1 Introduction
In recent years, torsion invariants for knots arising from Khovanov homology appeared in many contexts. For example, they give rise to lower bounds for unknotting numbers and Gordian distance [Reference AlishahiAli19, Reference Alishahi and DowlinAD19, Reference Lewark, Marino and ZibrowiusLMZ24], rational unknotting numbers [Reference Iltgen, Lewark and MarinoILM21], band unknotting numbers [Reference ZhuangZhu22], ribbon distance [Reference SarkarSar20, Reference GujralGuj20], and Turaev genus [Reference Caprau, González, Lee, Lowrance, Sazdanović and ZhangCGL+21].
They are defined from deformations of Khovanov homology over a polynomial ring with coefficients in a field
$\mathbb {F}$
, using the maximal torsion order of the homology viewed as a module over the polynomial ring. These deformations come with spectral sequences that start with the Khovanov homology of the knot and converge to the (shifted) Khovanov homology of the unknot. There is a close relation between the torsion order and the number of pages of the spectral sequence. The odd one out here is the X-torsion order
$\operatorname {\mathrm {xo}}_{\mathbb {F}}(K)$
, which only satisfies
$\operatorname {\mathrm {xo}}_{\mathbb {F}}(K)\in \{2k-3, 2k-2\}$
with k the number of pages in the Lee spectral sequence (we assume that the
$E_1$
-page is the Khovanov homology, and
$E_k$
the first page equal to
$E_\infty $
). By using the X-action on the Lee complex, one can get a spectral sequence where this is more precise, but our main theorem states that we can also use the reduced Bar-Natan–Lee–Turner spectral sequence.
Theorem 1.1 Let K be a knot and
$\mathbb {F}$
a field of characteristic different from
$2$
. Then
where
${\widetilde {\mathrm{pg}}}_{\mathbb {F}}(K)$
is the number of pages in the reduced Bar-Natan–Lee–Turner spectral sequence of K with coefficients in
$\mathbb {F}$
.
2 Lee and Bar-Natan homology
A (commutative) Frobenius system is a tuple
$\mathcal {F}=(R,A,\varepsilon , \Delta )$
with A a commutative ring and a subring R,
$\varepsilon \colon A\to R$
an R-module map,
$\Delta \colon A\to A\otimes _R A$
an A-bimodule map that is co-associative and co-commutative, such that
$(\varepsilon \otimes \operatorname {\mathrm {id}})\circ \Delta = \operatorname {\mathrm {id}}$
.
Given a Frobenius system
$\mathcal {F}= (R,A,\varepsilon ,\Delta )$
such that A is free of rank
$2$
over R, Khovanov [Reference KhovanovKho06] showed that for a link diagram D one can define a cochain complex
$C(D;\mathcal {F})$
over R whose homology is a link invariant.
The original example of Khovanov homology is obtained by choosing
$R=\mathbb {Z}$
,
$A=Z[X]/(X^2)$
,
$\varepsilon (1) = 0$
and
$\varepsilon (X) = 1$
, and
$\Delta $
is given by
$\Delta (1) = 1\otimes X + X\otimes 1$
. With
$\Delta (X) = X\otimes X$
one has indeed that
$\Delta $
is an A-bimodule map.
We will be mainly interested in two deformations of this system, which we name after Lee and Bar-Natan.
2.1 Lee homology
The Lee deformation of Khovanov homology can be described as follows. For the ground ring we use
$R[T]$
, and
$A = R[X,T]/(X^2-T)$
. Both rings are graded by declaring
$\deg (1) = 0$
,
$\deg (T) = -4$
and
$\deg (X) = -2$
. The Frobenius system is given by
and co-unit
$\varepsilon \colon A \to R[T]$
given by
$\varepsilon (1) = 0$
,
$\varepsilon (X) = 1$
. Note that since tensor products are over
$R[T]$
,
$T\otimes 1 = 1\otimes T$
.
We denote this Frobenius system by
$\mathcal {F}_{\operatorname {\mathrm {Lee}}}$
and the resulting link homology chain complex for a link diagram D by
$C_{\operatorname {\mathrm {Lee}}}(D;R[T])$
. Using creative grading shifts, one can ensure that this complex is bigraded, that is, it has a grading different from the homological grading, called the q-grading, which is preserved by the boundary.
