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Trace Embeddings from Zero Surgery Homeomorphisms

Kai Nakamura University of Texas at Austin
Department of Mathematics
2515 Speedway. Austin, TX 78712 USA
[email protected]
Abstract.

Manolescu and Piccirillo recently initiated a program to construct an exotic S4S^{4} or #n2\#n\mathbb{CP}^{2} by using zero surgery homeomorphisms and Rasmussen’s ss-invariant [MP21]. They find five knots that if any were slice, one could construct an exotic S4S^{4} and disprove the Smooth 44-dimensional Poincaré conjecture. We rule out this exciting possibility and show that these knots are not slice. To do this, we use a zero surgery homeomorphism to relate slice properties of two knots stably after a connected sum with some 44-manifold. Furthermore, we show that our techniques will extend to the entire infinite family of zero surgery homeomorphisms constructed by Manolescu and Piccirillo. However, our methods do not completely rule out the possibility of constructing an exotic S4S^{4} or #n2\#n\mathbb{CP}^{2} as Manolescu and Piccirillo proposed. We explain the limits of these methods hoping this will inform and invite new attempts to construct an exotic S4S^{4} or #n2\#n\mathbb{CP}^{2}. We also show a family of homotopy spheres constructed by Manolescu and Piccirillo using annulus twists of a ribbon knot are all standard.

1. Introduction

1.1. Background

The study of 44-manifolds is distinguished by the remarkable difference between smooth and topological 44-manifolds compared to other dimensions. This manifests in the failure of Smale’s h-cobordism theorem which Smale used to prove the high dimensional Poincaré conjecture [Sma60]. This left open the 44-dimensional Poincaré conjecture which asserts that every smooth 44-manifold homotopy equivalent to S4S^{4}, i.e. a homotopy S4S^{4}, is homeomorphic to S4S^{4}. Freedman resolved the 44-dimensional Poincaré conjecture and showed that simply connected, smooth 44-manifolds are determined up to homeomorphism by their intersection forms [Fre82]. Donaldson contrasted this topological simplicity with his Diagonalization Theorem and showed that 44-manifolds do not smoothly admit such a straightforward classification [Don83]. The resulting study of 44-manifolds have yielded an abundance of exotic pairs of 44-manifolds: pairs of 44-manifolds homeomorphic, but not diffeomorphic to each other. Unique to dimension 44 are phenomena such as infinite families of exotic smooth structures on 4\mathbb{R}^{4} and small closed 44-manifolds such as 2#2¯2\mathbb{CP}^{2}\#2\overline{\mathbb{CP}}^{2} [Tau87, AP10]. Remarkably, this exotic behavior has not been shown to occur with the 44-sphere: the most basic example of a closed 44-manifold. This is the focus of the Smooth 44-dimensional Poincaré conjecture (SPC4).

Smooth 4-Dimensional Poincaré Conjecture (SPC4).

Every homotopy 44-sphere is diffeomorphic to the standard 44-sphere

The various flavors of the Poincaré conjecture motivated and revolutionized 20th century topology with SPC4 the last low dimensional case that remains unresolved.

Historically, the consensus among experts is that SPC4 is false due to the aforementioned exotica and the many constructions of homotopy spheres that are not known to be standard. The difficulty with exhibiting an exotic S4S^{4} is that the invariants used to distinguish smooth structures are typically known to vanish on homotopy 44-spheres. This changed with Rasmussen’s invention of his eponymous ss-invariant [Ras10], a slice obstruction coming from Khovanov Homology [Kho00]. A knot is smoothly slice if it is the boundary of a smooth properly embedded disk in B4B^{4}. Rasmussen defined the ss-invariant s(K)2s(K)\in 2\mathbb{Z} for any knot KK and showed that if s(K)0s(K)\neq 0, then KK is not slice. Unlike prior slice obstructions, it is not clear that the ss-invariant vanishes on knots slice in a homotopy ball other than B4B^{4}. In theory, one could show that a homotopy sphere Σ\Sigma is exotic by finding a knot KK slice in the homotopy ball Σint(B4)\Sigma-\mathop{\rm int}(B^{4}) and has s(K)0s(K)\neq 0. Then KK would not be slice in the standard B4B^{4} and sliceness of KK smoothly distinguishes Σ\Sigma from the standard S4S^{4}.

Freedman, Gompf, Morrison, and Walker (FGMW) attempted this strategy on the intensely studied family of Cappell-Shaneson spheres Σn\Sigma_{n}. They found knots slice in Σnint(B4)\Sigma_{n}-\mathop{\rm int}(B^{4}), hoping that one of these knots would have non-vanishing ss-invariant. They were only able to do the calculations for two of their knots and got zero for both [FGMW10]. Surprisingly, only six days after FGMW posted their results, Akbulut showed that all Σn\Sigma_{n} are standard [Akb10]. Indirectly, this shows that all of the knots FGMW considered had vanishing ss-invariant.

Piccirillo’s acclaimed proof that the Conway knot is not slice has renewed interest in the ss-invariant. Piccirillo’s proof takes advantage of and makes apparent the uniqueness of Rasmussen’s ss-invariant among other slice obstructions [Pic20]. It now seems more likely that the ss-invariant could be used to distinguish a homotopy sphere from S4S^{4}. However, the Cappell-Shaneson spheres Σn\Sigma_{n} were the most promising potentially exotic homotopy spheres. With Σn\Sigma_{n} now standardized, we are left with a dearth of homotopy spheres.

Recently, Piccirillo worked with Manolescu to revive this idea of FGMW to use the ss-invariant to find an exotic S4S^{4}. Unlike FGMW, they don’t use knots slice in a known homotopy sphere and in some sense, they reverse the FGMW approach. They propose a way to build a new homotopy sphere Σ\Sigma which comes with such a knot already. To construct an exotic S4S^{4}, they propose to take a pair of knots (K,K)(K,K^{\prime}) which satisfy three conditions:

K is slice,s(K)0,ϕ:S03(K)S03(K)K\text{ is slice},\ \ \ s(K^{\prime})\neq 0,\ \ \ \phi:S^{3}_{0}(K)\rightarrow S^{3}_{0}(K^{\prime})

This would allow one to construct a homotopy sphere Σ\Sigma where KK^{\prime} is slice in Σint(B4)\Sigma-\mathop{\rm int}(B^{4}). Then Σ\Sigma would have the properties that FGMW wanted and would be an exotic S4S^{4}. Manolescu and Piccirillo initiated a search for such a pair of knots, but did not find any that satisfied all three conditions. They did find pairs (K,K)(K,K^{\prime}) which have homeomorphic zero surgeries, s(K)<0s(K^{\prime})<0, and could not immediately determine the sliceness of KK. They conclude the following:

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((b))
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((c))
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((e))
Figure 1. If any are slice, then an exotic S4S^{4} exists. Figure 11 of [MP21].
Theorem (1.3 of [MP21]).

If any of the knots K1,,K5K_{1},\dots,K_{5} of Figure 1 are slice, then an exotic S4S^{4} exists.

SPC4 is a difficult, long open problem and disproving it by constructing an exotic S4S^{4} is an ambitious task. Another difficult, long open problem that might be more approachable is to construct an exotic positive definite 44-manifold. Historically, we have had more and earlier success constructing exotic 44-manifolds closer to positive definite with larger topology. In particular, it is easier to construct exotic 44-manifolds with larger b2(X)=rank(H2(X))b_{2}(X)=\mathop{\rm rank}(H_{2}(X)). We can adapt the above strategy to #n2\#n\mathbb{CP}^{2} using an adjunction inequality for the ss-invariant in #n2\#n\mathbb{CP}^{2} [MMSW19]. We now want KK to be HH-slice in #n2\#n\mathbb{CP}^{2}, that is KK should bound a null-homologous disk DD in #n2int(B4)\#n\mathbb{CP}^{2}-\mathop{\rm int}(B^{4}). To obstruct HH-sliceness of KK^{\prime} in #n2\#n\mathbb{CP}^{2}, we need s(K)<0s(K^{\prime})<0. Manolescu and Piccirillo again found pairs of knots in their search that satisfied all but one of the necessary conditions.

Theorem (1.4 of [MP21]).

If any of the knots K1,,K23K_{1},\dots,K_{23} are HH-slice in some #n2\#n\mathbb{CP}^{2}, then an exotic #n2\#n\mathbb{CP}^{2} exists111See Figure 2323 of [MP21] for K6,,K23K_{6},\dots,K_{23}.

1.2. Results

The knots K1,,K5K_{1},\dots,K_{5} are good candidates to be slice. They have Alexander polynomial 11 and are topologically slice by Freedman [Fre82], that is they bound topologically, locally flat disks in B4B^{4}. Therefore, all obstructions to topological sliceness automatically vanish on these knots. Many smooth concordance invariants such as Ozsváth-Szabó’s τ\tau-invariant and Rasmussen’s ss-invariant also vanish on them. In addition, the knots K1,,K5K_{1}^{\prime},\dots,K_{5}^{\prime} would be slice in a homotopy B4B^{4} and many of the necessary invariants vanish on these knots. At first thought, one would need new slice obstructions that are stronger than those currently available. Despite all of this we are able to show the following:

Theorem 1.1.

The knots K1,,K23K_{1},\dots,K_{23} are not slice. Furthermore, these knots are not HH-slice in any #n2\#n\mathbb{CP}^{2}.

The difficulty here is the vanishing of invariants that obstruct sliceness or HH-sliceness of KiK_{i}. This is the same problem that arises when trying to determine sliceness of the Conway knot. For the Conway knot, Piccirillo finds a knot KK that shares a zero trace with the Conway knot. Since sliceness is determined by the zero trace, the Conway knot is slice if and only if KK is slice. Calculating s(K)s(K) shows that KK is not slice and therefore the Conway knot is not slice [Pic20]. One might hope to extend the zero surgery homeomorphism S03(Ki)S03(Ki)S^{3}_{0}(K_{i})\rightarrow S^{3}_{0}(K_{i}^{\prime}) to a zero trace diffeomorphism. For many of these pairs, the zero surgery homeomorphisms do not extend and it appears they may never have homeomorphic traces. Without a trace diffeomorphism, we can’t access the trace embedding lemma to identify sliceness of KK and KK^{\prime}. Instead, we extend S03(Ki)S03(Ki)S^{3}_{0}(K_{i})\rightarrow S^{3}_{0}(K_{i}^{\prime}) to a diffeomorphism of the traces after blowing up. This allows us to relate their slice properties stably and work with HH-sliceness of KiK_{i}^{\prime} instead of the difficult KiK_{i}.

Manolescu and Piccirillo considered an infinite six parameter family of zero surgery homeomorphisms. They found the knots K1,,K23K_{1},\dots,K_{23} by checking 33753375 zero surgery homeomorphisms in this family. One might try to expand the search and consider more pairs from this family. We show that such an effort would be in vain and prove a stronger version of Theorem 1.1.

Theorem 1.2.

Let (K,K)(K,K^{\prime}) be a pair of knots with homeomorphic zero surgeries from the Manolescu-Piccirillo family.

