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A note on band surgery and the signature of a knot

Allison H. Moore  and  Mariel Vazquez Allison H. Moore
Department of Mathematics & Applied Mathematics
Virginia Commonwealth University
Richmond, VA 23284
USA
Mariel Vazquez
Department of Mathematics, Department of Microbiology and Molecular Genetics
University of California, Davis
Davis, CA 95616
USA
Abstract.

Band surgery is an operation relating pairs of knots or links in the three-sphere. We prove that if two quasi-alternating knots KK and KK^{\prime} of the same square-free determinant are related by a band surgery, then the absolute value of the difference in their signatures is either 0 or 8. This obstruction follows from a more general theorem about the difference in the Heegaard Floer dd-invariants for pairs of L-spaces that are related by distance one Dehn fillings and satisfy a certain condition in first homology. These results imply that T(2,5)T(2,5) is the only torus knot T(2,m)T(2,m) with mm square-free that admits a chirally cosmetic banding, i.e. a band surgery operation to its mirror image. We conclude with a discussion on the scarcity of chirally cosmetic bandings.

1991 Mathematics Subject Classification:
57K10, 57K18 (primary), 57R58, 57M12 (secondary)

1. Introduction

Band surgery is an operation on knots or links in the three-sphere. Let LL be a link, and let b:I×IS3b:I\times I\rightarrow S^{3} be an embedding of the unit square with Lb(I×I)=b(I×I)L\cap b(I\times I)=b(I\times\partial I). Let LL^{\prime} denote the link obtained by replacing b(I×I)b(I\times\partial I) in LL with b(I×I)b(\partial I\times I). We say that the link LL^{\prime} results from band surgery along LL. See Figure 1 for two examples of band surgeries relating pairs of knots. When LL and LL^{\prime} are oriented links and band surgery respects their orientations, the operation is called coherent band surgery. Otherwise, it is called non-coherent. Coherent band surgery converts a knot into a two-component link, whereas non-coherent band surgery converts a knot to another knot.

In this article we are concerned only with non-coherent band surgery operations relating unoriented knots. Elsewhere in the literature non-coherent band surgery is called incoherent band surgery or unoriented banding (e.g. [AK14, Kan16, IJM18]). Band surgery is of interest in low-dimensional topology, in particular in knot theory, and in the study of surfaces in four-manifolds. It is of independent interest in DNA topology; for a more detailed commentary on this perspective, we refer the reader to [LMV19, Section 5] and [MV20], which review the relevance of band surgery to the study of DNA.

In Theorem 4.4, we find a new obstruction to band surgery for quasi-alternating knots via two knot invariants, the determinant and signature of a knot. Both the determinant det(K)\det(K) and the signature σ(K)\sigma(K) of a knot are integer-valued (det(K)\det(K) is odd and σ(K)\sigma(K) is even) and are determined by the Seifert module [GL78, Tro62]. A quasi-alternating knot is a generalization of an alternating knot due to Ozsváth and Szabó [OS05b]. All alternating knots are quasi-alternating. Two pairs of knots for which Theorem 4.4 applies are shown in Figure 1. Note that any banding relating a pair of knots is necessarily a non-coherent band surgery.

Theorem 4.4.

Let KK and KK^{\prime} be a pair of quasi-alternating knots and suppose that det(K)=m=det(K)\det(K)=m=\det(K^{\prime}) for some square-free integer mm. If there exists a band surgery relating KK and KK^{\prime}, then |σ(K)σ(K)||\sigma(K)-\sigma(K^{\prime})| is 0 or 88.

Refer to caption
Refer to caption
Figure 1. Non-coherent band surgery (indicated by the shaded area) relates the knots 717_{1} and 525_{2}^{*} (left), and the knots 626_{2} and 727_{2} (right). The knot 525_{2}^{*} is the mirror of 525_{2}. Diagrams corresponding with these band moves were found by Zeković [Zek15]. In contrast, Theorem 4.4 implies there cannot exist a band surgery between 717_{1} and 525_{2}, since det(71)=7=det(52)\det(7_{1})=7=\det(5_{2}) and |σ(71)σ(52)|=4|\sigma(7_{1})-\sigma(5_{2})|=4. Likewise, there is no band surgery between 626_{2} and 727_{2}^{*}. See example 4.7 for details.

The determinant of a knot, or more generally the first homology of its branched double cover, can often provide an effective obstruction to the existence of a band surgery relating a pair of knots (see for example [AK14, KM14, Kan16]). However, when a pair of knots K,KK,K^{\prime} have branched double covers with isomorphic first homology (which implies det(K)=det(K)\det(K)=\det(K^{\prime})), such obstructions do not apply. Theorem 4.4 fills this gap in the case where mm is square-free. Theorem 4.4 is reminiscent of Murasugi’s well-known statement that |σ(L)σ(L)|1|\sigma(L)-\sigma(L^{\prime})|\leq 1 when LL and LL^{\prime} are related by a coherent band surgery [Mur65, Lemma 7.1]. In the case of non-coherent band surgery, the signature of a knot may change by an arbitrary amount. For example, the torus knot T(2,m)T(2,m), with m>0m>0 odd, has signature 1m1-m and is related by a single band surgery operation to the unknot, which has zero signature.

Murasugi also proved that for any knot KK, the signature controls the determinant of a knot modulo 4 [Mur65, Theorem 5.6]. More precisely, if |σ(K)|0|\sigma(K)|\equiv 0 (resp. 2) modulo 4, then |det(K)|1|\det(K)|\equiv 1 (resp. 3) modulo 4. This immediately implies

|σ(K)σ(K)||det(K)det(K)|(mod4),|\sigma(K)-\sigma(K^{\prime})|\equiv|\det(K)-\det(K^{\prime})|\pmod{4},

for any pair of knots, which provides an explanation for the significance of the numbers 0 and 8 in Theorem 4.4.

Theorem 4.4 follows as a corollary of Theorem 3.5, a more general statement about the Heegaard Floer dd-invariants of pairs of L-spaces related by integral surgery.

Theorem 3.5.

Let YY and YY^{\prime} be L-spaces with H1(Y)/d1/d2/dkH1(Y)H_{1}(Y)\cong\mathbb{Z}/d_{1}\oplus\mathbb{Z}/d_{2}\oplus\cdots\oplus\mathbb{Z}/d_{k}\cong H_{1}(Y^{\prime}), where each did_{i} is an odd square-free integer. If YY^{\prime} is obtained by a distance one surgery along any knot KK in YY, then

|d(Y,𝔱)d(Y,𝔱)|=2 or 0|d(Y,\mathfrak{t})-d(Y^{\prime},\mathfrak{t}^{\prime})|=2\text{ or }0

where 𝔱\mathfrak{t} and 𝔱\mathfrak{t}^{\prime} denote the unique self-conjugate Spinc\text{Spin}^{c} structures on YY and YY^{\prime}.

Heegaard Floer homology is a powerful package of three and four-manifold invariants due to Ozsváth and Szabó [OS03]. An L-space is a rational homology sphere whose Heegaard Floer homology is as simple as possible. One particularly useful Heegaard Floer invariant is the d-invariant of the pair (Y,𝔱)(Y,\mathfrak{t}), where YY is an oriented rational homology sphere and tt is an element of Spinc(Y)H2(Y;)\text{Spin}^{c}(Y)\cong H^{2}(Y;\mathbb{Z}). The dd-invariant is a rational number, defined as the minimal grading of a certain submodule of the Heegaard Floer module HF+(Y,𝔱)HF^{+}(Y,\mathfrak{t}) [OS03]. The reader is referred to [OS03] for an introduction to these invariants. All required background for this note is in sections 2 and 3.

The distance between two Dehn surgery slopes refers to their minimal geometric intersection number. A surgery slope that intersects the meridian of a knot exactly once is called a distance one surgery, or an integral surgery. Given two knots or links related by band surgery, the Montesinos trick [Mon76] implies that their branched double covers may be obtained by distance one Dehn fillings of a three-manifold with torus boundary. To prove Theorem 3.5 we apply the Heegaard Floer mapping cone formula of Ozsváth and Szabó [OS11], and a theorem of Ni and Wu [NW15, Proposition 1.6] which describes the dd-invariants of a manifold obtained by integral surgery along a null-homologous knot in an L-space in terms of certain integer-valued knot invariants due to Rasmussen [Ras03].

Refer to caption
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Figure 2. (Left) A banding relating the torus knot T(2,5)=51T(2,5)=5_{1} to its mirror T(2,5)=51T(2,-5)=5_{1}^{*}. The existence of this band move is due to Zeković [Zek15]. (Right) A banding relating the pair 888_{8}^{*} and 888_{8}. This band was discovered via computer simulations (see section 4.3).

Applications to chirally cosmetic banding. A special case of Theorem 4.4 occurs when a band surgery relates a knot KK with its mirror image KK^{*}. See Figure 2 for an example. This is called a chirally cosmetic banding. The following is an immediate consequence of Theorem 4.4.

Corollary 4.8.

The only nontrivial torus knot T(2,m)T(2,m), with mm square free, admitting a chirally cosmetic banding is T(2,5)T(2,5).

In section 4, we compare the square-free condition of Theorem 4.4 with the constructive examples of chirally cosmetic bandings given in [IJM18]. Using Monte Carlo simulations we find examples of knots admitting chirally cosmetic bandings. Additionally, in all cases these appear with low probability. Amongst knots of up to eight crossings, the results of our simulations produce three such examples: 515_{1}, 888_{8}, and 8208_{20}. The chirally cosmetic banding along 888_{8} was previously not known to exist. An isotopy of the banding is shown in Figure 2 (right).

Organization. In section 2 we introduce notation and establish some prerequisite topological information. Section 3 contains the necessary background in Heegaard Floer homology along with the proof of Theorem 3.5. In section 4 we prove Theorem 4.4, further consider the case of chirally cosmetic pairs and detail the methods of the computer simulations.