As an
$R[T]$
-module, A is free of rank
$2$
, with a basis given by
$\{1,X\}$
. Since
$T= X^2$
in A, we have
$A\cong R[X]$
. By choosing a base point on D, we can turn
$C_{\operatorname {\mathrm {Lee}}}(D;R[T])$
into an
$R[X]$
-chain complex.
If
$R=\mathbb {F}$
is a field, then
$\mathbb {F}[X]$
is a Euclidean domain, and therefore
where I is a finite set,
$D_i$
is either a single copy of
$\mathbb {F}[X]$
, or
$D_i$
is concentrated in two adjacent homological degrees, and is of the form
where
$k_i$
is a non-negative integer. This follows from the usual Smith-Normalization process, noting that we can keep this grading-preserving at every step. Also, we allow
$k_i = 0$
, so that we get an isomorphism of
$\mathbb {F}[X]$
complexes in (1). As
$T=X^2$
, we can also view this as an isomorphism of
$\mathbb {F}[T]$
complexes.
Note that the free part for a knot is just one copy, see Turner [Reference TurnerTur20]. More generally, if L is a c-component link and
$\mathbb {F}$
a field of characteristic different from
$2$
, the homology of
$C_{\operatorname {\mathrm {Lee}}}(D;\mathbb {F}[T])$
decomposes into
$\mathbb {F}[X]^{2^{c-1}}\oplus T(L)$
, where
Definition 2.1 Let L be a link with basepoint and
$\mathbb {F}$
a field of characteristic different from
$2$
. The X-torsion order of L, denoted
$\operatorname {\mathrm {xo}}_{\mathbb {F}}(L)$
, is defined as the minimal n such that
$X^nT(L) = 0$
.
Notice that
$\operatorname {\mathrm {xo}}_{\mathbb {F}}(L)$
is the largest
$k_i$
that appears in the decomposition (1).
Remark 2.2 For a knot the basepoint does not affect
$\operatorname {\mathrm {xo}}_{\mathbb {F}}(L)$
, but for a link it can make a difference. The easiest way to see this is to consider a split link with an unknot component.
Lee [Reference LeeLee05] originally worked over
$\mathbb {Q}$
. To get the cochain complex from [Reference LeeLee05], we only need to use the change of base ring homomorphism
$\eta \colon \mathbb {Q}[T]\to \mathbb {Q}$
sending T to
$1$
.
2.2 Bar-Natan homology
To get the Bar-Natan deformation of Khovanov homology we write the ground ring as
$R[H]$
and use
$B = R[X,H]/(X^2-XH)$
, with co-multiplication given by
and co-unit
$\varepsilon \colon B\to R[H]$
given by
$\varepsilon (1) = 0$
,
$\varepsilon (X) = 1$
.
We write
$\mathcal {F}_{\operatorname {\mathrm {BN}}}$
for this Frobenius system. Again we get gradings on the ground ring and B by setting
$\deg (1) = 0$
,
$\deg (H) = -2 = \deg (X)$
.
For a link diagram D, we denote the resulting chain complex by
$C_{\operatorname {\mathrm {BN}}}(D; R[H])$
and the homology by
$H_{\operatorname {\mathrm {BN}}}(D;R[H])$
. Again this is bigraded.
As in the case of the Lee complex, when viewed as an
$R[H]$
-module, B is free of rank
$2$
with basis given by
$\{1,X\}$
. However, as
$X (X-H) = 0$
in B, we do not get an isomorphism with
$R[X]$
.
The advantage of the Bar-Natan complex is that it behaves better over
$\mathbb {Z}$
, and in particular, over
$\mathbb {F}_2$
, the field with two elements. If
$\mathbb {F}$
is a field of characteristic different from
$2$
, it is also closely related to the Lee complex, as we will see in Section 3.
To explain what we mean by “behaving better” than the Lee complex, consider the following two observations.
