lefschetz duality isomorphisms [4, Theorem VI.8.3], given by cap product, applied with XX (or X1X_{1} or ν¯Σ1\overline{\nu}\Sigma_{1}) union an open exterior collar. The top left square commutes by [4, Lemma VI.8.1]; we note that Bredon only considers the case of a pair, but the proof readily extends to the case of a triple, as in our case.

For the lower left square, the right-most and lower maps are inclusion-induced. We postpone the definition of the map α\alpha and the proof that the square commutes to the upcoming Lemma 2.14. As the particulars are not relevant to this proof, we will proceed, assuming this map is defined and the square commutes. For future reference, the lemma applies, using

XX=(X1X)(ν¯Σ10)andXY=int(X1X)int(ν¯Σ10),X\setminus\partial X=(X_{1}\setminus\partial X)\cup(\overline{\nu}\Sigma_{1}\setminus\partial_{0})\quad\text{and}\quad X\setminus Y=\mathrm{int}(X_{1}\setminus\partial X)\sqcup\mathrm{int}(\overline{\nu}\Sigma_{1}\setminus\partial_{0}),

in the notation of that lemma.

The lower right square is all inclusion-induced and thus commutes. The inclusions are all from deformation retracts and thus all are isomorphisms.

In the top right square the horizontal arrows are inclusion-induced, and hence the square commutes by naturality of Poincaré-Alexander-Lefschetz duality. To see that the top arrow in this square is an isomorphism, consider that the Mayer-Vietoris sequence for

(X,Y)=(X1ν¯Σ1,X1ν¯Σ1)(X,Y)=\left(X_{1}\cup\overline{\nu}\Sigma_{1},\partial X_{1}\cup\partial\overline{\nu}\Sigma_{1}\right)

yields an isomorphism

H3(X,Y)H3(X1,X1)H3(ν¯Σ1,ν¯Σ1),H^{3}(X,Y)\xrightarrow{\cong}H^{3}(X_{1},\partial X_{1})\oplus H^{3}(\overline{\nu}\Sigma_{1},\partial\overline{\nu}\Sigma_{1}),

since the other terms in the long exact sequence are

Hn(X1ν¯Σ1,X1ν¯Σ1)=0H^{n}(X_{1}\cap\overline{\nu}\Sigma_{1},\partial X_{1}\cap\partial\overline{\nu}\Sigma_{1})=0

as X1ν¯Σ1=X1ν¯Σ1X_{1}\cap\overline{\nu}\Sigma_{1}=\partial X_{1}\cap\partial\overline{\nu}\Sigma_{1}.

Having established the diagram, we now use it to prove the lemma. The top right horizontal isomorphism in the diagram is induced by inclusions (X1,X1)(X,Y)(X_{1},\partial X_{1})\subseteq(X,Y) and (ν¯Σ1,ν¯Σ1)(X,Y)(\overline{\nu}\Sigma_{1},\partial\overline{\nu}\Sigma_{1})\subseteq(X,Y). We may now apply Lemma 2.7 to each of these inclusions. More precisely, in order to arrange that these are inclusions of open submanifolds, use open neighbourhoods ν(Xi)X\nu(X_{i})\subseteq X and ν(ν¯Σi)X\nu(\overline{\nu}{\Sigma_{i}})\subseteq X as the manifolds ViV_{i} in the respective applications of the lemma. We thus see that cs(F^ rel. νY)H3(X,Y)\mathrm{cs}(\text{$\widehat{F}$ rel.~$\nu Y$})\in H^{3}(X,Y) is mapped to

(cs(F),cs(F^|ν¯Σ1))H3(X1,X1)H3(ν¯Σ1,ν¯Σ1)(\mathrm{cs}(F),\mathrm{cs}(\widehat{F}|_{\overline{\nu}\Sigma_{1}}))\in H^{3}(X_{1},\partial X_{1})\oplus H^{3}(\overline{\nu}\Sigma_{1},\partial\overline{\nu}\Sigma_{1})

under this isomorphism. Since F^\widehat{F} is smooth on ν¯Σ1\overline{\nu}\Sigma_{1}, Lemma 2.10, implies that cs(F^|ν¯Σ1)=0\mathrm{cs}(\widehat{F}|_{\overline{\nu}\Sigma_{1}})=0, so in fact the image of cs(F^ rel. νY)H3(X,Y)\mathrm{cs}(\text{$\widehat{F}$ rel.~$\nu Y$})\in H^{3}(X,Y) is

(cs(F),0)H3(X1,X1)H3(ν¯Σ1,ν¯Σ1).(\mathrm{cs}(F),0)\in H^{3}(X_{1},\partial X_{1})\oplus H^{3}(\overline{\nu}\Sigma_{1},\partial\overline{\nu}\Sigma_{1}).

The top left horizontal map in the diagram is part of the long exact sequence of the triple (X,Y,X)(X,Y,\partial X) and we consider the subsequent map H3(X,Y)H3(X,X)H^{3}(X,Y)\to H^{3}(X,\partial X) in that long exact sequence (this map is not depicted in the diagram). Another application of Lemma 2.7 shows that the element cs(F^ rel. νY)\mathrm{cs}(\text{$\widehat{F}$ rel.~$\nu Y$}) maps to cs(F^)H3(X,X)\mathrm{cs}(\widehat{F})\in H^{3}(X,\partial X) under this subsequent map. As F^\widehat{F} is topologically isotopic rel. boundary to a diffeomorphism, we have cs(F^)=0\mathrm{cs}(\widehat{F})=0. Hence there exists some class dH2(Y,X)d\in H^{2}(Y,\partial X) mapping to cs(F^ rel. νY)H3(X,Y)\mathrm{cs}(\text{$\widehat{F}$ rel.~$\nu Y$})\in H^{3}(X,Y) along the top left horizontal map.

Sending dd clockwise around the boundary of the diagram to the bottom right corner gives (PD(cs(F)),0)H1(X1)H1(ν¯Σ1)(\mathrm{PD}(\mathrm{cs}(F)),0)\in H_{1}(X_{1})\oplus H_{1}(\overline{\nu}\Sigma_{1}). Here, we have used that one definition of Poincaré-Lefschetz duality is as the composition of the the right-most column of this diagram [4, § VI.9]. Now consider sending dd anti-clockwise around the diagram to the bottom right corner. Define e:=αPALD(d)H1(101)e:=\alpha\circ\mathrm{PALD}(d)\in H_{1}(\partial_{1}\setminus\partial_{01}). By commutativity of the diagram we have that the image of (ke,e)(k_{*}e,\ell_{*}e) in H1(X1)H1(ν¯Σ1)H_{1}(X_{1})\oplus H_{1}(\overline{\nu}\Sigma_{1}) is (PD(cs(F)),0)(\mathrm{PD}(\mathrm{cs}(F)),0). This shows that e=0\ell_{*}e=0, and we claim this is enough to show that ee is a sum of meridians of Σ1\Sigma_{1}. Given this, it follows that PD(cs(F))H1(X1)\mathrm{PD}(\mathrm{cs}(F))\in H_{1}(X_{1}), which equals the image of kek_{*}e under H1(X1X)H1(X1)H_{1}(X_{1}\setminus\partial X)\to H_{1}(X_{1}), is a sum of meridians. This completes the proof, modulo the claim.

It remains to prove the claim. For this consider the Leray–Serre spectral sequence for the fibration

S1(101)(Σ1Σ1).S^{1}\to(\partial_{1}\setminus\partial_{01})\to(\Sigma_{1}\setminus\partial\Sigma_{1}).

The E2E^{2} page is

Ep,q2Hp(Σ1Σ1,Hq(S1)).E^{2}_{p,q}\cong H_{p}(\Sigma_{1}\setminus\partial\Sigma_{1};H_{q}(S^{1})).

For p+q=1p+q=1 this leads to E1,0H1(Σ1Σ1)E^{\infty}_{1,0}\cong H_{1}(\Sigma_{1}\setminus\partial\Sigma_{1}) and

E0,1coker(d2,02:H2(Σ1Σ1)H0(Σ1Σ1;H1(S1))),E^{\infty}_{0,1}\cong\coker\big(d^{2}_{2,0}\colon H_{2}(\Sigma_{1}\setminus\partial\Sigma_{1})\to H_{0}(\Sigma_{1}\setminus\partial\Sigma_{1};H_{1}(S^{1}))\big),

where cokerd2,02\coker d^{2}_{2,0} is generated by meridians [γj][\gamma_{j}], j=1,,Nj=1,\dots,N, i.e. boundaries of D2D^{2}-fibres of a tubular neighbourhood, to a sub-collection of the connected components of Σ1Σ1\Sigma_{1}\setminus\partial\Sigma_{1}. We obtain a short exact sequence

0cokerd2,02H1(101)H1(Σ1Σ1)0.0\to\coker d^{2}_{2,0}\to H_{1}(\partial_{1}\setminus\partial_{01})\to H_{1}(\Sigma_{1}\setminus\partial\Sigma_{1})\to 0.

The right hand map factors as

H1(101)H1(ν¯Σ1)H1(Σ1Σ1).H_{1}(\partial_{1}\setminus\partial_{01})\to H_{1}(\overline{\nu}\Sigma_{1})\xrightarrow{\cong}H_{1}(\Sigma_{1}\setminus\partial\Sigma_{1}).

It follows that every element of the kernel of the map H1(101)H1(ν¯Σ1)H_{1}(\partial_{1}\setminus\partial_{01})\to H_{1}(\overline{\nu}\Sigma_{1}) is a sum of meridians j=1N[γj]\sum_{j=1}^{N}[\gamma_{j}], as desired. ∎

We now prove the lemma promised in the proof of Proposition 2.13.

Lemma 2.14.