2. Preliminaries

2.1. Homological preliminaries

In this section we state some homological preliminaries and set notation. We assume all singular (co)homology groups have coefficients in \mathbb{Z}. Let KK be a knot in a rational homology sphere YY, and let M=YN(K)M=Y-N(K) denote the complement of KK in YY. A slope is an isotopy class of an unoriented simple closed curve on the boundary of MM. The Dehn filling M(η)M(\eta) is the closed, oriented three-manifold obtained by gluing a solid torus VV to MM by a homeomorphism which identifies a meridian of V\partial V to the slope η\eta on M\partial M. The distance between two surgery slopes on M\partial M is the minimal geometric intersection number of the two curves, denoted Δ(η,ν)\Delta(\eta,\nu) for any pair of slopes η,ν\eta,\nu. In this note we are particularly concerned with surgery slopes which intersect the meridian of KK exactly once, i.e. distance one surgeries, or integral surgeries.

When KK is null-homologous, there is a standard choice of a meridian μ\mu and Seifert longitude λ\lambda on the bounding torus M\partial M. Here, the meridian μ\mu is a simple closed curve on M=N(K)\partial M=\partial N(K) that bounds a disk in the solid torus N(K)N(K). The preferred longitude is the slope determined by the intersection of a Seifert surface for the knot and N(K)\partial N(K). A slope η\eta may be written in terms of this standard basis as η=aμ+bλ\eta=a\mu+b\lambda. Rational Dehn surgery with the surgery coefficient a/ba/b along KK in YY is then well-defined, and the result of surgery is denoted by Ya/b(K)=M(η)Y_{a/b}(K)=M(\eta). Indeed, when KK is null-homologous a homological argument (see for example [Gai18, Lemma 8.1]) shows that H1(M)H1(Y)H_{1}(M)\cong\mathbb{Z}\oplus H_{1}(Y), where the \mathbb{Z}-summand is generated by the meridian of KK. This implies that H1(Ya/b(K))/aH1(Y)H_{1}(Y_{a/b}(K))\cong\mathbb{Z}/a\oplus H_{1}(Y) by a standard Mayer-Vietoris argument. Notice that the Seifert longitude controls the first homology of the Dehn filling, in the sense that |H1(Ya/b(K))|=|M(η)|=|H1(Y)|Δ(η,λ)|H_{1}(Y_{a/b}(K))|=|M(\eta)|=|H_{1}(Y)|\cdot\Delta(\eta,\lambda).

When KK is not null-homologous, we have that H1(M)HH_{1}(M)\cong\mathbb{Z}\oplus H for some finite group HH. Let ii_{*} denote the map induced by inclusion in the long exact sequence of the pair (M,M)(M,\partial M),

H2(M)H2(M,M)H1(M)iH1(M)H1(M,M).\cdots\rightarrow H_{2}(M)\rightarrow H_{2}(M,\partial M)\rightarrow H_{1}(\partial M)\stackrel{{\scriptstyle i_{*}}}{{\rightarrow}}H_{1}(M)\rightarrow H_{1}(M,\partial M)\rightarrow\cdots.

The kernel and image of ii_{*} are both rank one. In particular, the kernel of ii_{*} is generated by kλMk\lambda_{M}, where λM\lambda_{M} is a primitive class [λM][\lambda_{M}] in H1(M)H_{1}(\partial M) uniquely determined up to sign. This class determines a well-defined slope in M\partial M:

Definition 2.1.

The rational longitude λM\lambda_{M} is the unique slope in M\partial M characterized by the property that its image i(λM)i_{*}(\lambda_{M}) is of finite order in HH1(M)H\subset H_{1}(M).

When we work with knots that are non-trivial in H1(Y)H_{1}(Y), we will use the rational longitude to fix a basis (μ,λM)(\mu,\lambda_{M}) for H1(M)H_{1}(\partial M), where μ\mu now denotes some slope with Δ(μ,λM)=1\Delta(\mu,\lambda_{M})=1. Just as with the case of the Seifert longitude for null-homologous knots, the rational longitude also controls the order of the first homology of the filling.

Lemma 2.2.

[Wat12, Lemma 3.2] For any filling slope ηλM\eta\neq\lambda_{M} on M\partial M,

(1) |H1(M(η)|=ordHi(λM)|H|Δ(η,λM)|H_{1}(M(\eta)|=\operatorname{ord}_{H}i_{*}(\lambda_{M})\cdot|H|\cdot\Delta(\eta,\lambda_{M})

where ordHi(λM)\operatorname{ord}_{H}i_{*}(\lambda_{M}) denotes the (necessarily finite) order of the rational longitude in HH.

In [Wat12, Lemma 3.2], this is proved with a careful analysis of the long exact sequence of the pair. Under the homomorphism i:H1(M)H1(M)i_{*}:H_{1}(\partial M)\rightarrow H_{1}(M), the basis elements μ\mu and λM\lambda_{M} are mapped to (,u)(\ell,u) and (0,h)(0,h), respectively, where ||=ordHi(λM)|\ell|=\operatorname{ord}_{H}i_{*}(\lambda_{M}), and u,hu,h are some elements of HH.

Let us introduce some notation. Consider a decomposition of the finite abelian group HH as /r1/rk\mathbb{Z}/r_{1}\oplus\cdots\oplus\mathbb{Z}/r_{k}. We will write u=(u1,,uk)\vec{u}=(u_{1},\cdots,u_{k}) and v=(v1,,vk)\vec{v}=(v_{1},\cdots,v_{k}) for elements u,vHu,v\in H written with respect to this decomposition. The notation IrI_{\vec{r}} will stand for the k×kk\times k diagonal matrix with ii-th diagonal entry rir_{i} where r1,,rkr_{1},\dots,r_{k} are the invariant factors of HH.

For a filling slope η=pμ+qλM\eta=p\mu+q\lambda_{M}, Watson observes that H1(M(η))=H1(M)/(p,pu+qh)H_{1}(M(\eta))=H_{1}(M)/(p\ell,pu+qh) has a block form presentation matrix

(2) (p0pu+qhIr),\left(\begin{array}[]{cc}p\ell&0\\ p\vec{u}+q\vec{h}&I_{\vec{r}}\end{array}\right),

The statement of the lemma then follows.

The reader may notice that the proof of Lemma 2.3 below is adapted from the argument given in [LM17, Theorem 2.4]. In general, we will use the Smith normal form of the presentation matrix (2). Recall that the Smith normal form is a diagonal matrix IδI_{\vec{\delta}} where δi|δi+1\delta_{i}|\delta_{i+1}. Each δi=Γi/Γi1\delta_{i}=\Gamma_{i}/\Gamma_{i-1}, where Γi\Gamma_{i} is the greatest common divisor of the the i×ii\times i minors of AA, and Γ0=1\Gamma_{0}=1.

Lemma 2.3.

Suppose that H1(Y)/d1/d2/dkH1(Y)H_{1}(Y)\cong\mathbb{Z}/d_{1}\oplus\mathbb{Z}/d_{2}\oplus\cdots\oplus\mathbb{Z}/d_{k}\cong H_{1}(Y^{\prime}) where each did_{i} is an odd square-free integer. If YY^{\prime} is obtained from YY by a distance one surgery on a knot KK in YY, then KK is null-homologous and the surgery coefficient is ±1\pm 1.

Proof.

Let M=YN(K)M=Y-N(K) and fix (μ,λM)(\mu,\lambda_{M}) as a basis of H1(M)H_{1}(\partial M), where μ\mu is some curve dual to the rational longitude λM\lambda_{M}. In this basis, filling slopes α\alpha and β\beta yielding YY and YY^{\prime}, respectively, may be written as α=pμ+qλM\alpha=p\mu+q\lambda_{M} and β=rμ+sλM\beta=r\mu+s\lambda_{M} for some integers p,r>0p,r>0 and q,sq,s relatively prime to p,rp,r.

By assumption |H1(M(α))|=|H1(M(β))||H_{1}(M(\alpha))|=|H_{1}(M(\beta))|. Applying Lemma 2.2, we have

ordHi(λM)|H|Δ(α,λM)=|H1(M(α))|=|H1(M(β))|=ordHi(λM)|H|Δ(β,λM).\operatorname{ord}_{H}i_{*}(\lambda_{M})\cdot|H|\cdot\Delta(\alpha,\lambda_{M})=|H_{1}(M(\alpha))|=|H_{1}(M(\beta))|=\operatorname{ord}_{H}i_{*}(\lambda_{M})\cdot|H|\cdot\Delta(\beta,\lambda_{M}).

This implies that p=Δ(α,λM)=Δ(β,λM)=rp=\Delta(\alpha,\lambda_{M})=\Delta(\beta,\lambda_{M})=r. The assumption that YY^{\prime} is obtained by a distance one surgery along KK means that Δ(α,β)\Delta(\alpha,\beta) is one. Therefore

1=Δ(α,β)=p(qs),1=\Delta(\alpha,\beta)=p(q-s),

and so |p|=1|p|=1 and |qs|=1|q-s|=1. After possibly multiplying by 1-1 to ensure p=1p=1, we may write α=μ+qλM\alpha=\mu+q\lambda_{M} and β=μ+(q±1)λM\beta=\mu+(q\pm 1)\lambda_{M}. With the change of basis (μ,λM)(μ+qλM,λM)(\mu,\lambda_{M})\mapsto(\mu+q\lambda_{M},\lambda_{M}), we can further assume α=μ\alpha=\mu and β=μ±λM\beta=\mu\pm\lambda_{M}.

By (1), we have that

|H1(Y)|=|H1(M(α))|=ordHi(λM)|H|.|H_{1}(Y)|=|H_{1}(M(\alpha))|=\operatorname{ord}_{H}i_{*}(\lambda_{M})\cdot|H|.

