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research
Mass-deformed ABJM Theory and LLM Geometries: Exact Holography
Authors
Dongmin Jang
Yoonbai Kim
O-Kab Kwon
D. D. Tolla
Publication date
16 March 2017
Publisher
'Springer Science and Business Media LLC'
Doi
View
on
arXiv
Abstract
We present a detailed account and extension of our claim in arXiv:1610.01490. We test the gauge/gravity duality between the
N
=
6
{\cal N} = 6
N
=
6
mass-deformed ABJM theory with U
k
(
N
)
Γ
_k(N)\times
k
β
(
N
)
Γ
U
β
k
(
N
)
_{-k}(N)
β
k
β
(
N
)
gauge symmetry and the 11-dimensional supergravity on LLM geometries with SO(4)/
Z
k
{\mathbb Z}_k
Z
k
β
Γ
\times
Γ
SO(4)/
Z
k
{\mathbb Z}_k
Z
k
β
isometry, in the large
N
N
N
limit. Our analysis is based on the evaluation of vacuum expectation values of chiral primary operators from the supersymmetric vacua of mass-deformed ABJM theory and from the implementation of Kaluza-Klein holography to the LLM geometries. We focus on the chiral primary operator with conformal dimension
Ξ
=
1
\Delta = 1
Ξ
=
1
. We show that
β¨
O
(
Ξ
=
1
)
β©
=
N
3
2
β
f
(
Ξ
=
1
)
\langle {\cal O}^{(\Delta=1)}\rangle= N^{\frac32} \, f_{(\Delta=1)}
β¨
O
(
Ξ
=
1
)
β©
=
N
2
3
β
f
(
Ξ
=
1
)
β
for all supersymmetric vacuum solutions and LLM geometries with
k
=
1
k=1
k
=
1
, where the factor
f
(
Ξ
)
f_{(\Delta)}
f
(
Ξ
)
β
is independent of
N
N
N
. We also confirm that the vacuum expectation value of the the energy momentum tensor is vanishing as expected by the supersymmetry. We extend our results to the case of
k
β
1
k\ne 1
k
ξ
=
1
for LLM geometries represented by rectangular-shaped Young-diagrams. In analogy with the Coulomb branch of the
N
=
4
{\cal N} = 4
N
=
4
super Yang-Mills theory, we argue that the discrete Higgs vacua of the mABJM theory as well as the corresponding LLM geometries are parametrized by the vevs of the chiral primary operators.Comment: 44 pages, 1 figure, major corrections in section 3 and 5, references added, title change
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Last time updated on 04/06/2019