ScalingStacks

5.1 Left-twisted curl

Let DD be a plane diagram with n−1n-1 double points and let D1D_{1} be a diagram constructed from DD by adding a left-twisted curl. Denote by ℐ′\mathcal{I}^{\prime} the set of double points of D1,D_{1}, by aa the double point in the curl and by ℐ\mathcal{I} the set of double points of D.D. There is a natural bijection of sets ℐ→ℐ′∖{a},\mathcal{I}\to\mathcal{I}^{\prime}\setminus\{a\}, coming from identifying a double point of DD with the corresponding double point of D1.D_{1}. We will use this bijection to identify the two sets ℐ\mathcal{I} and ℐ′∖{a}.\mathcal{I}^{\prime}\setminus\{a\}.

The crossing aa of D1D_{1} can be resolved in two ways. The 0-resolution of aa is a diagram D2D_{2} which is a disjoint union of DD and a circle. The 1-resolution is a diagram isotopic to DD and we will identify this diagram with D.D.

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In this section we will define a quasi-isomorphism of the complexes C⁡(D)C(D) and C⁡(D1).C(D_{1}). This quasi-isomorphism arises from a splitting of the ℐ′\mathcal{I}^{\prime}-cube VD1V_{D_{1}} as a direct sum of two cubes, VD1=V′⊕V′′.V_{D_{1}}=V^{\prime}\oplus V^{\prime\prime}. This splitting will induce a decomposition of the complex C⁡(D1)C(D_{1}) into a direct sum of an acyclic complex and a complex isomorphic to C⁡(D).C(D).

Recall that VD,VD1V_{D},V_{D_{1}} and VD2V_{D_{2}} are the cubes associated with the diagrams D,D1D,D_{1} and D2D_{2} respectively. VD1V_{D_{1}} has index set ℐ′,\mathcal{I}^{\prime}, while VDV_{D} and VD2V_{D_{2}} are ℐ\mathcal{I}-cubes.

From the decomposition of D2D_{2} as a union of DD and a simple circle we get a canonical isomorphism of cubes

VD2=VD⊗AV_{D_{2}}=V_{D}\otimes A (65)

where VD⊗AV_{D}\otimes A is the ℐ\mathcal{I}-cube obtained from VDV_{D} by tensoring graded RR-modules VD​(ℒ),ℒ⊂ℐV_{D}(\mathcal{L}),\mathcal{L}\subset\mathcal{I} with AA and tensoring the structure maps ξaVD​(ℒ)\xi^{V_{D}}_{a}(\mathcal{L}) with the identity map of AA.

Let U⊂ℝ2U\subset\mathbb{R}^{2} be a small neighborhood of aa that contains the curl:

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The picture above depicts how the diagram D1D_{1} looks inside U.U. The boundary of UU is shown by a dashed circular line. Intersections of UU with diagrams DD and D2D_{2} are depicted below

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Outside of UU diagrams D,D1D,D_{1} and D2D_{2} coincide. It is explained in Section 4.3 how surfaces in U×[0,1]U\times[0,1], satisfying certain conditions, give rise to cube maps. Using this construction we now define three cube maps between cubes VDV_{D} and VD2:V_{D_{2}}:

ma:\displaystyle m_{a}: VD2⟶VD\displaystyle V_{D_{2}}\longrightarrow V_{D} (66)
Δa:\displaystyle\Delta_{a}: VD⟶VD2\displaystyle V_{D}\longrightarrow V_{D_{2}} (67)
ιa:\displaystyle\iota_{a}: VD⟶VD2\displaystyle V_{D}\longrightarrow V_{D_{2}} (68)

The map mam_{a} is associated to the following surface:

[Uncaptioned image]

Here and further on we depict surfaces embedded in U×[0,1]U\times[0,1] by a sequence of their cross-sections U×{t},t∈[0,1],U\times\{t\},t\in[0,1], the leftmost one being the intersection of the surface with U×{0}U\times\{0\}, the rightmost being the intersection with U×{1}.U\times\{1\}. For such a surface S∈U×[0,1]S\in U\times[0,1] we will call the projection S→[0,1]S\to[0,1] the height function of SS. These surfaces will have only nondegenerate critical points relative to the height function. We depict enough sections of SS to make it obvious what surface we are considering, sometimes adding extra information, i.e., that the above surface has one saddle point and no other critical points relative to the height function.