If ordHi(λM)=1\operatorname{ord}_{H}i_{*}(\lambda_{M})=1, then λM\lambda_{M} bounds in MM. Because λM\lambda_{M} is homologous to the core of the filling torus N(K)N(K) in M(α)M(\alpha), this also means that KK is null-homologous in Y=M(α)Y=M(\alpha). Thus we aim to show that ordHi(λM)=1\operatorname{ord}_{H}i_{*}(\lambda_{M})=1.

Suppose now it is not the case, so that ordHi(λM)=||1\operatorname{ord}_{H}i_{*}(\lambda_{M})=|\ell|\neq 1. Consider the presentation matrices AA and BB for H1(M(α))H_{1}(M(\alpha)) and H1(M(β))H_{1}(M(\beta)),

A=(u1r1ukrk) and B=(u1±h1r1uk±hkrk),A=\left(\begin{array}[]{ccccc}\ell&\\ u_{1}&r_{1}\\ \vdots&&\ddots\\ u_{k}&&&r_{k}\end{array}\right)\text{ and }B=\left(\begin{array}[]{ccccc}\ell&\\ u_{1}\pm h_{1}&r_{1}\\ \vdots&&\ddots\\ u_{k}\pm h_{k}&&&r_{k}\end{array}\right),

where we have multiplied the first column by a unit to ensure that =ordHi(λM)\ell=\operatorname{ord}_{H}i_{*}(\lambda_{M}).

We claim that each uiu_{i} is a multiple of gcd(,ri)\gcd(\ell,r_{i}). If not, then there is some uiu_{i} for which there exists a prime power pjp^{j} that divides both \ell and rir_{i}, but not uiu_{i}. Consider now det(A)=|r1rk|=|δ1δk+1|\det(A)=|\ell r_{1}\cdots r_{k}|=|\delta_{1}\cdots\delta_{k+1}|. Since p|p|\ell and p|rip|r_{i} we know that pt|det(A)p^{t}|\det(A) for some power tt. However, if we consider the k×kk\times k minor A1,i+1A_{1,i+1} we see (by, say, cofactor expansion at uiu_{i}) that det(A1,i+1)=|r1ri1uiri+1rk|\det(A_{1,i+1})=|r_{1}\cdots r_{i-1}u_{i}r_{i+1}\cdots r_{k}| is divisible by at most pt2p^{t-2}. Consider now the Smith normal form of AA. By definition δk+1=det(A)/Γk\delta_{k+1}=\det(A)/\Gamma_{k}. In particular, Γk\Gamma_{k} is divisible by at most pt2p^{t-2}. But this implies p2|δk+1p^{2}|\delta_{k+1}, and hence some invariant factor is not square-free. Because we have assumed that the did_{i} are square-free, we must also have that the δi\delta_{i} are square free. Hence we have reached a contradiction.

Notice that the same argument will apply to the presentation matrix BB for H1(M(β))H_{1}(M(\beta)) to show that gcd(,ri)|(ui±hi)\gcd(\ell,r_{i})|(u_{i}\pm h_{i}) for i=1,,ki=1,\cdots,k. Since gcd(,ri)|(ui±hi)\gcd(\ell,r_{i})|(u_{i}\pm h_{i}) and gcd(,ri)|ui\gcd(\ell,r_{i})|u_{i}, we also have gcd(,ri)|hi\gcd(\ell,r_{i})|h_{i}. With this, we may write

B=(u1+b1gcd(,r1)r1uk+bkgcd(,rk)rk),B=\left(\begin{array}[]{ccccc}\ell&\\ u_{1}+b_{1}\gcd(\ell,r_{1})&r_{1}\\ \vdots&&\ddots\\ u_{k}+b_{k}\gcd(\ell,r_{k})&&&r_{k}\end{array}\right),

for some integers b1,,bkb_{1},\cdots,b_{k}.

Observe that hHh\in H is trivial if and only if h\vec{h} is in the column space of Ir=B1,1I_{\vec{r}}=B_{1,1}. In particular, since =ordHi(λM)\ell=\operatorname{ord}_{H}i_{*}(\lambda_{M}), we have that h\ell\vec{h} is in the column space of B1,1B_{1,1}. Thus there exist integers xix_{i} so that for all i=1,,ki=1,\cdots,k.

hi=bigcd(,ri)=xiri.\ell h_{i}=\ell b_{i}\gcd(\ell,r_{i})=x_{i}r_{i}.

This then implies ri/gcd(,ri)r_{i}/\gcd(\ell,r_{i}) is a divisor of bib_{i}, so that bi=yiri/gcd(,ri)b_{i}=y_{i}r_{i}/\gcd(\ell,r_{i}) for some yiy_{i}. We can then write hi=yirih_{i}=y_{i}r_{i}. This shows h\vec{h} is in the column space of B1,1B_{1,1}, which implies i(λM)=(0,h)Hi_{*}(\lambda_{M})=(0,h)\in\mathbb{Z}\oplus H is trivial.

We have established that ordHi(λM)=1\operatorname{ord}_{H}i_{*}(\lambda_{M})=1 and hence KK is null-homologous in Y=M(α)Y=M(\alpha). Now we take may take the preferred basis (μ,λ)(\mu,\lambda) on H1(M)H_{1}(\partial M), where μ\mu is the meridian of KK and λ\lambda is a Seifert longitude. The condition that the slope yielding YY^{\prime} is distance one from the meridian implies the slope must in fact be μ±λ\mu\pm\lambda, i.e. the surgery coefficient is ±1\pm 1.∎

For the remainder of the article, we will assume that KK is a null-homologous knot in YY with meridian μ\mu and longitude λ\lambda. We will be primarily concerned with slopes of the form nμ+λn\mu+\lambda, for nn\in\mathbb{Z}, which are framing curves on the boundary of a neighborhood of KK. These slopes intersect the meridian once transversely and inherit an orientation from KK. The notation Yn(K)Y_{n}(K) will denote the result of integral surgery along KK, and KnK_{n} will denote the core of the surgery Yn(K)Y_{n}(K).

The set Spinc(Y)\text{Spin}^{c}(Y) is the space of nowhere vanishing vector fields on YY modulo homotopy outside of a ball. There is a non-canonical correspondence Spinc(Y)H2(Y)\text{Spin}^{c}(Y)\cong H^{2}(Y) [Tur97]. We write 𝔱\mathfrak{t} to denote an element of Spinc(Y)\text{Spin}^{c}(Y), and write Spinc¯(Y,K)\underline{\mathrm{Spin}^{c}}(Y,K) to denote the relative Spinc\text{Spin}^{c} structures on (M,M)(M,\partial M). Note that Spinc¯(Y,K)\underline{\mathrm{Spin}^{c}}(Y,K) has an affine identification with H2(Y,K)H^{2}(Y,K), which by excision is isomorphic with H2(M,M)H1(M)H^{2}(M,\partial M)\cong H_{1}(M). In particular, because KK is null-homologous and H1(M)H1(Y)H_{1}(M)\cong H_{1}(Y)\oplus\mathbb{Z}, we may label an element ξ\xi of Spinc¯(Y,K)\underline{\mathrm{Spin}^{c}}(Y,K) by ξ=(𝔱,s)\xi=(\mathfrak{t},s), where 𝔱Spinc(Y)\mathfrak{t}\in\text{Spin}^{c}(Y) and ss\in\mathbb{Z}. The correspondence Spinc¯(Y,K)H2(M,M)\underline{\mathrm{Spin}^{c}}(Y,K)\equiv H^{2}(M,\partial M) is non-canonical, and the labelling that we adopt follows closely to that of [Gai18]. When H1(Y)H_{1}(Y) has odd order, there is a unique self-conjugate Spinc\text{Spin}^{c} structure 𝔱0\mathfrak{t}_{0}, distinguished from the others by the requirement that it satisfies c1(𝔱0)=0H2(Y)c_{1}(\mathfrak{t}_{0})=0\in H^{2}(Y) (see for example [Section 2][MO07]).

3. Heegaard Floer invariants and the proof of Theorem 3.5

3.1. Heegaard Floer background and the mapping cone formula

We will assume some familiarity with Heegaard Floer homology, referring the reader to [OS03, OS11] for more information. We take all Heegaard Floer complexes with coefficients in the field 𝔽=/2\mathbb{F}=\mathbb{Z}/2. One of the main components of the Heegaard Floer package we will use is the dd-invariant d(Y,𝔱)d(Y,\mathfrak{t}), or correction term, which is a rational number associated to a Spinc\text{Spin}^{c} rational homology sphere (Y,𝔱)(Y,\mathfrak{t}). More specifically, given a rational homology sphere YY, the Heegaard Floer module HF+(Y)HF^{+}(Y) splits over Spinc\text{Spin}^{c} structures, and in each summand we have

(3) HF+(Y,𝔱)=𝔽[U,U1]/U𝔽[U]HFred+(Y,𝔱),HF^{+}(Y,\mathfrak{t})=\mathbb{F}[U,U^{-1}]/U\cdot\mathbb{F}[U]\oplus HF^{+}_{red}(Y,\mathfrak{t}),

as 𝔽[U]\mathbb{F}[U]-modules. The first summand is abbreviated 𝒯d+\mathcal{T}_{d}^{+} and referred to as the tower. The second summand is a torsion 𝔽[U]\mathbb{F}[U]-module. An L-space is a rational homology sphere whose Heegaard Floer homology HF+(Y)HF^{+}(Y) is a free 𝔽[U]\mathbb{F}[U]-module with rank |H2(Y;)||H^{2}(Y;\mathbb{Z})|. That is, the torsion summand in (3) vanishes, leaving only a tower in each Spinc\text{Spin}^{c} structure. The dd-invariant d:=d(Y,𝔱)d:=d(Y,\mathfrak{t}) is defined to be the minimal Maslov grading of the tower. The dd-invariants switch sign under orientation-reversal [OS03].

