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Moduli Space of Curves.

White Rose Research Online URL for this paper:

http://eprints.whiterose.ac.uk/132933/

Version: Accepted Version

Article:

Buryak, A (2017) Double Ramification Cycles and the n-Point Function for the Moduli

Space of Curves. Moscow Mathematical Journal, 17 (1). pp. 1-13. ISSN 1609-3321

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(2)

DOUBLE RAMIFICATION CYCLES AND THE

n

-POINT FUNCTION FOR

THE MODULI SPACE OF CURVES

ALEXANDR BURYAK

Abstract. In this paper, using the formula for the integrals of theψ-classes over the double ramification cycles found by S. Shadrin, L. Spitz, D. Zvonkine and the author, we derive a new explicit formula for then-point function of the intersection numbers on the moduli space of curves.

1.

Introduction

Consider the moduli space

M

g,n

of stable complex algebraic curves of genus

g

with

n

marked

points. The class

ψ

i

H

2

(

M

g,n

,

Q

) is defined as the first Chern class of the line bundle

over

M

g,n

formed by the cotangent lines at the

i

-th marked point. We define the intersection

numbers by

h

τ

d1

τ

d2

· · ·

τ

dn

i

g

:=

Z

Mg,n

ψ

d1

1

ψ

d2 2

· · ·

ψ

dn

n

.

(1.1)

In the unstable case 2

g

2 +

n

0 we define the bracket to be equal to zero. The bracket (1.1)

vanishes unless the dimension constraint

n

X

i=1

d

i

= 3

g

3 +

n

is satisfied. Introduce variables

t

0

, t

1

, t

2

, . . .

. The celebrated conjecture of E. Witten [Wit91],

proved by M. Kontsevich [Kon92], says that for the following generating function

F

(

t

0

, t

1

, . . .

) :=

X

g≥0

n≥1

X

d1,...,dn≥0

h

τ

d1

· · ·

τ

dnig

t

d1

· · ·

t

dn

n

!

,

the exponent

e

F

is a tau-function of the KdV hierarchy in the variables

T

2i+1

=

(2i+1)!!ti

.

In this paper we discuss a different generating function for the intersection numbers (1.1).

Let

n

1. Introduce variables

x

1

, . . . , x

n

. Define

F

(

x

1

, . . . , x

n

) :=

X

g≥0

F

g

(

x

1

, . . . , x

n

)

,

where

F

g

(

x

1

, . . . , x

n

) :=

X

d1,...,dn≥0

h

τ

d1

· · ·

τ

dn

i

g

x

d1

1

· · ·

x

dnn

.

The function

F

(

x

1

, . . . , x

n

) is often called the

n

-point function. There are several known

closed formulas for it [BDY15, BH07, Oko02]. In this paper we derive a simple new formula

for

F

(

x

1

, . . . , x

n

) using the result of [BSSZ15]. We believe that our approach can be useful for

the understanding of the structure of more general Gromov-Witten invariants.

2010Mathematics Subject Classification. Primary 14H10, Secondary 14C17.

Key words and phrases. Moduli space of curves, intersection numbers.

The author was supported by grant Russian Science Foundation N16-11-10260, project ”Geometry and mathematical physics of integrable systems”. We are grateful to R. Pandharipande and S. Shadrin for useful discussions and to an anonymous referee for a number of suggestions that helped us to improve the exposition of the paper.

(3)

Let us formulate our main result. Introduce variables

a

1

, a

2

, . . . , a

n

. We will use the following

notations.

Let

ζ

(

x

) :=

e

x2

e

− x 2

.

For a permuation

σ

S

n

denote

a

′i

:=

a

σ(i)

and

x

′i

:=

x

σ(i)

.

Finally,

a b

c d

=

ad

bc.

We define the functions

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

) by

P

1

(

a

1

;

x

1

) :=

1

x

1

,

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

) :=

(1.2)

=

X

σ∈Sn

σ(1)=1

x

2

· · ·

x

n1

ζ

a

1

a

2

x

1

x

2

ζ

a

1

+

a

2

a

3

x

1

+

x

2

x

3

· · ·

ζ

a

1

+

· · ·

+

a

n1

a

n

x

1

+

· · ·

+

x

n1

x

n

a

1

a

2

x

1

x

2

a

2

a

3

x

2

x

3

· · ·

a

n1

a

n

x

n1

x

n

,

n

2

.

