Extended Conformal Symmetry and Recursion Formulae for ...soken.editorial/soken... · We found the...

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Shoichi Kanno (Titech) 2013.8.20 基研研究会2013 Extended Conformal Symmetry and Recursion Formulae for Nekrasov Partition Function Y.Matsuo,H.Zhang,SK (arXiv:1306.1523 JHEP08(2013)028)

Transcript of Extended Conformal Symmetry and Recursion Formulae for ...soken.editorial/soken... · We found the...

Page 1: Extended Conformal Symmetry and Recursion Formulae for ...soken.editorial/soken... · We found the recursion formulae for Nekrasov partition function which connect different instanton

Shoichi Kanno (Titech)

2013.8.20 基研研究会2013

Extended Conformal Symmetry andRecursion Formulae for Nekrasov Partition Function

Y.Matsuo,H.Zhang,SK (arXiv:1306.1523 JHEP08(2013)028)

Page 2: Extended Conformal Symmetry and Recursion Formulae for ...soken.editorial/soken... · We found the recursion formulae for Nekrasov partition function which connect different instanton

Introduction and summary

We derive infinite many recursion formulae of Nekrasov partition function for 4D N=2 U(N) linear quiver guage theory,which relates those have different instanton number.

But their meaning is obscure in terms of gauge theory.

◆ AGT conjecture insist that

U(N) Nekrasov function = conformal block

Instanton number = level of descendant state

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This work is generalization of our previous paper (arXiv:1207.5658)for arbitrary Ω-background.

Introduction and summary

In 2D CFT, Ward identity is natural formula that relate different descendant contribution (= different instanton contribution) toconformal block function (= Nekrasov function)

We try to understand the recursion formulae as Ward identity andfind that they can be interprited as the action of SHc algebra (or degenerate double affine Hecke algebra)

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Contents

◆ Introduction and summary

◆ Recursion formulae for Nekrasov partition function

◆ Two dimensional interpretation

◆ Conclusion

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Recursion relation for Nekrasov partition function

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Biulding block of Nekrasov partition function

N=2 conformal linear quiver

N-tuple Young diagram # of Instanton = # of box

vector antifund. hyper

bifund.hyper fund.hyper

mass of matter filed

vev of adjoint scalar

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Rewrite Nekrasov partition function as

Building block of Nekrasov partition function

Building block

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Notation

for

:One box added diagram at k-th rectangle of Y

:One box subtracted diagram at k-th rectangle of Y

1 box added1 box subtracted

generalized hook length

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Notation

For U(N) instanton with adjoint scalar vev

1 box added1 box subtracted

(generalized hook length assosiated with the added/subtracted box)

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Recursion formulae By explicit calculation, we find the following relation

where

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Recursion formulae By explicit calculation, we find the following relation

where

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We want to understand it in terms of 2D CFT point of view,especially as Ward identity for “three-point function”

Recursion formulae

SHc algebra (or degenerate double affine Hecke algebra)

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Two-dimensional interpretation

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fundamental commutation relationgenerator

level

spin l+1

non linear

SHc algebra

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higher level generators are defined by

level

spin

1 2 3 n

s+1

s

SHc algebra

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Representation of SHc algebra

◆representation space

◆action of the generators

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U(1) × Virasoro subalgebra of

◆ U(1) current

◆ Virasoro algebra

In our representation

Virasoro central charge

◆ independent of momenta

◆ same as the central charge of

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U(1) × Virasoro subalgebra of

◆ eigen value of zero mode

where

Weyl vector

Conformal dimension of the state with Toda momentum

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“Vertex operator”

To understand the recursion formulae as Ward identity, we must know a commutater between “vertex operator” and the generators.

Vertex oprerator is product of part and U(1) part

According to AGT conjeture, is primary field

with the Toda momentum

Conformal dimension

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U(1) part vertex operator

Not primary field

Free U(1) part vertex operator should be

U(1) vertex operator must satisfy the following two conditions

(1) reproduces correct U(1) factor

(2) becomes a primaly field at

(Fateev-Litvinov 1109.4042)

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The free boson representation implies thatcommutators with U(1) and Virasoro should be

◆ U(1) current

◆ Virasoro algebra

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Recursion formulae as Ward identity

Assumption

(1) There exist three point function

(2) It equals to building block of Nekrasov function

Write Ward identity for U(1)×Virasoro generators

Do they coincide with the recursion relation or not ?

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Result

We have confirmed constraint for three point function   same as the recursion relation for l=0,1

Note

The anomalous form of the U(1) vertex operator is essential to reproduce the recursion formulae

◆ The special form of the Toda momentum of vertex operateris neccesary.

(vertex operator corresponding to “simple puncture”)

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Conclusion

Future direction

We found the recursion formulae for Nekrasov partition functionwhich connect different instanton contributions (instanton numbersDiffer by one.)

They might be understood as Ward identity of algebra,which is symmetry of U(N) instanton moduli space.

Examine the recursion for l > 1 generators

More general quiver cases

Interpretation in string or M-theory