Associated to (Y,K)(Y,K) and each relative Spinc\text{Spin}^{c} structure ξ\xi in Spinc¯(Y,K)\underline{\mathrm{Spin}^{c}}(Y,K) is the knot Floer chain complex Cξ=CFK(Y,K,ξ)C_{\xi}=CFK^{\infty}(Y,K,\xi) [Ras03, OS04, OS11]. The complex is \mathbb{Z}-filtered over 𝔽[U,U1]\mathbb{F}[U,U^{-1}] with a second filtration induced by the action of the variable UU. We denote these two filtrations as (i,j)=(i,j)= (algebraic, Alexander). The chain complex also has a homological Maslov grading that we suppress in the notation. Multiplication by UU decreases the Maslov grading by two and the Alexander filtration by one, and the action of PD[μ]PD[\mu] on ξ\xi shifts the Alexander filtration by one, i.e. Cξ+PD[μ]=Cξ[(0,1)]C_{\xi+PD[\mu]}=C_{\xi}[(0,-1)]. Recall that μ\mu denotes the (class of a) meridian.

As in [OS11], for each ξ\xi in Spinc¯(Y,K)\underline{\mathrm{Spin}^{c}}(Y,K) there are complexes Aξ+=Cξ{max{i,j}0}A^{+}_{\xi}=C_{\xi}\{\max\{i,j\}\geq 0\} and Bξ+=Cξ{i0}B^{+}_{\xi}=C_{\xi}\{i\geq 0\}. The complex Bξ+B^{+}_{\xi} is CF+(Y,GY,K(ξ))CF^{+}(Y,G_{Y,K}(\xi)). The map GY,K:Spinc¯(Y,K)Spinc(Y)G_{Y,K}:\underline{\mathrm{Spin}^{c}}(Y,K)\rightarrow\text{Spin}^{c}(Y) is defined in [OS11, Section 2.2], and sends a relative Spinc\text{Spin}^{c} structure to a Spinc\text{Spin}^{c} structure in the target manifold indicated by the subscript. The complex Aξ+A^{+}_{\xi} represents the Heegaard Floer complex of a large surgery YN(K)Y_{N}(K) in a certain Spinc\text{Spin}^{c} structure, where YN(K)Y_{N}(K) is obtained by Dehn surgery along a framing curve Nμ+λN\mu+\lambda with N>>0N>>0. There are analogous complexes in the ‘hat’ version of Heegaard Floer homology. In particular we have A^ξ=Cξ{max{i,j}=0}\widehat{A}_{\xi}=C_{\xi}\{\max\{i,j\}=0\} and B^ξ=Cξ{i=0}CF^(Y,GY,K(ξ))\widehat{B}_{\xi}=C_{\xi}\{i=0\}\cong\widehat{CF}(Y,G_{Y,K}(\xi)). The complexes are related by chain maps

(4) vξ+:Aξ+Bξ+,hξ+:Aξ+Bξ+PD[Kn]+,v^ξ:A^ξB^ξ,h^ξ:A^ξB^ξ+PD[Kn],\begin{array}[]{r@{} r@{\qquad} l}v^{+}_{\xi}:A^{+}_{\xi}\to B^{+}_{\xi},&&h^{+}_{\xi}:A^{+}_{\xi}\to B^{+}_{\xi+PD[K_{n}]},\\ \widehat{v}_{\xi}:\widehat{A}_{\xi}\to\widehat{B}_{\xi},&&\widehat{h}_{\xi}:\widehat{A}_{\xi}\to\widehat{B}_{\xi+PD[K_{n}]},\end{array}

where KnK_{n} is the push-off of KK inside YN(K)Y-N(K) using framing nμ+λn\mu+\lambda. In [OS11, Theorem 4.1], it is shown that the maps vξ+v^{+}_{\xi} and hξ+h^{+}_{\xi} correspond with a negative definite cobordism WN:YN(K)YW^{\prime}_{N}:Y_{N}(K)\rightarrow Y equipped with the Spinc\text{Spin}^{c} structures 𝔳\mathfrak{v} and 𝔥=𝔳+PD[F^]\mathfrak{h}=\mathfrak{v}+PD[\widehat{F}], respectively, which extend a given Spinc\text{Spin}^{c} structure on YN(K)Y_{N}(K). Here, [F^][\widehat{F}] generates H2(WN,Y)H_{2}(W^{\prime}_{N},Y) and is represented by a capped-off Seifert surface for KK.

The complexes Aξ+A^{+}_{\xi} and Bξ+B^{+}_{\xi} each contain a non-torsion summand, i.e. a tower. On homology, each of the maps vξ+v^{+}_{\xi} and hξ+h^{+}_{\xi} induces an endomorphism of the towers, which is multiplication by UξVU^{V}_{\xi} or UξHU^{H}_{\xi} for integers Vξ0V_{\xi}\geq 0 and Hξ0H_{\xi}\geq 0. This defines the knot invariants VξV_{\xi} and HξH_{\xi}, which appeared originally as the local h-invariants in [Ras03]. We remark for later use that when Vξ>0V_{\xi}>0, the corresponding map v^ξ\widehat{v}_{\xi} is identically zero, and similarly Hξ>0H_{\xi}>0 implies h^ξ\widehat{h}_{\xi} is zero.

Recall that because KK is null-homologous, Spinc¯(Y,K)Spinc(Y)\underline{\mathrm{Spin}^{c}}(Y,K)\cong\text{Spin}^{c}(Y)\oplus\mathbb{Z}, where the \mathbb{Z}-summand is generated by the meridian of KK [Gai18, Lemma 8.1]. We write ξ=(𝔱,s)\xi=(\mathfrak{t},s) for 𝔱Spinc(Y)\mathfrak{t}\in\text{Spin}^{c}(Y) and ss\in\mathbb{Z}. Fixing 𝔱Spinc(Y)\mathfrak{t}\in\text{Spin}^{c}(Y), we have the subgroup {𝔱}\{\mathfrak{t}\}\oplus\mathbb{Z}\cong\mathbb{Z}. Because the following properties have appeared in various forms throughout the literature, we provide just a sketch of the proof.

Property 3.1.

Let KK be a null-homologous knot in a rational homology sphere YY and let 𝔱\mathfrak{t} be a self-conjugate Spinc\text{Spin}^{c} structure on YY. Then the invariants V(𝔱,s)V_{(\mathfrak{t},s)} and H(𝔱,s)H_{(\mathfrak{t},s)} satisfy:

  1. (1)

    V(𝔱,s)V(𝔱,s+1)V(𝔱,s)1V_{(\mathfrak{t},s)}\geq V_{(\mathfrak{t},s+1)}\geq V_{(\mathfrak{t},s)}-1,

  2. (2)

    V(𝔱,s)=H(𝔱,s)V_{(\mathfrak{t},s)}=H_{(\mathfrak{t},-s)},

  3. (3)

    H(𝔱,s)V(𝔱,s)H_{(\mathfrak{t},s)}\geq V_{(\mathfrak{t},s)} for s0s\geq 0.

(sketch).

Since Spinc¯(Y,K)Spinc(Y)\underline{\mathrm{Spin}^{c}}(Y,K)\cong\text{Spin}^{c}(Y)\oplus\mathbb{Z}, we have that ξ+PD[μ]=(𝔱,s)+PD[μ]=(𝔱,s+1)\xi+PD[\mu]=(\mathfrak{t},s)+PD[\mu]=(\mathfrak{t},s+1). When we fix a self-conjugate Spinc\text{Spin}^{c} structure on 𝔱\mathfrak{t} on YY, the statements above relating V(𝔱,s)V_{(\mathfrak{t},s)} and H(𝔱,s)H_{(\mathfrak{t},s)} are analogous to those for the invariants VsV_{s} and HsH_{s}, with ss\in\mathbb{Z}, for the case of a knot in an integer homology sphere. In particular, Property 1 follows as a direct analogue of [Ras03, Property 7.6] (see also [NW15, Lemma 2.4]). Next, because conjugation changes the sign of the first Chern class and the H2H^{2}-action, we may verify using the formulas of [OS08, Section 4.3] that 𝔥(𝔱,s)\mathfrak{h}_{(\mathfrak{t},s)} and 𝔳(𝔱,s)\mathfrak{v}_{(\mathfrak{t},s)} are conjugate Spinc\text{Spin}^{c} structures on the four-manifold cobordism WNW^{\prime}_{N}. This implies Property 2. Finally, 1 and 2 imply 3. See also [HLZ15, Lemmas 2.3-2.5]. ∎

The proof of Theorem 3.5 below will require the mapping cone formula for the Heegaard Floer homology of the integral surgery Yn(K)Y_{n}(K). We give only a terse review here, sending the reader to Ozsváth and Szabó for details [OS08, OS11]. The generalization of the mapping cone formula specific to rational surgeries on null-homologous knots in L-spaces is also reviewed in [NW15, Gai18]. Note that for our applications, we only require the formulation for integral surgery and ‘hat’ homology.

