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(1)

YOU-CHENG CHOU

0.1. nKdV-hierarchy. We consider the operator

L =

nx+1

+ a

1

( x )

nx1

+ · · · + a

n

( x ) , For any pair

( α, p ) , α = 1, . . . , n, p = 0, 1, . . .

we consider the following system of PDEs for functions a

1

( x, t ) , . . . , a

n

( x, t ) :

tα,p

L = [ L, ( L

nα+1+p

)

+

] ,

where ( L

n+α1+p

)

+

denotes the differential part of the pseudodifferential op- erator L

n+α1+p

.

To construct pseudodifferential operator L

n+α1+p

, it suffice to construct L

n+11

=

x

+ l

1

( x )

x1

+ l

2

( x )

x2

+ · · · ,

where

1

is the inverse operator to ∂ and its commutator with function f ( x ) is as follows:

[

x1

, f ( x )] = f

x

x1

+ f

xx

x2

. . . .

The last rule and equation ( L

n+11

)

n+1

= L allow us to solve l

i

( x ) recursively.

0.2. Constructing Solutions to the KdV Hierarchy from the Sato Grass- manian.

Definition 0.1. A Sato space is an infinite dimensional vector subspace W C (( z )) such that

W =< f

1

, f

2

, · · · >

for some f

j

( z ) = z

j

+ αz

j+1

+ · · · = z

j

( 1 + ◦( 1 )) .

Let T

1

, T

2

, . . . be an infinite sequence of formal variables, and denote by M ( z; T

1

, T

2

, . . . ) the function

M ( z; T

1

, T

2

, . . . ) = e

T1z1+T2z2+...

.

For a Sato space W =< f

1

, f

2

, · · · > , we define the τ-function associated it as the fraction

τ

W

( T

1

, T

2

, . . . ) = ( · · · ∧ M f

3

M f

2

M f

1

) z

0

z

1

z

2

. . .

· · · ∧ z

3

z

2

z

1

z

0

z

1

z

2

. . . .

It depends on the space W itself, and not on the specific choice of the basis f

1

, f

2

, . . . .

1

(2)

Proposition 0.2. Let W be a Sato space such that z

2

W W. Then we have (1) τ

W

( T

1

, T

2

, . . . ) does not depend on T

2i

for i > 0;

(2) the second order differential operators

L =

2x

+ 2∂

2T1

logτ

W

( x + T

1

, T

3

, T

5

, . . . ) satisfyies the KdV hierarchy

T2k+1

L = [ L, ( L

2k2+1

)

+

] .

Proposition 0.3. Let W be a Sato space generated by f

i

= z

i

( 1 + ◦( 1 )) . Then for any N 0,

det ( f

i

( z

j

))

detz

j i

= τ

W

( T

1

( z

) , T

2

( z

) , . . . ) , where T

k

( z

) : =

1k

iN=1

z

ki

.

0.3. Witten’s Conjecture.

Let M

g,n

( M

g,n

) be the moduli space of smooth (nodal) genus g, n-pointed stable curves, L

i

be line bundle on M

g,n

whose fiber at the moduli point ( C; x

1

, . . . , c

n

) is T

xi

C and let ψ

i

: = c

1

( L

i

) .

The intersection number is defined by

< τ

d1

· · · τ

dn

> : =

Mg,n

ψ

d11

· · · ψ

dnn

,

where g =

∑ di+33n

. We consider the formal power series of intersection number

F ( t

0

, t

1

, . . . ) = ∑

n≥0

d1≥0,...,dn0

1

n! < τ

d1

· · · τ

dn

> t

d1

· · · t

dn

.

Theorem 0.4 (Witten’s Conjecture). e

F

is the τ-function for KdV with respect to variables T

2i+1

=

(2i+ti1)!!

Remark 0.5. F ( t

0

, t

1

, . . . ) is completely determined by F ( t

0

, 0, 0, . . . ) =

16

t

30

, KdV-hierarchy, string equation and dilaton equation.

0.4. Combinatorial Model. Let X be a compact Riemann surface and ρ be a meromorphic quadratic differential on X. Locally, ρ = ϕ ( z )( dz )

2

, where ϕ ( z ) is a meromorphic function. In our case, we assume ϕ has only simple or double poles.

We define the horizontal line field as

{ ν TX | ϕ ( z )( dz ( ν ))

2

> 0 } . Its integral curve is called horizontal trajectory.

