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The dimension of Kronheimer-Mrowka instanton homology group for plane trivalent graphs

Zipei Zhuang
Abstract

We proved that the dimension of the 𝔽\mathbb{F}-vector space J#(G)J^{\#}(G) for a plane trivalent graph GG, defined by Kronheimer and Mrowka in [7], is equal to the number of Tait colorings of GG.

1 Introduction

Let GG be a trivalent graph. A 𝐓𝐚𝐢𝐭𝐜𝐨𝐥𝐨𝐫𝐢𝐧𝐠\mathbf{Tait\ coloring} of GG is a function from the edges of GG to a 3-element set of ”colors” {1,2,3} such that edges of three different colors are incident at each vertex. The famous four-color theorem is euqivalent to that every bridgeless planar trivalent graph admits a Tait coloring.

In [7], Kronheimer and Mrowka used their SO(3)SO(3) instanton Floer homology to construct an 𝔽\mathbb{F}-vector space J#(G)J^{\#}(G) (𝔽\mathbb{F} is the field of 2 elements) for each trivalent graph in 3\mathbb{R}^{3}. They conjectured that when GG is planar, the dimension of J#(G)J^{\#}(G) is equal to the number T(G)T(G) of Tait colorings of GG. If it were true, the non-vanishing theorem they proved ([7] Theorem 1.1) which says that J#(G)J^{\#}(G) is zero if and only if GG has an embedded bridge, would provide an alternative proof of the four-color theorem.

J#(G)J^{\#}(G) is a indeed a functor, from the category of webs and foams to the category of 𝔽\mathbb{F}-vector space, satisfying a series of local properties analogous to Khovanov’s sl3sl_{3} homology H3H_{3} for MOY graphs[3]. Indeed, they also proposed a combinatorial counterpart JbJ^{b} to J#J^{\#} for plane trivalent graphs by imitating the construction of sl3sl_{3} homology, whose well-definedness is proved in [5].

Khovanov used the invariant H3H_{3} to construct a homology theory for knots. More specifically, given a knot diagram DD, he resolutes each crossing point in two ways and get 2n2^{n} MOY graphs, where nn is the number of crossings in DD. The sl3sl_{3} homology groups of these 2n2^{n} graphs are organized into a complex C3(D)C_{3}(D). Using the local relations of H3H_{3} on foams he proved that the chain homotopy type of C3(D)C_{3}(D) is independent of the choice of DD, i.e., invariant under the Reidemeister moves. In particular, the homology and the Euler characteristic of the complex are invariants of the knot. The construction of C3(D)C_{3}(D) can be explained by the picture:

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Figure 1: Local relation of the complex of Khovanov’s sl3sl_{3} knot homology

This construction motivates us to prove the conjecture via Penrose’s approach to the number of Tait colorings([10], see also [2]). The Penrose number, which is defined for plane trivalent graphs “with crossings”, can be defined through a “skein relation”(see 2), and is equal to the number of Tait colorings when the graph has no crossings.

From now on we use JJ to denote the J#J^{\#} in [7], suggesting that our methods also works for JbJ^{b} in that paper.

Theorem 1.

Let GG be a plane trivalent graph , then the dimension of J(G)J(G) is equal to the number of Tait colorings of GG.

Our strategy to prove Theorem 1 is to generalize the definition of JJ to any plane trivalent graph with crossings, just as Khovanov’s definition of knot homology group from the sl3sl_{3} homology of MOY graphs, and to prove that the Euler characteristic of JJ satisfies the relation of Penrose number in Prop. 2.

In Section 2 we review the concept of plane trivalent graphs with crossings, and the basic properties of Penrose number. In Section 3 we review the local relations of JJ proved in [7], which is needed in Section 4 when proving the chain homotopy invariance. Then in Section 4 we generalize JJ to any plane trivalent graphs with crossings, for which the well-definedness follows from a similar argument for proving that Khovanov’s sl3sl_{3} knot homology is well-defined.

2 The Penrose number

In this paper a web is a plane trivalent graph. We need a more general concept.

Let GG be a trivalent graph. We can draw GG on the plane, with a finite number of crossing points. We call such a drawing a virtual web, with underlying graph GG. Two virtual webs are equivalent if they are related by a sequence of plane isotopies and virtual Reidemeister moves as in Fig 2 .

An immediate observation is:

Lemma 1.

If a virtual web has no vertices, then it is (equivalent to) a collection of circles.

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virtual RV I
virtual RV II
virtual RV III
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Figure 2: Virtual Reidemeister moves

From now on when we say a virtual web, we mean an equivalence class of virtual webs. See Fig 3 for 3 different virtual webs for the θ\theta-graph. Note that the cyclic order of three edges at each vertex is an invariant of a virtual web.