If M=NNM=N\cup_{\partial}N^{\prime} is a union of nn-manifolds along their boundary N=N\partial N=\partial N^{\prime} then for all r0r\geq 0 there is a map α\alpha such that the following diagram commutes.

(2) Hr(M,N̊N̊,/2){\lx@inpgf@ignorespaces H_{r}(M,\mathring{N}\sqcup\mathring{N}^{\prime};\mathbb{Z}/2)}Hr1(N̊N̊,/2){\lx@inpgf@ignorespaces H_{r-1}(\mathring{N}\sqcup\mathring{N}^{\prime};\mathbb{Z}/2)}Hr1(N,/2){\lx@inpgf@ignorespaces H_{r-1}(\partial N;\mathbb{Z}/2)}Hr1(N,/2)Hr1(N,/2).{\lx@inpgf@ignorespaces H_{r-1}(N;\mathbb{Z}/2)\oplus H_{r-1}(N^{\prime};\mathbb{Z}/2).}\scriptstyle{\lx@inpgf@ignorespaces\partial}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}ι\scriptstyle{\lx@inpgf@ignorespaces\iota}(k,)\scriptstyle{\lx@inpgf@ignorespaces(k_{*},\ell_{*})}

Here, the bottom and right maps are inclusion-induced and \partial is the connecting map in the long exact sequence of the pair.

Proof.

Throughout this proof, /2\mathbb{Z}/2-coefficients in homology are understood. To begin, we make some abstract observations. For any space AA, the long exact sequence of the pair (A×[1,1],A×[1,0)(0,1])(A\times[-1,1],A\times[-1,0)\sqcup(0,1]) has the following portion.

Hr(A×[1,1])0Hr(A×[1,1],A×[1,0)(0,1])Hr1(A×[1,0))Hr1(A×(0,1])Hr1(A×{1})Hr1(A×{1})(i,i+)Hr1(A×[1,1]) \dots\to H_{r}(A\times[-1,1])\xrightarrow{0}H_{r}(A\times[-1,1],A\times[-1,0)\sqcup(0,1])\\ \xrightarrow{\partial}\underbrace{H_{r-1}(A\times[-1,0))\oplus H_{r-1}(A\times(0,1])}_{\cong\,{H_{r-1}(A\times\{-1\})\oplus H_{r-1}(A\times\{1\})}}\xrightarrow{(i_{-},i_{+})}H_{r-1}(A\times[-1,1])\to\dots{}

Identifying A=A×{±1}A=A\times\{\pm 1\}, the image of the connecting map is the diagonal subgroup

Δ:=Im()=ker(i+,i)={(x,x)|xHr1(A)}Hr1(A)Hr1(A).\Delta:=\operatorname{Im}(\partial)=\ker(i_{+},i_{-})=\{(x,x)\,|\,x\in H_{r-1}(A)\}\subseteq H_{r-1}(A)\oplus H_{r-1}(A).

Note that we have a canonical isomorphism Δ=Hr1(A)\Delta=H_{r-1}(A). In addition, (i+,i)(i_{+},i_{-}) is surjective, justifying the zero map displayed in our sequence. This shows that \partial is injective. Combining all this, \partial determines an isomorphism to the diagonal subgroup, which we will write as

β:Hr(A×[1,1],A×[1,0)(0,1])Hr1(A).\beta\colon H_{r}(A\times[-1,1],A\times[-1,0)\sqcup(0,1])\xrightarrow{\cong}H_{r-1}(A).

We turn to the proof of the lemma. We consider diagram (3) below; its purpose is to define the isomorphism α\alpha and to show that the topmost triangle commutes. The left vertical arrow is the excision isomorphism, where we excise M(N×[1,1])MM\setminus(\partial N\times[-1,1])\subseteq M, the complement of a closed tubular neighbourhood of N\partial N. The map (k,)(k^{\prime},\ell^{\prime}) is induced by the inclusion into each component of push-offs of N=N\partial N=\partial N^{\prime} into the respective interiors. The map β\beta was defined above, taking A=NA=\partial N, as was the down-and-right pointing inclusion map.

(3) Hr(M,N̊N̊){\lx@inpgf@ignorespaces H_{r}(M,\mathring{N}\sqcup\mathring{N}^{\prime})}Hr1(N̊N̊){\lx@inpgf@ignorespaces H_{r-1}(\mathring{N}\sqcup\mathring{N}^{\prime})}Δ=Hr1(N){\lx@inpgf@ignorespaces\Delta=H_{r-1}(\partial N)}Hr(N×[1,1],N×[1,0)(0,1]){\lx@inpgf@ignorespaces H_{r}(\partial N\times[-1,1],\partial N\times[-1,0)\sqcup(0,1])}Hr1(N×[1,0)(0,1]){\lx@inpgf@ignorespaces H_{r-1}(\partial N\times[-1,0)\sqcup(0,1])}\scriptstyle{\lx@inpgf@ignorespaces\partial}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\subseteq}(k,)\scriptstyle{\lx@inpgf@ignorespaces(k^{\prime}{,}\ell^{\prime})}\scriptstyle{\lx@inpgf@ignorespaces\partial}\scriptstyle{\lx@inpgf@ignorespaces\cong}exc\scriptstyle{\lx@inpgf@ignorespaces\mathrm{exc}}β\scriptstyle{\lx@inpgf@ignorespaces\beta}\scriptstyle{\lx@inpgf@ignorespaces\cong}

The rightmost triangle commutes by definition of (k,)(k^{\prime},\ell^{\prime}). The abstract discussion above, again with A=NA=\partial N, implies that the lower triangle commutes. The isomorphism α\alpha is then defined as βexc1\beta\circ\mathrm{exc}^{-1}, making the leftmost triangle commute. The outer square of diagram (3) commutes because it is induced by an inclusion of pairs. The commutativity of the topmost triangle then follows from combining all of the other commutativity statements.

Now we use this to prove that diagram (2) commutes. For the clockwise route in (2) from Hr1(N)H_{r-1}(\partial N) to Hr1(N)Hr1(N)H_{r-1}(N)\oplus H_{r-1}(N^{\prime}), the topmost triangle in (3) yields

ια1=ι(k,).\iota\circ\partial\circ\alpha^{-1}=\iota\circ(k^{\prime}_{*},\ell^{\prime}_{*}).

Then observe that ι(k,)=(k,)\iota\circ(k^{\prime}_{*},\ell^{\prime}_{*})=(k_{*},\ell_{*}), which is the anti-clockwise route. So diagram (2) commutes as claimed. ∎

3. Killing the Casson-Sullivan invariant at the expense of stabilisation

In this section, we recall a realisation result for the Casson-Sullivan invariant derived by the first named author using unpublished work of R. Lee. We then show how to use this to kill the Casson-Sullivan invariant at the expense of stabilisation.

The following statement was shown in [11]*Proposition 3.1, making use of unpublished work of R. Lee to show that one stabilisation suffices; see [10].

Proposition 3.1.

There exists a homeomorphism

f:(S1×S3)#W1C0(S1×S3)#W1f\colon(S^{1}\times S^{3})\#W_{1}\xrightarrow{\cong_{C^{0}}}(S^{1}\times S^{3})\#W_{1}

with cs(f)0\mathrm{cs}(f)\neq 0, inducing f=IdH2((S1×S3)#W1)f_{*}=\operatorname{Id}_{H_{2}((S^{1}\times S^{3})\#W_{1})}, and such that f|ν¯(S1×pt)=Idν¯(S1×pt)f|_{\overline{\nu}(S^{1}\times\pt)}=\operatorname{Id}_{\overline{\nu}(S^{1}\times\pt)}.

We now recall the technique from [11] for using the homeomorphism from Proposition 3.1 to kill the Casson-Sullivan invariant of FF, at the expense of stabilising the manifold once.

Suppose F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2)\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}) is a homeomorphism that is smooth near Σ1\Sigma_{1}. Let μX̊1\mu\subseteq\mathring{X}_{1} be an embedded loop in the interior of X1X_{1}. We consider the circle sum operation of X1X_{1} and X2X_{2} with (S1×S3)#W1(S^{1}\times S^{3})\#W_{1}, along μ\mu and F(μ)F(\mu) respectively, to obtain

X1#μ=S1×pt((S1×S3)#W1)X1#W1X_{1}\#_{\mu=S^{1}\times\mathrm{pt}}\big((S^{1}\times S^{3})\#W_{1}\big)\cong X_{1}\#W_{1}

and

X2#F(μ)=S1×pt((S1×S3)#W1)X2#W1.X_{2}\#_{F(\mu)=S^{1}\times\mathrm{pt}}\big((S^{1}\times S^{3})\#W_{1}\big)\cong X_{2}\#W_{1}.

Recall that F:X1X2F\colon X_{1}\to X_{2} is the restriction of F^\widehat{F} to the surface exteriors. As the homeomorphism

f:(S1×S3)#W1C0(S1×S3)#W1,f\colon(S^{1}\times S^{3})\#W_{1}\xrightarrow{\cong_{C^{0}}}(S^{1}\times S^{3})\#W_{1},

from Proposition 3.1 fixes a neighbourhood of S1×ptS^{1}\times\mathrm{pt} pointwise, it makes sense to extend the homeomorphism FF over the circle-summed manifolds to obtain a homeomorphism

G:=F#μ=S1×ptf:X1#W1C0X2#W1.G^{\prime}:=F\#_{\mu=S^{1}\times\mathrm{pt}}f\colon X_{1}\#W_{1}\xrightarrow{\cong_{C^{0}}}X_{2}\#W_{1}.
Theorem 3.2.