Remark 0.6. For a generic quadratic differential, a generic horizontal trajec- tory is nonclosed.

Here we define a special kind of quadratic differential:

(3)

Definition 0.7. A Jenkins-Strebel differential is a quadratic differential with only finite nonclosed horizontal trajectory.

By a local analysis, we can see that if z

0

zero of order d of ρ, then there are d + 2 horizontal trajectories issuing from z

0

. If z

0

is a simple pole, then there is a unique horizontal trajectory issuing from z

0

. Finally, if z

0

is a dou- ble pole with negative residue, then z

0

is surrounded by closed horizontal trajectories. We further list some properties of Jenkins-Strebel differential that we will need later.

Proposition 0.8. Let X be a Riemann surface of finite type and ρ ( z ) = ϕ ( z ) dz

2

be a Jenkin-Strebel differential on X. Then

the connected component of X \ {graph of nonclosed horizontal trajectory}

is either open annulus or open disk;

all closed horizontal trajectory in the same connected component have the same length. (We use the metric dl

2

= | ϕ ( z ) || dz |

2

.)

Theorem 0.9. (Strebel) For any 2n + 1-tuples ( X; x

1

, . . . , x

n

; p

1

, . . . , p

n

) , where X is a Riemann surface of finite type, x

i

are distinct points of X, p

i

> 0, and n > χ ( X ) , there exists a unique Jenkins-Strebel differential such that

it has double pole at x

i

and no other poles;

connected components of X \ { graph of nonclosed horizontal trajectory } are open disks;

the length of horizontal trajectory associated to x

i

is p

i

.

We call the unique Jenkins-Strebel differential defined above the canoni- cal Jenkins-Strebel differential.

Conversely, given an embedded graph (a graph in oriented topological surface X) with

each valencies of vertex 3,

face marked by x

1

, . . . , x

n

fixed lengths of its edges,

complement of embedded graph is a disjoint, union of open disks, there exists unique complex structure such that its corresponding canonical Jenkins-Strebel differential determines the given embedded graph.

Now, we define M

combg,n

: = {the moduli space of genus g connected em- bedded graphs with each valencies of vertex 3, n-marked faces, fixed lengths of its edges, and complement being a disjoint union of open disks }.

Theorem 0.10. M

g,n

× R

n+

= M

combg,n

as real orbifolds.

We can further generalize the above discussion to stable curve.

Definition 0.11. For a stable curve C with given perimeter on its marked points,

the canonical Jenkins-Strebel differential on C is a quadratic differential ρ such

that:

(4)

ρ 0 on the unmarked components;

ρ is the canonical Jenkins-Strebel differential on the puntured marked com- ponents.

M

combg,n

: = { the space of stable genus g embedded graphs with vertices of valencies 3 on smooth point, at most one valency on nodal points, n- marked faces, complement being disjoint union of open disks, and fixed length of edges on marked component and no graph on unmarked compo- nents.}

To determine the relation between M

g,n

and M

combg,n

, we introduce the equivalence relation as follows: Let C be a stable curve with genus g and n marked points. We can canonically decompose C as the union of two curves C = C

+

C

0

, where C

+

is the union of all the components of C containing marked points, and C

0

is the union of those containing no marked points. Let ξ

1

, . . . , ξ

u

be the points that C

+

has in common with C

0

. We say that [( C; x

1

, . . . , x

n

)] is equivalent to [( C

, x

1

, . . . , x

n

)] if there is a family of nodal curves { C

0s

}

s∈S

over a connected base S, together with sections of smooth points τ

1

, . . . , τ

u

, with the property that ( C; x

1

, . . . , x

n

) (resp., ( C

, x

1

, . . . , x

n

) ) can be obtained from C

+

and C

s0

(resp.,C

0s

) by identi- fying ξ

i

with τ

i

( s ) (resp.,τ

i

( s

) ) for i = 1, . . . , u.

It is easy to check that what we just defined is an equivalence relation.

We let

Q : M

g,n

→ M

g,n

denote the projection via the equivalence relation. Now we can state the similar identifications for stable curves:

Theorem 0.12. H : M

g,n

× R

n+

→ M

combg,n

is a homeomorphism.