At first sight it appears that for

n

2 the function

P

n

(

a

;

x

) has simple poles along the

hy-perplanes

{

a

i

x

j

a

j

x

i

= 0

}

, but in [BSSZ15, Remark 1.6] it was shown that for

n

2 the

function

P

n

(

a

;

x

) is a power series in

x

1

, . . . , x

n

with coefficients in

C

[

a

1

, . . . , a

n

]. Moreover,

by [BSSZ15, Remark 1.5], the function

P

n

(

a

;

x

) is symmetric with respect to simultaneous

permutations of the variables

a

1

, . . . , a

n

and the variables

x

1

, . . . , x

n

. Our main result is the

following theorem.

Theorem 1.1.

We have

(1.3)

F

(

x

1

, . . . , x

n

) =

=

e

(Pxi)3 24

(

P

x

i

)

Q

2

πx

i

Z

Rn

e

P a2i 2xi

P

n

(

1

a

1

, . . . ,

1

a

n

;

x

1

, . . . , x

n

)

da

δ

n,1

x

2

1

δ

n,2

x

1

+

x

2

,

where

da

:=

da

1

· · ·

da

n

.

Let us make a few comments about the right-hand side of equation (1.3) and, in particular,

show that it is a power series in

x

1

, . . . , x

n

. Note that for

x >

0 and

d

0 we have

1

2

πx

Z

R

a

d

e

−a 2 2x

da

=

(

(

d

1)!!

x

d2

,

if

d

is even

,

0

,

if

d

is odd

.

(1.4)

Therefore, the transformation

1

Q

2

πx

i

Z

Rn

e

P a2i 2xi

P

n

(

1

a

;

x

)

da

(1.5)

just means that we replace each monomial

a

d1

1

· · ·

a

dnn

in

P

n

(

a

;

x

) by

(

1)

12 P

di

Y

(

d

i

1)!!

x

di 2

i

,

if all exponents

d

i

are even and by zero otherwise. The transformation (1.5) can also be

interpreted as the Laplace transformation. For

n

3, in [BSSZ15, Remark 1.6] it was shown

that the function

xPn(a;x)

1+···+xn

is a power series in

x

1

, . . . , x

n

with coefficients from

C

[

a

1

, . . . , a

n

].

Therefore, the right-hand side of (1.3) is a power series in

x

1

, . . . , x

n

. In the case

n

= 2, again

from [BSSZ15, Remark 1.6] we know that

P2(a1,a2;x1,x2)

x1+x2

1

x1+x2

is a power series in

x

1

, x

2

with

(4)

DR CYCLES AND THE n-POINT FUNCTION 3

and

x

2

. For

n

= 1 we immediately see that the right-hand side of (1.3) is equal to

e x31 24−1

x21

that

is of course a power series in

x

1

.

Let us describe briefly the plan of the proof of Theorem 1.1. The double ramification

cy-cle DR

g

(

a

1

, . . . , a

n

) is a cohomology class in

H

2g

(

M

g,n

,

Q

). It depends on a list of integers

a

1

, . . . , a

n

satisfying

P

a

i

= 0. In [BSSZ15] the authors derived an explicit formula for the

generating series

X

g≥0 2g−2+n>0

X

d1,...,dn≥0

Z

Mg,n

DR

g

(

a

1

, . . . , a

n

)

ψ

1d1

· · ·

ψ

ndn

!

x

d1

1

· · ·

x

dnn

.

We recall it in Section 2. Denote by

π

m

:

M

g,n

→ M

g,n−m

the forgetful map that forgets the

last

m

marked points. Let

a

1

, . . . , a

n

and

b

1

, . . . , b

g

be arbitrary integers and let

A

:=

P

a

i

and

B

:=

P

b

j

. The push-forward

π

g∗DRg

(

a

1

, . . . , a

n

,

A

B, b

1

, . . . , b

g

) is a cohomology class of

degree 0 and it is equal to

g

!

b

2

1

b

22

· · ·

b

2g

times the unit. This observation together with the string

equation for the intersection numbers (1.1) implies that

g

!

b

21

· · ·

b

2g

X

x

i

F

g

(

x

1

, . . . , x

n

) =

=

X

d1,...,dn≥0

Z

Mg,n+g+1

π

g∗

DR

g

(

a

1

, . . . , a

n

,

A

B, b

1

, . . . , b

g

)

ψ

d11

· · ·

ψ

ndn

!

x

d1

1

· · ·

x

dnn

.