Suppose F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2)\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}) is a homeomorphism that is smooth near Σ1\Sigma_{1}, and that F^\widehat{F} is topologically isotopic rel. boundary to a diffeomorphism. Let μX̊1\mu\subseteq\mathring{X}_{1} be an embedded loop homologous to PD(cs(F))\mathrm{PD}(\mathrm{cs}(F)). Then the circle-summed homeomorphism along μ\mu

G:=F#μ=S1×ptf:X1#W1C0X2#W1.G^{\prime}:=F\#_{\mu=S^{1}\times\mathrm{pt}}f\colon X_{1}\#W_{1}\xrightarrow{\cong_{C^{0}}}X_{2}\#W_{1}.

has trivial Casson-Sullivan invariant.

Proof.

The result follows from a direct application of [11]*Theorem 3.2. ∎

Corollary 3.3.

After some number k1k-1 of further stabilisations, G#IdWk1G^{\prime}\#\operatorname{Id}_{W_{k-1}} is topologically pseudo-isotopic to a diffeomorphism, denoted

G:X1#WkCX2#Wk.G\colon X_{1}\#W_{k}\xrightarrow{\cong_{C^{\infty}}}X_{2}\#W_{k}.
Proof.

Combine Proposition 2.6 and Theorem 3.2. ∎

4. Obtaining a diffeomorphism of X#WkX\#W_{k} sending Σ1\Sigma_{1} to Σ2\Sigma_{2} that is topologically pseudo-isotopic to the identity

Suppose F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2)\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}) is a homeomorphism that is smooth near Σ1\Sigma_{1}, that is also topologically isotopic rel. boundary to the identity. The outcome of the previous section is that, after a single stabilisation of X1X_{1} and X2X_{2}, there is a way to extend F:X1X2F\colon X_{1}\to X_{2}, the restriction of F^\widehat{F}, across the added W1=S2×S2W_{1}=S^{2}\times S^{2}, in such a way that the resulting homeomorphism G:X1#W1X1#W1G^{\prime}\colon X_{1}\#W_{1}\to X_{1}\#W_{1} has trivial Casson-Sullivan invariant. This means we may stabilise GG^{\prime} and obtain a homeomorphism topologically isotopic, rel. boundary, to a diffeomorphism GG between the stabilised exteriors. This can then be filled back in to give a diffeomorphism of stabilised XX. In this section, we will argue that, because the original F^\widehat{F} was topologically isotopic rel. boundary to the identity, the eventual diffeomorphism of the stabilised XX can be chosen so as to be topologically pseudo-isotopic to the identity.

We will need the following lemma in this section.

Lemma 4.1.

If g,h:MC0Mg,h\colon M\xrightarrow{\cong_{C^{0}}}M are two orientation-preserving homeomorphisms of a compact 44-manifold MM such that g=hg=h on MP̊M\setminus\mathring{P}, where PP is a compact, simply-connected codimension 00 submanifold PM̊P\subseteq\mathring{M}, with P\partial P connected, dimH1(P,)1\dim H_{1}(\partial P;\mathbb{Q})\leq 1, and g=h:H2(P)H2(P)g_{*}=h_{*}\colon H_{2}(P)\to H_{2}(P), then gg is topologically isotopic rel. boundary to hh.

Proof.

Apply [18]*Corollary C to conclude that g|Pg|_{P} and h|Ph|_{P} are topologically isotopic rel. boundary. Extend this by the identity isotopy to the rest of MM to conclude that gg is topologically isotopic rel. boundary to hh. ∎

We describe a standard way to “fill” a homeomorphism between the surface-exteriors back to a homeomorphism of the whole manifold.

Definition 4.2.

Suppose F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2)\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}) is a homeomorphism that is smooth near Σ1\Sigma_{1}. Let n0n\geq 0. For any homeomorphism G:X1#WnX2#WnG\colon X_{1}\#W_{n}\to X_{2}\#W_{n} such that G=F^G=\widehat{F} on 1X1\partial_{1}X_{1}, define the extension

G^:=GF^|νΣ1:X#WnX#Wn.\widehat{G}:=G\cup\widehat{F}|_{\nu\Sigma_{1}}\colon X\#W_{n}\to X\#W_{n}.

If GG is a diffeomorphism then G^\widehat{G} is also a diffeomorphism. Note G^\widehat{G} sends Σ1\Sigma_{1} to Σ2\Sigma_{2}.

Lemma 4.3.

Suppose F^:(X,ν¯Σ1)C0,C(X,ν¯Σ2)\widehat{F}\colon(X,\overline{\nu}\Sigma_{1})\xrightarrow{\cong_{C^{0},C^{\infty}}}(X,\overline{\nu}\Sigma_{2}) is a homeomorphism that is smooth near Σ1\Sigma_{1}, and that F^\widehat{F} is topologically isotopic rel. boundary to IdX\operatorname{Id}_{X}. Then for some choice of embedded loop μX̊1\mu\subseteq\mathring{X}_{1} homologous to PD(cs(F))\mathrm{PD}(\mathrm{cs}(F)), the resultant GG^{\prime} from Theorem 3.2 and corresponding

G:X1#WkCX2#WkG\colon X_{1}\#W_{k}\xrightarrow{\cong_{C^{\infty}}}X_{2}\#W_{k}

from Corollary 3.3 are such that the diffeomorphism G^:X#WkCX#Wk\widehat{G}\colon X\#W_{k}\xrightarrow{\cong_{C^{\infty}}}X\#W_{k} is topologically pseudo-isotopic to IdX#Wk\operatorname{Id}_{X\#W_{k}}.

Remark 4.4.

It is worth recalling again that our convention is isotopies are explicitly specified to be rel. boundary when relevant, but that all pseudo-isotopies are by definition rel. boundary, so we do not need to specify this property each time.

Proof.

By definition, F^\widehat{F}, and hence also suitable stabilisations thereof, is topologically isotopic rel. boundary to the identity. So IdX#Wk\operatorname{Id}_{X\#W_{k}} and F^#IdWk\widehat{F}\#\operatorname{Id}_{W_{k}} are topologically isotopic rel. boundary.

We now choose μ\mu. By Proposition 2.13, we may represent the homology class PD(cs(F))\mathrm{PD}(\mathrm{cs}(F)) by the sum j=1N[γj]H1(X1,/2)\sum_{j=1}^{N}[\gamma_{j}]\in H_{1}(X_{1};\mathbb{Z}/2), where {γj}j=1N\{\gamma_{j}\}_{j=1}^{N} is a collection of meridians to Σ\Sigma. For each j{1,,N1}j\in\{1,\dots,{N-1}\}, choose a smoothly embedded path αj,j+1X1\alpha_{j,j+1}\subseteq X_{1} from γj\gamma_{j} to γj+1\gamma_{j+1}. Perform band sums using this arc collection, and push this curve slightly off X1\partial X_{1}, to yield the desired μ\mu. Observe that the map GG^{\prime} from Theorem 3.2 and F^#IdW1\widehat{F}\#\operatorname{Id}_{W_{1}} agree upon restriction to

(X1#W1)(ν(μ)#W1).\big(X_{1}\#W_{1}\big)\setminus(\nu(\mu)\#W_{1}).

In particular G=F^G^{\prime}=\widehat{F} on 1X1\partial_{1}X_{1}, so we may extend GG^{\prime} over the tubular neighbourhood using F^\widehat{F}, to define G^\widehat{G}^{\prime}.

Now, for each j{1,,N1}j\in\{1,\dots,{N-1}\}, let djXd_{j}\subseteq X be a meridional disc to the connected component Σ1j\Sigma^{j}_{1} with boundary the meridian γj\gamma_{j}. We define

V:=ν(j=1Ndjj=1N1αj,j+1)#W1.V:=\nu\Big(\bigcup_{j=1}^{N}d_{j}\cup\bigcup_{j=1}^{N-1}\alpha_{j,j+1}\Big)\#W_{1}.

Lemma 4.1 may now be applied to the maps G^\widehat{G}^{\prime} and F^#IdW1\widehat{F}\#\operatorname{Id}_{W_{1}}, with M=X#W1M=X\#W_{1} and P=VP=V in the language of that lemma. To see this, note that since νμV\nu\mu\subseteq V, we have G^=F^#IdW1\widehat{G}^{\prime}=\widehat{F}\#\operatorname{Id}_{W_{1}} on XVX\setminus V. Moreover, π1(V)={1}\pi_{1}(V)=\{1\}, PS3\partial P\cong S^{3} and (G^)=Id=(F^#IdW1)(\widehat{G}^{\prime})_{*}=\operatorname{Id}=(\widehat{F}\#\operatorname{Id}_{W_{1}})_{*} on H2(P)H_{2}(P). Thus Lemma 4.1 implies that F^#IdW1\widehat{F}\#\operatorname{Id}_{W_{1}} and G^\widehat{G}^{\prime} are topologically isotopic rel. boundary. Thus F^#IdWk\widehat{F}\#\operatorname{Id}_{W_{k}} and G^#IdWk1\widehat{G}^{\prime}\#\operatorname{Id}_{W_{k-1}} are topologically isotopic rel. boundary.

Finally since G#IdWk1G^{\prime}\#\operatorname{Id}_{W_{k-1}} and GG are topologically pseudo-isotopic by Corollary 3.3, it follows that after filling in we have that G^#IdWk1\widehat{G}^{\prime}\#\operatorname{Id}_{W_{k-1}} and G^\widehat{G} are topologically pseudo-isotopic.

We consider the two isotopies produced above as pseudo-isotopies, and concatenate all three pseudo-isotopies to obtain the desired pseudo-isotopy between G^\widehat{G} and IdX#Wk\operatorname{Id}_{X\#W_{k}}. ∎

In the next lemma we make use of the topological Hatcher–Wagoner obstruction ΣTop(Ψ)Wh2(π)\Sigma^{\mathrm{Top}}(\Psi)\in\Wh_{2}(\pi) of a topological pseudo-isotopy Ψ:X×IX×I\Psi\colon X\times I\to X\times I, developed by Nonino and the first-named author [12].

Lemma 4.5.

