Makoto Sakaguchi (Okayama Institute for Quantum Physics ...qft/2009/slides/Sakaguchi.pdfMakoto...

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Makoto Sakaguchi (Okayama Institute for Quantum Physics) 2009/7/9 @ 基研研究会「場の理論と弦理論」 based on ``Super Galilean conformal algebra in AdS/CFT,'' arXiv:0905.0188 [hep-th].

Transcript of Makoto Sakaguchi (Okayama Institute for Quantum Physics ...qft/2009/slides/Sakaguchi.pdfMakoto...

Page 1: Makoto Sakaguchi (Okayama Institute for Quantum Physics ...qft/2009/slides/Sakaguchi.pdfMakoto Sakaguchi (Okayama Institute for Quantum Physics) 2009/7/9 @ 基研研究会「場の理論と弦理論」

Makoto Sakaguchi (Okayama Institute for Quantum Physics)

2009/7/9 @ 基研研究会「場の理論と弦理論」

based on

``Super Galilean conformal algebra in AdS/CFT,'' arXiv:0905.0188 [hep-th].

Page 2: Makoto Sakaguchi (Okayama Institute for Quantum Physics ...qft/2009/slides/Sakaguchi.pdfMakoto Sakaguchi (Okayama Institute for Quantum Physics) 2009/7/9 @ 基研研究会「場の理論と弦理論」

Introduction

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AdS/CFT correspondence

IIB string in AdS5 x S5

weakN=4 super Yang-Mills in 4-dim

strong

Applications AdS/CMPsuperconductor [Gubser '0801, Hartnoll-Herzog-Horowitz '0810, …]

quantum Hall effect [Keski-Vakkuri-Kraus '0805, Davis-Kraus-Shah '0809, …]

fermions at unitarity [Son '0804, Balasubramanian-McGreevy '0804,…]

Non-relativistic CFTSchrödinger symmetry

Galilean conformal symmetry

conformal

∪ NR limit

Poincare Galilei

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• symmetry of (free) Schrödinger equation [Hagen'72, Niederer'72]

• subalgebra of conformal algebra in one higher dimensions

NR limit

• relativistic FT Schrödinger-invariant FT (for example [Jackiw-Pi’90])

• z=2 case

Schrödinger symmetryGalilean symmetry { H, Pi, Jij, Gi }

dilatation D, Galilean special conformal K

central charge M

z: dynamical exponent

anisotropic scale transformation D

3

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Galilean conformal symmetryGalilean symmetry { H, Pi, Jij, Gi }

dilatation D, Galilean special conformal K

acceleration Ki

z=1 case

PLAN

• Inönü-Wigner contraction of conformal algebra (review)

• bulk realization of GCA

• supersymmetric GCA

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GCA from conformal algebra

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confd+1

IW contraction

and

Galilean conformal algebra

cf: [Lukierski-Stichel-Zakrzewski '0511]

:

:

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GCA1+d

so(2,1) + so(d)

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confd+1 GCAd+1

contraction[Lukierski-Stichel-Zakrzewski '0511]

bulk realization of GCA

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AdSd+2

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confd+1 GCAd+1

contraction[Lukierski-Stichel-Zakrzewski '0511]

bulk realization of GCA

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AdSd+2 ???

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confd+1 GCAd+1

contraction

contraction[Lukierski-Stichel-Zakrzewski '0511]

bulk realization of GCA

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AdSd+2 ???

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confd+1 GCAd+1

contraction

contraction[Lukierski-Stichel-Zakrzewski '0511]

bulk realization of GCA

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AdSd+2 Newton-Hooke string

algebra

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confd+1 GCAd+1

contraction

contraction

[Gomis-Gomis-Kamimura '0507]

[Lukierski-Stichel-Zakrzewski '0511]

GCA is realized as NH string algebra in the bulk

bulk realization of GCA

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[Gomis-Gomis-Kamimura '0507]

AdS2 string worldsheet

close-up of AdS2 string worldsheet

NR string [GGK'0507, MS-Yoshida'0703,'0709,'0712]

GCA and Newton-Hooke string algebraAdSd+2

Newton-Hooke string algebraAdS2

so(d)

32 susy NH algebras [GGK ‘0507, MS-Yoshida ‘0605]

bo

un

da

ry

(0,d+1)

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NH string algebra

so(2,1) + so(d)

GCA1+d

so(2,1) + so(d)

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Close-up of AdS brane in AdSd+1

NH brane algebra semi-GCA

[Brugues-Gomis-Kamimura'0603]

semi-GCA is realized as NH brane algebra in the bulk

[Alishahiha-Davody-Vahedi’0903]

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supersymmetric GCA1+3 from psu(2,2|4)

psu(2,2|4) super GCA1+3

AdS5 x S5

contraction

We are interested in

dynamical susy

susy on AdS2

ρ p=1 p=3 p=5 p=7

σ1 , σ3 (2,0) (2,4), (4,2)

iσ2 (3,1), (1,3) (5,3), (3,5)

1 (1,1) (1,5), (3,3), (5,1)

a pair of 16 component Majorana-Weyl spinors

1/2 BPS brane configurations in AdS5 x S5

[MS-Yoshida ‘0605]

[MS, de Azcarraga-Lukierski ‘0905]

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IW contraction

and

32 susy GCA1+3

GCA iso(5)

dynamical susy

1/2 susy subalgebra

so(2,1) so(3) so(5)

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16 susy GCA1+3

u(1) x su(2)GCA

[MS, de Azcarraga-Lukierski ‘0905]

su(2,2|2) psu(2,2|4)

IW contraction

32 susy GCA1+3

so(2,1) + so(3) + so(5) + 16 susy

16 susy GCA1+3 from su(2,|2)

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32 susy GCA from osp(8|4)

GCA

M2 (AdS2 x S1) in AdS4 x S7

16 susy GCA from osp(4|4)

GCA so(3) x iso(2)

8 susy GCA from osp(2|4)

GCA u(1)

super GCA1+2

close-up of S1 in S7

[MS ‘0905]

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32 susy semi-GCA from osp(8*|4)

iso(4)semi-GCA

M2 (AdS3) in AdS7 x S4

so(2,2) so(4) + so(4)

16 susy semi-GCA from osp(8*|2)

su(2)semi-GCA

super semi-GCA1+5[MS ‘0905]

AdS3

1/2 susy subalgebra

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Summary GCA is a boundary realization of NH string algebra

semi-GCA is a boundary realization of NH brane algebra

super GCA1+3 from SCA4, psu(2,2|4) and su(2,2|2)

string(AdS2) in AdS5

super GCA1+2 from SCA3, osp(8|4), osp(4|4) and osp(2|4)

M2(AdS2 x S1) in AdS4 x S7

super semi-GCA1+5 from SCA6, osp(8*|4) and osp(8*|2)

M2(AdS3) in AdS7

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super GCAs for other 1/2 BPS branes

NRCFT with GCA and NR string

Wilson line in SYM4

infinitely extended super GCA

and so on

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Thank you very much.