  1. (1)

    If KK is HH-slice in some #n2\#n\mathbb{CP}^{2}, then s(K)0s(K^{\prime})\geq 0.

  2. (2)

    If KK is HH-slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}, then s(K)0s(K^{\prime})\leq 0.

  3. (3)

    If KK is slice, then s(K)=0s(K^{\prime})=0.

This is proved in a more general form in Theorem 3.9. This theorem rules out finding an exotic S4S^{4} (or #n2\#n\mathbb{CP}^{2}) using the ss-invariant and zero surgery homeomorphisms from the Manolescu-Piccirillo family. This does not show the stronger statement that such (K,K)(K,K^{\prime}) can not be used to construct an exotic S4S^{4}. In principal, a (K,K)(K,K^{\prime}) from the Manolescu-Piccirillo family could still have KK slice and KK^{\prime} not slice. Such a pair would exhibit an exotic S4S^{4}, but this theorem shows that the ss-invariant s(K)s(K^{\prime}) would not obstruct sliceness and detect exoticness.

In Theorem 3.13, we attempt to generalize the above theorem assuming a conjectural inequality for Rasmussen’s ss-invariant. We establish conditions on when these methods apply and would rule out using the ss-invariant with zero surgery homeomorphisms to construct an exotic S4S^{4} or #n2\#n\mathbb{CP}^{2}. These methods are not special to the ss-invariant and might also apply to other obstructions to HH-sliceness in #n2\#n\mathbb{CP}^{2} or other 44-manifolds. As new and stronger concordance invariants are inevitably constructed, there will surely be new attempts to construct exotic 44-manifolds using HH-sliceness and zero surgery homeomorphisms. Such hypothetical future attempts will likely need to revisit this work.

Our methods do not apply to all zero surgery homeomorphisms and leaves hope that the ss-invariant could be used to find an exotic S4S^{4} or #n2\#n\mathbb{CP}^{2}. We construct an infinite family of zero surgery homeomorphisms which are not susceptible to our methods. These zero surgery homeomorphisms are not a serious attempt at constructing an exotic S4S^{4} or #n2\#n\mathbb{CP}^{2}. Instead they are an illustration of the continued viability of Manolescu and Piccirillo’s approach and an invitation to the topological community to continue it.

Manolescu and Piccirillo also consider pairs of knots (K,K)(K,K^{\prime}) which have have homeomorphic 0-surgeries, KK is slice, and KK^{\prime} has indeterminate sliceness. They give a family of knots {Jn|n}\{J_{n}\ |\ n\in\mathbb{Z}\} related by annulus twist homeomorphisms ϕn:S03(J0)S03(Jn)\phi_{n}:S^{3}_{0}(J_{0})\rightarrow S^{3}_{0}(J_{n}). J0J_{0} bounds a ribbon disk and this gives a family of homotopy spheres Zn=E(D)ϕnX0(Jn)Z_{n}=E(D)\cup_{\phi_{n}}-X_{0}(J_{n}).

Theorem 1.3.

The homotopy 44-spheres ZnZ_{n} are all diffeomorphic to S4S^{4} (and therefore each JnJ_{n} is slice).

To prove this, we draw these manifolds upside down as X0(Jn)E(D)X_{0}(J_{n})\cup-E(D). Drawing the exterior upside down directly with the standard algorithm is difficult and results in a complicated diagram. Instead we will describe an algorithm for any ribbon knot KK bounding a ribbon disk DD, how to draw a Kirby diagram of S4S^{4} as X0(K)E(D)X_{0}(K)\cup-E(D). We can then use this to draw a Kirby diagram of Zn-Z_{n} showing the trace embedding X0(Jn)ZnX_{0}(J_{n})\subset-Z_{n}. Using this diagram of Zn-Z_{n}, we then show that each ZnZ_{n} is standard.

1.3. Conventions

All manifolds are smooth and oriented. Any embeddings or homeomorphism are orientation preserving. Boundaries are oriented with outward normal first. All homology groups have integral coefficients.

1.4. Acknowledgments

The author would like to thank Ciprian Manolescu and Lisa Piccirillo for helpful correspondences as well as for allowing the author to use the images in Figure 1. The author would also like to thank his advisors Bob Gompf and John Luecke for their help and support. As noted in [MP21], some cases of the above results were already established by others. Dunfield and Gong showed that K6,,K21K_{6},\dots,K_{21} are not slice using their program to compute twisted Alexander polynomial [DG] and Kyle Hayden showed that Z1Z_{1} is standard

2. Preliminaries

2.1. H-slice Knots and Zero Surgery Homeomorphisms

We will need to recall Manolescu and Piccirillo’s proposed construction of an exotic S4S^{4} or #n2\#n\mathbb{CP}^{2}. To simplify the discussion, we combine these cases into one and define #02\#0\mathbb{CP}^{2} to be S4S^{4} via the empty connected sum. Whenever #n2\#n\mathbb{CP}^{2} appears it will be implicit that n0n\geq 0 and likewise with #n¯2\#n\overline{\mathbb{CP}}^{2}.

Let XX be a smooth, closed, oriented 44-manifold and let X=Xint(B4)X^{\circ}=X-\mathop{\rm int}(B^{4}).

Definition 2.1.

A knot KS3K\subset S^{3} is said to be HH-slice in XX^{\circ} or XX if KK is the boundary of a smoothly, properly embedded disk DD in XX^{\circ} such that [D]=0H2(X,X)[D]=0\in H_{2}(X^{\circ},\partial X^{\circ}).

HH-sliceness is a generalization of sliceness: a knot is slice (in B4B^{4}) if and only if it is HH-slice in S4S^{4}. Recall that the kk-trace Xk(K)X_{k}(K) of KK is obtained by attaching a 22-handle to B4B^{4} along KK with framing kk. The classical trace embedding lemma asserts a knot KK is slice if and only if the zero trace X0(K)X_{0}(K) smoothly embeds in S4S^{4}. We have an analogous statement for a knot to be HH-slice in XX.

Lemma 2.2 (H-slice Trace Embedding Lemma, Lemma 3.5 of [MP21]).

A knot KK is HH-slice in XX if and only if X0(K)-X_{0}(K) smoothly embeds in XX by an embedding that induces the zero map on second homology.

Suppose KK is HH-slice in XX with HH-slice disk DXD\subset X^{\circ} and there is a zero surgery homeomorphism ϕ:S03(K)S03(K)\phi:S^{3}_{0}(K)\rightarrow S^{3}_{0}(K^{\prime}). Let ν(D)\nu(D) be a tubular neighborhood of DD and let the exterior of DD be E(D)=Xν(D)E(D)=X^{\circ}-\nu(D). The exterior naturally has boundary S03(K)S^{3}_{0}(K) and we can define X=E(D)ϕX0(K)X^{\prime}=E(D)\cup_{\phi}-X_{0}(K^{\prime}). KK^{\prime} is HH-slice in XX^{\prime} by Lemma 2.2 and if XX is simply connected, XX^{\prime} is homeomorphic to XX (Lemma 3.33.3 of [MP21]). If KK^{\prime} is not HH-slice in XX, then HH-sliceness of KK^{\prime} smoothly distinguishes XX^{\prime} from XX.

Constructing an exotic #n2\#n\mathbb{CP}^{2} with zero surgery homeomorphisms sounds promising, but there are difficulties with this approach which have only recently been resolved. The first challenge was overcoming the Akbulut-Kirby conjecture which asserts that knots with homeomorphic zero surgeries are concordant. HH-sliceness is preserved by concordance and therefore this construction would be more difficult than producing counterexamples to the Akbulut-Kirby conjecture. Fortunately, Yasui disproved the Akbulut-Kirby conjecture in 20152015. In doing so, he showed that concordance invariants, such as the Ozsváth-Szabó τ\tau-invariant or Rasmussen’s ss-invariant, could distinguish knots in concordance that share a zero surgery [Yas15].

This brings us to the second difficulty with this strategy. We need to obstruct HH-sliceness of KK^{\prime} in the standard #n2\#n\mathbb{CP}^{2} without obstructing HH-sliceness of KK in a homotopy #n2\#n\mathbb{CP}^{2}. Obstruction from gauge and Floer theoretic concordance invariants, like the τ\tau-invariant, tend to apply in any homotopy #n2\#n\mathbb{CP}^{2} [OS03]. In particular, such invariants always vanish on knots slice in a homotopy S4S^{4}. However, Rasmussen’s ss-invariant does provide an obstruction to HH-sliceness in #n2\#n\mathbb{CP}^{2} that may not hold in a homotopy #n2\#n\mathbb{CP}^{2}.

Lemma 2.3 (Theorem 1.81.8 of [MMSW19]).

If Σ#n2(int(B4)int(B4))\Sigma\subset\#n\mathbb{CP}^{2}-(\mathop{\rm int}(B^{4})\sqcup\mathop{\rm int}(B^{4})) is a null homologous, oriented cobordism from a link L1L_{1} to L2L_{2} with each component of Σ\Sigma having a boundary component in L1L_{1}, then s(L2)s(L1)χ(Σ)s(L_{2})-s(L_{1})\geq\chi(\Sigma). In particular, if a knot KK is HH-slice in some #n2\#n\mathbb{CP}^{2}, then s(K)0s(K)\geq 0.

By reversing orientation, we see that if KK is HH-slice in #n¯2\#n\overline{\mathbb{CP}}^{2}, then s(K)0s(K)\leq 0. Furthermore, if KK is HH-slice in #n¯2\#n\overline{\mathbb{CP}}^{2} and #n2\#n\mathbb{CP}^{2} for some nn, then s(K)=0s(K)=0. Such knots are called biprojectively H-slice by Manolescu and Piccirillo. These include all slice knots and some non-slice knots like the figure eight knot.

Putting this together, we can construct an exotic #n2\#n\mathbb{CP}^{2} if we have a pair of knots (K,K)(K,K^{\prime}) such that

K is H-slice in #n2,s(K)<0,ϕ:S03(K)S03(K)K\text{ is H-slice in }\#n\mathbb{CP}^{2},\ \ \ s(K^{\prime})<0,\ \ \ \phi:S^{3}_{0}(K)\rightarrow S^{3}_{0}(K^{\prime})

For HH-sliceness in #02=S4\#0\mathbb{CP}^{2}=S^{4}, i.e. standard sliceness, we could also consider s(K)0s(K^{\prime})\neq 0 to obstruct sliceness. However, Manolescu and Piccirillo focus on negative s(K)s(K^{\prime}) and in their search find no viable examples with positive s(K)s(K^{\prime}).

Recall that a framed knot is a knot KK in S3S^{3} together with a framing kk\in\mathbb{Z}. We will denote a framed knot by (K,k)(K,k) and extend this naturally to framed links. To conduct their search, Manolescu and Piccirillo need a source of zero surgery homeomorphisms and so they define special RBG-links.

Definition 2.4.