Let

Ψ:(X#Wk)×IC0(X#Wk)×I\Psi\colon(X\#W_{k})\times I\xrightarrow{\cong_{C^{0}}}(X\#W_{k})\times I

be a pseudo-isotopy as produced by Lemma 4.3. Then the primary Hatcher–Wagoner obstruction ΣTop(Ψ)\Sigma^{\mathrm{Top}}(\Psi) lies in the image of

Wh2(π1(X1))Wh2(π).\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi).
Proof.

This follows from the construction of Ψ\Psi. The first two pseudo-isotopies in the construction come from topological isotopies, so these have vanishing obstructions in Wh2(π)\Wh_{2}(\pi). The final pseudo-isotopy is obtained from a pseudo-isotopy of X1#WkX_{1}\#W_{k} by filling in the tubular neighbourhoods of the Σi\Sigma_{i}, and hence by naturality of ΣTop\Sigma^{\mathrm{Top}} [12]*Proposition 1.3 we see that ΣTop(Ψ)\Sigma^{\mathrm{Top}}(\Psi) lies in the image of Wh2(π1(X1))Wh2(π)\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi), as desired. ∎

5. Improving Ψ\Psi to a smooth pseudo-isotopy after further stabilisations

The next step will be to improve our topological pseudo-isotopy Ψ\Psi into a smooth pseudo-isotopy, possibly after further stabilising X#WkX\#W_{k} to X#WmX\#W_{m} for some mkm\geq k. Before splitting into cases, we collect some results that will be useful during the proofs.

5.1. The smoothing obstruction for topological pseudo-isotopies

Given a smooth, compact 4-manifold UU and a topological pseudo-isotopy F:U×IU×IF\colon U\times I\to U\times I that is smooth near (U×I)\partial(U\times I), Orson–Powell–Randal-Williams defined an obstruction 𝖪𝖲(F)H2(U,/2)\mathsf{KS}(F)\in H_{2}(U;\mathbb{Z}/2), as follows. Let σ\sigma denote the product smooth structure on U×IU\times I. We consider U×I×IU\times I\times I as a topological manifold and place a smooth structure on its boundary. Endow U×I×{1}U\times I\times\{1\} with the pullback smooth structure FσF^{*}\sigma, and then use the standard structure on the rest of (U×I×I)\partial(U\times I\times I). Denote the resulting smooth manifold by (U×I×I)F(U\times I\times I)_{F}. We then consider the Kirby-Siebenmann obstruction to extending this smooth structure over X×I×IX\times I\times I:

ks(U×I×I,(U×I×I)F)H4(X×I×I,;/2).\mathrm{ks}(U\times I\times I,\partial(U\times I\times I)_{F})\in H^{4}(X\times I\times I,\partial;\mathbb{Z}/2).

Taking its Poincaré dual, and implicitly applying that UU×I×IU\simeq U\times I\times I, we obtain:

𝖪𝖲(F):=PD(ks(U×I×I,(U×I×I)F))H2(U,/2).\mathsf{KS}(F):=PD\big(\mathrm{ks}(U\times I\times I,\partial(U\times I\times I)_{F})\big)\in H_{2}(U;\mathbb{Z}/2).

The next proposition gives some useful properties of 𝖪𝖲\mathsf{KS}, that it is a homomorphism, it detects the difference between smooth and topological pseudo-isotopies, and that it satisfies a gluing formula.

Proposition 5.1.

Let Q(U)Q(U) denote the group of topological pseudo-isotopies F:U×IU×IF\colon U\times I\to U\times I such that F1:=F|U×{1}F_{1}:=F|_{U\times\{1\}} is smooth, up to topological pseudo-isotopy relative a smooth pseudo-isotopy on U×I×{1}U\times I\times\{1\} and to the identity on the rest of (U×I×I)\partial(U\times I\times I). The group structure comes from composition.

  1. (i)

    The map 𝖪𝖲\mathsf{KS} is a homomorphism 𝖪𝖲:Q(U)H2(U,/2)\mathsf{KS}\colon Q(U)\to H_{2}(U;\mathbb{Z}/2).

  2. (ii)

    We have that 𝖪𝖲(F)=0\mathsf{KS}(F)=0 if and only if FF is topologically isotopic rel. (U×I)\partial(U\times I) to a smooth pseudo-isotopy.

  3. (iii)

    Suppose MM and NN are manifolds with corners, where M=0M1M\partial M=\partial_{0}M\cup\partial_{1}M, N=0N1N\partial N=\partial_{0}N\cup\partial_{1}N and 1M=1N\partial_{1}M=\partial_{1}N. Let U=M1M=1NNU=M\cup_{\partial_{1}M=\partial_{1}N}N. Let Ψ^:U×IC0U×I\widehat{\Psi}\colon U\times I\xrightarrow{\cong_{C^{0}}}U\times I be a topological pseudo-isotopy that restricts to a smooth pseudo-isotopy ΨM:M×ICM×I\Psi_{M}\colon M\times I\xrightarrow{\cong_{C^{\infty}}}M\times I and to a topological pseudo-isotopy ΨN:N×IC0N×I\Psi_{N}\colon N\times I\xrightarrow{\cong_{C^{0}}}N\times I. Then under the inclusion induced map

    (iN):H2(N,/2)\displaystyle(i_{N})_{*}\colon H_{2}(N;\mathbb{Z}/2) H2(U,/2)\displaystyle\to H_{2}(U;\mathbb{Z}/2)
    𝖪𝖲(ΨN)\displaystyle\mathsf{KS}(\Psi_{N}) 𝖪𝖲(Ψ^).\displaystyle\mapsto\mathsf{KS}(\widehat{\Psi}).
Proof.

Part (i) is proven in [17]*Lemma 3.2, and part (ii) is proven in [17]*Theorem A. We prove (iii). Let

A:=M×I×I,B:=N×I×I,C:=A,D:=B, and E:=CD=AB.\displaystyle A:=M\times I\times I,\;\;\;B:=N\times I\times I,\;\;\;C:=\partial A,\;\;\;D:=\partial B,\text{ and }E:=C\cap D=A\cap B.
A=M×I×IA=M\times I\times IB=N×I×IB=N\times I\times IE=CD=ABE=C\cap D=A\cap BC=(M×I×I)C=\partial(M\times I\times I)D=(N×I×I)D=\partial(N\times I\times I)
Figure 2. A schematic for the decomposition used in the proof of Proposition 5.1.

Endow CDC\cup D with the standard smooth structure on (U×I×{0})((MN)×I×[0,1))(U\times I\times\{0\})\cup((\partial M\cup\partial N)\times I\times[0,1)) and on U×I×{1}U\times I\times\{1\} pull back the smooth structure using Ψ^\widehat{\Psi}. As the restriction Ψ^|(MN)×I\widehat{\Psi}|_{(\partial M\cup\partial N)\times I} is a diffeomorphism, this indeed determines a smooth structure on CDC\cup D. Consider the diagram

H4(A,C,/2)H4(B,D,/2){\lx@inpgf@ignorespaces H^{4}(A,C;\mathbb{Z}/2)\oplus H^{4}(B,D;\mathbb{Z}/2)}H4(AB,CD,/2){\lx@inpgf@ignorespaces H^{4}(A\cup B,C\cup D;\mathbb{Z}/2)}H4(AB,(AB),/2){\lx@inpgf@ignorespaces H^{4}(A\cup B,\partial(A\cup B);\mathbb{Z}/2)}H2(M,/2)H2(N,/2){\lx@inpgf@ignorespaces H_{2}(M;\mathbb{Z}/2)\oplus H_{2}(N;\mathbb{Z}/2)}H2(U,/2){\lx@inpgf@ignorespaces H_{2}(U;\mathbb{Z}/2)}PDPD\scriptstyle{\lx@inpgf@ignorespaces PD\oplus PD}\scriptstyle{\lx@inpgf@ignorespaces\cong}\scriptstyle{\lx@inpgf@ignorespaces\cong}PD\scriptstyle{\lx@inpgf@ignorespaces PD}\scriptstyle{\lx@inpgf@ignorespaces\cong}

where the top left map comes from the Mayer-Vietoris sequence

0=H3(E,E)H4(AB,CD,/2)H4(A,C,/2)H4(B,D,/2)H4(E,E)=0,0=H^{3}(E,E)\to H^{4}(A\cup B,C\cup D;\mathbb{Z}/2)\xrightarrow{\cong}H^{4}(A,C;\mathbb{Z}/2)\oplus H^{4}(B,D;\mathbb{Z}/2)\to H^{4}(E,E)=0,

noting that E=AB=CDE=A\cap B=C\cap D. The top right map is induced by inclusion. The diagram commutes by naturality and linearity of cap products. As CC and DD have smooth structures, there are Kirby-Siebenmann invariants ks(A,C)H4(A,C,/2)\mathrm{ks}(A,C)\in H^{4}(A,C;\mathbb{Z}/2) and ks(B,D)H4(B,D,/2)\mathrm{ks}(B,D)\in H^{4}(B,D;\mathbb{Z}/2). By naturality of the Kirby-Siebenmann invariant, we have that

(ks(A,C),ks(B,D))ks(AB,CD)ks(AB,(AB))(\mathrm{ks}(A,C),\mathrm{ks}(B,D))\mapsto\mathrm{ks}(A\cup B,C\cup D)\mapsto\mathrm{ks}(A\cup B,\partial(A\cup B))

along the top row of the diagram. The clockwise composition around the diagram thus sends (ks(A,C),ks(B,D))(\mathrm{ks}(A,C),\mathrm{ks}(B,D)) to 𝖪𝖲(Ψ^)\mathsf{KS}(\widehat{\Psi}). The Kirby-Siebenmann invariant ks(A,C)\mathrm{ks}(A,C) vanishes because the restriction of Ψ^\widehat{\Psi} to M×IM\times I is a diffeomorphism, so the standard smooth structure on M×I×IM\times I\times I extends that on the boundary CC. Thus the anticlockwise composition is (ks(A,C),ks(B,D))=(0,ks(B,D))(0,𝖪𝖲(ΨN))0+(iN)𝖪𝖲(ΨN)(\mathrm{ks}(A,C),\mathrm{ks}(B,D))=(0,\mathrm{ks}(B,D))\mapsto(0,\mathsf{KS}(\Psi_{N}))\mapsto 0+(i_{N})_{*}\mathsf{KS}(\Psi_{N}). Thus (iN)𝖪𝖲(ΨN)=𝖪𝖲(Ψ^)(i_{N})_{*}\mathsf{KS}(\Psi_{N})=\mathsf{KS}(\widehat{\Psi}) as claimed. ∎

We will also need realisation results for the smoothing obstruction 𝖪𝖲\mathsf{KS}. The first one allows us to realise all possible values, at the expense of stabilising the 44-manifold (which in the context of this article is no problem).