0.5. Matrix Integral Model. We recall some facts about matrix integral.

Let B be a n × n positive definite symmetric matrix. We consider the integral

c

Rn

e

12(Bx,x)

n i=1

dx

i

,

where c is chosen such that the integral equals 1. With this normalization we have

< x

i

x

j

> : = c

Rn

x

i

x

j

e

12(Bx,x)

n i=1

dx

i

= ( B

1

)

ij

. We can further generalized this computation.

Theorem 0.13 (Wick’s formula). Let f

1

, . . . , f

2k

be linear functions of x

1

, . . . , x

n

. Then

< f

1

f

2

· · · f

2k

>=

p1<···<pk

q1<···<qk

< f

p1

f

q1

> · · · < f

pk

f

qk

> .

(5)

Let Λ = ( Λ

i

)

1iN

be a diagonal matrix with Re ( Λ

i

) > 0 and H = ( h

ij

) = ( x

ij

+

1y

ij

) be a Hermitian matrix. We consider the following measure on the space of Hermitian matrices

Λ

( H ) = C

Λ,N

e

12trH2Λ

N i=1

dx

ii

i<j

dx

ij

dy

ij

, where C

Λ,N

is chosen such that

HN

Λ

( H ) = 1.

By direct computation, we have C

Λ,N

= ( )

N22

iN=1

Λ

i12

i<j

( Λ

i

+ Λ

j

) . In coordinated x

ii

, x

ij

, y

ij

, we can write tr ( H

2

Λ ) = ( Bx, x ) , where

B =

 

 

 

 

 

 

 

 Λ

1

. ..

Λ

N

Λ

1

+ Λ

2

. ..

Λ

N−1

+ Λ

N

Λ

1

+ Λ

2

. ..

Λ

N−1

+ Λ

N

 

 

 

 

 

 

 

 .

Hence we have

< x

2ii

>

Λ,N

: =

HN

x

2ii

Λ

( H ) = 1 Λ

1

, < x

2ij

>

Λ,N

=< y

2ij

>

Λ,N

= 1 Λ

i

+ Λ

j

, and similarly

< h

ij

h

ji

>

Λ,N

= 2

Λ

i

+ Λ

j

, < h

ij

h

kl

>

Λ,N

= 0 if ( i, j ) ̸= ( l, k ) . Now we compute

< e

1

6 tr(H3)

>

Λ,N

=< ( 1 1 2!

1

6

2

( tr ( H

3

))

2

+ 1 4!

1

6

4

( tr ( H

3

))

4

) − · · · >

Λ,N

. By Wick’s formula, the right hand side can be presented as the monomial of < h

injn

h

imkm

> . Notice that each term can correspond to the gluing of 3-stars.

i

1

k

1

j

1

j

1

i

1

k

1

i

2

k

2

j

2

j

2

i

2

k

2

i

2n

k

2n

j

2n

j

2n

i

2n

k

2n

. . . t t

t t t t t t t JJJJ JJJJ J

t t t t t t t t t JJJJ JJJJ J

t t

t t

t t

t t

t

JJJJ JJJJ J

(6)

In this case an edge of the gluing corresponds to a pair < h

injn

h

imkm

> . We define the weight of an gluing the product

Λ

i

+ 2 Λ

j

taken over all edges of the gluing.

Now we can rewrite the Kontsevich’s model into graph sum:

< e

1

6 tr(H3)

>

Λ,N

G∈G3,N

(

√−1 2

)

|V(G)|

| AutG |

e∈E(G)

2 Λ

e

+ Λ

e

,

where G

3,N

is set of equivalent class with 3-valent graphs and with N pos- sible colors Λ

1

, · · · , Λ

N

drawing on the face.

It can be observed by the following proposition:

Proposition 0.14.

< ( trH )

α1

· · · ( tr ( H

k

))

αk

>

Λ,N

= α

1

! · · · α

k

!2

α2

· · · k

αk

G∈GN

1

| AutG |

e∈E(G)

2 Λ

e

+ Λ

e

. 0.6. Proof of Witten conjecture. The first step of the proof is to give a com- binatorial formula for ψ

i

. Let π

i

: S

1

( L

combi

) → M

combg,n

. We want to find a closed 2-form w

i

on M

combg,n

such that π

i

( w

i

) = dϕ and

S1

ϕ |

fiber

= 1.