The intersections S∩U×{0},S∩U×{1}S\cap U\times\{0\},S\cap U\times\{1\} of the surface SS depicted above with the boundary disks U×{0},U×{1}U\times\{0\},U\times\{1\} are isomorphic to the intersections D2∩(U×{0})D_{2}\cap(U\times\{0\}), respectively D∩(U×{1}).D\cap(U\times\{1\}). Thus, SS defines a map mam_{a} from the cube VD2V_{D_{2}} to VD.V_{D}.

The cube map Δa\Delta_{a} is associated to the surface

[Uncaptioned image]

This surface has one saddle point and no other critical points relative to the height function.

ιa\iota_{a} is associated to

[Uncaptioned image]

The only critical point of the height function is a local minimum.

The cube maps ma,Δa,ιam_{a},\Delta_{a},\iota_{a} are graded maps and change the grading by −1,−1,1-1,-1,1 respectively. So let’s keep in mind that ma,Δa,ιam_{a},\Delta_{a},\iota_{a} become grading-preserving if we appropriately shift gradings of our cubes, for example,

ma:\displaystyle m_{a}: VD2⟶VD​{−1}\displaystyle V_{D_{2}}\longrightarrow V_{D}\{-1\} (69)
Δa:\displaystyle\Delta_{a}: VD⟶VD2​{−1}\displaystyle V_{D}\longrightarrow V_{D_{2}}\{-1\} (70)
ιa:\displaystyle\iota_{a}: VD⟶VD2​{1}\displaystyle V_{D}\longrightarrow V_{D_{2}}\{1\} (71)

are grading-preserving maps of cubes over R​-mod0.R{\mbox{-mod}_{0}}.

The composition ma​ιam_{a}\iota_{a} is equal to the identity map from VDV_{D} to itself. Denote by ȷa\jmath_{a} the map

ȷa=defΔa−ιa​ma​Δa:VD⟶VD2\jmath_{a}\stackrel{{\scriptstyle\mbox{\scriptsize def}}}{{=}}\Delta_{a}-\iota_{a}m_{a}\Delta_{a}:V_{D}\longrightarrow V_{D_{2}} (72)

The map ȷa\jmath_{a} is a graded map of degree −1.-1.

0PLA

Proposition 11 The ℐ\mathcal{I}-cube VD2V_{D_{2}} splits as a direct sum:

VD2=ιa​(VD)⊕ȷa​(VD).V_{D_{2}}=\iota_{a}(V_{D})\oplus\jmath_{a}(V_{D}). (73)

Proof: It is enough to consider the case when DD is a single circle. Then ℐ′={a},ℐ=∅,VD=A\mathcal{I}^{\prime}=\{a\},\mathcal{I}=\emptyset,V_{D}=A and ιa​(VD)=𝟏⊗A.\iota_{a}(V_{D})=\mathbf{1}\otimes A. But

ȷa​𝟏=\displaystyle\jmath_{a}\mathbf{1}= (Δa−ιa​ma​Δa)​𝟏=X⊗𝟏−𝟏⊗X+c​X⊗X\displaystyle(\Delta_{a}-\iota_{a}m_{a}\Delta_{a})\mathbf{1}=X\otimes\mathbf{1}-\mathbf{1}\otimes X+cX\otimes X
ȷa​X=\displaystyle\jmath_{a}X= (Δa−ιa​ma​Δa)​X=X⊗X\displaystyle(\Delta_{a}-\iota_{a}m_{a}\Delta_{a})X=X\otimes X

and, thus, A⊗AA\otimes A is a direct sum of 𝟏⊗A\mathbf{1}\otimes A and the RR-submodule spanned by ȷa​𝟏\jmath_{a}\mathbf{1} and ȷa​X.\jmath_{a}X.

□\square

Note that

ma​ȷa=ma​(Δa−ιa​ma​Δa)=0m_{a}\jmath_{a}=m_{a}(\Delta_{a}-\iota_{a}m_{a}\Delta_{a})=0 (74)

because ma​ιa=I​d.m_{a}\iota_{a}=Id.