Moreover, this polynomial is the term of the lowest degree 3

g

2 +

n

with respect to the

x

-variables in the infinite series

X

m≥0

X

d1,...,dn≥0

Z

Mg,n+g+1

π

g∗DRm

(

a

1

, . . . , a

n

,

A

B, b

1

, . . . , b

g

)

ψ

d11

· · ·

ψ

ndn

!

x

d1 1

· · ·

x

dn

n

.

In Section 2 we derive an explicit formula for this series and then in Section 3 prove Theorem 1.1.

In Section 4 we do an explicit computation of the one-point and the two-point functions

using our general formula.

2.

Double ramification cycles

Let

n

2 and let

a

1

, . . . , a

n

be a list of integers satisfying

P

a

i

= 0. The double ramification

cycle DR

g

(

a

1

, . . . , a

n

) is a cohomology class in

H

2g

(

M

g,n

,

Q

). If not all of

a

i

’s are equal to zero,

then the restriction

DR

g

(

a

1

, . . . , a

n

)

|

Mg,n

to the moduli space of smooth curves

M

g,n

⊂ M

g,n

can be defined as the Poincar´e dual to

the locus of pointed smooth curves [

C, p

1

, . . . , p

n

] satisfying

O

C

(

P

a

i

p

i

)

=

O

C

. We refer the

reader, for example, to [BSSZ15] for the general definition of the double ramification cycle on

the whole moduli space

M

g,n

. We will often consider the Poincar´e dual to the double

ramifica-tion cycle DR

g

(

a

1

, . . . , a

n

). It is an element of

H

2(2g−3+n)

(

M

g,n

,

Q

) and, abusing our notation

a little bit, it will also be denoted by DR

g

(

a

1

, . . . , a

n

). An explicit formula for the double

ram-ification cycle DR

g

(

a

1

, . . . , a

n

) in terms of tautological classes in the cohomology

H

(

M

g,n

,

Q

)

was recently obtained in [JPPZ16]. In particular, it implies that the double ramification

cy-cle DR

g

(

a

1

, . . . , a

n

) depends polynomially on the parameters

a

1

, . . . , a

n

.

Let us now formulate the main result of [BSSZ15]. Let

d

1

, . . . , d

n

be non-negative integers

satisfying

P

d

i

= 2

g

3 +

n

. Then the integral

Z

DRg(a1,...,an)

ψ

d1

1

· · ·

ψ

dn

n

(5)

is equal to the coefficient of

x

d1

1

· · ·

x

dnn

in the generating function

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

ζ

(

x

1

+

· · ·

+

x

n

)

δ

n,2

x

1

+

x

2

.

(2.2)

As it was discussed in the introduction, this generating series is a power series in

x

1

, . . . , x

n

with

coefficients from

C

[

a

1

, . . . , a

n

]. We see that the integral (2.1) is a polynomial in

a

1

, . . . , a

n

. Note

that

ζ

(

x

) =

P

i0 x2i+1

22i(2i+1)!

, then from the definition (1.2) it is easy to see that the series (2.2)

has the form

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

ζ

(

x

1

+

· · ·

+

x

n

)

δ

n,2

x

1

+

x

2

=

X

j≥0 2j−2+n>0

X

i

f

i,j

(

a

)

g

i,j

(

x

)

,

where

g

i,j

(

x

)

C

[

x

1

, . . . , x

n

] is a polynomial of degree 2

j

3 +

n

,

f

i,j

(

a

)

C

[

a

1

, . . . , a

n

] and

for any fixed

j

the second summation is finite. From this we conclude that all terms in the

series (2.2) have the geometrical meaning and, thus,

X

g≥0 2g−2+n>0

X

d1,...,dn≥0

Z

DRg(a1,...,an)

ψ

d1

1

· · ·

ψ

ndn

!

x

d1

1

· · ·

x

dnn

=

P

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

ζ

(

x

1

+

· · ·

+

x

n

)

δ

n,2

x

1

+

x

2

.

(2.3)

Now we want to generalize formula (2.3) for the integrals over the double ramification cycles

with forgotten points. We begin with the following lemma.

Lemma 2.1.

For

n

2

we have

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

|

xn=0

=

ζ

(

a

n

(

x

1

+

· · ·

+

x

n−1

))

a

n

P

n−1

(

a

1

, . . . , a

n−1

;

x

1

, . . . , x

n−1

)

.