For each 𝔱Spinc(Y)\mathfrak{t}\in\text{Spin}^{c}(Y) and 0i<n0\leq i<n, sum up the complexes A^ξ=A^(𝔱,s)\widehat{A}_{\xi}=\widehat{A}_{(\mathfrak{t},s)} and B^ξ=B^(𝔱,s)\widehat{B}_{\xi}=\widehat{B}_{(\mathfrak{t},s)} into

𝔸^(𝔱,i)=s(s,A^(𝔱,i+ns)) and 𝔹^(𝔱,i)=s(s,B^(𝔱,i)),\widehat{\mathbb{A}}_{(\mathfrak{t},i)}=\bigoplus_{s\in\mathbb{Z}}(s,\widehat{A}_{(\mathfrak{t},i+ns)})\text{ and }\widehat{\mathbb{B}}_{(\mathfrak{t},i)}=\bigoplus_{s\in\mathbb{Z}}(s,\widehat{B}_{(\mathfrak{t},i)}),

where the first component of each tuple records the index of the summand. Using the maps v^ξ\widehat{v}_{\xi} and h^ξ\widehat{h}_{\xi} from equation (4) above, we define the map 𝔻^(𝔱,i):𝔸^(𝔱,i)𝔹^(𝔱,i)\widehat{\mathbb{D}}_{(\mathfrak{t},i)}:\widehat{\mathbb{A}}_{(\mathfrak{t},i)}\rightarrow\widehat{\mathbb{B}}_{(\mathfrak{t},i)} by

𝔻^(𝔱,i),n(s,as)=(s,v^(𝔱,i+ns)(as))+(s+1,h^(𝔱,i+ns)(as)).\widehat{\mathbb{D}}_{(\mathfrak{t},i),n}(s,a_{s})=(s,\widehat{v}_{(\mathfrak{t},i+ns)}(a_{s}))+(s+1,\widehat{h}_{(\mathfrak{t},i+ns)}(a_{s})).

The mapping cone complex of 𝔻^(𝔱,i),n\widehat{\mathbb{D}}_{(\mathfrak{t},i),n} is denoted 𝕏^(𝔱,i),n\widehat{\mathbb{X}}_{(\mathfrak{t},i),n}. Let us omit the surgery coefficient ‘nn’ and write the summand of the cone corresponding to the equivalence class of ξ=(𝔱,i)\xi=(\mathfrak{t},i) more concisely as 𝕏^ξ\widehat{\mathbb{X}}_{\xi}.

Theorem 3.2 (Ozsváth and Szabó, [OS11]).

Let ξSpinc¯(Y,K)\xi\in\underline{\mathrm{Spin}^{c}}(Y,K). Then there is a relatively-graded isomorphism of groups

(5) H(𝕏^ξ)HF^(Yn(K),GYn(K),Kn(ξ)).H_{*}(\widehat{\mathbb{X}}_{\xi})\cong\widehat{HF}(Y_{n}(K),G_{Y_{n}(K),K_{n}}(\xi)).\\

Given a Spinc\text{Spin}^{c} structure in Spinc(Yn(K))Spinc(Y)/n\text{Spin}^{c}(Y_{n}(K))\cong\text{Spin}^{c}(Y)\oplus\mathbb{Z}/n, there is a unique Spinc\text{Spin}^{c} structure on YY which extends over the two-handle cobordism Wn(K):YYn(K)W_{n}(K):Y\rightarrow Y_{n}(K) and this defines the projection from Spinc(Yn(K))\text{Spin}^{c}(Y_{n}(K)) to Spinc(Y)\text{Spin}^{c}(Y). This projection appears in the following result of Ni and Wu, which will allow us to describe the dd-invariants of surgeries in terms of the invariants V𝔱,iV_{\mathfrak{t},i}, which crucially, are non-negative integers.

Proposition 3.3 (Proposition 1.6 in [NW15]).

Fix an integer n>0n>0 and a self-conjugate Spinc\text{Spin}^{c} structure 𝔱\mathfrak{t} on an L-space YY. Let KK be a null-homologus knot in YY. Then, there exists a bijective correspondence i𝔱ii\leftrightarrow\mathfrak{t}_{i} between /n\mathbb{Z}/n and the Spinc\text{Spin}^{c} structures on Spinc(Yn(K))\text{Spin}^{c}(Y_{n}(K)) that extend 𝔱\mathfrak{t} over Wn(K)W_{n}(K) such that

(6) d(Yn(K),𝔱i)=d(Y,𝔱)+d(L(n,1),i)2N𝔱,id(Y_{n}(K),\mathfrak{t}_{i})=d(Y,\mathfrak{t})+d(L(n,1),i)-2N_{\mathfrak{t},i}

where N𝔱,i=max{V𝔱,i,V𝔱,ni}N_{\mathfrak{t},i}=\max\{V_{\mathfrak{t},i},V_{\mathfrak{t},n-i}\}. Here, we assume that 0i<n0\leq i<n.

Proposition 3.3 was originally proved for knots in the three-sphere, but it generalizes immediately to the case of a null-homologous knot in an L-space [NW15], which is the version stated here (see also [LMV19]). The term on the right includes the dd-invariants of the lens space L(n,1)L(n,1), which are made explicit in section 3.3.

The following proposition will be useful in the proofs of the main results. A proof of Proposition 3.4 is given in [LMV19, Proposition 2.10].

Proposition 3.4 (Lidman-Moore-Vazquez [LMV19]).

Let KK be a null-homologous knot in a /2\mathbb{Z}/2-homology sphere YY. Let 𝔱\mathfrak{t} be the self-conjugate Spinc\text{Spin}^{c} structure on YY, and let 𝔱0\mathfrak{t}_{0} be the Spinc\text{Spin}^{c} structure on Yn(K)Y_{n}(K) described in Proposition 3.3. Then 𝔱0\mathfrak{t}_{0} is also self-conjugate on Yn(K)Y_{n}(K).

3.2. Proof of Theorem 3.5

In this section we prove the main result. The requirement that YY and YY^{\prime} are L-spaces in the statement of Theorem 3.5 is necessary both to calculate the differences in their dd-invariants via the surgery formula of Proposition 3.3, and to use the surgery formula directly to determine the value of the invariant V𝔱,0V_{\mathfrak{t},0}. The L-space condition will surface again when we apply Theorem 3.5 to alternating and quasi-alternating knots to obtain Corollary 4.3 and Theorem 4.4. The significance in this context is that quasi-alternating knots have branched double covers that are L-spaces, and there is a connection between the signature of the knot and a certain dd-invariant of the branched double cover.

Theorem 3.5.

Let YY and YY^{\prime} be L-spaces with H1(Y)/d1/d2/dkH1(Y)H_{1}(Y)\cong\mathbb{Z}/d_{1}\oplus\mathbb{Z}/d_{2}\oplus\cdots\oplus\mathbb{Z}/d_{k}\cong H_{1}(Y^{\prime}), where each did_{i} is an odd square-free integer. If YY^{\prime} is obtained by a distance one surgery along any knot KK in YY, then

(7) |d(Y,𝔱)d(Y,𝔱)|=2 or 0|d(Y,\mathfrak{t})-d(Y^{\prime},\mathfrak{t}^{\prime})|=2\text{ or }0

where 𝔱\mathfrak{t} and 𝔱\mathfrak{t}^{\prime} denote the unique self-conjugate Spinc\text{Spin}^{c} structures on YY and YY^{\prime}.

Proof.

Suppose that the homological condition on YY and YY^{\prime} is satisfied and that YY^{\prime} is obtained by a distance one surgery along some knot KK in YY. By Lemma 2.3, KK is null-homologous in YY and the surgery coefficient is ±1\pm 1.

Let us first consider when the surgery coefficient is exactly n=+1n=+1, that is, the filling slope yielding YY^{\prime} is μ+λ\mu+\lambda. Since KK is a null-homologous knot in an L-space YY along which there exists an integral surgery to YY^{\prime}, we may apply Proposition 3.3. In particular, fixing the unique self-conjugate Spinc\text{Spin}^{c} structure 𝔱\mathfrak{t} on YY, there is one Spinc\text{Spin}^{c}-structure 𝔱0\mathfrak{t}_{0} on Spinc(Y)Spinc(Y)/m\text{Spin}^{c}(Y^{\prime})\cong\text{Spin}^{c}(Y)\cong\mathbb{Z}/m that extends 𝔱\mathfrak{t} over W1(K)W_{1}(K). By Proposition 3.4, 𝔱0\mathfrak{t}_{0} is self-conjugate on YY^{\prime}. But there is a unique self-conjugate Spinc\text{Spin}^{c} structure 𝔱\mathfrak{t}^{\prime} in YY^{\prime}. Therefore 𝔱0=𝔱\mathfrak{t}_{0}=\mathfrak{t}^{\prime} and by equation (6) we have

(8) d(Y,𝔱)=d(Y,𝔱)+d(L(1,1),0)2N𝔱,0.d(Y^{\prime},\mathfrak{t}^{\prime})=d(Y,\mathfrak{t})+d(L(1,1),0)-2N_{\mathfrak{t},0}.

Because L(1,1)L(1,1) is the three-sphere, the term d(L(1,1),0)d(L(1,1),0) vanishes, leaving

(9) d(Y,𝔱)d(Y,𝔱)=2N𝔱,0,d(Y,\mathfrak{t})-d(Y^{\prime},\mathfrak{t}^{\prime})=2N_{\mathfrak{t},0},

where N𝔱,0=max{V𝔱,0,V𝔱,1}N_{\mathfrak{t},0}=\max\{V_{\mathfrak{t},0},V_{\mathfrak{t},1}\}. We claim that V𝔱,0V_{\mathfrak{t},0} is at most one.

Consider the mapping cone formula for the Heegaard Floer chain complex of YY^{\prime}. Recall that Y=Yn(K)Y^{\prime}=Y_{n}(K), where we have assumed that n=+1n=+1. By assumption, both YY and YY^{\prime} are L-spaces. Therefore H(B^ξ)𝔽H_{*}(\widehat{B}_{\xi})\cong\mathbb{F}, and H(𝕏^ξ)𝔽H_{*}(\widehat{\mathbb{X}}_{\xi})\cong\mathbb{F} for any ξSpinc¯(Y,K)\xi\in\underline{\mathrm{Spin}^{c}}(Y,K).

By [OS05a, Proposition 2.1], any sufficiently large surgery YN(K)Y_{N}(K) will also be an L-space. Since the Heegaard Floer complex of the large surgery YN(K)Y_{N}(K) (in some Spinc\text{Spin}^{c}-structure) is quasi-isomorphic with the complex A^ξ\widehat{A}_{\xi}, we have that the homology of every summand A^ξ\widehat{A}_{\xi} is torsion-free. In particular,

(10) H(A^ξ)𝔽 for all ξSpinc¯(Y,K).H_{*}(\widehat{A}_{\xi})\cong\mathbb{F}\text{ for all }\xi\in\underline{\mathrm{Spin}^{c}}(Y,K).

