Exact holography of the mass-deformed M2-brane theory

Abstract We test the holographic relation between the vacuum expectation values of gauge invariant operators in $${\mathcal {N}} = 6$$ N = 6 U $$_k(N)\times \mathrm{U}_{-k}(N)$$ k ( N ) × U - k ( N ) mass-deformed ABJM theory and the LLM geometries with $${\mathbb {Z}}_k$$ Z k orbifold in 11-dimensi...

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Main Authors: Dongmin Jang, Yoonbai Kim, O-Kab Kwon, D. D. Tolla
Format: Article
Language:English
Published: SpringerOpen 2017-05-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-4909-3
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spelling doaj-13277419fd224cb5b3461b36511c403b2020-11-25T01:01:55ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-05-017751710.1140/epjc/s10052-017-4909-3Exact holography of the mass-deformed M2-brane theoryDongmin Jang0Yoonbai Kim1O-Kab Kwon2D. D. Tolla3Department of Physics, BK21 Physics Research Division, Institute of Basic Science, Sungkyunkwan UniversityDepartment of Physics, BK21 Physics Research Division, Institute of Basic Science, Sungkyunkwan UniversityDepartment of Physics, BK21 Physics Research Division, Institute of Basic Science, Sungkyunkwan UniversityDepartment of Physics, BK21 Physics Research Division, Institute of Basic Science, Sungkyunkwan UniversityAbstract We test the holographic relation between the vacuum expectation values of gauge invariant operators in $${\mathcal {N}} = 6$$ N = 6 U $$_k(N)\times \mathrm{U}_{-k}(N)$$ k ( N ) × U - k ( N ) mass-deformed ABJM theory and the LLM geometries with $${\mathbb {Z}}_k$$ Z k orbifold in 11-dimensional supergravity. To do so, we apply the Kaluza–Klein reduction to construct a 4-dimensional gravity theory and implement the holographic renormalization procedure. We obtain an exact holographic relation for the vacuum expectation values of the chiral primary operator with conformal dimension $$\Delta = 1$$ Δ = 1 , which is given by $$\langle {\mathcal {O}}^{(\Delta =1)}\rangle = N^{\frac{3}{2}} \, f_{(\Delta =1)}$$ ⟨ O ( Δ = 1 ) ⟩ = N 3 2 f ( Δ = 1 ) , for large N and $$k=1$$ k = 1 . Here the factor $$f_{(\Delta )}$$ f ( Δ ) is independent of N. Our results involve an infinite number of exact dual relations for all possible supersymmetric Higgs vacua and so provide a non-trivial test of gauge/gravity duality away from the conformal fixed point. We extend our results to the case of $$k\ne 1$$ k ≠ 1 for LLM geometries represented by rectangular-shaped Young diagrams. We also discuss the exact mapping of the gauge/gravity at finite N for classical supersymmetric vacuum solutions in field theory side and corresponding classical solutions in gravity side.http://link.springer.com/article/10.1140/epjc/s10052-017-4909-3
collection DOAJ
language English
format Article
sources DOAJ
author Dongmin Jang
Yoonbai Kim
O-Kab Kwon
D. D. Tolla
spellingShingle Dongmin Jang
Yoonbai Kim
O-Kab Kwon
D. D. Tolla
Exact holography of the mass-deformed M2-brane theory
European Physical Journal C: Particles and Fields
author_facet Dongmin Jang
Yoonbai Kim
O-Kab Kwon
D. D. Tolla
author_sort Dongmin Jang
title Exact holography of the mass-deformed M2-brane theory
title_short Exact holography of the mass-deformed M2-brane theory
title_full Exact holography of the mass-deformed M2-brane theory
title_fullStr Exact holography of the mass-deformed M2-brane theory
title_full_unstemmed Exact holography of the mass-deformed M2-brane theory
title_sort exact holography of the mass-deformed m2-brane theory
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2017-05-01
description Abstract We test the holographic relation between the vacuum expectation values of gauge invariant operators in $${\mathcal {N}} = 6$$ N = 6 U $$_k(N)\times \mathrm{U}_{-k}(N)$$ k ( N ) × U - k ( N ) mass-deformed ABJM theory and the LLM geometries with $${\mathbb {Z}}_k$$ Z k orbifold in 11-dimensional supergravity. To do so, we apply the Kaluza–Klein reduction to construct a 4-dimensional gravity theory and implement the holographic renormalization procedure. We obtain an exact holographic relation for the vacuum expectation values of the chiral primary operator with conformal dimension $$\Delta = 1$$ Δ = 1 , which is given by $$\langle {\mathcal {O}}^{(\Delta =1)}\rangle = N^{\frac{3}{2}} \, f_{(\Delta =1)}$$ ⟨ O ( Δ = 1 ) ⟩ = N 3 2 f ( Δ = 1 ) , for large N and $$k=1$$ k = 1 . Here the factor $$f_{(\Delta )}$$ f ( Δ ) is independent of N. Our results involve an infinite number of exact dual relations for all possible supersymmetric Higgs vacua and so provide a non-trivial test of gauge/gravity duality away from the conformal fixed point. We extend our results to the case of $$k\ne 1$$ k ≠ 1 for LLM geometries represented by rectangular-shaped Young diagrams. We also discuss the exact mapping of the gauge/gravity at finite N for classical supersymmetric vacuum solutions in field theory side and corresponding classical solutions in gravity side.
url http://link.springer.com/article/10.1140/epjc/s10052-017-4909-3
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