The ℐ′\mathcal{I}^{\prime}-cube VD1V_{D_{1}} contains VDV_{D} and VD2V_{D_{2}} as subcubes of codimension 1.1. Namely, we have canonical isomorphisms

VD1(∗0)\displaystyle V_{D_{1}}(\ast 0) ≅\displaystyle\cong VD2\displaystyle V_{D_{2}} (75)
VD1(∗1)\displaystyle V_{D_{1}}(\ast 1) ≅\displaystyle\cong VD​{−1}\displaystyle V_{D}\{-1\} (76)

Recall from Section 3.2 that VD1(∗0)V_{D_{1}}(\ast 0) denotes the ℐ′∖{a}\mathcal{I}^{\prime}\setminus\{a\}-cube (i.e. ℐ\mathcal{I}-cube) with VD1(∗0)(ℒ)=VD1(ℒ)V_{D_{1}}(\ast 0)(\mathcal{L})=V_{D_{1}}(\mathcal{L}) for ℒ⊂ℐ,\mathcal{L}\subset\mathcal{I}, etc.

Under these isomorphisms the structure map ξaVD1\xi_{a}^{V_{D_{1}}} (denoted below by ξa\xi_{a}) for the ℐ′\mathcal{I}^{\prime}-cube VD1V_{D_{1}}

ξa:VD1(∗0)⟶VD1(∗1)\xi_{a}:V_{D_{1}}(\ast 0)\longrightarrow V_{D_{1}}(\ast 1) (77)

is equal to the map mam_{a} of ℐ\mathcal{I}-cubes, i.e., the following diagram is commutative

VD1(∗0)→ξaVD1(∗1)↓≅↓≅VD2→maVD​{−1}\begin{CD}V_{D_{1}}(\ast 0)@>{\xi_{a}}>{}>V_{D_{1}}(\ast 1)\\ @V{}V{\cong}V@V{}V{\cong}V\\ V_{D_{2}}@>{m_{a}}>{}>V_{D}\{-1\}\end{CD}

Using the splitting (73) of VD2V_{D_{2}} we can decompose the ℐ′\mathcal{I}^{\prime}-cube VD1V_{D_{1}} as a direct sum of two ℐ′\mathcal{I}^{\prime}-cubes as follows:

VD1=V′⊕V′′V_{D_{1}}=V^{\prime}\oplus V^{\prime\prime} (78)

where

V′(∗0)\displaystyle V^{\prime}(\ast 0) =\displaystyle= ȷa​(VD)\displaystyle\jmath_{a}(V_{D}) (79)
V′(∗1)\displaystyle V^{\prime}(\ast 1) =\displaystyle= 0\displaystyle 0 (80)
V′′(∗0)\displaystyle V^{\prime\prime}(\ast 0) =\displaystyle= ιa​(VD)\displaystyle\iota_{a}(V_{D}) (81)
V′′(∗1)\displaystyle V^{\prime\prime}(\ast 1) =\displaystyle= VD1(∗1)\displaystyle V_{D_{1}}(\ast 1) (82)

Some explanation: in the formula (79) ȷa​(VD)\jmath_{a}(V_{D}) is a subcube of VD2V_{D_{2}} and, due to (75), ȷa​(VD)\jmath_{a}(V_{D}) sits inside VD1V_{D_{1}} as a subcube of codimension 1. Equation (80) means that V′(∗1)(ℒ)=0V^{\prime}(\ast 1)(\mathcal{L})=0 for all ℒ⊂ℐ′.\mathcal{L}\subset\mathcal{I}^{\prime}. Thus, V′​(ℒ)=ȷa​(VD​(ℒ))⊂VD1​(ℒ)V^{\prime}(\mathcal{L})=\jmath_{a}(V_{D}(\mathcal{L}))\subset V_{D_{1}}(\mathcal{L}) for ℒ⊂ℐ′,\mathcal{L}\subset\mathcal{I}^{\prime}, if ℒ\mathcal{L} does not contain a.a. If ℒ\mathcal{L} contains a,a, V′​(ℒ)=0.V^{\prime}(\mathcal{L})=0.

Tensoring (78) with Eℐ′E_{\mathcal{I}^{\prime}} we get a splitting of skew-commutative ℐ′\mathcal{I}^{\prime}-cubes

VD1⊗Eℐ′=(V′⊗Eℐ′)⊕(V′′⊗Eℐ′)V_{D_{1}}\otimes E_{\mathcal{I}^{\prime}}=(V^{\prime}\otimes E_{\mathcal{I}^{\prime}})\oplus(V^{\prime\prime}\otimes E_{\mathcal{I}^{\prime}}) (83)

This induces a splitting of complexes associated to these skew-commutative ℐ′\mathcal{I}^{\prime}-cubes

C¯​(VD1⊗Eℐ′)=C¯​(V′⊗Eℐ′)⊕C¯​(V′′⊗Eℐ′)\overline{C}(V_{D_{1}}\otimes E_{\mathcal{I}^{\prime}})=\overline{C}(V^{\prime}\otimes E_{\mathcal{I}^{\prime}})\oplus\overline{C}(V^{\prime\prime}\otimes E_{\mathcal{I}^{\prime}}) (84)
0PLB

Proposition 12 The complex C¯​(V′′⊗Eℐ′)\overline{C}(V^{\prime\prime}\otimes E_{\mathcal{I}^{\prime}}) is acyclic.