Theorem 5.2.

There exists mkm\geq k such that for every xH2(X1#Wm,/2)x\in H_{2}(X_{1}\#W_{m};\mathbb{Z}/2) there is a topological pseudo-isotopy

Φ:(X1#Wm)×IC0(X1#Wm)×I\Phi\colon(X_{1}\#W_{m})\times I\xrightarrow{\cong_{C^{0}}}(X_{1}\#W_{m})\times I

such that Φ|=Id\Phi|_{\sqsubset}=\operatorname{Id}_{\sqsubset}, the restriction

Φ|(X1#Wm)×{1}:X1#Wm×{1}CX1#Wm×{1}\Phi|_{(X_{1}\#W_{m})\times\{1\}}\colon X_{1}\#W_{m}\times\{1\}\xrightarrow{\cong_{C^{\infty}}}X_{1}\#W_{m}\times\{1\}

is a diffeomorphism, and 𝖪𝖲(Φ)=xH2(X1#Wm,/2)\mathsf{KS}(\Phi)=x\in H_{2}(X_{1}\#W_{m};\mathbb{Z}/2).

Proof.

This is an application of Orson–Powell–Randal-Williams [17]*Theorem E. ∎

In Theorem 5.2 we obtain a topological pseudo-isotopy from the identity to some diffeomorphism, but we have no control on the diffeomorphism that arises on X1#Wm×{1}X_{1}\#W_{m}\times\{1\}. In the next result, also proven in Orson–Powell–Randal-Williams, we obtain more control on this diffeomorphism, at the expense of requiring more assumptions.

Theorem 5.3.

Let UU be a compact, smooth, orientable 4-manifold with π:=π1(U)\pi:=\pi_{1}(U). Suppose that the map I2:H2(π,(2))L6(π)(2)I_{2}\colon H_{2}(\pi;\mathbb{Z}_{(2)})\to L_{6}(\mathbb{Z}\pi)_{(2)} is zero, and there is no 2-torsion in H1(π,)H_{1}(\pi;\mathbb{Z}). Then for every xH2(U,/2)x\in H_{2}(U;\mathbb{Z}/2) there is an topological pseudo-isotopy Φ:U×IC0U×I\Phi\colon U\times I\xrightarrow{\cong_{C^{0}}}U\times I with 𝖪𝖲(Φ)=x\mathsf{KS}(\Phi)=x and Φ|(U×I)=IdU×I\Phi|_{\partial(U\times I)}=\operatorname{Id}_{U\times I}, i.e. Φ\Phi is an inertial pseudo-isotopy.

Proof.

This follows directly from the proof of [17]*Theorem C, where it is shown that the composition π1(Homeo~+(U))Q(U)𝖪𝖲H2(U,/2)\pi_{1}(\widetilde{\operatorname{Homeo}}\mkern 0.0mu^{+}_{\partial}(U))\to Q(U)\xrightarrow{\mathsf{KS}}H_{2}(U;\mathbb{Z}/2) is surjective; see the start of [17]*Section 5. ∎

Theorem 5.2 will be used for case (i) of A, while Theorem 5.3 will be needed for case (ii).

5.2. Smoothing the topological pseudo-isotopy when the obstruction is supported on the surface exterior

The proof of Theorem A in case (i) will make use of the following key result.

Proposition 5.4.

Let G^:XCX\widehat{G}\colon X\xrightarrow{\cong_{C^{\infty}}}X be a diffeomorphism sending Σ1\Sigma_{1} to Σ2\Sigma_{2} and write GG for the restriction of G^\widehat{G} to X1=ν¯Σ1X_{1}=\overline{\nu}\Sigma_{1}. Let

Ψ:(X#Wk)×IC0(X#Wk)×I\Psi\colon(X\#W_{k})\times I\xrightarrow{\cong_{C^{0}}}(X\#W_{k})\times I

be a topological pseudo-isotopy from G^\widehat{G} to the identity map IdX#Wk\operatorname{Id}_{X\#W_{k}}. Assume that 𝖪𝖲(Ψ)Im(H2(X1,/2)H2(X,/2))\mathsf{KS}(\Psi)\in\operatorname{Im}(H_{2}(X_{1};\mathbb{Z}/2)\to H_{2}(X;\mathbb{Z}/2)). Then there exists mkm\geq k and a diffeomorphism

L:X1#WmCX2#WmL\colon X_{1}\#W_{m}\xrightarrow{\cong_{C^{\infty}}}X_{2}\#W_{m}

with L^:X#WmX#Wm\widehat{L}\colon X\#W_{m}\to X\#W_{m} smoothly pseudo-isotopic to the identity, via a smooth pseudo-isotopy

Ξ:(X#Wm)×IC(X#Wm)×I\Xi\colon(X\#W_{m})\times I\xrightarrow{\cong_{C^{\infty}}}(X\#W_{m})\times I

with the property that Σ(Ξ)Im(Wh2(π1(X1))Wh2(π))\Sigma(\Xi)\in\operatorname{Im}(\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)).

Proof.

Write 𝖪𝖲(Ψ)=xH2(X,/2)\mathsf{KS}(\Psi)=x\in H_{2}(X;\mathbb{Z}/2). By assumption, we may choose a lift x¯H2(X1,/2)\overline{x}\in H_{2}(X_{1};\mathbb{Z}/2) of xx. Now apply Theorem 5.2 to x¯\overline{x}, to obtain, for some mkm\geq k, a topological pseudo-isotopy

Φ:(X1#Wm)×IC0(X1#Wm)×I\Phi\colon(X_{1}\#W_{m})\times I\xrightarrow{\cong_{C^{0}}}(X_{1}\#W_{m})\times I

with 𝖪𝖲(Φ)=x¯H2(X1,/2)\mathsf{KS}(\Phi)=\overline{x}\in H_{2}(X_{1};\mathbb{Z}/2), that restricts on (X1#Wm)×{1}(X_{1}\#W_{m})\times\{1\} to a diffeomorphism. Extend Φ\Phi to the whole of XX using the trivial pseudo-isotopy on ν¯Σ1×I\overline{\nu}\Sigma_{1}\times I, to obtain

Φ^:(X#Wm)×IC0(X#Wm)×I.\widehat{\Phi}\colon(X\#W_{m})\times I\xrightarrow{\cong_{C^{0}}}(X\#W_{m})\times I.

We therefore have that

x=i(x¯)=i(𝖪𝖲(Φ))=𝖪𝖲(Φ^),x=i_{*}(\overline{x})=i_{*}(\mathsf{KS}(\Phi))=\mathsf{KS}(\widehat{\Phi}),

where i:X1Xi\colon X_{1}\to X is the inclusion, and the last equality follows from Proposition 5.1 (iii).

Compose Φ^\widehat{\Phi} with Ψ\Psi (stabilised by extending by the identity on Wmk×IW_{m-k}\times I, but still denoted by Ψ\Psi) to form a topological pseudo-isotopy

ΨΦ^:(X#Wm)×IC(X#Wm)×I.\Psi\circ\widehat{\Phi}\colon(X\#W_{m})\times I\xrightarrow{\cong_{C^{\infty}}}(X\#W_{m})\times I.

The restriction of this to (X1#Wm)×{1}(X_{1}\#W_{m})\times\{1\} yields L:=(G#IdWmk)Φ1:X1#WmCX2#WmL:=(G\#\operatorname{Id}_{W_{m-k}})\circ\Phi_{1}\colon X_{1}\#W_{m}\xrightarrow{\cong_{C^{\infty}}}X_{2}\#W_{m}, and the restriction to (X#Wm)×{1}(X\#W_{m})\times\{1\} yields

L^:=(G^#IdWmk)Φ1:X#WmCX#Wm.\widehat{L}:=(\widehat{G}\#\operatorname{Id}_{W_{m-k}})\circ\Phi_{1}\colon X\#W_{m}\xrightarrow{\cong_{C^{\infty}}}X\#W_{m}.

Since 𝖪𝖲\mathsf{KS} is a homomorphism Proposition 5.1 (i), we have 𝖪𝖲(ΨΦ^)=𝖪𝖲(Ψ)+𝖪𝖲(Φ^)=x+x=0\mathsf{KS}(\Psi\circ\widehat{\Phi})=\mathsf{KS}(\Psi)+\mathsf{KS}(\widehat{\Phi})=x+x=0. Hence by Proposition 5.1 (ii), we have that ΨΦ^\Psi\circ\widehat{\Phi} is topologically isotopic rel. boundary to a smooth pseudo-isotopy, as desired, which we denote by Ξ\Xi.