Thus, the Heegaard Floer homology of Yn(K)Y_{n}(K) is completely determined by the numbers VξV_{\xi} and HξH_{\xi} for each ξSpinc¯(Y,K)\xi\in\underline{\mathrm{Spin}^{c}}(Y,K) (for this statement, nn need not be one).

Since the mapping cone splits over Spinc(Y)\text{Spin}^{c}(Y), we may restrict our attention to the unique self-conjugate Spinc\text{Spin}^{c} structure 𝔱\mathfrak{t} on YY. We have that the ‘hat version’ of the mapping cone formula specialized to n=+1n=+1 surgery along KK and restricted to 𝔱\mathfrak{t} on YY is given by

\textstyle{\ldots\ignorespaces\ignorespaces\ignorespaces\ignorespaces}A^(𝔱,0)\textstyle{\widehat{A}_{(\mathfrak{t},0)}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}v^(𝔱,0)\scriptstyle{\widehat{v}_{(\mathfrak{t},0)}}h^(𝔱,0)\scriptstyle{\widehat{h}_{(\mathfrak{t},0)}}A^(𝔱,1)\textstyle{\widehat{A}_{(\mathfrak{t},1)}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}v^(𝔱,1)\scriptstyle{\widehat{v}_{(\mathfrak{t},1)}}h^(𝔱,1)\scriptstyle{\widehat{h}_{(\mathfrak{t},1)}}A^(𝔱,2)\textstyle{\widehat{A}_{(\mathfrak{t},2)}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}v^(𝔱,2)\scriptstyle{\widehat{v}_{(\mathfrak{t},2)}}h^(𝔱,2)\scriptstyle{\widehat{h}_{(\mathfrak{t},2)}}\textstyle{\ldots}\textstyle{\ldots}B^(𝔱,0)\textstyle{\widehat{B}_{(\mathfrak{t},0)}}B^(𝔱,1)\textstyle{\widehat{B}_{(\mathfrak{t},1)}}B^(𝔱,2)\textstyle{\widehat{B}_{(\mathfrak{t},2)}}\textstyle{\ldots}

where we have written ξ=(𝔱,s)\xi=(\mathfrak{t},s) in the above diagram for clarity.

Now suppose that V(𝔱,0)2V_{(\mathfrak{t},0)}\geq 2. Property 3.1(1) implies that V(𝔱,1)1V_{(\mathfrak{t},1)}\geq 1. Property 3.1(2) implies that H(𝔱,0)2H_{(\mathfrak{t},0)}\geq 2, and Property 3.1(3) then implies that H(𝔱,1)1H_{(\mathfrak{t},1)}\geq 1. Together these imply that the maps v^(𝔱,0),v^(𝔱,1),h^(𝔱,0)\widehat{v}_{(\mathfrak{t},0)},\widehat{v}_{(\mathfrak{t},1)},\widehat{h}_{(\mathfrak{t},0)} and h^(𝔱,1)\widehat{h}_{(\mathfrak{t},1)} are zero. In particular, A^(𝔱,0)\widehat{A}_{(\mathfrak{t},0)} and A^(𝔱,1)\widehat{A}_{(\mathfrak{t},1)} are in the kernel of (𝔻^ξ)(\widehat{\mathbb{D}}_{\xi})_{*}, and so

rank ker((𝔻^ξ))2.\text{rank }\ker((\widehat{\mathbb{D}}_{\xi})_{*})\geq 2.

By [Gai17, Lemma 12], the map induced by 𝔻^(𝔱,i)\widehat{\mathbb{D}}_{(\mathfrak{t},i)} on homology is surjective. Thus the long exact triangle

(11)
H(𝔸^ξ)\textstyle{H_{*}(\widehat{\mathbb{A}}_{\xi})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(𝔻^ξ)\scriptstyle{(\widehat{\mathbb{D}}_{\xi})_{*}}H(𝔹^ξ)\textstyle{H_{*}(\widehat{\mathbb{B}}_{\xi})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}H(𝕏^ξ)\textstyle{H_{*}(\widehat{\mathbb{X}}_{\xi})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

implies that ker((𝔻^ξ))H(𝕏^ξ)\ker((\widehat{\mathbb{D}}_{\xi})_{*})\cong H_{*}(\widehat{\mathbb{X}}_{\xi}). But now (10) and (11) imply that

rank ker((𝔻^ξ))=rank H(𝕏ξ+)=rank HF^(Y,𝔱)2,\text{rank }\ker((\widehat{\mathbb{D}}_{\xi})_{*})=\text{rank }H_{*}(\mathbb{X}^{+}_{\xi})=\text{rank }\widehat{HF}(Y^{\prime},\mathfrak{t}^{\prime})\geq 2,

which contradicts that YY^{\prime} is an L-space. Therefore V𝔱,0V_{\mathfrak{t},0} is at most one. This verifies the claim.

Finally, since N𝔱,0=max{V𝔱,0,V𝔱,1}=V𝔱,0N_{\mathfrak{t},0}=\max\{V_{\mathfrak{t},0},V_{\mathfrak{t},1}\}=V_{\mathfrak{t},0}, this completes the proof of the theorem in the case that the surgery coefficient is n=+1n=+1.

If instead the surgery coefficient is n=1n=-1, then we may reverse the roles of YY and YY^{\prime}. In particular, we consider n=+1n=+1 surgery along a null-homologous knot K1K_{1} in YY^{\prime} yielding the manifold YY (here K1K_{1} is the core of the previous surgery). The above argument applies with the corresponding change in notation. ∎

3.3. Lens spaces and dd-invariants

The dd-invariants of lens spaces can be computed with the following recursive formula of Ozsváth and Szabó.

Theorem 3.6 (Proposition 4.8 in [OS03]).

Let p>q>0p>q>0 be relatively prime integers. Then, there exists an identification Spinc(L(p,q))/p\text{Spin}^{c}(L(p,q))\cong\mathbb{Z}/p such that

(12) d(L(p,q),i)=14+(2i+1pq)24pqd(L(q,r),j)d(L(p,q),i)=-\frac{1}{4}+\frac{(2i+1-p-q)^{2}}{4pq}-d(L(q,r),j)

for 0i<p+q0\leq i<p+q. Here, rr and jj are the reductions of pp and i(modq)i\pmod{q} respectively.

It is well-known (see for example [OS06, Section 3.4]), that the self-conjugate Spinc\text{Spin}^{c} structures on the lens space L(p,q)L(p,q) correspond with the set

(13) {p+q12 , q12}.\mathbb{Z}\cap\{\frac{p+q-1}{2}\text{ , }\frac{q-1}{2}\}.

Note that when pp is odd, there is a unique self conjugate Spinc\text{Spin}^{c} structure.

Corollary 3.7.

Suppose that m>0m>0 is a square-free odd integer. There exists a distance one surgery along any knot KK in L(m,1)L(m,1) yielding L(m,1)-L(m,1) if and only if m=1m=1 or m=5m=5.

Proof.

Suppose first that m>0m>0 is a square-free odd integer and there exists a distance one surgery along any knot KK in L(m,1)L(m,1). Observe that H1(L(m,1))/mH_{1}(L(m,1))\cong\mathbb{Z}/m. Because the dd-invariants change sign under orientation-reversal [OS03], Theorem 3.5 implies that d(L(m,1),𝔱0)=0d(L(m,1),\mathfrak{t}_{0})=0 or 11. By equation (13), the Spinc\text{Spin}^{c} structure 𝔱0\mathfrak{t}_{0} corresponds with 0, hence by equation (12) in Theorem 3.6 we have

d(L(m,1),0)=m14.d(L(m,1),0)=\frac{m-1}{4}.

The dd-invariant is equal 0 for m=1m=1 and equal 11 for m=5m=5.

For the reverse direction, note that the branched double cover of T(2,m)T(2,m) is the lens space L(m,1)L(m,1), and that L(1,1)L(1,1) is the three-sphere. The Montesinos trick implies that any banding along T(2,m)T(2,m) lifts to a distance one Dehn surgery in L(m,1)L(m,1). In the case m=5m=5, a chirally cosmetic banding from the torus knot T(2,5)T(2,5) to its mirror image T(2,5)T(2,-5) exists [Zek15] and is pictured in Figure 2. This band move lifts to a distance one filling taking L(2,5)L(2,5) to L(2,5)-L(2,5). In the case m=1m=1, the relevant banding is induced by a Reidemeister-I move along an unknot (see Figure 3). ∎

Refer to caption
Figure 3. A non-coherent banding induced by a Reidemeister-I move.

Corollary 3.7 is used in section 4 to show that the only nontrivial torus knot T(2,m)T(2,m) with mm square free admitting a chirally cosmetic banding is T(2,5)T(2,5).

4. Band surgery and chirally cosmetic bandings

4.1. Band surgery

A band surgery can be described as a two-string tangle replacement as follows. After possibly isotoping LL and LL^{\prime}, the pairs (S3,L)(S^{3},L) and (S3,L)(S^{3},L^{\prime}) can be decomposed as

(S3,L)=(Bo,to)(B,t) and (S3,L)=(Bo,to)(B,t)(S^{3},L)=(B_{o},t_{o})\cup(B,t)\qquad\text{ and }\qquad(S^{3},L^{\prime})=(B_{o},t_{o})\cup(B,t^{\prime})

where S3S^{3} is the union of the two three-balls BB and BoB_{o} glued along their boundary, the sphere B=Bo\partial B=\partial B_{o} intersects each of LL and LL^{\prime} transversely in four points, and (B,t)(B,t), (B,t)(B,t^{\prime}), and (Bo,to)(B_{o},t_{o}) are two-string tangles where t=(BL)t=(B\cap L), t=(BL)t^{\prime}=(B\cap L^{\prime}) and to=(BoL)=(BoL)t_{o}=(B_{o}\cap L)=(B_{o}\cap L^{\prime}). Note that the “outside” tangle (Bo,to)(B_{o},t_{o}) is shared by both of (S3,L)(S^{3},L) and (S3,L)(S^{3},L^{\prime}). In particular, we may isotope LL and LL^{\prime} (possibly complicating the outside tangle) until (B,t)(B,t) and (B,t)(B,t^{\prime}) are the specific two-string rational tangles (B,t)=()=(0)(B,t)=(\hsmoothing)=(0) and (B,t)=()=()(B,t^{\prime})=(\smoothing)=(\infty), where (0)(0) and ()(\infty) correspond to the Conway notation. See [Kaw96, Mur96] for a general discussion of tangles.