A special RBG-link L=(R,r)(B,0)(G,0)S3L=(R,r)\cup(B,0)\cup(G,0)\subset S^{3} is a three component integrally framed link where RR has framing rr\in\mathbb{Z}, BB and GG have framing b=g=0b=g=0. Furthermore, surgery on this framed link has H1(Sr,0,03(R,B,G))=H_{1}(S^{3}_{r,0,0}(R,B,G))=\mathbb{Z} and if μR\mu_{R} is a meridian of RR, there exist link isotopies

RGRμRRBR\cup G\cong R\cup\mu_{R}\cong R\cup B

Given a special RBG-link we can define a pair of knots and a zero surgery homeomorphism between them. The following proposition and its proof is the first half of Theorem 1.21.2 of [MP21] for a special RBG-link. We reproduce it here because understanding the special RBG-link construction will be fundamental to proving our key lemmas.

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Figure 2. Initial slide used to exhibit KBK_{B}
Proposition 2.5.

For any special RBG-link LL, there is an associated pair of knots KBK_{B} and KGK_{G} and a homeomorphism ϕL:S03(KB)S03(KG)\phi_{L}:S^{3}_{0}(K_{B})\rightarrow S^{3}_{0}(K_{G}).

Proof.

The assumption that (G,0)(G,0) is zero framed meridian of (R,r)(R,r) implies there is a slam dunk homeomorphism ψB:Sr,03(R,G)S3\psi_{B}:S^{3}_{r,0}(R,G)\rightarrow S^{3}. Let KB=ψB(B)K_{B}=\psi_{B}(B), the slam dunk homeomorphism takes a framing on BB to a framing on KBK_{B} that surgers to Sr,b,g3(R,B,G)S^{3}_{r,b,g}(R,B,G). The assumption on homology implies that this must be the zero framing. Reusing notation, the slam dunk on (R,r)(G,0)(R,r)\cup(G,0) induces a homeomorphism ψB:Sr,b,g3(R,B,G)S03(KB)\psi_{B}:S^{3}_{r,b,g}(R,B,G)\rightarrow S^{3}_{0}(K_{B}). We can do the same with (G,0)(G,0) by slam dunking (R,r)(B,0)(R,r)\cup(B,0) to get a homeomorphism ψG:Sr,b,g3(R,B,G)S03(KG)\psi_{G}:S^{3}_{r,b,g}(R,B,G)\rightarrow S^{3}_{0}(K_{G}) and the desired homeomorphism is then ϕL=ψBψG1:S03(KB)S03(KG)\phi_{L}=\psi_{B}\circ\psi_{G}^{-1}:S^{3}_{0}(K_{B})\rightarrow S^{3}_{0}(K_{G}). ∎

Given a diagram of LL, we can perform this construction diagrammatically. We take LL to be a surgery diagram of Sr,b,g3(R,B,G)S^{3}_{r,b,g}(R,B,G) and slam dunk (R,r)(G,0)(R,r)\cup(G,0). To do this, first isotope (G,0)(G,0) into meridianal position so (G,0)(G,0) bounds a disk ΔG\Delta_{G}. This disk intersects (B,0)(B,0) in some number of points as shown in Figure 2(a). Slide (B,0)(B,0) over (R,r)(R,r) so that it no longer intersects ΔG\Delta_{G} as shown in Figure 2(b). To finish the slam dunk, delete (R,r)(R,r) and (G,0)(G,0) leaving (KB,0)(K_{B},0).

2.2. Projective Slice Framings

Let WW be a smooth, closed, oriented 44-manifold. If DD is a disk properly embedded in WW^{\circ}, then DD has a well defined tubular neighborhood ν(D)=D×2\nu(D)=D\times\mathbb{R}^{2}. Then D=D×{0}D=D\times\{0\} has a parallel pushoff D=D×{p}ν(D)D^{*}=D\times\{p\}\subset\nu(D) for some nonzero pp. K=DK^{*}=\partial D^{*} is a knot parallel to KK and defines a framing on KK.

Definition 2.6.

A framed knot (K,k)(K,k) in S3S^{3} is said to be slice in WW or WW^{\circ} if KK is the boundary of a disk DD smoothly, properly embedded in WW which induces the framing kk on KK.

If we say KK is kk-slice in WW with kk\in\mathbb{Z}, then we mean (K,k)(K,k) is slice in WW. This framing kk will be equal to the negative of the self intersection number of DD, i.e. k=[D][D]k=-[D]\cdot[D]. The exterior E(D)=Wν(D)E(D)=W^{\circ}-\nu(D) of DD has boundary E(D)\partial E(D) naturally identified with Sk3(K)S^{3}_{k}(K). We can view the deleted ν(D)\nu(D) and int(B4)int(B^{4}) as a trace and get a trace embedding lemma.

Lemma 2.7 (Framed Trace Embedding Lemma, Lemma 3.3 of [HP21]).

A framed knot (K,k)(K,k) in S3S^{3} is smoothly slice in WW if and only if Xk(K)-X_{k}(K) smoothly embeds in WW.

This will allow us later to construct framed slice disks by finding trace embeddings. We will be working with framed slice disks in #n¯2\#n\overline{\mathbb{CP}}^{2} and in this setting, it is often more practical to construct the disks directly. To construct knots HH-slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}, one can use a full positive twist along algebraically zero strands as in Lemma 3.23.2 of [MP21]. This generalizes to framed sliceness, but now we need to keep track of how the framing changes.

Lemma 2.8.

Suppose (K,k)(K,k) is the framed boundary of a disk DWD\subset W^{\circ} and Δ\Delta a disk embedded in S3S^{3} intersecting KK transversely in \ell points counted with sign. Let K+K_{+} be a knot obtained from KK by performing a positive full twist through Δ\Delta, then (K+,k+2)(K_{+},k+\ell^{2}) is slice in W#¯2W\#\overline{\mathbb{CP}}^{2}.

Proof.

Attach a 1-1 framed 22-handle to WW^{\circ} along Δ\partial\Delta to get W(Δ,1)2h=(W#¯2)W^{\circ}\cup_{(\partial\Delta,-1)}2h=(W\#\overline{\mathbb{CP}}^{2})^{\circ}. Then DD in W(Δ,1)2hW^{\circ}\cup_{(\partial\Delta,-1)}2h has boundary (K,k)S13(Δ)(K,k)\subset S^{3}_{-1}(\partial\Delta) and a blowdown of (Δ,1)(\partial\Delta,-1) identifies it with (K+,k+2)(K_{+},k+\ell^{2}). ∎

The above lemma can be used to show that an arbitrary knot KK will be slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}. First observe that a crossing change can be realized as a positive twist on two strands. Then a sequence of crossing changes that unknot KK can be used to construct a slice disk DD for KK with some framing in #n¯2\#n\overline{\mathbb{CP}}^{2}. Our arguments require checking that certain framed knots associated to a zero surgery homeomorphism are slice in some #n¯2\#n\overline{\mathbb{CP}}^{2} or #n2\#n\mathbb{CP}^{2}. To quantify this we define the projective slice framings.

Definition 2.9.

Let KK be a knot in S3S^{3}. The positive projective slice framing 𝔽+(K)\mathbb{PF}_{+}(K) of KK is the smallest framing kk such that (K,k)(K,k) is slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}. The negative projective slice framing 𝔽(K)\mathbb{PF}_{-}(K) is defined analogously.

Homological considerations imply that a strictly negative framed knot cannot be slice in a negative definite 44-manifold and therefore 𝔽+(K)0\mathbb{PF}_{+}(K)\geq 0. Furthermore, in a negative definite 44-manifold, the only homology class with self intersection number zero is the zero homology class.

Lemma 2.10.

𝔽+(K)=0\mathbb{PF}_{+}(K)=0 if and only if KK is HH-slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}. 𝔽(K)=0\mathbb{PF}_{-}(K)=0 if and only if KK is HH-slice in some #n2\#n\mathbb{CP}^{2}. 𝔽+(K)=𝔽(K)=0\mathbb{PF}_{+}(K)=\mathbb{PF}_{-}(K)=0 if and only if KK is biprojectively HH-slice. ∎

Once we have one of these framings, Lemma 2.8 immediately realizes any framing larger than 𝔽+(K)\mathbb{PF}_{+}(K). Take DD a disk realizing 𝔽+(K)\mathbb{PF}_{+}(K) and Δ\Delta a meridianal disk of KK.

Corollary 2.11.

If k𝔽+(K)k\geq\mathbb{PF}_{+}(K), then (K,k)(K,k) is slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}. If k𝔽(K)k\leq\mathbb{PF}_{-}(K), then (K,k)(K,k) is slice in some #n2\#n\mathbb{CP}^{2}. ∎

We can construct framed slice disks in #n¯2\#n\overline{\mathbb{CP}}^{2}, but we would also like to have lower bounds on these framings as well. To do so, we can use the adjunction inequality for the Ozsváth-Szabó τ\tau-invariant.

Lemma 2.12 (Theorem 1.1 of [OS03]).

Let WW be a smooth 44-manifold with negative definite intersection form, b1(W)=0b_{1}(W)=0, and W=S3\partial W=S^{3}. Let e1,,ene_{1},\dots,e_{n} be an orthonormal basis for H2(W)H_{2}(W) and if α=s1e1+snen\alpha=s_{1}e_{1}+\dots s_{n}e_{n}, then let |α|=|s1|++|sn||\alpha|=|s_{1}|+\dots+|s_{n}|. If Σ\Sigma is smooth, properly embedded surface in WW with boundary W=K\partial W=K, then we have the following inequality:

2τ(K)+|[Σ]|+[Σ][Σ]2g(Σ)2\tau(K)+|[\Sigma]|+[\Sigma]\cdot[\Sigma]\leq 2g(\Sigma)
Corollary 2.13.
𝔽(K)+|𝔽(K)|2τ(K)𝔽+(K)𝔽+(K)\mathbb{PF}_{-}(K)+\sqrt{|\mathbb{PF}_{-}(K)|}\leq 2\tau(K)\leq\mathbb{PF}_{+}(K)-\sqrt{\mathbb{PF}_{+}(K)}
Proof.

Let Σ\Sigma be a disk in #n¯2int(B4)\#n\overline{\mathbb{CP}}^{2}-int(B^{4}) with framed boundary (K,k)(K,k) and let x=2τ(K)x=2\tau(K). We have [Σ][Σ]=k[\Sigma]\cdot[\Sigma]=-k and so x+|[Σ]|kx+|[\Sigma]|\leq k by Lemma 2.12. We see that k=s12++sn2(|s1|++|sn|)2=|[Σ]|2k=s_{1}^{2}+\dots+s_{n}^{2}\leq(|s_{1}|+\cdots+|s_{n}|)^{2}=|[\Sigma]|^{2}, therefore k|[Σ]|\sqrt{k}\leq|[\Sigma]| and xkkx\leq k-\sqrt{k}. ∎

There is an analogous adjunction inequality conjectured for the ss-invariant.

Conjecture 2.14 (Conjecture 9.8 of [MMSW19]).