Fix p = ( p

1

, . . . , p

n

) R

n+

, we have the commutative diagram:

M

g,n Q

||yyy yyy yy

f

I $$I I I I I I I I

M

g,n h

// M

combg,n

( p )

By the way Q was constructed, the line bundle L

i

restricts to a trivial line bundle on the fibers of Q and therefore drops to a well-defined line bundle L

i

on M

g,n

with Q

( L

i

) = L

i

. Let L

combi

be the pullback of L

i

via h

1

, so that

h

( L

combi

) = L

i

, f

( L

combi

) = L

i

.

Now our goal becomes giving the combinatorial expression for its first Chern class.

Let | a |

a

be an orbisimplex of M

combg,n

( p ) , where a corresponds to an embedded graph ( G

a

; x

1

, . . . , x

n

) whose i-th perimeter is equal to p

i

and Γ

a

= Aut (( G

a

; x

1

, . . . , x

n

)) . The coordinates relative to the simplex | a | are the lengths

{ l

e

}

e∈E(Ga)

of the edges of G

a

. At each point x

i

, we consider a cyclically ordered set of oriented edges of G

a

( e

1

, . . . , e

ν

)

(7)

with possible repetitions. A repetition happens when the edge bounds the same component of G

a

. We set

( w

i

)

|a|

= ∑

1≤s<t≤ν−1

d ( l

es

p

i

) d ( l

et

p

i

)

Lemma 0.15. For each x

i

and p R

n+

,

[ w

i

] = c

1

( L

combi

) H

2

( M

combg,n

( p )) . In particular,

[ f

( w

i

)] = c

1

( L

i

) H

2

( M

g,n

) . Now we can rewrite the intersection number

< τ

d1

, . . . , τ

dn

>=

Mg,n

ψ

1d1

· · · ψ

ndn

=

Mcombg,n (p)

w

d11

· · · w

dnn

=

Mcombg,n (p)

w

d11

· · · w

dnn

The last equality is true since the boundary is measure zero.

Let Ω =

ni=1

p

2i

w

i

.

Rn0

e

∑ λipi

(

Mcombg,n (p)

d

d!

)

dp

1

· · · dp

n

= ∑

d1+···dn=d

< τ

d1

· · · τ

dn

>

n i=1

2d

i

!

d

i

! λ

i 2(di+1)

= ( 1 ) , where Re( λ

i

) > 0 and d = 3g 3 + n.

We use the combinatorial theorem due to Kontsevich.

Theorem 0.16.

d!d

dp

1

∧ · · · ∧ dp

n

= 2

2n+5g5

dl

e1

∧ · · · ∧ dl

e6g6+3n

. We have

( 1 ) =

Rn0

e

∑ λipi

(

Mcombg,n (p)

2

2n+5g5

dl

e1

∧ · · · ∧ dl

e6g6+3n

)

= ∑

G∈G3,cg,n

2

2n+5g5

| AutG |

|a(G)|

e

∑ λipi

dl

e1

∧ · · · ∧ dl

e6g6+3n

,

where G

g,n3,c

is the isomorphism class of connected 3-valent embedded graph with genus g and n-marked points. We further do some change of vari- ables.

n i=1

λ

i

p

i

= ∑

e∈E(G)

( λ

e

+ λ

e

) l

e

,

where λ

e

and λ

e

are the perimeter of the two faces adjacent to the edge e.

Now we have the relation ( ∗)

G

3,cg,n

2

−|V(G)|

| Aut ( G ) |

e∈E(G)

2

λ

e

+ λ

e

= ∑

d1+···+dn=d

< τ

d1

· · · τ

dn

>

n i=1

( 2d

i

1 ) !!

λ

2di i+1

.

(8)

Theorem 0.17. Let F ( t

0

, t

1

, · · · ) =

n≥0

d1,...,dn0

1

n! < τ

d1

· · · τ

dn

> t

d1

· · · t

dn

. Set Λ = diag ( Λ

1

, . . . Λ

N

) with Re ( Λ

i

) > 0 and t

i

( Λ ) = −( 2i 1 ) !!Tr ( Λ

2i1

) . Then

F ( t

0

( Λ ) , t

1

( Λ ) , . . . ) = ∑

G∈G3,c,N

(

√−1 2

)

|V(G)|

| Aut ( G ) |

e∈E(G)

2 Λ

e

+ Λ

e

,

where G

3,c,N

is the isomorphism class of connected 3-valent embedded graph with N-possible colors Λ

1

, · · · , Λ

N

drawing on the face.