Proof.

For

n

= 2 we have

P

2

(

a

1

, a

2

;

x

1

, x

2

) =

ζ

(

a

1

x

2

a

2

x

1

)

a

1

x

2

a

2

x

1

.

Therefore,

P

2

(

a

1

, a

2

;

x

1

, x

2

)

|

x2=0

=

ζ

(

a

2

x

1

)

a

2

x

1

=

ζ

(

a

2

x

1

)

a

2

P

1

(

a

1

;

x

1

)

.

Suppose

n

3. Note that if we set

x

n

= 0, then the product

x

′2

· · ·

x

′n−1

on the right-hand

side of (1.2) vanishes unless

σ

(

n

) =

n

. Therefore, we obtain

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

|

xn=0

=

X

σ∈Sn

σ(1)=1, σ(n)=n

x

2

· · ·

x

n1

×

×

ζ

a

1

a

2

x

1

x

2

· · ·

ζ

a

1

+

a

2

+

· · ·

+

a

n2

a

n1

x

1

+

x

2

+

· · ·

+

x

n2

x

n1

ζ

a

1

+

· · ·

+

a

n1

a

n

x

1

+

· · ·

+

x

n1

0

a

1

a

′2

x

1

x

′2

· · ·

a

n−2

a

′n−1

x

n−2

x

′n−1

a

n−1

a

n

x

n−1

0

=

=

ζ

(

a

n

(

x

1

+

· · ·

+

x

n−1

))

a

n

X

σ∈Sn−1

σ(1)=1

x

2

. . . x

n2

ζ

a

1

a

2

x

1

x

′2

· · ·

ζ

a

1

+

a

2

+

· · ·

+

a

n2

a

n1

x

1

+

x

′2

+

· · ·

+

x

′n−2

x

′n−1

a

1

a

2

x

1

x

2

· · ·

a

n2

a

n1

x

n2

x

n1

=

=

ζ

(

a

n

(

x

1

+

· · ·

+

x

n−1

))

a

n

P

n−1

(

a

1

, . . . , a

n−1

;

x

1

, . . . , x

n−1

)

.

The lemma is proved.

(6)

DR CYCLES AND THE n-POINT FUNCTION 5

Lemma 2.2.

Let

n

3

,

m

0

and

a

1

, . . . , a

n

, b

1

, . . . , b

m

be integers satisfying

P

a

i

+

P

b

j

= 0

.

Then we have

X

g≥0

X

d1,...,dn≥0

Z

DRg(a1,...,an,b1,...,bm)

ψ

d1

1

· · ·

ψ

dn

n

!

x

d1 1

· · ·

x

dn

n

=

=

Q

m

i=1

S

(

b

i

X

)

S

(

X

)

X

m−1

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

,

where

X

:=

P

x

i

.

Proof.

Using equation (2.3) and Lemma 2.1, we compute

X

g≥0

X

d1,...,dn≥0

Z

DRg(a1,...,an,b1,...,bm)

ψ

d1

1

· · ·

ψ

ndn

!

x

d1

1

· · ·

x

dnn

=

=

P

n+m

(

a

1

, . . . , a

n

, b

1

, . . . , b

m

;

x

1

, . . . , x

n+m

)

ζ

(

x

1

+

· · ·

+

x

n+m

)

xn+1=···=xn+m=0

=

=

1

ζ

(

X

)

m

Y

i=1

ζ

(

b

i

X

)

b

i

!

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

) =

=

Q

m

i=1

S

(

b

i

X

)

S

(

X

)

X

m−1

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

.

The lemma is proved.

We keep the assumptions of the last lemma. Recall that by

π

m

:

M

g,n+m

→ M

g,n

we denote

the forgetful map that forgets the last

m

marked points. For a subset

I

⊂ {

1

, . . . , m

}

let

B

I

:=

X

i∈I

b

i

.

The following proposition generalizes formula (2.3).

Proposition 2.3.

We have

(2.4)

X

g≥0

X

d1,...,dn≥0

Z

πm∗DRg(a1,...,an,b1,...,bm)

ψ

d1

1

· · ·

ψ

dn

n

!

x

d1 1

· · ·

x

dn

n

=

=

1

S

(

X

)

X

I0⊔I1⊔...⊔In={1,...,m}

X

|I0|−1

n

Y

i=1

(

x

i

)

|Ii|

Y

i∈I0

S

(

b

i

X

)

P

n

(

a

1

+

B

I1

, . . . , a

n

+

B

In

;

x

)

.