The Montesinos trick [Mon76] implies that the branched double covers of knots (or links) related by a band surgery are obtained from distance one Dehn fillings of a three-manifold MM with torus boundary. This three-manifold MM is the double cover of the ball BoB_{o} branched over tot_{o}. Alternatively, MM can be described as Σ(L)N(K)\Sigma(L)-N(K), where the knot KK is the lift in the branched cover of the properly embedded arc arising as the core of the band in (B,t)(B,t). The filling slope α\alpha yielding Σ(L)\Sigma(L) is the meridian of KK, and the filling slope β\beta yielding Σ(L)\Sigma(L^{\prime}) is distance one from α\alpha, meaning α\alpha and β\beta intersect geometrically once.

4.2. Signature-based obstruction to the existence of a band surgery relating two knots

Here we give Theorem 4.4 as a corollary to Theorem 3.5. Recall that the double cover Σ(K)\Sigma(K) of the three-sphere branched over a knot KK is a rational homology sphere with H1(Σ(K))H_{1}(\Sigma(K)) of odd order. Ozsváth and Szabó [OS03] defined an integer-valued knot invariant

(14) δ(K)=2d(Σ(K),𝔱0),\delta(K)=2d(\Sigma(K),\mathfrak{t}_{0}),

where 𝔱0\mathfrak{t}_{0} is the Spinc\text{Spin}^{c} structure induced by the unique spin structure on Σ(K)\Sigma(K). For alternating knots, and for knots of small crossing number, Manolescu and Owens proved that δ(K)\delta(K) is determined by the signature σ(K)\sigma(K) [MO07].

Theorem 4.1 (Theorems 1.2 and 1.3 in [MO07]).

If the knot KK is alternating or if KK has nine or fewer crossings, then δ(K)=σ(K)/2\delta(K)=-\sigma(K)/2.

In [LO15, Theorem 1] Lisca and Owens generalized Theorem 4.1 to quasi-alternating knots. The class QAQA of quasi-alternating links generalizes alternating links [OS05b] (see Definition 4.2). Tables of quasi-alternating knots up to 12 crossings can be found in [Jab14].

Refer to caption
Figure 4. A non-coherent band surgery taking 8198_{19} to 313_{1}^{*} is obtained by the unoriented skein resolution indicated with the red arcs.
Definition 4.2.

The set QAQA of quasi-alternating links is the smallest set of links satisfying that the unknot is in QAQA, and that the set is closed under the following operation. If LL is a link which admits a diagram with a crossing such that

  1. (1)

    both resolutions L0=()L_{0}=(\hsmoothing) and L=()L_{\infty}=(\smoothing) are in QAQA

  2. (2)

    det(L0)0\det(L_{0})\neq 0, det(L)0\det(L_{\infty})\neq 0, and

  3. (3)

    det(L)=det(L0)+det(L)\det(L)=\det(L_{0})+\det(L_{\infty}),

then LL is in QAQA.

In sum, the signature of a knot is determined by δ(K)=2d(Σ(K),𝔱0)\delta(K)=2d(\Sigma(K),\mathfrak{t}_{0}) for alternating knots, quasi-alternating knots, and all knots of up to nine-crossings.

Corollary 4.3.

Let KK and KK^{\prime} be a pair of quasi-alternating knots and suppose that H1(Σ(K))/d1/d2/dkH1(Σ(K))H_{1}(\Sigma(K))\cong\mathbb{Z}/d_{1}\oplus\mathbb{Z}/d_{2}\oplus\cdots\oplus\mathbb{Z}/d_{k}\cong H_{1}(\Sigma(K^{\prime})), where each did_{i} is a square-free integer. If there exists a band surgery relating KK and KK^{\prime}, then |σ(K)σ(K)||\sigma(K)-\sigma(K^{\prime})| is 0 or 88.

Proof.

If KK and KK^{\prime} are quasi-alternating knots, then their branched double covers Σ(K)\Sigma(K) and Σ(K)\Sigma(K^{\prime}) are L-spaces [OS05b] and by assumption, H1(Σ(K))/d1/d2/dkH1(Σ(K))H_{1}(\Sigma(K))\cong\mathbb{Z}/d_{1}\oplus\mathbb{Z}/d_{2}\oplus\cdots\oplus\mathbb{Z}/d_{k}\cong H_{1}(\Sigma(K^{\prime})). If KK and KK^{\prime} differ by a band move, then Σ(K)\Sigma(K^{\prime}) is obtained by a distance one filling along a knot in Σ(K)\Sigma(K) (and vice versa). Therefore,

|d(Σ(K),𝔱0)d(Σ(K,𝔱0)|\displaystyle|d(\Sigma(K),\mathfrak{t}_{0})-d(\Sigma(K^{\prime},\mathfrak{t}_{0}^{\prime})| =2 or 0\displaystyle=2\text{ or }0
\displaystyle\Rightarrow |δ(K)δ(K)|\displaystyle|\delta(K)-\delta(K^{\prime})| =4 or 0\displaystyle=4\text{ or }0
\displaystyle\Rightarrow |σ(K)σ(K)|\displaystyle|\sigma(K)-\sigma(K^{\prime})| =8 or 0\displaystyle=8\text{ or }0

where the first line follows from Theorem 3.5, the second is the definition of δ\delta in equation (14), and the third line follows from Theorem 4.1 and its generalization [LO15, Theorem 1]. ∎

Note that Theorem 4.4 as stated in the introduction is the specific case of Corollary 4.3 when each did_{i} is a distinct prime.

Theorem 4.4.

Let KK and KK^{\prime} be a pair of quasi-alternating knots and suppose that det(K)=m=det(K)\det(K)=m=\det(K^{\prime}) for some square-free integer mm. If there exists a band surgery relating KK and KK^{\prime}, then |σ(K)σ(K)||\sigma(K)-\sigma(K^{\prime})| is 0 or 88.

Corollary 4.5.

Excluding 8198_{19}, let KK and KK^{\prime} be knots of eight or fewer crossings with det(K)=m=det(K)\det(K)=m=\det(K^{\prime}) for mm a square-free integer. If there exists a banding from KK to KK^{\prime}, then |σ(K)σ(K)|=0|\sigma(K)-\sigma(K^{\prime})|=0 or 88.

Proof.

All knots of up to eight crosings are alternating with the exception of 8198_{19}, 8208_{20} and 8218_{21}. Of these, 8208_{20} and 8218_{21} are quasi-alternating. So excluding 8198_{19}, all knots of up to eight crossings are quasi-alternating. The statement follows from Theorem 4.1. ∎

Table 1. Nomenclature conversion chart. Here KK^{*} denotes the mirror of KK. Our convention on nomenclature for mirroring agrees with that of [WFV18], and the slogan that “positive knots have negative signature” [Tra88, CG88]. In the last line nn can be any odd integer.
Writhe-guided Rolfsen Knotplot
313_{1} 313_{1}^{*} 313_{1} T(2,3)T(2,3)
515_{1} 515_{1}^{*} 515_{1} T(2,5)T(2,5)
525_{2} 525_{2}^{*} 525_{2}
626_{2} 626_{2}^{*} 626_{2}
717_{1} 717_{1}^{*} 717_{1} T(2,7)T(2,7)
888_{8} 888_{8} 888_{8}^{*}
8198_{19} 8198_{19} 8198_{19}^{*}
8208_{20} 8208_{20}^{*} 8208_{20}
n1n_{1} n1n_{1}^{*} n1n_{1} T(2,n)T(2,n)
Example 4.6.

Recall that the branched double cover of any alternating or quasi-alternating knot is an L-space. The knot 8198_{19} is not quasi-alternating (in fact, it is homology-thick) and its branched double cover is not an L-space, hence it is excluded from Corollary 4.5. However, a band surgery relates 313_{1}^{*} and 8198_{19}. (See Figure 4.) Here, det(31)=3=det(819)\det(3_{1}^{*})=3=\det(8_{19}) is square-free, and |σ(31)σ(819)|=|2(6)|=8|\sigma(3_{1}^{*})-\sigma(8_{19})|=|2-(-6)|=8. It is unknown whether the criterion of Corollary 4.5 always holds for 8198_{19}.

Example 4.7.

Consider the knots 626_{2} and 727_{2}, for which det(62)=11=det(72)\det(6_{2})=11=\det(7_{2}) and σ(62)=2=σ(72)\sigma(6_{2})=-2=\sigma(7_{2}). A single band surgery relates 626_{2} and 727_{2} (and hence 626_{2}^{*} and 727_{2}^{*}) [Zek15]. Theorem 4.4 implies there is no band surgery relating 626_{2} and 727_{2}^{*}. Similarly, consider 717_{1} and 525_{2}. In this case, det(71)=det(52)=7\det(7_{1})=\det(5_{2})=7, while σ(71)=6\sigma(7_{1})=-6 and σ(52)=2\sigma(5_{2})=-2, so there cannot be a band move relating 717_{1} and 525_{2}. However, Figure 1 illustrates the existence of a band surgery relating 717_{1} and 525_{2}^{*} [Zek15]. For the knots in this article, Table 1 provides a nomenclature conversion to Rolfsen [Rol90].