Corollary 0.18. F ( t

0

( Λ ) , t

1

( Λ ) , · · · ) is the asymptotic expansion of log < e

1

6 trH3

>

Λ,N

as Λ

1

0.

Here we recall some properties of Airy function. We first study its as- ymptotic behaviour by stationary phase method.

a ( y ) =

e

√−1(x3/3−xy)

dx

U(y1/2)

e

1(x3/3xy)

dx +

U(−y1/2)

e

1(x3/3xy)

dx

const ·

±y1/2

y

43

e

2

1

3 y32

f

1

( y

12

) , and similarly we have

a

j1

( y ) =

(

1x )

j1

e

√−1(x3/3−xy)

dx

const ·

±y1/2

y

43

e

2

1

3 y32

f

j

( y

12

) , where f

j

( y ) = y

j

( 1 + ◦( 1 )) .

We have similar expression for matrix Airy function:

A ( Y ) =

HN

e

√−1tr(X3/3−XY)

dX

Y1/2

U(Y12)

e

1tr(X3/3XY)

dX

= ∑

Y1/2

U(0)

e

√−1tr((X+Y1/2)3/3−(X+Y1/2)Y)

dX

= ∑

Y1/2

e

2

1 3 trY3/2

U(0)

e

1tr(X3/3X2Y1/2)

dX

const ·

Y1/2

e

2

1

3 trY3/2

Y

i1/4

i<j

( Y

i1/2

+ Y

j1/2

)

1/2

e

F(t˜0(Y1/2),··· )

− ( 1 ) ,

where ˜t

i

( Y

1/2

) = 2

−(2i+1)/3

( 2i 1 ) !!tr ( Y

i1/2

) . We can express matrix

Airy function in another form.

(9)

Lemma 0.19. If Φ is a conjugacy invariant function on H

N

, then for any diagonal real matrix Y,

HN

Φ ( X ) e

√−1trXY

dX

= ( 2 π

1 )

N(N1)/2

detY

ij1

· · ·

Φ ( D ) e

1trDY

detD

ij1

dD

1

· · · dD

N

Now we have A ( Y ) = (

1 )

N(N1)/2

detY

ij1

· · ·

i

e

√−1tr(D3i/3−DiYi)

detD

ij1

dD

1

· · · dD

N

const ·

Y1/2

e

2

1

3 trY3/2 N

i=1

Y

i34

det f

j

( Y

i1/2

) detY

ij1

− ( 2 ) . We can compare ( 1 ) and ( 2 ) . Then we get

e

F(t0(Λ),...)

det ( f

j

( Λ

i

)) det ( Λ

i j

) .

We conclude that e

F(t0(Λ),...)

safisties KdV hierarchy with respect to vari- ables:

T

2i+1

= 1

2i + 1 TrΛ

2i1

= ( 1 )

2i+1

t

i

( 2i + 1 ) !! .

Finally, notice that T

i

c

i

T

i

also satisfies KdV hierarchy. This proves Wit- ten conjecture.

R EFERENCES

[1] Enrico Arbarello, maurizio Cornalba, Pillip A. Griffiths: Geometry of Algebraic Curves, vol. 2, chap. 20.

[2] S. K. Lando, A.K. Zvonkin: Graphs on Surfaces and their Applications, chap.3, 4.

[3] M. Kontsevich: Intersection Theory on the Moduli Space of Curves and the Matrix

Airy Function.

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We would like to point out that unlike the pure potential case considered in [RW19], here, in order to guarantee the bulk decay of ˜u, we also need the boundary decay of ∇u due to

In particular, we present a linear-time algorithm for the k-tuple total domination problem for graphs in which each block is a clique, a cycle or a complete bipartite graph,

Jing Yu, NTU, Taiwan Values at Algebraic Points.. Thiery 1995) Suppose the Drinfeld module ρ is of rank 1. Drinfeld modules corresponding to algebraic points can be defined over ¯

The Liouville CFT on C g,n describes the UV region of the gauge theory, and the Seiberg-Witten (Gaiotto) curve C SW is obtained as a ramified double cover of C g,n ... ...

We investigate some properties related to the generalized Newton method for the Fischer-Burmeister (FB) function over second-order cones, which allows us to reformulate the

Monopolies in synchronous distributed systems (Peleg 1998; Peleg

From all the above, φ is zero only on the nonnegative sides of the a, b-axes. Hence, φ is an NCP function.. Graph of g functions given in Example 3.9.. Graphs of generated NCP