Proof.

For a subset

I

=

{

i

1

, i

2

, . . . , i

|I|

} ⊂ {

1

, . . . , m

}

, where

i

1

< i

2

<

· · ·

< i

|I|

, we denote

by

b

I

the string

b

i1

, b

i2

, . . . , b

i|I|

. Clearly, formula (2.4) follows from Lemma 2.2 and the equation

Z

πm∗DRg(a1,...,an,b1,...,bm)

ψ

d1

1

· · ·

ψ

ndn

=

X

`n

i=0Ii={1,...,m}

|Ii|≤di

(

1)

m−|I0|

Z

DRg

(

a1+BI1,...,an+BIn,bI0

)

n

Y

i=1

ψ

di−|Ii|

i

.

(2.5)

(7)

Z

πm∗DRg(a1,...,an,b1,...,bm)

ψ

d1

1

· · ·

ψ

dn

n

=

Z

(πm−1)∗DRg(a1,...,an,bm,b1,...,bm−1)

ψ

d1

1

· · ·

ψ

dn

n

(2.6)

X

1≤i≤n

di>0

Z

(πm−1)∗DRg(a1,...,ai+bm,...,an,b1,...,bm−1)

ψ

di−1

i

Y

j6=i

ψ

dj

j

.

For this we write

π

m

=

π

1

π

m−1

, where

π

m−1

:

M

g,n+m

→ M

g,n+1

and

π

1

:

M

g,n+1

→ M

g,n

.

Then we have

Z

πm∗DRg(a1,...,an,b1,...,bm)

ψ

d1

1

· · ·

ψ

ndn

=

Z

(πm−1)∗DRg(a1,...,an,bm,b1,...,bm−1)

π

1

ψ

d1

1

· · ·

ψ

ndn

.

For an integer

N

2 and a subset

J

∈ {

1

, . . . , N

}

,

|

J

| ≥

2, denote by

δ

J

0

the cohomology class

in

H

2

(

M

g,N

,

Q

) that is Poincar´e dual to the divisor whose generic point is a nodal curve made

of one smooth component of genus 0 with the marked points labeled by the set

J

and of another

smooth component of genus

g

with the remaining marked points, joined at a separating node.

If 1

i

n

and

d

1, then we have

π

1

ψ

d

i

=

ψ

di

δ

{i,n+1}

0

π

1∗

ψ

id−1

. Therefore,

π

1

ψ

d1

1

· · ·

ψ

ndn

=

ψ

d1

1

· · ·

ψ

dnn

X

1≤i≤n di>0

δ

0{i,n+1}

π

1

ψ

di−1

i

Y

j6=i

ψ

dj

j

!

.

We have (see [BSSZ15] and, in particular, Section 2.1 there for the explanation of the

nota-tion

)

δ

{0i,n+1}

·

(

π

m−1

)∗

DR

g

(

a

1

, . . . , a

n

, b

m

, b

1

, . . . , b

m−1

) =

= (

π

m−1

)

(DR

0

(

a

i

, b

m

,

a

i

b

m

)

DR

g

(

a

1

, . . . ,

a

b

i

, . . . , a

n

, b

1

, . . . , b

m−1

, a

i

+

b

m

))

.

Therefore,

Z

(πm−1)∗DRg(a1,...,an,bm,b1,...,bm−1)

δ

{0i,n+1}

π

1

ψ

di−1

i

Y

j6=i

ψ

dj

j

!

=

=

Z

(πm−1)∗DRg(a1,...,ai+bm,...,an,b1,...,bm−1)

ψ

di−1

i

Y

j6=i

ψ

dj

j

.

This completes the proof of equation (2.6).

It is easy to see that, applying formula (2.6)

m

times, we get equation (2.5). The proposition

is proved.

Finally, let us formulate an important geometric property of the double ramification cycle

that we will use in the next section. Let

g

0,

n

3 and

a

1

, . . . , a

n

, b

1

, . . . , b

g

be integers

satisfying

P

a

i

+

P

b

j

= 0. Then we have (see [BSSZ15, Example 3.7])

π

g∗

DR

g

(

a

1

, . . . , a

n

, b

1

, . . . , b

g

) =

g

!

b

21

· · ·

b

2g

[

M

g,n

]

,

(2.7)

π

g∗DRm

(

a

1

, . . . , a

n

, b

1

, . . . , b

g

) = 0

,

m < g.