It remains to prove the statement regarding Σ(Ξ)\Sigma(\Xi). We calculate

Σ(Ξ)=ΣTop(Ξ)=ΣTop(ΨΦ^)=ΣTop(Ψ)+ΣTop(Φ^)Im(Wh2(π1(X1))Wh2(π)),\Sigma(\Xi)=\Sigma^{\mathrm{Top}}(\Xi)=\Sigma^{\mathrm{Top}}(\Psi\circ\widehat{\Phi})=\Sigma^{\mathrm{Top}}(\Psi)+\Sigma^{\mathrm{Top}}(\widehat{\Phi})\in\operatorname{Im}(\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)),

where the first equality follows from [12]*Theorem 1.1, the second from the definition of Ξ\Xi, and the third from the fact that ΣTop\Sigma^{\mathrm{Top}} is a homomorphism [12]*Lemma 3.12. That this sum is an element of the noted subgroup can be deduced as follows. The first summand is by Lemma 4.5 and the second summand is since Φ^\widehat{\Phi} was only supported on the exterior (X1#Wm)×I(X_{1}\#W_{m})\times I, and since ΣTop\Sigma^{\mathrm{Top}} is natural under inclusions of codimension zero submanifolds [12]*Proposition 1.3. ∎

5.3. Smoothing the pseudo-isotopy assuming at least one of the hypotheses of A hold

Next we prove that in both sets of assumptions of A, we can improve Ψ\Psi, after further stabilising, to a smooth pseudo-isotopy, while preserving its other useful properties. The aim is to prove the following result. The output is similar to Proposition 5.4, but instead of assuming that 𝖪𝖲(Ψ)Im(H2(X1,/2)H2(X,/2))\mathsf{KS}(\Psi)\in\operatorname{Im}(H_{2}(X_{1};\mathbb{Z}/2)\to H_{2}(X;\mathbb{Z}/2)), we assume one of the hypotheses of A.

Proposition 5.5.

Suppose that for some k0k\geq 0 there exists a diffeomorphism G^:X#WkCX#Wk\widehat{G}\colon X\#W_{k}\xrightarrow{\cong_{C^{\infty}}}X\#W_{k} that sends Σ1\Sigma_{1} to Σ2\Sigma_{2} and that is topologically pseudo-isotopic to the identity, via a topological pseudo-isotopy Ψ\Psi such that ΣTop(Ψ)Im(Wh2(π1(X1))Wh2(π))\Sigma^{\mathrm{Top}}(\Psi)\in\operatorname{Im}(\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)). Suppose that at least one of the conditions (i) or (ii) in A is satisfied.

Then there exists mkm\geq k and a diffeomorphism L:X1#WmCX2#WmL\colon X_{1}\#W_{m}\xrightarrow{\cong_{C^{\infty}}}X_{2}\#W_{m}, which extends to a diffeomorphism

L^:X#WmCX#Wm\widehat{L}\colon X\#W_{m}\xrightarrow{\cong_{C^{\infty}}}X\#W_{m}

that sends Σ1\Sigma_{1} to Σ2\Sigma_{2}, and is smoothly pseudo-isotopic to the identity, via a smooth pseudo-isotopy

Ξ:(X#Wm)×IC(X#Wm)×I\Xi\colon(X\#W_{m})\times I\xrightarrow{\cong_{C^{\infty}}}(X\#W_{m})\times I

such that Σ(Ξ)Im(Wh2(π1(X1))Wh2(π))\Sigma(\Xi)\in\operatorname{Im}(\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)).

The proof of Proposition 5.5 in case (i) reduces to showing that the assumption of Proposition 5.4 can be arranged to hold, and then applying Proposition 5.4. The proof for case (ii) uses Theorem 5.3 instead.

5.3.1. Proof of Proposition 5.5 in case (i)

In this scenario we assume that for each connected component Σ1j\Sigma_{1}^{j} of Σ1\Sigma_{1}, we have that  λ/2(x,[Σ1j])=0/2\lambda^{\mathbb{Z}/2}(x,[\Sigma_{1}^{j}])=0\in\mathbb{Z}/2 for all xH2(X,/2)x\in H_{2}(X;\mathbb{Z}/2).

We consider the inclusion i:X1Xi\colon X_{1}\to X. We want to show that the hypothesis of Proposition 5.4, that

i:𝖪𝖲(Ψ)Im(i:H2(X1;/2)H2(X;/2)),i_{*}\colon\mathsf{KS}(\Psi)\in\operatorname{Im}(i_{*}\colon H_{2}(X_{1};\mathbb{Z}/2)\to H_{2}(X;\mathbb{Z}/2)),

is satisfied. Then Proposition 5.4 directly implies Proposition 5.5.

To show this, we first compute that

H2(X,X1,/2)\displaystyle H_{2}(X,X_{1};\mathbb{Z}/2) H2(ν¯Σ1,1ν¯Σ1,/2)H2(ν¯Σ1,0ν¯Σ1,/2)H2(Σ1,Σ1,/2)\displaystyle\xrightarrow{\cong}H_{2}(\overline{\nu}\Sigma_{1},\partial_{1}\overline{\nu}\Sigma_{1};\mathbb{Z}/2)\cong H^{2}(\overline{\nu}\Sigma_{1},\partial_{0}\overline{\nu}\Sigma_{1};\mathbb{Z}/2)\cong H^{2}(\Sigma_{1},\partial\Sigma_{1};\mathbb{Z}/2)
H0(Σ1,/2)(/2)c,\displaystyle\cong H_{0}(\Sigma_{1};\mathbb{Z}/2)\cong(\mathbb{Z}/2)^{c},

where cc is the number of connected components Σ1j\Sigma_{1}^{j} of Σ1\Sigma_{1}. Consider the exact sequence of the pair:

H2(X1,/2)iH2(X,/2)H2(X,X1,/2)(/2)c.H_{2}(X_{1};\mathbb{Z}/2)\xrightarrow{i_{*}}H_{2}(X;\mathbb{Z}/2)\to H_{2}(X,X_{1};\mathbb{Z}/2)\cong(\mathbb{Z}/2)^{c}.

The latter group is generated by meridional discs to the connected components of Σ1\Sigma_{1}. Then coker(i)(/2)c\coker(i_{*})\subseteq(\mathbb{Z}/2)^{c} is generated by a collection of homology classes {S}H2(X,/2)\{S_{\ell}\}\subseteq H_{2}(X;\mathbb{Z}/2) such that for each SS_{\ell} the /2\mathbb{Z}/2-intersection pairing

λ/2:H2(X,/2)×H2(X,X,/2)/2\lambda^{\mathbb{Z}/2}\colon H_{2}(X;\mathbb{Z}/2)\times H_{2}(X,\partial X;\mathbb{Z}/2)\to\mathbb{Z}/2

satisfies that λ/2(S,[Σ1j])=1/2\lambda^{\mathbb{Z}/2}(S_{\ell},[\Sigma_{1}^{j}])=1\in\mathbb{Z}/2 for some jj. If λ/2(x,[Σ1j])=0/2\lambda^{\mathbb{Z}/2}(x,[\Sigma_{1}^{j}])=0\in\mathbb{Z}/2 for all xH2(X,/2)x\in H_{2}(X;\mathbb{Z}/2), then there is no such collection {S}\{S_{\ell}\}. It follows that coker(i)=0\coker(i_{*})=0, so ii_{*} is surjective, and hence 𝖪𝖲(Ψ)Im(i:H2(X1;/2)H2(X;/2))\mathsf{KS}(\Psi)\in\operatorname{Im}(i_{*}\colon H_{2}(X_{1};\mathbb{Z}/2)\to H_{2}(X;\mathbb{Z}/2)) as desired. ∎

5.3.2. Proof of Proposition 5.5 in case (ii)

For case (ii), we assume that the component

I2:H2(π,(2))L6(π)(2)I_{2}\colon H_{2}(\pi;\mathbb{Z}_{(2)})\to L_{6}(\mathbb{Z}\pi)_{(2)}

of the algebraic assembly map is zero, there is no 2-torsion in H1(π,)H_{1}(\pi;\mathbb{Z}), and that Wh2(π)=0\Wh_{2}(\pi)=0.

Under the first two of these hypotheses, by Theorem 5.3, there exists a topological pseudo-isotopy from the identity to itself

Φ:(X#Wk)×IC0(X#Wk)×I,\Phi\colon(X\#W_{k})\times I\xrightarrow{\cong_{C^{0}}}(X\#W_{k})\times I,

such that 𝖪𝖲(Ψ)=𝖪𝖲(Φ)\mathsf{KS}(\Psi)=\mathsf{KS}(\Phi). Then since 𝖪𝖲\mathsf{KS} is a homomorphism by Proposition 5.1 (i), we have that 𝖪𝖲(ΦΨ)=0\mathsf{KS}(\Phi\circ\Psi)=0 so that ΦΨ\Phi\circ\Psi is topologically isotopic rel. boundary to a smooth pseudo-isotopy Ξ\Xi from Ξ|(X#Wk)×{1}=Ψ|(X#Wk)×{1}\Xi|_{(X\#W_{k})\times\{1\}}=\Psi|_{(X\#W_{k})\times\{1\}} to IdX#Wk\operatorname{Id}_{X\#W_{k}}. Note that L^:=Ξ|(X#Wk)×{1}\widehat{L}:=\Xi|_{(X\#W_{k})\times\{1\}} sends Σ1\Sigma_{1} to Σ2\Sigma_{2}.

Also since Wh2(π)=0\Wh_{2}(\pi)=0, it is automatic that Σ(Ξ)Im(Wh2(π1(X1))Wh2(π)=0)\Sigma(\Xi)\in\operatorname{Im}(\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)=0). Hence the smooth pseudo-isotopy Ξ\Xi satisfies the conclusion of Proposition 5.5. ∎

6. Completing the proof of A

The following results of Singh and Gabai, respectively, will be essentially used in the conclusion of the proof.

Theorem 6.1 ([22]*Theorem E).