If Σ\Sigma is smooth, properly embedded surface in W=#n¯2int(B4)W=\#n\overline{\mathbb{CP}}^{2}-int(B^{4}) with boundary Σ=K\partial\Sigma=K, then we have the following inequality:

s(K)+|[Σ]|+[Σ][Σ]2g(Σ)s(K)+|[\Sigma]|+[\Sigma]\cdot[\Sigma]\leq 2g(\Sigma)

[MMSW19] proved this in the nullhomologous case and conjectured this in analogy to the adjunction inequality for τ(K)\tau(K). We replace 2τ(K)2\tau(K) with s(K)s(K) like their slice genus bounds, but we limit this conjecture to W=#n¯2int(B4)W=\#n\overline{\mathbb{CP}}^{2}-\mathop{\rm int}(B^{4}). It’s not clear how to approach Conjecture 2.14 for arbitrary negative definite WW or even if it should hold in such WW. However, if this conjecture holds, we can replace x=2τ(K)x=2\tau(K) with s(K)s(K) throughout the proof of Corollary 2.13. When KK is (1)(-1)-slice in some #n2\#n\mathbb{CP}^{2}, we conjecturally get the same restriction on s(K)s(K) as we did when KK is HH-slice is some #n2\#n\mathbb{CP}^{2}.

Conjecture 2.15.

If KK is (1)(-1)-slice in some #n2\#n\mathbb{CP}^{2}, then s(K)0s(K)\geq 0.

3. Construction of Trace Embeddings

3.1. Obstructing H-sliceness of K1,,K23K_{1},\dots,K_{23} in #n2\#n\mathbb{CP}^{2}

In this subsection, we show that K1,,K23K_{1},\dots,K_{23} are not slice, nor are they H-slice in any #n2\#n\mathbb{CP}^{2}. To do this, we will relate H-sliceness of KiK_{i} in #n2\#n\mathbb{CP}^{2} stably with KiK_{i}^{\prime} after a connected sum with some #r2\#r\mathbb{CP}^{2}. We see this first at the level of traces as a stable trace diffeomorphism.

Lemma 3.1.

Let WW be a smooth, closed, oriented 44-manifold and L=(R,r)(B,0)(G,0)L=(R,r)\cup(B,0)\cup(G,0) be a special RBG-link with associated zero surgery homeomorphism ϕL:S03(KB)S03(KG)\phi_{L}:S^{3}_{0}(K_{B})\rightarrow S^{3}_{0}(K_{G}). If (R,r)(R,r) is slice in WW, then ϕL\phi_{L} extends to a diffeomorphism ΦL:X0(KB)#WX0(KG)#W\Phi_{L}:X_{0}(K_{B})\#W\cong X_{0}(K_{G})\#W

This is a generalization of techniques [Akb77, Pic19, Pic20] used to construct trace diffeomorphisms. The (R,r)=(U,0)(R,r)=(U,0) slice in B4B^{4} case of the lemma is the dualizable link construction and its proof is insightful here. Construct a Kirby diagram by placing a dot on RR and attaching 22-handles to BB and GG. Cancelling the dotted RR with BB or GG diagrammatically is a slam dunk resulting in X0(KG)X_{0}(K_{G}) and X0(KB)X_{0}(K_{B}) respectively. The framed sliceness of (R,r)(R,r) in WW allows us to “dot” (R,r)(R,r) and proceed in a similar manner.

Proof.

Let ZZ be the 44-manifold obtained from WW^{\circ} by removing a neighborhood ν(D)\nu(D) of a slice disk DD for (R,r)(R,r) and attaching 22-handles to (B,0)(B,0) and (G,0)(G,0). This description naturally identifies Z\partial Z as Sr,0,03(R,B,G)S^{3}_{r,0,0}(R,B,G). The 22-handle attached to (G,0)(G,0) fills E(D)E(D) because (G,0)(G,0) is isotopic to (μR,0)(\mu_{R},0). This is a diffeomorphism ΨB:E(D)(G,0)2hW\Psi_{B}:E(D)\cup_{(G,0)}2h\rightarrow W^{\circ} extending the slam dunk homeomorphism ψB:Sr,03(R,G)S3\psi_{B}:S^{3}_{r,0}(R,G)\rightarrow S^{3}. The 22-handle that was attached to (B,0)(B,0) is now attached to ψB(B,0)=(KB,0)\psi_{B}(B,0)=(K_{B},0) and therefore ΨB\Psi_{B} induces a diffeomorphism of ZZ and W(KB,0)2hW^{\circ}\cup_{(K_{B},0)}2h . Observe that W=B4#WW^{\circ}=B^{4}\#W and W(KB,0)2hW^{\circ}\cup_{(K_{B},0)}2h is simply X0(KB)#WX_{0}(K_{B})\#W. Reusing notation, we have a diffeomorphism from ΨB:ZX0(KB)#W\Psi_{B}:Z\rightarrow X_{0}(K_{B})\#W extending the homeomorphism ψB:Sr,0,03(R,B,G)S03(KB)\psi_{B}:S^{3}_{r,0,0}(R,B,G)\rightarrow S^{3}_{0}(K_{B}). Repeating this with GG instead and composing, we have the desired diffeomorphism ΦL=ΨBΨG1:X0(KB)#WX0(KG)#W\Phi_{L}=\Psi_{B}\circ\Psi_{G}^{-1}:X_{0}(K_{B})\#W\cong X_{0}(K_{G})\#W extending the homeomorphism ϕL=ψBψG1\phi_{L}=\psi_{B}\circ\psi_{G}^{-1}. ∎

When a zero surgery homeomorphism extends to a zero trace diffeomorphism, the HH-slice trace embedding lemma identifies the HH-sliceness of the two knots. If the zero surgery homeomorphism doesn’t extend, Lemma 3.1 sometimes allows us to extend to a diffeomorphism after a connected sum with W-W. This makes the trace embedding lemma available and allows us to relate HH-sliceness of the two knots.

Corollary 3.2.

Let XX be a smooth, closed, oriented 44-manifold. Suppose KBK_{B} is HH-slice in XX and KGK_{G} is then HH-slice in X=E(D)ϕLX0(KG)X^{\prime}=E(D)\cup_{\phi_{L}}-X_{0}(K_{G}). If (R,r)(R,r) is slice in WW, then X#WX^{\prime}\#-W is diffeomorphic to X#WX\#-W and therefore KGK_{G} is HH-slice in X#WX\#-W. ∎

Now we are ready to prove our first theorem.

Theorem 3.3.

The knots K1,,K23K_{1},\dots,K_{23} are not slice nor are they HH-slice in any #n2\#n\mathbb{CP}^{2}.

Proof.

By looking at Figure 1313 and Table 11 of [MP21], we see that each KiK_{i} arise from a special RBG-link where R=UR=U and r=a+b0r=a+b\geq 0. We have (R,r)=(U,r)(R,r)=(U,r) is slice in W=#r¯2W=\#r\overline{\mathbb{CP}}^{2} and if KiK_{i} is HH-slice in #n2\#n\mathbb{CP}^{2}, then KiK_{i}^{\prime} is HH-slice in #(n+r)2\#(n+r)\mathbb{CP}^{2} by Corollary 3.2. These knots have s(Ki)=2s(K_{i}^{\prime})=-2 which contradicts Lemma 2.3 and therefore KiK_{i} could not have been HH-slice in #n2\#n\mathbb{CP}^{2} in the first place. ∎

Remark 3.4.

For the knots in question, the diffeomorphism ΦL:X0(KG)#r¯2X0(KB)#r¯2\Phi_{L}:X_{0}(K_{G})\#r\overline{\mathbb{CP}}^{2}\cong X_{0}(K_{B})\#r\overline{\mathbb{CP}}^{2} can also be seen diagrammatically. Take LL and perform negative blow ups to (R,r)(R,r) turning it into a zero framed unknot (R,0)(R,0) with rr meridians (R1,1),,(Rr,1)(R_{1},-1),\dots,(R_{r},-1). This new framed link still describes the same zero surgery homeomorphism. Slam dunk (R,0)(R,0) with (B,0)(B,0) or (G,0)(G,0) and blow down (R1,1),,(Rr,1)(R_{1},-1),\dots,(R_{r},-1) to get (KG,0)(K_{G},0) or (KB,0)(K_{B},0) respectively (think of this as an RBG-link generalized to have RR be a framed link). Form a Kirby diagram by putting a dot on RR and attaching 22-handles to the other components. Now cancelling the dotted (R,0)(R,0) with (B,0)(B,0) or (G,0)(G,0) and sliding (R1,1),,(Rr,1)(R_{1},-1),\dots,(R_{r},-1) away results in X0(KG)#r¯2X_{0}(K_{G})\#r\overline{\mathbb{CP}}^{2} or X0(KB)#r¯2X_{0}(K_{B})\#r\overline{\mathbb{CP}}^{2} respectively.

We have dispensed of the main question relatively quickly and have shown that K1,,K23K_{1},\dots,K_{23} are not slice or HH-slice in any #n2\#n\mathbb{CP}^{2}. However, to prove this we needed that the associated special RBG-links all had r0r\geq 0. If we had negative r<0r<0 instead, then (R,r)(R,r) would be slice in #|r|2\#|r|\mathbb{CP}^{2}. If KK was HH-slice in #n2\#n\mathbb{CP}^{2}, then KK^{\prime} would be HH-slice in #n2#|r|¯2\#n\mathbb{CP}^{2}\#|r|\overline{\mathbb{CP}}^{2} by Corollary 3.2. This would not contradict s(K)<0s(K^{\prime})<0 and our proof would not work. It seems quite mysterious that we had this necessary condition on rr for all 2323 pairs of knots. Fortunately, we can explain this and do so in the following subsection. Before we proceed, we take a short detour to provide a generalization of Corollary 3.2 from special RBG-links to arbitrary zero surgery homeomorphisms. One can safely skip to the next subsection, but this method may offer some useful benefits in practice.

Lemma 3.5.

Let ϕ:S03(K)S03(K)\phi:S^{3}_{0}(K)\rightarrow S^{3}_{0}(K^{\prime}) be a zero surgery homeomorphism and represent ϕ1(μK,0)S03(K)\phi^{-1}(\mu_{K^{\prime}},0)\subset S^{3}_{0}(K) as some framed knot (m,k)(m,k) in S3S^{3}. If KK is HH-slice in XX and (m,k)(m,k) is slice in some 44-manifold WW, then KK^{\prime} is HH-slice in X#WX\#-W.

Proof.