-
• If
$\eta \colon \mathbb {Z}[H]\to S$
is a ring homomorphism such that
$\eta (H)$
is a unit, then
$H_{\operatorname {\mathrm {BN}}}(K;S) = H(C_{\operatorname {\mathrm {BN}}}\otimes _{\mathbb {Z}[H]}S)\cong S\oplus S$
, concentrated in homological degree
$0$
. This follows from [Reference Lipshitz and SarkarLS22, Proposition 2.1]. -
• There is a well defined reduced complex
after choosing a basepoint on the link diagram D. With
$$\begin{align*}\widetilde{C}_{\operatorname{\mathrm{BN}}}(D;\mathbb{Z}[H]) = X\cdot C_{\operatorname{\mathrm{BN}}}(D;\mathbb{Z}[H]) \end{align*}$$
$\eta $
as above we get
$\widetilde {H}_{\operatorname {\mathrm {BN}}}(L;S) = H(\widetilde {C}_{\operatorname {\mathrm {BN}}}\otimes _{\mathbb {Z}[H]} S) \cong S^{2^{c-1}}$
for a c-component link L.
3 Proof of the main theorem
In this section,
$\mathbb {F}$
is a field of characteristic different from
$2$
.
Let us introduce a formal variable
$T^{\frac {1}{2}}$
with
$(T^{\frac {1}{2}})^2 = T$
and consider the inclusion
$\mathbb {F}[T]\to \mathbb {F}[T^{\frac {1}{2}}]$
. We get a new Frobenius system
$\overline {\mathcal {F}}_{\operatorname {\mathrm {Lee}}} = \mathcal {F}_{\operatorname {\mathrm {Lee}}}\otimes _{\mathbb {F}[T]}\mathbb {F}[T^{\frac {1}{2}}]$
, that is, the ground ring is
$\mathbb {F}[T^{\frac {1}{2}}]$
, A is given by
$\mathbb {F}[X,T^{\frac {1}{2}}]/(X^2-T)$
, and
$\varepsilon $
and
$\Delta $
are as in
$\mathcal {F}_{\operatorname {\mathrm {Lee}}}$
. The resulting link complex is denoted by
$C_{\operatorname {\mathrm {Lee}}}(D;\mathbb {F}[T^{\frac {1}{2}}]) = C_{\operatorname {\mathrm {Lee}}}(D;\mathbb {F}[T])\otimes _{\mathbb {F}[T]}\mathbb {F}[T^{\frac {1}{2}}]$
.
We can define a ring isomorphism
by sending H to
$T^{\frac {1}{2}}$
and X to
$\frac {1}{2}(X+T^{\frac {1}{2}})$
. Note that this sends
$X-H$
to
$\frac {1}{2}(X-T^{\frac {1}{2}})$
(making it a well defined ring homomorphism) and
$2X-H$
to X.
This does not quite induce an isomorphism of Frobenius systems
$\mathcal {F}_{\operatorname {\mathrm {BN}}}$
to
$\overline {\mathcal {F}}_{\operatorname {\mathrm {Lee}}}$
, but it does if we twist the latter by
$\frac {1}{2}$
, compare [Reference KhovanovKho06]. In particular, it induces a grading preserving isomorphism of
$\mathbb {F}[H]$
-cochain complexes
Here we treat the latter as an
$\mathbb {F}[H]$
-complex using the identification of
$\mathbb {F}[H]$
and
$\mathbb {F}[T^{\frac {1}{2}}]$
by restricting
$\Phi $
to
$\mathbb {F}[H]$
.
Recall the isomorphism (1) and treat it as an isomorphism over
$\mathbb {F}[T]$
. It induces an isomorphism of
$\mathbb {F}[T^{\frac {1}{2}}]$
-cochain complexes
Combining with
$\Phi $
and using that
$\Phi (2X-H) = X$
this shows that
$C_{\operatorname {\mathrm {BN}}}(D;\mathbb {F}[H])$
to a direct summand of complexes
$\overline {D}_i$
, each either being a single free copy
$\mathbb {F}[X,H]/(X^2-XH)$
, or a complex of the form
with
$k_i\geq 0$
. Passing to the reduced complex shows that
$\widetilde {C}_{\operatorname {\mathrm {BN}}}(D;\mathbb {F}[H])$
is isomorphic to a direct sum of free copies of
$\mathbb {F}[H]$
and complexes of the form
From this isomorphism it follows that the spectral sequence starting with the reduced Khovanov homology with coefficients in
$\mathbb {F}$
collapses after k steps, where k is the maximum of the
$k_i$
. Since this maximum is also
$\operatorname {\mathrm {xo}}_{\mathbb {F}}(K)$
, as follows from (1), this proves Theorem 1.1.