Proof: The complex C¯​(V′′⊗Eℐ′)\overline{C}(V^{\prime\prime}\otimes E_{\mathcal{I}^{\prime}}) is isomorphic to the cone of the identity map of the complex C¯​(VD⊗Eℐ)​[−1]​{−1}.\overline{C}(V_{D}\otimes E_{\mathcal{I}})[-1]\{-1\}.

□\square

0PLC

Proposition 13 The complexes C¯​(V′⊗Eℐ′)\overline{C}(V^{\prime}\otimes E_{\mathcal{I}^{\prime}}) and C¯​(VD⊗Eℐ)​{1}\overline{C}(V_{D}\otimes E_{\mathcal{I}})\{1\} are isomorphic.

Proof: We have a chain of isomorphisms of complexes

C¯​(V′⊗Eℐ′)\displaystyle\overline{C}(V^{\prime}\otimes E_{\mathcal{I}^{\prime}}) =\displaystyle= C¯(V′(∗0)⊗Eℐ)\displaystyle\overline{C}(V^{\prime}(\ast 0)\otimes E_{\mathcal{I}})
=\displaystyle= C¯​(VD​{1}⊗Eℐ)\displaystyle\overline{C}(V_{D}\{1\}\otimes E_{\mathcal{I}})
=\displaystyle= C¯​(VD⊗Eℐ)​{1}\displaystyle\overline{C}(V_{D}\otimes E_{\mathcal{I}})\{1\}
0PLD

Corollary 3 The complexes C¯​(D1)\overline{C}(D_{1}) and C¯​(D)​{1}\overline{C}(D)\{1\} are quasiisomorphic.

Proof: We have

C¯​(D1)\displaystyle\overline{C}(D_{1}) =\displaystyle= C¯​(VD1⊗Eℐ′)\displaystyle\overline{C}(V_{D_{1}}\otimes E_{\mathcal{I}^{\prime}})
=\displaystyle= C¯​(V′⊗Eℐ′)⊕C¯​(V′′⊗Eℐ′)\displaystyle\overline{C}(V^{\prime}\otimes E_{\mathcal{I}^{\prime}})\oplus\overline{C}(V^{\prime\prime}\otimes E_{\mathcal{I}^{\prime}})
=\displaystyle= C¯​(VD⊗Eℐ)​{1}⊕C¯​(V′′⊗Eℐ′)\displaystyle\overline{C}(V_{D}\otimes E_{\mathcal{I}})\{1\}\oplus\overline{C}(V^{\prime\prime}\otimes E_{\mathcal{I}^{\prime}})
=\displaystyle= C¯​(D)​{1}⊕(Acyclic complex)\displaystyle\overline{C}(D)\{1\}\oplus(\mbox{Acyclic complex})

□\square

Note that x⁡(D1)=x⁡(D)x(D_{1})=x(D) and y⁡(D1)=y⁡(D)+1.y(D_{1})=y(D)+1. By (45)

C⁡(D)=C¯​(D)​[x⁡(D)]​{2​x​(D)−y⁡(D)}C(D)=\overline{C}(D)[x(D)]\{2x(D)-y(D)\} (85)

and

C⁡(D1)\displaystyle C(D_{1}) =\displaystyle= C¯​(D1)​[x⁡(D1)]​{2​x​(D1)−y⁡(D1)}\displaystyle\overline{C}(D_{1})[x(D_{1})]\{2x(D_{1})-y(D_{1})\}
=\displaystyle= C¯​(D1)​[x⁡(D)]​{2​x​(D)−y⁡(D)−1}.\displaystyle\overline{C}(D_{1})[x(D)]\{2x(D)-y(D)-1\}.

Therefore, complexes C⁡(D)C(D) and C⁡(D1)C(D_{1}) are quasiisomorphic. Q.E.D.

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

Mikhail Khovanov

Original source: arXiv:math/9908171v2