By turning the handle decomposition of X0(K)X_{0}(K^{\prime}) upside down, one can obtain XX^{\prime} from E(D)E(D) by attaching a 22-handle to (m,k)(m,k) and capping off with a 44-handle. We can regard (X)(X^{\prime})^{\circ} as XX^{\prime} with a 44-handle deleted and (X)=E(D)(m,k)2h(X^{\prime})^{\circ}=E(D)\cup_{(m,k)}2h. This can be used to build the following sequence of inclusions:

X0(K)(X)=E(D)(m,k)2hX(m,k)2h=X#Xk(m)X#W-X_{0}(K^{\prime})\subset(X^{\prime})^{\circ}=E(D)\cup_{(m,k)}2h\subset X^{\circ}\cup_{(m,k)}2h=X\#X_{k}(m)\subset X\#-W

The first inclusion comes from the HH-slice trace embedding lemma and the second inclusion is induced by E(D)XE(D)\subset X^{\circ}. As we observed in the proof of Lemma 3.1, X(m,k)2hX^{\circ}\cup_{(m,k)}2h is simply X#Xk(m)X\#X_{k}(m). The final inclusion comes from the framed trace embedding lemma with (m,k)(m,k) slice in WW. The composition is a nullhomologous trace embedding of X0(K)-X_{0}(K^{\prime}) into X#WX\#-W and therefore KK^{\prime} is HH-slice in X#WX\#-W. ∎

For a special RBG-link homeomorphism, one can take (m,k)(m,k) to be (R,r)(R,r). This recovers the conclusion of Corollary 3.2 and gives another proof of Theorem 3.3. However, we do not get a stable diffeomorphism X#WX#WX^{\prime}\#-W\cong X\#-W like in Corollary 3.2. The advantage of this is that it does not need a special RBG-link and has the further benefit that the input data is more malleable. It seems non-trivial to find special RBG-links representing a given zero surgery homeomorphism with a different (R,r)(R,r). However, (m,k)(m,k) was a choice of diagrammatic representative of ϕ1(μK,0)S03(K)\phi^{-1}(\mu_{K^{\prime}},0)\subset S^{3}_{0}(K) and can be modified via slides over KK.

3.2. The Manolescu-Piccirillo Family

This section is devoted to explaining why rr was positive for all of Manolescu and Piccirillo’s knot pairs. We observed after proving Theorem 3.3 that we needed the relevant special RBG-link to have r0r\geq 0 for our proof to work. Having positive r0r\geq 0 for all 2323 knot pairs seems unlikely and it would be quite unsatisfactory if a necessary hypothesis in our proof was left unexplained. We investigate this by widening our view and considering the infinite six parameter family of special RBG-links L(a,b,c,d,e,f)L(a,b,c,d,e,f) that these knot pairs arose from. These L(a,b,c,d,e,f)L(a,b,c,d,e,f) were constructed by Manolescu and Piccirillo as a source of candidates for their exotic #n2\#n\mathbb{CP}^{2} construction. We prove that this would always occurs for any member L(a,b,c,d,e,f)L(a,b,c,d,e,f) of the Manolescu-Piccirillo family: if r<0r<0, then s(K),s(K)0s(K),s(K^{\prime})\geq 0. This allows us to prove a strong generalization of Theorem 3.3 from K1,,K23K_{1},\dots,K_{23} to any (K,K)(K,K^{\prime}) coming from some L(a,b,c,d,e,f)L(a,b,c,d,e,f).

To show that s(K),s(K)s(K),s(K^{\prime}) are non-negative when r<0r<0, we construct and analyze slice disks for (K,1)(K,-1) and (K,1)(K^{\prime},-1) in #|r|2\#|r|\mathbb{CP}^{2}. We build these slice disks by exploiting two properties of the special RBG-links L(a,b,c,d,e,f)L(a,b,c,d,e,f). The first was that they had R=UR=U and the second was that they were small.

Definition 3.6.

A small RBG-link is a special RBG-link LL such that

  • BB bounds a properly embedded disk ΔB\Delta_{B} that intersects RR in exactly one point, and intersects GG in at most 22 points.

  • GG bounds a properly embedded disk ΔG\Delta_{G} that intersects RR in exactly one point, and intersects BB in at most 22 points.

Equivalently, one needs at most two slides of BB and GG over RR in the special RBG-link construction for LL.

Some small RBG-links with R=UR=U will not to be useful to construct an exotic #n2\#n\mathbb{CP}^{2}. If either of the intersection numbers ΔBG\Delta_{B}\cap G or ΔGB\Delta_{G}\cap B is strictly less than 22, then KB=KGK_{B}=K_{G} by Proposition 4.114.11 of [MP21]. If R=UR=U and r0r\geq 0, then the proof of Theorem 3.3 can be applied. What remains can be dealt with via the following lemma.

Lemma 3.7.

Suppose LL is a small RBG-link with R=UR=U and r<0r<0. Then both KK and KK^{\prime} are (1)(-1)-slice in #|r|2\#|r|\mathbb{CP}^{2} with slice disks D,D(#|r|2)D,D^{\prime}\subset(\#|r|\mathbb{CP}^{2})^{\circ} that intersects one of the exceptional spheres 1\mathbb{CP}^{1} geometrically in 33 points and the remaining |r|1|r|-1 exceptional spheres 1\mathbb{CP}^{1} nullhomologously.

Proof.

We will prove this in the case that the intersection numbers ΔBG\Delta_{B}\cap G and ΔGB\Delta_{G}\cap B are both precisely 22. Otherwise KB=KGK_{B}=K_{G} and will not be of interest. The lemma remains true in that case and can be proved in a similar way. We will prove the lemma by induction on the framing rr with base case r=1r=-1 and we induct by showing the r<1r<-1 case of the lemma follows from the r+1r+1 case. This is one of those peculiar induction problems where the base case is the hard part so we will save it for last.

Refer to caption
((a))
Refer to caption
((b))
Refer to caption
((c))
Figure 3. Constructing a slice disk for (KB,1)(K_{B},-1) in #|r|2\#|r|\mathbb{CP}^{2}

To prove the inductive step, let LL be a small RBG-link with R=UR=U and r<1r<-1. According to a linking matrix calculation at the start of Section 4.14.1 of [MP21], BB and GG in a special RBG-link have linking number =0\ell=0 or have r=2r\ell=2. Since \ell is just ΔBG=ΔGB=2\Delta_{B}\cap G=\Delta_{G}\cap B=2 counted with sign, we must have =0\ell=0 when r<1r<-1. This \ell also counts the number of slides in the slam dunk with sign. Therefore the two strands of BB we slid in the slam dunk are running in opposite directions along RR and through the rr twist box as shown in Figure 3(a). Let LL^{*} be the special RBG-link obtained from LL by increasing rr to r+1r+1. The knot KBK_{B}^{*} arising from LL^{*} differs from KBK_{B} by having an r+1r+1 twist box in Figure 3(a). Therefore, KBK_{B} can be obtained from KBK_{B}^{*} by a negative nullhomologous twist through the two strands running through the twist box. If (KB,1)(K_{B}^{*},-1) bounds the disk DD^{*} in #|r+1|2\#|r+1|\mathbb{CP}^{2} intersecting a 1\mathbb{CP}^{1} in 33 points, then we can construct such a disk DD for (KB,1)(K_{B},-1) as in Lemma 2.8. The disk DD in #|r|2\#|r|\mathbb{CP}^{2} is simply DD^{*} after attaching a (+1)(+1)-framed 22-handle to (#|r+1|2)(\#|r+1|\mathbb{CP}^{2})^{\circ} along an unknot surrounding the twist box of D=KB\partial D^{*}=K_{B}^{*}.

To prove the r=1r=-1 base case, let (R,r)(KB,1)(R,r)\cup(K_{B},-1) be the framed link depicted in Figure 3(b). This link is obtained from L=(R,r)(B,0)(G,0)L=(R,r)\cup(B,0)\cup(G,0) by sliding (B,0)(B,0) over (R,r)(R,r) to get (KB,0)(K_{B},0), removing (G,0)(G,0), and decreasing the framing of KBK_{B} to 1-1. Identify ¯2int(B4B4)\overline{\mathbb{CP}}^{2}-\mathop{\rm int}(B^{4}\sqcup B^{4}) as S3×IS^{3}\times I with a 22-handle attached to S3×1S^{3}\times 1 along (R,r)=(U,1)(R,r)=(U,-1). Use this to define the cobordism EE in ¯2\overline{\mathbb{CP}}^{2} as KB×IK_{B}\times I under this identification. Next we slide EE over the 22-handle attached to (R,r)(R,r) and we will represent this by slides of (KB,1)(K_{B},-1) in (R,r)(KB,1)(R,r)\cup(K_{B},-1). Starting with Figure 3(b), reverse the two slides from the slam dunk to get (R,r)(B,1)(R,r)\cup(B,-1) as in Figure 3(c). We can slide (B,1)(B,-1) off (R,r)(R,r) turning it into a zero framed unknot (U,0)(U,0) disjoint from (R,r)(R,r). We turn EE upside down and cap off (U,0)(U,0) with a disk in B4B^{4} to get a slice disk DD for (KB,1)(K_{B},-1) in 2\mathbb{CP}^{2}.

It remains to check that DD intersects 1\mathbb{CP}^{1} in three points. Observe that EE was slid three times over the 22-handle attached to (R,r)(R,r) and now EE has three intersections with the cocore CC of this 22-handle. C=μR\partial C=\mu_{R} is disjoint from the (U,0)(U,0) boundary component of EE. After turning EE and CC upside down, they can be capped off without adding new intersections. The capped off CC is a copy of 1\mathbb{CP}^{1} that intersects DD in three points. ∎

We have a (1)(-1)-framed slice disk in #|r|2\#|r|\mathbb{CP}^{2} when r<0r<0 and Conjecture 2.15 would immediately tell us that s(K)0s(K^{\prime})\geq 0. However, that conjecture is currently unconfirmed and this disk is non-trivial in homology, so we can’t appeal to Lemma 2.3. Despite this, the approach used in [MMSW19] to prove Lemma 2.3 will be insightful. Let Σ\Sigma be a smooth, properly embedded, nullhomologous surface in (#n¯2)(\#n\overline{\mathbb{CP}}^{2})^{\circ} with Σ=K\partial\Sigma=K. First remove neighborhoods ν(¯1)=(¯2)\nu(\overline{\mathbb{CP}}^{1})=(\overline{\mathbb{CP}}^{2})^{\circ} tubed together leaving S3×IS^{3}\times I. By taking these neighborhoods ν(¯1)\nu(\overline{\mathbb{CP}}^{1}) small enough, one can ensure that Σ\Sigma meets ν(¯1)\partial\nu(\overline{\mathbb{CP}}^{1}) in some link Fp,p(1)F_{p,p}(1). What remains of Σ\Sigma is a cobordism CC in S3×IS^{3}\times I from a disjoint union of Fp,p(1)F_{p,p}(1) to KK. Now one needs to complete the difficult task of calculating s(Fp,p(1))s(F_{p,p}(1)) for this infinite family. Once this is done, we apply our understanding of the ss-invariant for a cobordism CC in S3×IS^{3}\times I and get constraints on s(K)s(K). By keeping careful track of the intersection data in Lemma 3.7, we will be able to proceed in a similar manner.

Corollary 3.8.

Suppose LL is a small RBG-link with R=UR=U and r<0r<0. Then s(K),s(K)0s(K),s(K^{\prime})\geq 0.

Proof.