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Figure 3: Three virtual webs with underlying graph θ\theta

Let GG be a trivalent graph, and DD is a virtual web for GG. Denote by T(G)T(G) the set of Tait colorings of GG. Suppose fT(G)f\in T(G). A vertex vv of DD is said to be positive with respect to ff if the colors incident to vv are 1,2,3 in the clockwise order, otherwise it is negative. Let n+(f),n(f)n^{+}(f),n^{-}(f) be the number of positive and negative vertices of DD with respect to ff. Define

sD(f)={1 if n+(f)n(f) mod 41 otherwises_{D}(f)=\begin{cases}1\text{ \quad if }n^{+}(f)\equiv n^{-}(f)\text{ mod 4}\\ -1\text{ \quad otherwise}\end{cases} (1)

The Penrose number P(D)P(D) of DD is defined to be the sum of sD(f)s_{D}(f) over all Tait colorings ff of GG. It is obviously invariant under the virtual Reidemeister moves.

Proposition 1.

([2], Propersition 1) Let DD be a web with underlying graph GG, then T(G)=P(D)T(G)=P(D).

Proposition 2.

([2], Propersition 2) Let D,D,D′′D,D^{\prime},D^{\prime\prime} be three virtual webs which differ only within a small circle as in Fig 4 . Then P(D)=P(D)P(D′′)P(D)=P(D^{\prime})-P(D^{\prime\prime}).

Obviously this relation together with the fact that P(Un)=3nP(U_{n})=3^{n} where UnU_{n} is the n-component unlink, uniquely characterize PP.

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Figure 4: Local relation of Penrose number

3 Local relations of the functor JJ

A closed pre-foam FF is a compact 2-dimensional CW-complex such that each point has an open neighborhood that is either an open disk, the product of a tripod and an open interval, or the cone over the 1-skeleton of a tetrahedron. The subspace s(F)s(F) of points of tha last two kinds is a four-valent graph. Closed prefoams can be decorated by finite number of points(called dots) on their facets. These dots can float on facets but cannot cross s(F)s(F).

A closed foam FF is a closed pre-foam together with a piece-wise linear embedding into 4\mathbb{R}^{4}. A 3-dimensional space T34T\cong\mathbb{R}^{3}\subset\mathbb{R}^{4} intersects a closed foam FF generically if FTF\cap T is a trivalent graph GG in TT, and for a tubular neighborhoood NN of TT, (NF,N)(N\cap F,N) is piecewise-linearly homeomorphic to (G×(ϵ,ϵ),3×(ϵ,ϵ))(G\times(-\epsilon,\epsilon),\mathbb{R}^{3}\times(-\epsilon,\epsilon)).

A foam(with boundary) is the intersection of a closed foam FF with 3×[0,1]\mathbb{R}^{3}\times[0,1] in 4\mathbb{R}^{4} such that FF generically intersects 3×{0}\mathbb{R}^{3}\times\{0\} and 3×{1}\mathbb{R}^{3}\times\{1\}. We can view a foam FF as a cobordism from 0F=F3×{0}\partial_{0}F=F\cap\mathbb{R}^{3}\times\{0\} to 1F=F3×{1}\partial_{1}F=F\cap\mathbb{R}^{3}\times\{1\}. In particular, a closed foam is a foam withoout boundary and is a cobordism from the empty graph to itself.

If F,GF,G are 2 foams such that the webs 0F,1G\partial_{0}F,\partial_{1}G are identical, define the composition GFGF by concatenating along their common boundary. In this way we obtain a category FoamsFoams, with webs as objects and isomorphism classes of foams with boundary as morphisms.

In [7], Kronheimer and Mrowka defined a functor

J#:FoamsVect𝔽J^{\#}:Foams\longrightarrow Vect_{\mathbb{F}} (2)

where Vect𝔽Vect_{\mathbb{F}} is the category of vector spaces over the 2-elements field 𝔽\mathbb{F}. We list the properties of J#J^{\#} we need afterwards.

Proposition 3.

For the empty graph \emptyset, J()=𝔽J(\emptyset)=\mathbb{F}.

If FF is a closed foam, then J(F):𝔽𝔽J(F):\mathbb{F}\longrightarrow\mathbb{F} is characterized by the image of 1𝔽J()1\in\mathbb{F}\cong J(\emptyset). Still denote this scalar by J(F)J(F).

Proposition 4.

([7], Prop. 5.1) For a circle UU, J()=𝔽3J(\emptyset)=\mathbb{F}^{3}.

Proposition 5.

([7], Prop. 5.2) If a foam FF has 3 or more dots on one of its facets, then J(F)=0.J(F)=0.

Proposition 6.

([7], Corollary 4.4) If W=W1W2W=W_{1}\sqcup W_{2} is a disjoint unnion of 2 webs, then J(W)=J(W1)J(W2).J(W)=J(W_{1})\otimes J(W_{2}).

Corollary 1.

If WW is a disjoint union of kk circles, then J(F)=𝔽3kJ(F)=\mathbb{F}^{3k}.

Proposition 7.