(2.8)

The last property implies that the coefficient of a monomial

x

d1

1

· · ·

x

dnn

in the generating

se-ries (2.4) is zero, if

P

d

i

<

3

m

3 +

n

. We will use this observation in the next section.

3.

Proof of Theorem 1.1

(8)

DR CYCLES AND THE n-POINT FUNCTION 7

3.1.

Reduction to the case

n

3

.

The intersection numbers

h

τ

d1

· · ·

τ

dn

i

g

satisfy the string

equation

h

τ

0

τ

d1

· · ·

τ

dn

i

g

=

X

1≤i≤n di>0

*

τ

di−1

Y

j6=i

τ

dj

+

g

,

with one exceptional case

h

τ

03

i0

= 1. The string equation implies that for

n

2 we have

F

(

x

1

, . . . , x

n

)

|

xn=0

= (

x

1

+

· · ·

+

x

n−1

)

F

(

x

1

, . . . , x

n−1

) +

δ

n,3

.

(3.1)

Denote the right-hand side of (1.3) by

G

(

x

1

, . . . , x

n

). Let us show that the function

G

also

satisfies equation (3.1). We compute

1

Q

n i=1

2

πx

i

Z

Rn

e

Pn i=1

a2i 2xi

P

n

1

a

1

, . . . ,

1

a

n

;

x

1

, . . . , x

n

da

1

· · ·

da

n

xn=0

=

=

1

(2

π

)

n2

Z

Rn

e

−Pni=1 a2i

2

P

n

x

1

a

1

, . . . ,

x

n

a

n

;

x

1

, . . . , x

n

da

1

· · ·

da

n

xn=0

by Lemma 2.1

=

=

x

1

+

· · ·

+

x

n−1

(2

π

)

n2

Z

Rn

e

−Pni=1 a2i

2

P

n

−1

x

1

a

1

, . . . ,

x

n−1

a

n−1

;

x

1

, . . . , x

n−1

da

1

· · ·

da

n

=

=

x

1

Q

+

n

· · ·

1

+

x

n−1

i=1

2

πx

i

Z

Rn−1

e

Pn−1 i=1

a2i 2xi

P

n−1

1

a

1

, . . . ,

1

a

n−1

;

x

1

, . . . , x

n−1

da

1

· · ·

da

n−1

.

Thus, we obtain

G

(

x

1

, . . . , x

n

)

|

xn=0

= (

x

1

+

· · ·

+

x

n−1

)

G

(

x

1

, . . . , x

n−1

) +

δ

n,3

.

(3.2)

We see that if equation (1.3) holds for

n

=

n

0

, then it holds for all

n

n

0

. Hence, it is sufficient

to prove equation (1.3) for

n

3.

3.2.

Case

n

3

.

We assume that

n

3. Let

g

0 and consider arbitrary integers

a

1

, . . . , a

n

and

b

1

, . . . , b

g

. Let

A

:=

n

X

i=1

a

i

,

B

:=

g

X

i=1

b

i

,

X

:=

n

X

i=1

x

i

.

Equations (2.7) and (3.1) imply that

g

!

b

21

· · ·

b

2g

X

F

g

(

x

1

, . . . , x

n

) =

g

!

b

12

· · ·

b

2g

F

g

(

x

1

, . . . , x

n

, x

n+1

)

|

xn+1=0

=

=

X

d1,...,dn≥0

Z

πg∗DRg(a1,...,an,−A−B,b1,...,bg)

ψ

d1

1

· · ·

ψ

ndn

!

x

d1

1

· · ·

x

dnn

(3.3)

independently of

a

1

, . . . , a

n

. Moreover, by the remark at the end of Section 2, expression (3.3)

is equal to the term of the lowest degree 3

g

2 +

n

with respect to the

x

-variables in the series

X

m≥0

X

d1,...,dn≥0

Z

πg∗DRm(a1,...,an,−A−B,b1,...,bg)

ψ

d1

1

· · ·

ψ

dn

n

!

x

d1 1

· · ·

x

dn

n

.