4.3. Chirally cosmetic bandings

A chirally cosmetic banding refers to a non-coherent band surgery taking a knot to its mirror image. The results in the previous section immediately imply the following corollary.

Corollary 4.8.

The only nontrivial torus knot T(2,m)T(2,m), with mm square free, admitting a chirally cosmetic banding is T(2,5)T(2,5).

Proof.

The statement follows from Corollary 3.7 because the branched double cover of T(2,m)T(2,m) is the lens space L(m,1)L(m,1). Alternatively, we may use Theorem 4.4. Without loss of generality, let m>0m>0. The torus knot T(2,m)T(2,m) has determinant mm and signature 1m1-m, whereas the mirror T(2,m)T(2,-m) has determinant mm and signature 1+m-1+m. The absolute value of the difference in signature between T(2,m)T(2,m) and T(2,m)T(2,-m) is 0 when m=1m=1 and is 88 when m=5m=5. The case of m=1m=1 is the unknot. The chirally cosmetic banding for the case m=5m=5 is pictured in Figure 2. ∎

Refer to caption
(A) The knots 888_{8} and 8208_{20}.
Refer to caption
Refer to caption
(B) Chirally cosmetic banding along 888_{8}^{*} and 8208_{20}.
Figure 5. (A) The knots 888_{8} and 8208_{20} are symmetric unions. (B) Chirally cosmetic bandings relating the pair 888_{8}^{*} and 888_{8} (left) and the pair 8208_{20} and 8208^{*}_{20} (right). The banding for 888_{8}^{*} was discovered via computer simulation. The banding for 8208_{20} induces a “4-move.”

The knot KK in L(5,1)L(5,1) along which there exists a distance one filling yielding L(5,1)-L(5,1) descends under the covering involution to the core of the band move from T(2,5)=51T(2,5)=5_{1} to T(2,5)=51T(2,-5)=5_{1}^{*}. As observed in [IJM18], the complement of this knot is the hyperbolic knot complement known as the “figure-eight sibling” and is well known to be amphichieral [MP06, Wee85]. The special symmetries of this manifold suggest an explanation for the uniqueness of T(2,5)T(2,5); see [IJM18] for a discussion of this perspective.

In addition to 515_{1}, several constructions of knots admitting chirally cosmetic bandings are described in [IJM18]. These include: the knot 9279_{27}, which has determinant 49; Whitehead doubles of achiral knots (i.e. certain satellites), which have determinant 1; and a general construction of certain symmetric unions. A symmetric union is a connected sum of a knot and its mirror image, modified by a tangle replacement such that the resulting diagram admits an axis of mirror symmetry (see Figure 5A). The determinant of a symmetric union is always a square [KT57, Moo16]. Indeed, excluding 515_{1}, all of the examples of knots admitting chirally cosmetic bandings presented in [IJM18] have determinant a square.

Numerical exploration of chirally cosmetic bandings. Corollary 4.8 and the observation that most known constructions of knots admitting chirally cosmetic bandings are symmetric unions suggest that this phenomenon is uncommon. To search for any further chirally cosmetic bandings amongst low crossing knots, we performed computer simulations (described at the end of this section) of non-coherent band surgery along knots. In brief, each knot type KK was embedded in the cubic lattice. The embeddings were randomized using a Monte Carlo algorithm, where 6×1066\times 10^{6} polygons were sampled for each chiral pair and a non-coherent band surgery was performed on each polygon.

Table 2. Chirally cosmetic bandings observed in numerical experiments. Here we report the number of chirally cosmetic bandings for knots of up to eight crossings observed by computer simulation, where 6×1066\times 10^{6} total band moves were performed on each chiral pair. Because the BFACF algorithm may change the length of the polygon, the last column indicates the length range observed in sampled polygons.
Chiral pairs Number observed [min,max\ell_{min},\ell_{max}]
(51,51)(5_{1},5_{1}^{*}) 188 [42,2016][42,2016]
(88,88)(8_{8},8_{8}^{*}) 1 [100,2894][100,2894]
(820,820)(8_{20},8_{20}^{*}) 2677 [68,2370][68,2370]

We found chirally cosmetic bandings to be exceedingly rare. Chirally cosmetic bandings were observed in the numerical experiments for only three knot types. The numbers of bandings relating each of these three knots with its mirror image (or vice versa) is given in Table 2.

The band move for 515_{1} was previously reported in [Zek15] and is shown in Figure 2. Only a single band move was observed for the pair 888_{8} and 888_{8}^{*}. An isotopy of this banding, discovered only by simulation, is shown in Figure 5B (left). A banding for 8208_{20} can more easily be found by hand, as in Figure 5B (right). The banding pictured is a “4-move” in a symmetric union diagram, where a 4-move refers to the replacement of a positive 2-twist with a negative 2-twist. Although 888_{8} is known to admit a symmetric union presentation [Lam19] (see Figure 5A), it is not known to the authors whether a 4-move in such a diagram relates 888_{8} to its mirror. See [IJM18] for a definition of 4-moves.

These observations prompt the following question:

Question 4.9.

Suppose that a pair of knots KK and KK^{\prime} are related by band surgery. What is the likelihood that KK and KK^{\prime} are of different chirality?

When KK is a chiral knot and KK^{\prime} is the mirror of KK, it is clear what we mean by different chirality. In a forthcoming numerical study propose a method to quantify what it means for arbitrary knots to have different chirality. We expand on the preliminary simulations conducted here and report on the chirality trends with respect to band surgery operations along cubic lattice knots.

Numerical methods. In order to identify candidate pairs (K,K)(K,K^{*}) for chirally cosmetic bandings, we systematically performed band surgery operations on all nontrivial prime chiral knots with 8 or fewer crossings. Independent simulations were performed for each member of a chiral pair (K,K)K,K^{*}). Because we excluded fully amphichiral and negative amphichiral knots, a total of 28 knot types were considered. The computer simulations were conducted by adapting software previously developed in our group, the implementation and methods of which are detailed in [SYB+17].

The details of the simulations are as follows. For each knot KK, we used the BFACF algorithm [MS93] to sample the space of lattice embeddings of KK. Here a cubic lattice representative of a knot KK is an embedding of KK contained in the cubic lattice (××)(××)(××)(\mathbb{R}\times\mathbb{Z}\times\mathbb{Z})\cup(\mathbb{Z}\times\mathbb{R}\times\mathbb{Z})\cup(\mathbb{Z}\times\mathbb{Z}\times\mathbb{R}), where the end points of the line segments are contained in the integer lattice 3\mathbb{Z}^{3}. The BFACF algorithm is a dynamic Monte Carlo method that samples the space of cubic lattice polygons of a specific knot type. In each step of the BFACF Markov chain, the algorithm attempts to locally perturb a polygonal chain as pictured in Figure 6, at a randomly chosen location on edges in the polygon. Note that this can change the length of the polygon by 2,0-2,0, or 22. Janse van Rensburg and Whittington showed that the ergodicity classes are the knot types [vRW91], making this a good method for generating large ensembles of lattice embeddings of a specific knot type. The algorithm depends on one adjustable parameter zz. For any given starting knot type KK, fixing zz yields uniform sampling of polygons of type KK and fixed mean length.

Refer to caption
Figure 6. The elementary moves of the BFACF algorithm.

Our implementation is based on the algorithm described in [MS93] and runs in constant time on the number of edges in the polygons. In particular, we use the BFACF algorithm in conjunction with a multiple Markov chain procedure to generate a large, random ensemble of polygonal representatives of each fixed knot type KK. From this much larger ensemble, we uniformly sample a smaller subset of 3×1063\times 10^{6} polygons. Amongst the sample set, we search for candidate banding locations by finding parallel unit edges at distance one, pick one such site at random and perform one non-coherent band surgery operation. Locally, the operation is as illustrated in Figure 1. We identify the knot type of the resulting knot using an implementation of the HOMFLY-PT polynomial [FYH+85, PT87] based on published algorithms [GMGCL99, Jen89]. In cases where the HOMFLY-PT may lead to ambiguous knot identification, we apply KnotFinder [LM20]. The outcome is a directed, weighted graph where the nodes are the knot types and the edges indicate transitions between knot types with corresponding transition probabilities.

It is worth remarking that the sample sets of conformations generated for a knot KK and for its mirror image KK^{*} are not related by mirroring in the cubic lattice, as each set is a uniform random sample of a large set of polygons generated to represent each knot. For example, a non-coherent banding was performed for each of 3×1063\times 10^{6} lattice embeddings of 888_{8} and 3×1063\times 10^{6} lattice embeddings of 888_{8}^{*}. Out of these bandings, only one was a chirally cosmetic banding relating 888_{8}^{*} to 888_{8}. Here, because the experiments were designed to find rare events, the lengths of the polygons was allowed to vary widely, as can be seen in Table 2. The BFACF algorithm guarantees uniform random sampling for each fixed knot type and fixed length. If the length is fixed in the simulations, then when the number of iterations is sufficiently large we expect the behavior of a knot to be equal to that of its mirror image, within a small margin of error. Of course, every time a banding is identified taking KK to KK^{*}, after mirroring there exists a cosmetic banding relating KK^{*} to KK. However, for the reasons stated above, the number of transitions observed in simulation for a knot and its mirror are not identical.

Acknowledgements

Many of the ideas in the article originated in discussions with Tye Lidman, who we thank for his willingness to discuss the mapping cone construction. We thank Cameron Gordon for helpful discussions and Michelle Flanner for preliminary computational data. We are grateful to In Dae Jong and Kazuhiro Ichihara for alerting us to an early error in knot identification pertaining to the skein equivalent knots 888_{8} and 1012910_{129}. AM and MV were partially supported by DMS-1716987. MV was also partially supported by DMS-1817156.

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