Let D(#|r|2)D\subset(\#|r|\mathbb{CP}^{2})^{\circ} be the slice disk for (K,1)(K,-1) from Lemma 3.7 that intersects an exceptional sphere 1\mathbb{CP}^{1} in three points. Delete a suitably small neighborhood ν(1)\nu(\mathbb{CP}^{1}) of this 1\mathbb{CP}^{1} such that DD meets ν(1)\partial\nu(\mathbb{CP}^{1}) in the link F2,1(1)-F_{2,1}(1). The link F2,1(1)F_{2,1}(1) is obtained by adding a positive twist through three parallel unknots with one oriented in the opposite direction of the other two (see section 9.29.2 of [MMSW19] for details). What remains of DD is a nullhomologous cobordism CC in #(|r|1)2\#(|r|-1)\mathbb{CP}^{2} from F2,1(1)-F_{2,1}(1) to KK and we can apply Lemma 2.3.

s(K)s(F2,1(1))χ(C)=2s(K)-s(-F_{2,1}(1))\geq\chi(C)=-2

Tucked away before Proposition 9.99.9 of [MMSW19], they note s(F2,1(1))=2s(F_{2,1}(1))=-2 and therefore s(K)0s(K)\geq 0. ∎

This guarantees the proof of Theorem 3.3 will be viable for every special RBG-link L(a,b,c,d,e,f)L(a,b,c,d,e,f) and allows us to prove the following theorem.

Theorem 3.9.

Let LL be a small RBG-link with R=UR=U and associated zero surgery homeomorphism ϕ:S03(K)S03(K)\phi:S^{3}_{0}(K)\rightarrow S^{3}_{0}(K^{\prime}).

  1. (1)

    If KK is HH-slice in some #n2\#n\mathbb{CP}^{2}, then s(K)0s(K^{\prime})\geq 0.

  2. (2)

    If KK is HH-slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}, then s(K)0s(K^{\prime})\leq 0.

  3. (3)

    If KK is slice (or more generally, biprojectively HH-slice), then s(K)=0s(K^{\prime})=0.

In particular, this applies to any special RBG-link L(a,b,c,d,e,f)L(a,b,c,d,e,f) from the Manolescu-Piccirillo family.

Proof.

It suffices to prove the first statement because the first two statements are equivalent and combining them gives the last statement. If r<0r<0, then s(K)0s(K^{\prime})\geq 0 by Corollary 3.8 and for the remaining r0r\geq 0, we proceed as in the proof of Theorem 3.3. ∎

This means that Manolescu and Piccirillo’s L(a,b,c,d,e,f)L(a,b,c,d,e,f) are not suitable for finding an exotic #n2\#n\mathbb{CP}^{2} using the ss-invariant. Let us emphasize that this still leaves open that some L(a,b,c,d,e,f)L(a,b,c,d,e,f) could be used to construct an exotic #n2\#n\mathbb{CP}^{2}. We could still have KK HH-slice in some #n2\#n\mathbb{CP}^{2} while KK^{\prime} is not. The above theorem shows that s(K)s(K^{\prime}) can not obstruct HH-sliceness of KK^{\prime} in #n2\#n\mathbb{CP}^{2} and detect exoticness. It would be interesting if one could show that this does not occur and generalize Theorem 3.9 on the level HH-sliceness in #n2\#n\mathbb{CP}^{2} without reference to a particular concordance invariant.

Problem 3.10.

Let ϕ:S03(K)S03(K)\phi:S^{3}_{0}(K)\rightarrow S^{3}_{0}(K^{\prime}) be a zero surgery homeomorphism arising from some L(a,b,c,d,e,f)L(a,b,c,d,e,f). Show that KK is HH-slice in some #n2\#n\mathbb{CP}^{2} if and only if KK^{\prime} is HH-slice in some (ideally the same) #n2\#n\mathbb{CP}^{2}.

3.3. Generalizing to Other Special RBG-links

Now that we’ve ruled out using L(a,b,c,d,e,f)L(a,b,c,d,e,f) with the ss-invariant to construct an exotic #n2\#n\mathbb{CP}^{2}, we are naturally led to consider other zero surgery homeomorphisms. One would not want to run into the same issues as L(a,b,c,d,e,f)L(a,b,c,d,e,f), so we will explain how Theorem 3.9 can be generalized to other special RBG-links. We hope that in doing so that future attempts to construct an exotic #n2\#n\mathbb{CP}^{2} can avoid having our techniques be applicable. For the remainder of this subsection, let (K,K)(K,K^{\prime}) be a pair of knots coming from a special RBG-link L=(R,r)(B,0)(G,0)L=(R,r)\cup(B,0)\cup(G,0). Our goal is to find conditions on (R,r)(R,r) that allow us to use HH-sliceness of KK in #n2\#n\mathbb{CP}^{2} to infer properties of s(K)s(K^{\prime}).

Key to Theorem 3.9 was to prove Corollary 3.8 to get control over s(K)s(K^{\prime}) when r<0r<0. This was done by analyzing particular slice disks in #|r|2\#|r|\mathbb{CP}^{2} constructed in Lemma 3.7. Corollary 3.2 and Lemma 3.5 of Subsection 3.1 produce nullhomologous trace embeddings using a zero surgery homeomorphism given a slice condition on (R,r)(R,r). The following is in the same spirit, but now we construct a framed trace embedding.

Lemma 3.11.

If (R,r+1)(R,r+1) is slice in some closed 44-manifold WW, then KK and KK^{\prime} are (1)(-1)-slice in W#2W\#\mathbb{CP}^{2}

Proof.

Let (R,r)(KB,1)(R,r)\cup(K_{B},-1) be the framed link obtained from L=(R,r)(B,0)(G,0)L=(R,r)\cup(B,0)\cup(G,0) by sliding (B,0)(B,0) over (R,r)(R,r) to turn it into (KB,0)(K_{B},0), removing (G,0)(G,0), and decreasing the framing of KBK_{B} to 1-1. Take this link to be a Kirby diagram of a 44-manifold ZZ and note that X1(KB)X_{-1}(K_{B}) clearly embeds in ZZ. Reverse the slides of the slam dunk turns (R,r)(KB,1)(R,r)\cup(K_{B},-1) into (R,r)(B,1)(R,r)\cup(B,-1). Then slide (R,r)(R,r) off (B,1)(B,-1) to get (R,r+1)(U,1)(R,r+1)\sqcup(U,-1). These slides induce a diffeomorphism of ZZ with Xr+1(R)#¯2X_{r+1}(R)\#\overline{\mathbb{CP}}^{2}. If (R,r+1)(R,r+1) is slice in WW, then Xr+1(R)-X_{r+1}(R) embeds in WW by the framed trace embedding lemma. Then Z=(Xr+1(R))#2-Z=(-X_{r+1}(R))\#\mathbb{CP}^{2} embeds in W#2W\#\mathbb{CP}^{2} and so does X1(KB)Z-X_{-1}(K_{B})\subset-Z, hence (KB,1)(K_{B},-1) is slice in W#2W\#\mathbb{CP}^{2}. ∎

Observe that these are roughly the same slides used in the r=1r=-1 case of Lemma 3.7 and these two proofs should be thought of as essentially the same. The above proof is much simpler because we used trace embeddings instead of directly constructing the slice disk. That was necessary in Lemma 3.7 because we had to keep careful track of intersection data to avoid Conjecture 2.15. That conjecture asserted that if a knot KK is (1)(-1)-slice in some #n2\#n\mathbb{CP}^{2}, then s(K)0s(K)\geq 0. Now we will just assume Conjecture 2.15 and apply it to the (1)(-1)-slicing of KK in #(n+1)2\#(n+1)\mathbb{CP}^{2} given by the above lemma with W=#n2W=\#n\mathbb{CP}^{2}. Here we’ll state this in terms of the projective slice framing 𝔽(R)\mathbb{PF}_{-}(R) from Subsection 2.2. If r<𝔽(R)r<\mathbb{PF}_{-}(R), then r+1𝔽(R)r+1\leq\mathbb{PF}_{-}(R) and (R,r+1)(R,r+1) is slice in some #n2\#n\mathbb{CP}^{2} according to Corollary 2.11.

Corollary 3.12.

If r<𝔽(R)r<\mathbb{PF}_{-}(R), then KK and KK^{\prime} are both (1)(-1)-slice in some #n2\#n\mathbb{CP}^{2}. If Conjecture 2.15 is true, then s(K),s(K)0s(K),s(K^{\prime})\geq 0. ∎

We apply this Corollary 3.12 with an arbitrary special RBG-link in the same way we used Corollary 3.8 for the Manolescu-Piccirillo L(a,b,c,d,e,f)L(a,b,c,d,e,f). This proves the following which characterizes when our methods can be applied to a zero surgery homeomorphism.

Theorem 3.13.

Let ϕ:S03(K)S03(K)\phi:S^{3}_{0}(K)\rightarrow S^{3}_{0}(K^{\prime}) be a zero surgery homeomorphism arising from a special RBG-link L=(R,r)(B,0)(G,0)L=(R,r)\cup(B,0)\cup(G,0) and assume Conjecture 2.15 is true.

  1. (1)

    Suppose r<𝔽(R)r<\mathbb{PF}_{-}(R) or r𝔽+(R)r\geq\mathbb{PF}_{+}(R). If KK is HH-slice in some #n2\#n\mathbb{CP}^{2}, then s(K)0s(K^{\prime})\geq 0.

  2. (2)

    Suppose r𝔽(R)r\leq\mathbb{PF}_{-}(R) or r>𝔽+(R)r>\mathbb{PF}_{+}(R). If KK is HH-slice in some #n¯2\#n\overline{\mathbb{CP}}^{2}, then s(K)0s(K^{\prime})\leq 0.

  3. (3)

    Suppose r<𝔽(R)r<\mathbb{PF}_{-}(R), r>𝔽+(R)r>\mathbb{PF}_{+}(R), or RR is biprojectively HH-slice with any rr\in\mathbb{Z}. If KK is slice (or biprojectively HH-slice), then s(K)=0s(K^{\prime})=0.

Moreover, if RR is biprojectively HH-slice, then the conditions on (R,r)(R,r) automatically hold.

Proof.

The r<𝔽(R)r<\mathbb{PF}_{-}(R) part of the first statement is Corollary 3.12. If r𝔽+(R)r\geq\mathbb{PF}_{+}(R), then (R,r)(R,r) is slice in some #k¯2\#k\overline{\mathbb{CP}}^{2} by Corollary 2.11. If we also have KK is HH-slice in some #n2\#n\mathbb{CP}^{2}, then we can conclude KK^{\prime} is HH-slice in #(n+k)2\#(n+k)\mathbb{CP}^{2} by Corollary 3.2 and s(K)0s(K^{\prime})\geq 0 by Lemma 2.3. For the final statement, the first two statements simultaneously apply when r<𝔽(R)r<\mathbb{PF}_{-}(R) and r>𝔽+(R)r>\mathbb{PF}_{+}(R). If RR is biprojectively HH-slice, then 𝔽+(R)=𝔽(R)=0\mathbb{PF}_{+}(R)=\mathbb{PF}_{-}(R)=0 by Lemma 2.10 and the first two statements simultaneously apply for any rr\in\mathbb{Z}. ∎

The special RBG-links L(a,b,c,d,e,f)L(a,b,c,d,e,f) all have biprojectively HH-slice R=UR=U and this might explain why Manolescu and Piccirillo were unsuccessful in their search. The appeal of the ss-invariant for detecting an exotic #n2\#n\mathbb{CP}^{2} was that it was not clear if the obstruction should apply in an exotic #n2\#n\mathbb{CP}^{2}. This theorem sometime recovers this obstruction if we only understand the ss-invariant in the standard #n2\#n\mathbb{CP}^{2}. Furthermore, this theorem could apply to other concordance invariants that shares the properties of the ss-invariant we used (e.g. any that satisfies an adjunction inequality in #n2\#n\mathbb{CP}^{2}). This is troubling for the prospect of constructing an exotic #n2\#n\mathbb{CP}^{2} from zero surgery homeomorphisms. Once we understand a concordance invariant in the standard #n2\#n\mathbb{CP}^{2}, it can often be enough to rule out using it to construct an exotic #n2\#n\mathbb{CP}^{2} with zero surgery homeomorphisms.