Let MM be a smooth, compact 44-manifold and xWh2(π1(M))x\in\Wh_{2}(\pi_{1}(M)). Then there exists NN\in\mathbb{N} and a smooth pseudo-isotopy

Λ:(M#WN)×I(M#WN)×I,\Lambda\colon(M\#W_{N})\times I\to(M\#W_{N})\times I,

restricting to the identity on (M#WN)×{0}(M\#W_{N})\times\{0\} and (M#WN)×I(\partial M\#W_{N})\times I, such that

Σ(Λ)=xWh2(π1(M#WN))=Wh2(π1(M)).\Sigma(\Lambda)=x\in\Wh_{2}(\pi_{1}(M\#W_{N}))=\Wh_{2}(\pi_{1}(M)).
Theorem 6.2 ([9]*Theorem 2.5).

Let f:MCMf\colon M\xrightarrow{\cong_{C^{\infty}}}M be an orientation-preserving diffeomorphism of a smooth, compact, oriented 44-manifold MM. Then ff is smoothly stably isotopic rel. boundary to IdM\operatorname{Id}_{M} if and only if ff is smoothly pseudo-isotopic to IdM\operatorname{Id}_{M} via a smooth pseudo-isotopy Ξ\Xi with vanishing Hatcher–Wagoner obstruction Σ(Ξ)=0Wh2(π1(M))\Sigma(\Xi)=0\in\mathrm{Wh}_{2}(\pi_{1}(M)).

We apply the results of Singh and Gabai in the following lemma, then proceed to complete the proof of the main theorem.

Lemma 6.3.

Suppose for some m0m\geq 0 that a diffeomorphism

L^:X#WmCX#Wm\widehat{L}\colon X\#W_{m}\xrightarrow{\cong_{C^{\infty}}}X\#W_{m}

satisfies L^(Σ1)=Σ2\widehat{L}(\Sigma_{1})=\Sigma_{2}. Suppose moreover that L^\widehat{L} is smoothly pseudo-isotopic to the identity via a smooth pseudo-isotopy

Ξ:(X#Wm)×IC(X#Wm)×I,\Xi\colon(X\#W_{m})\times I\xrightarrow{\cong_{C^{\infty}}}(X\#W_{m})\times I,

such that Σ(Ξ)Im(i:Wh2(π1(X1))Wh2(π))\Sigma(\Xi)\in\operatorname{Im}\big(i_{*}\colon\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)\big). Then after some number of stabilisations of XX, the surfaces Σ1\Sigma_{1} and Σ2\Sigma_{2} are smoothly isotopic rel. boundary.

Proof.

Write y:=Σ(Ξ)y:=\Sigma(\Xi) and choose y¯Wh2(π1(X1))\overline{y}\in\Wh_{2}(\pi_{1}(X_{1})) in the preimage of yWh2(π)-y\in\Wh_{2}(\pi). By Theorem 6.1, there exists nmn\geq m and a smooth pseudo-isotopy

Λ:(X1#Wn)×IC(X1#Wn)×I,\Lambda\colon(X_{1}\#W_{n})\times I\xrightarrow{\cong_{C^{\infty}}}(X_{1}\#W_{n})\times I,

restricting to the identity on (X1#Wn)×{0}(X_{1}\#W_{n})\times\{0\} and (X1#Wn)×I(\partial X_{1}\#W_{n})\times I, with Σ(Λ)=y¯\Sigma(\Lambda)=\overline{y}. Denote by Λ^:(X1#Wn)×I(X1#Wn)×I\widehat{\Lambda}\colon(X_{1}\#W_{n})\times I\to(X_{1}\#W_{n})\times I the extension of Λ\Lambda over (ν¯Σ1)×I(\overline{\nu}\Sigma_{1})\times I by the identity map. Stabilise Ξ\Xi with IdWnm×I\operatorname{Id}_{W_{n-m}\times I} to obtain a stabilised smooth pseudo-isotopy, which we continue to denote by Ξ\Xi, now as a diffeomorphism Ξ:(X#Wn)×I(X#Wn)×I\Xi\colon(X\#W_{n})\times I\to(X\#W_{n})\times I. We compute that

Σ(ΞΛ^)=Σ(Ξ)+Σ(Λ^)=yy=0,\Sigma(\Xi\circ\widehat{\Lambda})=\Sigma(\Xi)+\Sigma(\widehat{\Lambda})=y-y=0,

where the first equality uses that Σ\Sigma is a homomorphism and the second is due to the equality Σ(Λ^)=i(Σ(Λ))\Sigma(\widehat{\Lambda})=i_{*}(\Sigma(\Lambda)) which follows from the definition of the Hatcher–Wagoner obstruction, as Λ^\widehat{\Lambda} restricts to an isotopy outside of X1#WnX_{1}\#W_{n} (indeed, the product isotopy).

By Theorem 6.2, it follows that

(ΞΛ^)|(X#Wn)×{1}=:(ΞΛ^)1=L^Λ^1(\Xi\circ\widehat{\Lambda})|_{(X\#W_{n})\times\{1\}}=:(\Xi\circ\widehat{\Lambda})_{1}=\widehat{L}\circ\widehat{\Lambda}_{1}

is smoothly stably isotopic rel. boundary to the identity. Also note that both Λ^1:X1X1\widehat{\Lambda}_{1}\colon X_{1}\to X_{1} and L^:X1X2\widehat{L}\colon X_{1}\to X_{2} are obtained from filling in the surface tubular neighbourhoods, and so L^Λ^1\widehat{L}\circ\widehat{\Lambda}_{1} sends Σ1\Sigma_{1} to Σ2\Sigma_{2}. This completes the proof of the lemma. ∎

Proof of A.

Assume that Σ1\Sigma_{1} and Σ2\Sigma_{2} are topologically isotopic rel. boundary. Using Lemma 2.10, we may assume there exists a homeomorphism F^:XX\widehat{F}\colon X\to X such that the restriction F^|ν¯Σ1:ν¯Σ1ν¯Σ2\widehat{F}|_{\overline{\nu}\Sigma_{1}}\colon\overline{\nu}\Sigma_{1}\to\overline{\nu}\Sigma_{2} is a diffeomorphism sending Σ1\Sigma_{1} to Σ2\Sigma_{2} and such that F^\widehat{F} is topologically isotopic rel. boundary to the identity map IdX\operatorname{Id}_{X}. By Lemma 4.3, there exists k0k\geq 0 and a diffeomorphism

G^:X#WkCX#Wk\widehat{G}\colon X\#W_{k}\xrightarrow{\cong_{C^{\infty}}}X\#W_{k}

that sends Σ1\Sigma_{1} to Σ2\Sigma_{2} and is topologically pseudo-isotopic to IdX#Wk\operatorname{Id}_{X\#W_{k}}. Choosing such a topological pseudo-isotopy Ψ\Psi, by Lemma 4.5, we have that ΣTop(Ψ)Im(i:Wh2(π1(X1))Wh2(π))\Sigma^{\mathrm{Top}}(\Psi)\in\operatorname{Im}\big(i_{*}\colon\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)\big).

Next, by Proposition 5.5, assuming the hypotheses of A, we obtain mkm\geq k and a diffeomorphism

L^:X#WmCX#Wm\widehat{L}\colon X\#W_{m}\xrightarrow{\cong_{C^{\infty}}}X\#W_{m}

that sends Σ1\Sigma_{1} to Σ2\Sigma_{2} and is smoothly pseudo-isotopic to IdX#Wm\operatorname{Id}_{X\#W_{m}}, via a smooth pseudo-isotopy Ξ\Xi such that Σ(Ξ)Im(i:Wh2(π1(X1))Wh2(π))\Sigma(\Xi)\in\operatorname{Im}\big(i_{*}\colon\Wh_{2}(\pi_{1}(X_{1}))\to\Wh_{2}(\pi)\big). These are exactly the hypotheses of Lemma 6.3, and so that lemma implies that after some number of stabilisations of XX, the surfaces Σ1\Sigma_{1} and Σ2\Sigma_{2} are smoothly isotopic rel. boundary. ∎

Appendix A The case of simply-connected XX and simply-connected complement

The case of Theorem A when XX is simply-connected was first proved in [11]*Theorem 1.2. Specialising even more, to the case when moreover the surface complements are simply-connected, we are able to give an alternative proof based on work of Gompf [13], Boyer [3], Saeki [21], and Quinn [20] (with the correction in [8]).

Proposition A.1.

Let XX be a smooth, orientable, closed, simply-connected 44-manifold. Suppose Σ1,Σ2X\Sigma_{1},\Sigma_{2}\subseteq X are smooth, orientable, closed surfaces, each with simply-connected complements. Suppose that Σ1\Sigma_{1} and Σ2\Sigma_{2} are topologically isotopic. Then Σ1\Sigma_{1} and Σ2\Sigma_{2} are smoothly isotopic in some stabilisation of XX.

Proof.

Using Lemma 2.10, we may assume there exists a homeomorphism F^:XX\widehat{F}\colon X\to X such that the restriction F^|ν¯Σ1:ν¯Σ1ν¯Σ2\widehat{F}|_{\overline{\nu}\Sigma_{1}}\colon\overline{\nu}\Sigma_{1}\to\overline{\nu}\Sigma_{2} is a diffeomorphism sending Σ1\Sigma_{1} to Σ2\Sigma_{2} and such that F^\widehat{F} is topologically isotopic rel. boundary to the identity map IdX\operatorname{Id}_{X}. The restriction of F^\widehat{F} to the surface exteriors is a homeomorphism, which we denote F:X1X2F\colon X_{1}\to X_{2}. By Gompf’s theorem [13], there exists a k0k\geq 0 and a diffeomorphism G:X1#WkX2#WkG\colon X_{1}\#W_{k}\to X_{2}\#W_{k} that agrees with FF on the boundary (Gompf’s theorem is not stated rel. boundary, but from his proof it is clear this conclusion is available). Write G^:XX\widehat{G}\colon X\to X for the diffeomorphism obtained by extending GG over the tubular neighbourhoods of the surfaces, using the diffeomorphism F^|ν¯Σ1:ν¯Σ1ν¯Σ2\widehat{F}|_{\overline{\nu}\Sigma_{1}}\colon\overline{\nu}\Sigma_{1}\to\overline{\nu}\Sigma_{2}.