([7], Prop 5.3, Prop 6.2) If FF is an unknotted closed 2-manifold, then

J(F)={1F is the sphere with 2 dots, or the torus without dots0 otherwiseJ(F)=\left\{\begin{aligned} 1&\quad F\text{ is the sphere with 2 dots, or the torus without dots}\\ 0&\quad\text{ otherwise}\end{aligned}\right. (3)
Proposition 8.

([7], Prop 6.1) The foam evaluation satisfies the neck-cutting relation

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Figure 5: The neck-cutting relation
Proposition 9.

(Implicited in Proof of Prop 6.5,[7])

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Figure 6: The bigon relation
Proposition 10.

([7], Prop 5.6) For the theta foam with dots θ(k1,k2,k3)\theta(k_{1},k_{2},k_{3}),

J(θ(k1,k2,k3))={1if {k1,k2,k3}={0,1,2}0otherwiseJ(\theta(k_{1},k_{2},k_{3}))=\left\{\begin{aligned} 1&\quad\text{if }\{k_{1},k_{2},k_{3}\}=\{0,1,2\}\\ 0&\quad\text{otherwise}\end{aligned}\right. (4)
Proposition 11.

(Implicited in Proof of Prop 6.8,[7])

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Figure 7: The square relation

Figure The dimension of Kronheimer-Mrowka instanton homology group for plane trivalent graphs The dimension of Kronheimer-Mrowka instanton homology group for plane trivalent graphs illustrates some relations which are corollaries of 5 6 7

4 Generalization to virtual webs

From now on we consider oriented virtual webs, i.e., virtual webs with an orientation on each of its edges. The sole role that the orientations play is to specify the resolutions at the crossings, as stated below. We can resolute each virtual crossing in two ways, see Fig 8. If we resolute every crossing, we get a web(ignore the orientations), and we call it a complete resolution of the virtual web.

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Figure 8: Resolute a crossing of a virtual web

Let II be the set of crossings of a virtual web DD. To DD we associate an |I||I|-dimensional cube of 𝔽\mathbb{F}-vector spaces. Vertices of the cube are in a bijection with subsets of II. To JIJ\subset I we associate the complete resolution DJD_{J} of DD according to JJ: a crossing pIp\in I gets 1-resolution if and only if pJp\in J.

In the vertex JJ we place the graded 𝔽\mathbb{F} -vector space J(DJ)J(D_{J}), and to an inclusion JJ{b}J\subset J\cup\{b\}, where bI\Jb\in I\backslash J, we assign the homomorphism

J(DJ)J(DJ{b})J(D_{J})\longrightarrow J(D_{J\cup\{b\}}) (5)

induced by the basic cobordism in Fig 9.

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Figure 9: The basic cobordism

Since we work in 𝔽\mathbb{F} each square in the cube commute, and we can define the total complex F(D)F(D). More precisely. let F(D)i=|J|=iJ(DJ)F(D)_{i}=\bigoplus_{|J|=i}J(D_{J}), and the differential di:F(D)iF(D)i+1d^{i}:F(D)_{i}\longrightarrow F(D)_{i+1} is induced by the edge homomorphisms defined above. Fig 10 explains our construction of F(D)F(D).

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Figure 10: virtual Reidemeister move I
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Theorem 2.

The homotopy type of F(D)F(D) is an invariant of DD, i.e. it is invariant under the virtual Reidemeister moves.

Proof.

The argument is similar to the proof of invariance of Khovanov’ sl3sl_{3} homology under Reidemeister moves, since all the local relations used there have their counterparts in our theory(Section 3). For example, to prove the invariance under virtual Reidemeister moves I(Fig.10), we borrow the diagram from [9], Figure 7, and define the chain maps f,gf,g, the chain homotopy hh as illustrated in the graph. The statement there carries verbatim to show that f,gf,g are chain homotopy equivalences to each other.

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Figure 11: Chain homotopy equivalance under Virtual Reidemeister move I

An immediate corollary is

Corollary 2.

The Euler characteristic e(D)e(D) of F(D)F(D) is an invariant of DD.

Proof of Theorem 1

Let DD be an oriented virtual web. We proved that the Euler characteristic of F(D)F(D) is equal to the Penrose number of DD. In particular, when DD has no crossings, the dimension of J(D)J(D) is equal to the number of Tait colorings of DD by Prop 1.

If DD has no vertices, then it is a union of k circles(Lemma 1). By Corollary 1 2, e(D)=e(Uk)=dimJ(Uk)=3k=P(D)e(D)=e(U^{k})=dimJ(U^{k})=3^{k}=P(D) , where UkU^{k} is a disjoint union of k circles. Furthermore, from the definition of F(D)F(D), we have that e(D)e(D) satisfies the local relation in Prop. 2. This identifies e(D)e(D) with P(D)P(D). In particular, when DD is a web, dimJ(D)=e(D)=P(D)=T(D)dimJ(D)=e(D)=P(D)=T(D), by Prop 1.

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