However, this theorem does not immediately apply to all zero surgery homeomorphisms. This leaves open the possibility that some zero surgery homeomorphism could be used to construct an exotic #n2\#n\mathbb{CP}^{2}. We will construct an infinite family of special RBG-links for which our methods do not apply. Our special RBG-links will come in the form of a special RBG-link LL with a local connected sum by some knot JJ to RR. Call this new special RBG-link L[J]L[J] and the resulting knots KB[J],KG[J]K_{B}[J],K_{G}[J].

Dunfield and Gong used topological slice obstructions to show that K6,,K21K_{6},\dots,K_{21} are not slice. By viewing KB[J],KG[J]K_{B}[J],K_{G}[J] as satellites knots, we get some control over the topological sliceness of the resulting knots. Examining Figure 2, we see that KB[J]K_{B}[J] and KG[J]K_{G}[J] are both satellites PB(J)P_{B}(J) and PG(J)P_{G}(J) of JJ. These will be patterns PBP_{B} and PGP_{G} such that KB=PB(U)K_{B}=P_{B}(U) and KG=PG(U)K_{G}=P_{G}(U). These patterns have winding number equal to the linking number \ell of BB and GG. We will take LL to be one of the special RBG-links LiL_{i} associated to the five pairs {(Ki,Ki)}i=1,,5\{(K_{i},K_{i}^{\prime})\}_{i=1,\dots,5}. Denote the knots resulting from Li[J]L_{i}[J] by Ki[J]K_{i}[J] and Ki[J]K_{i}^{\prime}[J]. These LiL_{i} all have =0\ell=0 and so the associated satellite patterns have winding number zero. Ki[J]K_{i}[J] and Ki[J]K_{i}^{\prime}[J] will then have the same Alexander polynomials as KiK_{i} and KiK_{i}^{\prime} by Seifert’s formula for the Alexander polynomial of a satellite [Sei50]. In particular, Ki[J]K_{i}[J] and Ki[J]K_{i}^{\prime}[J] will have trivial Alexander polynomial and will be topologically slice by Freedman [Fre82].

Let rir_{i} denote the framing of RR in LiL_{i} which will be equal to 11, 22, or 33. To construct an exotic #n2\#n\mathbb{CP}^{2} from Li[J]L_{i}[J], Theorem 3.13 suggests we should have JJ not biprojectively HH-slice and have 𝔽(J)ri<𝔽+(J)\mathbb{PF}_{-}(J)\leq r_{i}<\mathbb{PF}_{+}(J). Note that the condition 𝔽(J)ri\mathbb{PF}_{-}(J)\leq r_{i} holds automatically so we only need to check that 𝔽+(J)>ri\mathbb{PF}_{+}(J)>r_{i}. Such JJ are in abundance as any JJ with τ(J)1\tau(J)\geq 1, such as the right hand trefoil, will suffice due to Corollary 2.13.

These Li[J]L_{i}[J] give an infinite family of special RBG-links which are not susceptible to topological slice obstructions or the methods of this paper. One could potentially apply the methodology of Manolescu and Piccirillo to these families. We do not propose these as a serious attempt at constructing an exotic #n2\#n\mathbb{CP}^{2}. It seems that going from (K,K)(K,K^{\prime}) to (K[J],K[J])(K[J],K^{\prime}[J]) would increase slice genus since the resulting knots are more complicated. Instead, we propose these as a setting to study how to relate the ss-invariants and HH-sliceness of knots with homeomorphic zero surgeries.

Problem 3.14.

Let ri<𝔽+(J)r_{i}<\mathbb{PF}_{+}(J), relate HH-sliceness of Ki[J],Ki[J]K_{i}[J],K_{i}^{\prime}[J] in #n2\#n\mathbb{CP}^{2} and their ss-invariants to each other. In particular, show that if one of these knots is HH-slice in some #n2\#n\mathbb{CP}^{2}, then the other has non-negative ss-invariant.

4. Annulus Twist Homotopy Spheres

Manolescu and Piccirillo constructed homotopy 44-spheres Zn=E(D)ϕnX0(Jn)Z_{n}=E(D)\cup_{\phi_{n}}-X_{0}(J_{n}) from annulus twisting a ribbon knot J0J_{0}. In this section, we show that these ZnZ_{n} are all standard by drawing them upside down as Zn=X0(Jn)ϕnE(D)-Z_{n}=X_{0}(J_{n})\cup_{\phi_{n}}-E(D). This proof was motivated by a desire to understand and visualize the trace embedding of X0(Jn)X_{0}(J_{n}) in Zn-Z_{n} as a Kirby diagram. We will first need to explain how this works for a ribbon knot and its associated trace embedding into S4S^{4}.

4.1. A Kirby Diagram of the Trace Embedding Lemma

A ribbon disk is a smoothly, properly embedded disk DD in B4B^{4} such that the height function on B4B^{4} restricted to DD has no index two critical points. A knot KK is called a ribbon knot if it bounds a ribbon disk. Similarly, an nn component link \mathcal{L} is called a ribbon link if it bounds a collection 𝒟=D1Dn\mathcal{D}=D_{1}\cup\dots\cup D_{n} of nn disjoint ribbon disks called a ribbon disk link. A ribbon disk is typically described by a ribbon diagram. This is an nn component unlink 𝒰\mathcal{U} together with a collection of n1n-1 ribbon bands. A ribbon band is an embedded I×II\times I attached to 𝒰\mathcal{U} along (I)×I(\partial I)\times I (respecting orientations). These ribbon bands I×II\times I must intersect the disks that bound 𝒰\mathcal{U} as some a×Ia\times I. The knot 616_{1} is ribbon and can be described by the ribbon diagram in Figure 4(a).

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((a))
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((b))
Figure 4. A ribbon diagram for 616_{1} and a Kirby diagram of the corresponding the ribbon disk exterior

Such a ribbon diagram for a knot KK defines a ribbon disk DD bounding KK. Each component of the unlink 𝒰\mathcal{U} becomes an index zero critical point of DD and each ribbon band becomes an index one critical point of DD. We can draw a Kirby diagram of the exterior E(D)=B4ν(D)E(D)=B^{4}-\nu(D) of DD from its Ribbon diagram with the algorithm presented in Section 6.26.2 of [GS99]. Using Figure 4(a), we draw a Kirby diagram for the exterior of a ribbon disk of 616_{1} in Figure 4(b). The index zero critical points of DD become 11-handles which we draw by putting a dot on each component of 𝒰\mathcal{U}. The index one critical points of DD become zero framed 22-handles which follow the boundary of the corresponding ribbon like in Figure 4(b).

To fill in E(D)E(D) in this diagram, we attach a zero framed 22-handle to a meridian of a dotted circle. We can then cancel this pair, the rest of the diagram “unravels”, and the remaining handles cancel. This leaves B4B^{4} and capping off with a 44-handle gives S4S^{4}. This gives a decomposition of S4S^{4} as E(D)E(D) with a 22-handle and 44-handle attached. These additional handles represent an embedded X0(K)-X_{0}(K) and this is the same embedding as the classical trace embedding lemma.

Lemma 4.1 (Trace Embedding Lemma).

KK is slice if and only if X0(K)X_{0}(K) (equivalently X0(K)-X_{0}(K)) embeds in S4S^{4}.

While such a diagram gives the same embedding of X0(K)-X_{0}(K), we don’t clearly see the embedded trace. It is represented as a 22-handle attached to a meridian of a dotted circle and a 44-handle. We would rather see the trace embedding as a 22-handle attached to KK in our diagram. To do this, we turn this decomposition upside down as X0(K)E(D)X_{0}(K)\cup-E(D) and draw the corresponding Kirby diagram. One could try to use the standard method to turn a Kirby diagram upside down as in Section 5.55.5 of [GS99]. The difficulty with that method is that turning E(D)E(D) upside down directly can result in a messy Kirby diagram. The method we will describe will result in simpler diagrams that can be read off directly from a ribbon diagram of DD. To do this, we will upgrade KK and DD to a ribbon link =KL1Ln1\mathcal{L}=K\cup L_{1}\cup\dots\cup L_{n-1} and ribbon disk link 𝒟=DD1Dn1\mathcal{D}=D\cup D_{1}\cup\dots\cup D_{n-1}. This ribbon disk link will have exterior E(𝒟)E(\mathcal{D}) consisting of only a 0-handle and nn 11-handles which can be turned upside down immediately. We will give pictures of how to do this for K=61K=6_{1} and DD its standard ribbon disk shown in Figure 4(a).

Draw a ribbon diagram of DD and add a small unknot LiL_{i} encircling each ribbon band to get a link =KL1Ln1\mathcal{L}=K\cup L_{1}\cup\dots\cup L_{n-1}. Since each LiL_{i} bounds a disk DiD_{i} in S3S^{3} that intersect KK in ribbon singularities, there is a ribbon disk link 𝒟=DD1Dn1\mathcal{D}=D\cup D_{1}\cup\dots\cup D_{n-1} for \mathcal{L} where each DiD_{i} has a unique index zero critical point. To draw a Kirby diagram for E(𝒟)E(\mathcal{D}), add a red dotted circle to each LiL_{i} in the diagram of E(D)E(D) as in Figure 5(a).

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((a))
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((b))
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((c))
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((d))
Figure 5. Simplifying E(𝒟)E(\mathcal{D})

To simplify, change the red dotted circles into a pair of balls to represent 11-handles as in Figure 5(b). Think of this change in notation as doing ribbon moves on KK and each of these balls as a pair of arcs on the banding of KK. We can pull each of the red balls along the band to get Figure 5(c). What is left is nn black dotted circles with n1n-1 22-handles each running through a pair of balls connecting them in consecutive pairs. Change the balls back to dotted notation as in Figure 5(d) and then move the red dotted circles off the rest of the diagram. Cancel the 22-handles leaving a single black dotted circle and n1n-1 red dotted circles. We conclude that E(𝒟)E(\mathcal{D}) admits a handle decomposition with one 0-handle with nn 11-handles attached.