Remark 3.1 Viewing the Lee complex
$C_{\operatorname {\mathrm {Lee}}}(D;\mathbb {F}[T])$
of a link with base point as an
$\mathbb {F}[X]$
-complex and using
$\eta \colon \mathbb {F}[X]\to \mathbb {F}$
with
$\eta (X)=1$
, gives rise to a filtered complex
$C_{\operatorname {\mathrm {Lee}}}(D;\mathbb {F}[T])\otimes _{\mathbb {F}[X]}\mathbb {F}$
. Our argument shows that the corresponding spectral sequence agrees with the reduced Bar-Natan–Lee–Turner spectral sequence.
4 Computations
In view of Theorem 1.1, we extend the definition of X-torsion for
$\mathbb {F}_2$
as follows.
Definition 4.1 Let L be a link with a basepoint. We then define
where
${\widetilde {\mathrm{pg}}}_{\mathbb {F}_2}(L)$
is the number of pages in the reduced Bar-Natan–Lee–Turner spectral sequence of K with coefficients in
$\mathbb {F}_2$
.
This agrees with the H-torsion order of [Reference AlishahiAli19].
Computations of
${\widetilde {\mathrm{pg}}}_{\mathbb {F}}(K)$
are readily available, for example, using knotjob, which can be found at the author’s website at
https://www.maths.dur.ac.uk/users/dirk.schuetz/knotjob.html.
For knots with up to
$14$
crossings,
$\operatorname {\mathrm {xo}}_{\mathbb {F}}(K)$
does not depend on
$\mathbb {F}$
. But there are five knots with
$15$
crossings where
$\operatorname {\mathrm {xo}}_{\mathbb {Q}}(K)> \operatorname {\mathrm {xo}}_{\mathbb {F}_2}(K)$
and one
$15$
-crossing knot with
$\operatorname {\mathrm {xo}}_{\mathbb {Q}}(K) < \operatorname {\mathrm {xo}}_{\mathbb {F}_2}(K)$
. There are also
$111$
knots with
$16$
crossings such that
$\operatorname {\mathrm {xo}}_{\mathbb {Q}}(K)\!= \operatorname {\mathrm {xo}}_{\mathbb {F}_2}(K)$
. For all knots with up to 16 crossings we have
$\operatorname {\mathrm {xo}}_{\mathbb {Q}}(K) = \operatorname {\mathrm {xo}}_{\mathbb {F}_3}(K)$
, and no X-torsion order is bigger than
$2$
.
The Manolescu–Marengon knot K, which is a counterexample to the Knight-move conjecture [Reference Manolescu and MarengonMM20], satisfies
$\operatorname {\mathrm {xo}}_{\mathbb {Q}}(K) = 3$
. Interestingly, we get
${\operatorname {\mathrm {xo}}_{\mathbb {F}_2}(K) = \operatorname {\mathrm {xo}}_{\mathbb {F}_3}(K) = 2}$
for this knot. In particular, this knot satisfies the Knight-move conjecture in characteristics
$2$
and
$3$
. There is a slight variation of this knotFootnote
1
,
$K'$
, which uses a full twist on
$8$
strands as opposed to
$6$
strands. Calculations show this knot satisfies
$\operatorname {\mathrm {xo}}_{\mathbb {Q}}(K') = 4$
. The next variation, which would use a full twist on
$10$
strands, is unfortunately outside of the range for calculations.
For torus knots examples with X-torsion order bigger than
$2$
for finite fields are known in the cases
$T(5,6)$
and
$T(7,8)$
, compare [Reference Bar-NatanBN07, Reference Caprau, González, Lee, Lowrance, Sazdanović and ZhangCGL+21]. More can be said about torus knots, but we only want to highlight the case
$T(8,9)$
, where
$\operatorname {\mathrm {xo}}_{\mathbb {Q}}(T(8,9)) =2 < 3 = \operatorname {\mathrm {xo}}_{\mathbb {F}_7}(T(8,9))$
, despite the Betti numbers of Khovanov homology being the same with
$\mathbb {Q}$
and
$\mathbb {F}_7$
coefficients.
Acknowledgements
The author would like to thank Nathan Dunfield for valuable discussions on the X-torsion order.