(3.4)

Proposition 2.3 and Lemma 2.1 imply that

X

m≥0

X

d1,...,dn≥0

Z

πg∗DRm(a1,...,an,−A−B,b1,...,bg)

ψ

d1

1

· · ·

ψ

ndn

!

x

d1

1

· · ·

x

dnn

=

(3.5)

=

S

((

A

B

)

X

)

S

(

X

)

X

`n

i=0Ii={1,...,g}

X

|I0|

n

Y

i=1

(

x

i

)

|Ii|

Y

i∈I0

(9)

In the last expression the multiplication by

S((−SA(XB))X)

doesn’t change the lowest degree term

with respect to the

x

-variables. Therefore, we obtain

g

!

b

21

· · ·

b

2g

X

F

g

(

x

1

, . . . , x

n

) =

=

X

`n

i=0Ii={1,...,g}

X

|I0|

n

Y

i=1

(

x

i

)

|Ii|

Y

i∈I0

S

(

b

i

X

)

P

n

(

a

1

+

B

I1

, . . . , a

n

+

B

In

;

x

)

3g−2+n

=

=

X

`n

i=0Ii={1,...,g}

X

|I0|

n

Y

i=1

(

x

i

)

|Ii|

Y

i∈I0

S

(

b

i

X

)

P

n

(

B

I1

, . . . , B

In

;

x

)

3g−2+n

,

where by [

·

]

d

we denote the degree

d

part with respect to the

x

-variables. Equivalently, we can

write

(3.6)

g

!

X

F

g

(

x

1

, . . . , x

n

) =

=

Coef

b21···b2 g

X

`n

i=0Ii={1,...,g}

X

|I0|

n

Y

i=1

(

x

i

)

|Ii|

Y

i∈I0

S

(

b

i

X

)

P

n

(

B

I1

, . . . , B

In

;

x

)

3g−2+n

.

From the definition (1.2) we see that the series

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

) satisfies the following

homogeneity property:

P

n

(

λ

−1

a

1

, . . . , λ

−1

a

n

;

λx

1

, . . . , λx

n

) =

λ

n−2

P

n

(

a

1

, . . . , a

n

;

x

1

, . . . , x

n

)

.

Therefore, the expression in the square brackets on the right-hand side of (3.6) has automatically

degree 3

g

2 +

n

in the

x

-variables. Since

S

(

z

) = 1 +

z2

24

+

. . .

, we have

Coef

b2 1···b2g

Y

i∈I0

S

(

b

i

X

)

P

n

(

B

I1

, . . . , B

In

;

x

)

!

=

X

2|I0|

24

|I0|

Coef

Q

i /∈I0b2i

P

n

(

B

I1

, . . . , B

In

;

x

)

.

Note that

Coef

Qi /I

0b 2 i

n

Y

i=1

B

di

Ii

=

(Q

n

i=1

di!

2di/2

,

if

d

i

= 2

|

I

i

|

,

0

,

otherwise

.

Therefore, we get

Coef

b2 1···b2g

X

`n

i=0Ii={1,...,g}

X

|I0|

n

Y

i=1

(

x

i

)

|Ii|

Y

i∈I0

S

(

b

i

X

)

P

n

(

B

I1

, . . . , B

In

;

x

) =

=

X

`n

i=0Ii={1,...,g}

X

3|I0|

24

|I0|

n

Y

i=1

(

x

i

)

|Ii|

(2

|

I

i

|

)!

2

|Ii|

Coef

Qn i=1a

2|Ii|

i

P

n

(

a

;

x

) =

=

X

m0,m1,...,mn≥0

m0+···+mn=g

g

!

m

0

!

· · ·

m

n

!

X

3

24

m0

Y

n

i=1

(

x

i

)

mi

(2

m

i

)!

2

mi

Coef

Qn i=1a

2mi

i

P

n

(

a

;

x

) =

=

X

m0,m1,...,mn≥0

m0+···+mn=g

g

!

m

0

!

X

3

24

m0

Y

n

i=1

((

x

i

)

mi

(2

m

i

1)!!) Coef

Qn i=1a

2mi

(10)

DR CYCLES AND THE n-POINT FUNCTION 9

Finally, we obtain

X

F

(

x

1

, . . . , x

n

) =

X

g≥0

X

F

g

(

x

1

, . . . , x

n

) =

=

X

m0,m1,...,mn≥0

1

m

0

!

X

3

24

m0

Y

n

i=1

((

x

i

)

mi

(2

m

i

1)!!) Coef

Qn i=1a

2mi i

P

n

(

a

;

x

)

by (1.4)

=

=

e

X3 24

Q

2

πx

i

Z

Rn

e

P a2i 2xi

P

n

1

a

;

x

da.