Let X0()X_{0}(\mathcal{L}) be obtained by attaching zero framed 22-handles to B4B^{4} along each component of \mathcal{L}. We attach E(𝒟)-E(\mathcal{D}) to X0()X_{0}(\mathcal{L}) to get a Kirby diagram of S4S^{4}. The handles of E(𝒟)E(\mathcal{D}) turn upside down to become 33 and 44-handles which attach uniquely. To summarize, we attach zero framed 22-handles to a ribbon knot KK and unknots encircling the n1n-1 ribbon bands of DD, then cap off with nn 33-handles and a 44-handle. For K=61K=6_{1}, we get the Kirby diagram in Figure 6.

Remark 4.2.

Some of the more adept practitioners of Kirby Calculus may have applied the standard method to turn a Kirby Diagram upside down and got the same diagram as Figure 6. However, this is an artifact of the simplicity of 616_{1} and you will not get the same diagram for a more complicated ribbon knot. One can see what goes wrong if one tries this with the ribbon knot shown in Figure 7 used in the following subsection. If one uses that method to draw the homotopy spheres of interest, one gets diagrams that do not seem as amenable to simplification.

Refer to caption
Figure 6. Kirby diagram of S4S^{4} as X0(61)E(D)X_{0}(6_{1})\cup-E(D)

4.2. Standardzing ZnZ_{n}

Refer to caption
Figure 7. Annulus presentation and ribbon diagram of J0J_{0}

Manolescu and Piccirillo constructed and drew diagrams of a family of homotopy spheres that we will call ZnZ_{n}. These ZnZ_{n} arise from a family of knots {Jn}n\{J_{n}\}_{n\in\mathbb{Z}} which are annulus twists on the ribbon knot J0=88J_{0}=8_{8}. The annulus presentation and ribbon diagram of J0J_{0} are depicted in Figure 7. The half fractional box notation in that figure represents half twists on the two strands passing through that box.

Annulus twisting was introduced by Osoinach in his construction of infinite collections of knots that share a zero surgery [Oso06]. The annulus presentation of J0J_{0} defines a family of homeomorphisms ϕn:S03(J0)S03(Jn)\phi_{n}:S^{3}_{0}(J_{0})\rightarrow S^{3}_{0}(J_{n}). In Figure 7, we see that 12\ell_{1}\cup\ell_{2} are the boundary of an annulus AA. This annulus induces orientations and framings on 1\ell_{1} and 2\ell_{2}. J0J_{0} was obtained by banding 12\ell_{1}\cup\ell_{2} and so all three cobound a pair of pants. Let AS03(J0)A^{\prime}\subset S^{3}_{0}(J_{0}) be an annulus formed by the union of the surgery disk and the pair of pants. Twisting along ν(A)\nu(A^{\prime}) gives a homeomorphism S03(J0)S0,1/n,1/n3(J0,1,2)S^{3}_{0}(J_{0})\rightarrow S^{3}_{0,1/n,-1/n}(J_{0},\ell_{1},\ell_{2}) (where framings on 12\ell_{1}\cup\ell_{2} are relative to their annulus framings). Then a twist on ν(A)S3\nu(A)\subset S^{3} gives a homeomorphism S1/n,1/n3(1,2)S3S^{3}_{1/n,-1/n}(\ell_{1},\ell_{2})\rightarrow S^{3} and identifies S0,1/n,1/n3(J0,1,2)S^{3}_{0,1/n,-1/n}(J_{0},\ell_{1},\ell_{2}) with zero surgery on some knot JnS3J_{n}\subset S^{3}. The annulus twist homeomorphisms ϕn:S03(J0)S03(Jn)\phi_{n}:S^{3}_{0}(J_{0})\rightarrow S^{3}_{0}(J_{n}) is the composition of these homeomorphisms.

J0J_{0} is ribbon and bounds a disk DD described by the ribbon move in Figure 7. We can use the annulus twist homeomorphisms to construct the homotopy spheres Zn=E(D)ϕnX0(Jn)Z_{n}=E(D)\cup_{\phi_{n}}-X_{0}(J_{n}). This decomposition as E(D)ϕnX0(Jn)E(D)\cup_{\phi_{n}}-X_{0}(J_{n}) is the one used to draw the diagrams of ZnZ_{n} in Figure 2020 of [MP21]. We will use the technique from the previous subsection to draw diagrams of these ZnZ_{n} upside down as X0(Jn)ϕnE(D)X_{0}(J_{n})\cup_{\phi_{n}}-E(D) and then show that each ZnZ_{n} is standard.

Theorem 4.3.

All ZnZ_{n} are diffeomorphic to S4S^{4}.

Proof.
Refer to caption
((a))
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((b))
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((c))
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((d))
Figure 8. Standardizing ZnZ_{n}

By definition, Z0=E(D)X0(J0)Z_{0}=E(D)\cup-X_{0}(J_{0}) is standard and we can draw Z0=X0(J0)E(D)-Z_{0}=X_{0}(J_{0})\cup-E(D) as shown in Figure 8(a). This diagram has no 11-handles and two 22-handles attached with zero framing to J0J_{0} and the knot LL that surrounds the ribbon band of J0J_{0}. To draw Zn=X0(Jn)ϕnE(D)-Z_{n}=X_{0}(J_{n})\cup_{\phi_{n}}-E(D), we attach the handles of E(D)-E(D) using the map ϕn\phi_{n}. The 33 and 44-handles attach uniquely so we only need to keep track of LL. The annulus twist homeomorphism is supported in a neighborhood of AA^{\prime} and AA disjoint from LL. Therefore, LL is unaffected by ϕn\phi_{n} and we can draw a diagram of Zn-Z_{n} as in Figure 8(b).

With the desired diagrams of Zn-Z_{n} now in hand, we can now proceed to show that each ZnZ_{n} is standard. First slide the band of JnJ_{n} over LL as shown by the blue arrow in Figure 8(b) to get Figure 8(c). This brings the band under the annulus with a twist which we absorb into the twist box on the left. Drag this band under the annulus via the dashed blue arrow to the position shown in solid blue in Figure 8(c). Spin the band around the annulus to undo the twists and get Figure 8(d). We get the same diagram for all nn, therefore all ZnZ_{n} must be diffeomorphic to each other and in particular Z0=S4Z_{0}=S^{4}. ∎

Corollary 4.4.

JnJ_{n} is slice for all nn\in\mathbb{Z}. ∎

This proof bears similarities to work of Akbulut and Gompf on the family {Σn}n\{\Sigma_{n}\}_{n\in\mathbb{Z}} Cappell-Shaneson spheres [Akb10, Gom10]. The resemblance is most immediate when compared to Akbulut’s diagrammatic proof that each Σn\Sigma_{n} is standard. Akbulut added a cancelling 22 and 33-handle pair to a Kirby diagram of Σn\Sigma_{n} and identified all Σn\Sigma_{n} with each other. In particular, every Σn\Sigma_{n} is diffeomorphic to Σ0\Sigma_{0} which was known to be standard by earlier work of Gompf [Gom91]. There seems to be a more opaque connection to Gompf’s work following up on Akbulut. There Gompf showed that certain torus twists don’t affect the Cappell-Shaneson construction to give a mostly Kirby calculus free proof. It would be interesting if one could think of these annulus twists in a way that recasts this proof in a similar manner.

Meier and Zupan recently gave a new proof that the Cappell-Shaneson spheres Σn\Sigma_{n} are standard using ideas from the theory of Generalized Property RR [MZ19]. We can give another proof that ZnZ_{n} is standard in a similar manner once we have the diagram shown in Figure 8(b).

Proof.

The diagram of Zn-Z_{n} has no 11-handles and 22-handles attached to the link JnLJ_{n}\cup L where LL is an unknot. To be able to attach the two 33-handles and the 44-handle, zero surgery on JnLJ_{n}\cup L must be #2S1×S2\#2S^{1}\times S^{2}. We can now appeal to Property 2R2R for the unknot.

Lemma 4.5 (Proposition 3.2 of [GST10]).

The unknot has Property 2R2R. Namely, if \mathcal{L} is a 22 component framed link with an unknotted component that surgers to #2S1×S2\#2S^{1}\times S^{2}, then there is a sequence of handle slides turning \mathcal{L} into a zero framed 22 component unlink.

We can do these handle slides to Zn-Z_{n} and then cancel the 22-handles with the 33-handles to get S4S^{4}. ∎

This only gives existence of handle slides that standardize ZnZ_{n}. We prefer the first proof where we directly see how to standardize these diagrams of Zn-Z_{n}. While using Property 2R2R may seem to be much slicker, it also relies on deep work of Gabai and Scharlemann [Sch90, Gab87]. The Property 2R2R approach has more and much harder technical prerequisites than the diagrammatic proof. Despite the moralizing about Property 2R2R, it does offer the serious benefit of being easy to implement in practice. Note that using Property 2R2R in this manner required that DD was a ribbon disk with a single index one critical point. Otherwise the Kirby diagram of Σ-\Sigma would have had more than two 22-handles. Fortunately, the Property 2R2R approach can be generalized to any ribbon disk. According to Theorem 5.15.1 of [MSZ16], surgery on #(n1)S1×S2\#(n-1)S^{1}\times S^{2} that results in #nS1×S2\#nS^{1}\times S^{2} must be on a zero framed unknot222Note that [MSZ16] cite it as a special case in expository work of Gordon [Gor97] who ascribes it to Gabai and Scharlemann [Sch90, Gab87]. We rephrase this in terms of Property nRnR as a direct generalization of Lemma 4.5.

Lemma 4.6 (Theorem 5.15.1 of [MSZ16]).

The n1n-1 component unlink 𝒰n1\mathcal{U}_{n-1} has Property nRnR. In particular, let =𝒰n1K\mathcal{L}=\mathcal{U}_{n-1}\cup K be an nn component framed link that contains an n1n-1 component unlink 𝒰n1\mathcal{U}_{n-1}. If \mathcal{L} surgers to #nS1×S2\#nS^{1}\times S^{2}, then there is a sequence of handle slides turning \mathcal{L} into a zero framed nn component unlink.

We can use this to check if the homotopy sphere Σ=E(D)ϕX0(K)\Sigma=E(D)\cup_{\phi}-X_{0}(K^{\prime}) is standard when DD is ribbon. Draw a Kirby diagram of S4=X0(K)E(D)S^{4}=X_{0}(K)\cup-E(D) with 22-handle attaching link =KL\mathcal{L}=K\cup L as described in the previous section. Draw a diagram of Σ-\Sigma as in the proof of Theorem 4.3, the attaching link for the 22-handles in this diagram is =Kϕ(L)\mathcal{L}^{\prime}=K^{\prime}\cup\phi(L). LL was originally an unlink and if ϕ(L)\phi(L) is still an unlink in this diagram, then Σ\Sigma is standard by Property nRnR for 𝒰n1\mathcal{U}_{n-1}. Somehow this is saying something unsurprising: LL represent some aspect of the ribbon structure of DD and if ϕ\phi leaves it unperturbed, then Σ\Sigma is standard.

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