In general, a homeomorphism of a compact 44-manifold (f,IdM):(M,M)(M,M)(f,\operatorname{Id}_{\partial M})\colon(M,\partial M)\to(M,\partial M) determines what is called in [18]*§2.2 a Poincaré variation. This is a certain homomorphism

Δf:H2(M,M)H2(M)\Delta_{f}\colon H_{2}(M,\partial M)\to H_{2}(M)

enjoying favourable interactions with Poincaré duality and algebraic properties; see [21] and [18] for more details. We will only need the property that a Poincaré variation recovers the ordinary map on absolute homology as

f=(IdΔfj):H2(M)H2(M),f_{*}=(\operatorname{Id}-\Delta_{f}\circ j)\colon H_{2}(M)\xrightarrow{\cong}H_{2}(M),

where jj is the map in the long exact sequence of the pair. Consider the Poincaré variation

(4) ΔFG1:H2(X2,X2)H2(X2)\Delta_{F\circ G^{-1}}\colon H_{2}(X_{2},\partial X_{2})\to H_{2}(X_{2})

induced by (FG1,IdX2):(X2,X2)(X2,X2)(F\circ G^{-1},\operatorname{Id}_{\partial X_{2}})\colon(X_{2},\partial X_{2})\to(X_{2},\partial X_{2}). By [21]*Theorem 3.7, there exists k0k\geq 0 and a diffeomorphism J:X2#WkX2#WkJ\colon X_{2}\#W_{k}\to X_{2}\#W_{k} with J|X2#Wk=IdX2#WkJ|_{\partial{X_{2}\#W_{k}}}=\operatorname{Id}_{\partial X_{2}\#W_{k}} realising the variation (4) smoothly stably

ΔJ=Δ(FG1)#IdWk=Δ(F#IdWk)(G1#IdWk).\Delta_{J}=\Delta_{(F\circ G^{-1})\#\operatorname{Id}_{W_{k}}}=\Delta_{(F\#\operatorname{Id}_{W_{k}})\circ(G^{-1}\#\operatorname{Id}_{W_{k}})}.

In particular, we have that JJ induces the homomorphism

(F#IdWk)(G#IdWk)1:H2(X2#Wk)H2(X2#Wk).(F\#\operatorname{Id}_{W_{k}})_{*}\circ(G\#\operatorname{Id}_{W_{k}})^{-1}_{*}\colon H_{2}(X_{2}\#W_{k})\to H_{2}(X_{2}\#W_{k}).

Write J^:X#WkX#Wk\widehat{J}\colon X\#W_{k}\to X\#W_{k} for the extension of JJ by the identity.

We now have a diffeomorphism

K^=J^G^:X#WkCX#Wk.\widehat{K}=\widehat{J}\circ\widehat{G}\colon X\#W_{k}\xrightarrow{\cong_{C^{\infty}}}X\#W_{k}.

that agrees agrees with F^\widehat{F} on restriction to ν¯Σ1\overline{\nu}\Sigma_{1}. Moreover, by construction, we have

(5) K^=(F^#IdWk):H2(X#Wk)H2(X#Wk).\widehat{K}_{*}=(\widehat{F}\#\operatorname{Id}_{W_{k}})_{*}\colon H_{2}(X\#W_{k})\to H_{2}(X\#W_{k}).

Components of the argument made in Boyer [3]*§4 now suffice to show K^\widehat{K} induces the identity map on H2(X#Wk)H_{2}(X\#W_{k}). We sketch the argument for the convenience of the reader. Set E:={xH2(X#Wk)|x[Σ1]=0}E:=\{x\in H_{2}(X\#W_{k})\,|\,x\cdot[\Sigma_{1}]=0\}. By  [3]*Lemma 4.1, we have E=Im(φj)E=\operatorname{Im}(\varphi_{j}) for j=1,2j=1,2, where φj:H2(Xj#Wk)H2(X#Wk)\varphi_{j}\colon H_{2}(X_{j}\#W_{k})\to H_{2}(X\#W_{k}) is the inclusion-induced map. We reproduce part of [3]*Figure 4.2, below, which is commutative diagram where the horizontal sequences are exact. Note, Boyer is using the diagram to construct a homeomorphism of the exteriors extending the map on the boundary, whereas we already have one, so the diagrams look a little different, but do agree.

0{\lx@inpgf@ignorespaces 0}H3(X#Wk,X1#Wk){\lx@inpgf@ignorespaces H_{3}(X\#W_{k},X_{1}\#W_{k})}H2(X1#Wk){\lx@inpgf@ignorespaces H_{2}(X_{1}\#W_{k})}E{\lx@inpgf@ignorespaces E}0{\lx@inpgf@ignorespaces 0}H3(ν¯Σ1,(X1#Wk)){\lx@inpgf@ignorespaces H_{3}(\overline{\nu}\Sigma_{1},\partial(X_{1}\#W_{k}))}H3(ν¯Σ2,(X2#Wk)){\lx@inpgf@ignorespaces H_{3}(\overline{\nu}\Sigma_{2},\partial(X_{2}\#W_{k}))}0{\lx@inpgf@ignorespaces 0}H3(X#Wk,X2#Wk){\lx@inpgf@ignorespaces H_{3}(X\#W_{k},X_{2}\#W_{k})}H2(X2#Wk){\lx@inpgf@ignorespaces H_{2}(X_{2}\#W_{k})}E{\lx@inpgf@ignorespaces E}0{\lx@inpgf@ignorespaces 0}K^\scriptstyle{\lx@inpgf@ignorespaces\widehat{K}_{*}}φ1\scriptstyle{\lx@inpgf@ignorespaces\varphi_{1}}K^\scriptstyle{\lx@inpgf@ignorespaces\widehat{K}_{*}}K^\scriptstyle{\lx@inpgf@ignorespaces\widehat{K}_{*}}\scriptstyle{\lx@inpgf@ignorespaces\cong}(F^#IdWk)\scriptstyle{\lx@inpgf@ignorespaces(\widehat{F}\#\operatorname{Id}_{W_{k}})_{*}}\scriptstyle{\lx@inpgf@ignorespaces\cong}φ2\scriptstyle{\lx@inpgf@ignorespaces\varphi_{2}}

A similar diagram could be produced, using the homeomorphism F^#IdWk\widehat{F}\#\operatorname{Id}_{W_{k}} in place of K^\widehat{K}. Using (5), we observe the left and central columns of such a diagram would then have the same maps as the left and central columns in our diagram. In a map of short exact sequences, the left and central vertical maps uniquely determine the right vertical map. Hence we conclude K^\widehat{K} and F^#IdWk\widehat{F}\#\operatorname{Id}_{W_{k}} induce the same map on EE. But F^\widehat{F} is topologically isotopic to the identity, and hence so is F^#IdWk\widehat{F}\#\operatorname{Id}_{W_{k}}. Thus the right vertical map in the diagram above is IdE\operatorname{Id}_{E}.

In the proof of [3]*Lemma 4.5, Boyer argues that the fact K^:H2(X#Wk)H2(X#Wk)\widehat{K}_{*}\colon H_{2}(X\#W_{k})\to H_{2}(X\#W_{k}) is the identity map on [Σ1][\Sigma_{1}] and on EE is enough to conclude it is the identity map overall. Briefly, in the case that the homology class [Σi][\Sigma_{i}] has nontrivial self-intersection, this follows because [Σ][\Sigma] and EE rationally generate H2(X#Wk)H_{2}(X\#W_{k}). In the case of trivial self-intersection H2(X#Wk)H_{2}(X\#W_{k}) is integrally generated by EE and an algebraic dual to [Σ1][\Sigma_{1}], which Boyer argues is enough for the conclusion. We refer the reader to [3]*Lemma 4.5 for full details of the argument.

By Quinn’s theorem [20] (with the correction in [8]), or alternatively Theorem 6.2, we thus have, possibly after further stabilisations of X#WkX\#W_{k}, that K^\widehat{K} is smoothly isotopic to the identity. ∎

Remark A.2.

In the introduction of [2], it was asserted that the combination of work Wall [25], Perron [19] and Quinn [20] would show homologous 22-spheres with simply-connected complement are topologically isotopic, and become smoothly isotopic in some stabilisation. In [1] it was asserted that the result of Proposition A.1 would follow from Perron [19] and Quinn [20]. We believe that in fact citations to Boyer and Saeki are also needed to make these arguments, as we explain next.

The statement that homologous surfaces with simply-connected complements in a simply-connected 44-manifold are topologically isotopic is a result due to Boyer [3]*Theorem F. In the proof, Boyer indeed appeals to the Perron–Quinn result that homeomorphisms of closed simply-connected 4-manifolds inducing the identity on second homology are topologically isotopic to the identity, however there is much work to be done before he can invoke that result.

For the statements that topological isotopy implies smooth stable isotopy, we think both implied proofs were intended to follow the structure of the proof we gave in Proposition A.1. We suspect Wall’s theorem [25] was intended to be used at the place where we invoked Saeki [21]. Wall’s theorem is insufficient to modify a diffeomorphism of a manifold with boundary, so this theorem cannot be applied in that way. Alternatively, one might try to apply Wall’s theorem after the surfaces have been filled back in, but this might void the carefully arranged condition that the diffeomorphism of the stabilised manifold sends Σ1\Sigma_{1} to Σ2\Sigma_{2}. So Saeki’s generalisation of Wall’s theorem to the case of nonempty boundary seems to be necessary.

References

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