This completes the proof of the theorem.

4.

Examples

For

n

= 1 Theorem 1.1 immediately gives the well-known formula (see e.g. [FP00])

F

(

x

1

) =

e

x

3 1 24

1

x

2 1

.

Suppose

n

= 2. We have

P

2

(

a

1

, a

2

;

x

1

, x

2

) =

ζ

(

a

1

x

2

a

2

x

1

)

a

1

x

2

a

2

x

1

=

S

(

a

1

x

2

a

2

x

1

) =

X

n≥0

(

a

1

x

2

a

2

x

1

)

2n

(2

n

+ 1)!2

2n

=

=

X

n≥0

X

m1+m2=2n

(

a

1

x

2

)

m1

(

a

2

x

1

)

m2

(2

n

+ 1)2

2n

m

1

!

m

2

!

.

Therefore, we obtain

e

(x1+x2) 3 24

2

π

x

1

x

2

Z

R2

e

a21 2x1

a22 2x2

P

2

(

1

a

1

,

1

a

2

;

x

1

, x

2

)

da

=

=

e

(x1+x2)3 24

2

π

x

1

x

2

X

n≥0

X

m1+m2=n

Z

R2

e

a21 2x1−

a22 2x2

(

1)

n

a

2m1

2

a

21m2

x

21m1

x

22m2

2

2n

(2

n

+ 1)(2

m

1

)!(2

m

2

)!

da

=

=

e

(x1+x2) 3

24

X

n≥0

X

m1+m2=n

(

1)

n

x

m1

2

x

m12

x

21m1

x

22m2

2

3n

(2

n

+ 1)

m

1

!

m

2

!

=

=

e

x 3 1+x32

24

e

x1x2(x1+x2)

8

X

n≥0

(

1)

n

(

x

1

x

2

(

x

1

+

x

2

))

n

8

n

(2

n

+ 1)

n

!

=

=

e

x 3 1+x32

24

X

n≥0

x

1

x

2

(

x

1

+

x

2

)

8

n

X

m1+m2=n

(

1)

m2

m

1

!

m

2

!(2

m

2

+ 1)

.

Let

C

n

:=

P

m1+m2=n

(−1)m2

m1!m2!(2m2+1)

. For

n

1 we compute

C

n

=

1

n

!

Z

1

0

(1

y

2

)

n

dy

=

2

(

n

1)!

Z

1

0

y

2

(1

y

2

)

n−1

dy

=

2

nC

n

+ 2

C

n−1

.

Therefore,

C

n

=

2n2+1

C

n−1

, and, since

C

0

= 1, we get

C

n

=

2

n

(2n+1)!!

. Hence, we obtain

e

(x1+x2) 3 24

2

π

x

1

x

2

Z

R2

e

a21 2x1−

a22

2x2

P

2

(

1

a

1

,

1

a

2

;

x

1

, x

2

)

da

=

e

x31+x32

24

X

n≥0

n

!

(2

n

+ 1)!

x

1

x

2

(

x

1

+

x

2

)

2

n

(11)

As a result, we get the following formula for the two-point function:

F

(

x

1

, x

2

) =

e

x31+x32 24

(

x

1

+

x

2

)

X

n≥0

n

!

(2

n

+ 1)!

x

1

x

2

(

x

1

+

x

2

)

2

n

x

1

1

+

x

2

.

This formula was found by R. Dijkgraaf (see e.g. [FP00]).

References

[BDY15] M. Bertola, B. Dubrovin, D. Yang. Correlation functions of the KdV hierarchy and applications to intersection numbers over Mg,n. Physica D. Nonlinear Phenomena 327 (2016), 30–57.

[BH07] E. Br´ezin, S. Hikami.Vertices from replica in a random matrix theory. Journal of Physics. A. Math-ematical and Theoretical 40 (2007), no. 45, 13545–13566.

[BS11] A. Buryak, S. Shadrin. A new proof of Faber’s intersection number conjecture. Advances in Mathe-matics 228 (2011), 22–42.

[BSSZ15] A. Buryak, S. Shadrin, L. Spitz, D. Zvonkine.Integrals of ψ-classes over double ramification cycles. American Journal of Mathematics 137 (2015), no. 3, 699–737.

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Department of Mathematics, ETH Z¨urich, Switzerland, and

Faculty of Mechanics and Mathematics, Lomonosov Moscow State University, Russian Fed-eration

References

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