Author:
Honda Masazumi,Pang Yi,Zhu Yaodong
Abstract
Abstract
We study physical consequences of adding orientifolds to the ABJ triality, which is among 3d
$$ \mathcal{N}=6 $$
N
=
6
superconformal Chern-Simons theory known as ABJ theory, type IIA string in AdS
4 × ℂℙ3 and
$$ \mathcal{N}=6 $$
N
=
6
supersymmetric (SUSY) Vasiliev higher spin theory in AdS
4. After adding the orientifolds, it is known that the gauge group of the ABJ theory becomes O(N
1) × USp(2N
2) while the background of the string theory is replaced by AdS
4 × ℂℙ3/Z
2, and the supersymmetries in the both theories reduce to
$$ \mathcal{N}=5 $$
N
=
5
. We propose that adding the orientifolds to the
$$ \mathcal{N}=6 $$
N
=
6
Vasiliev theory leads to
$$ \mathcal{N}=5 $$
N
=
5
SUSY Vasiliev theory. It turns out that the
$$ \mathcal{N}=5 $$
N
=
5
case is more involved because there are two formulations of the
$$ \mathcal{N}=5 $$
N
=
5
Vasiliev theory with either O or USp internal symmetry. We show that the two
$$ \mathcal{N}=5 $$
N
=
5
Vasiliev theories can be understood as certain projections of the
$$ \mathcal{N}=6 $$
N
=
6
Vasiliev theory, which we identify with the orientifold projections in the Vasiliev theory. We conjecture that the O(N
1) × USp(2N
2) ABJ theory has the two vector model like limits: N
2 ≫ N
1 and N
1 ≫ N
2 which correspond to the semi-classical
$$ \mathcal{N}=5 $$
N
=
5
Vasiliev theories with O(N
1) and USp(2N
2) internal symmetries respectively. These correspondences together with the standard AdS/CFT correspondence comprise the ABJ quadrality among the
$$ \mathcal{N}=5 $$
N
=
5
ABJ theory, string/M-theory and two
$$ \mathcal{N}=5 $$
N
=
5
Vasliev theories. We provide a precise holographic dictionary for the correspondences by comparing correlation functions of stress tensor and flavor currents. Our conjecture is supported by various evidence such as agreements of the spectra, one-loop free energies and SUSY enhancement on the both sides. We also predict the leading free energy of the
$$ \mathcal{N}=5 $$
N
=
5
Vasiliev theory from the CFT side. As a byproduct, we give a derivation of the relation between the parity violating phase in the
$$ \mathcal{N}=6 $$
N
=
6
Vasiliev theory and the parameters in the
$$ \mathcal{N}=6 $$
N
=
6
ABJ theory, which was conjectured in [1].
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
Reference107 articles.
1. C.-M. Chang, S. Minwalla, T. Sharma and X. Yin, ABJ triality: from higher spin fields to strings, J. Phys. A 46 (2013) 214009 [arXiv:1207.4485] [INSPIRE].
2. D.J. Gross, High-energy symmetries of string theory, Phys. Rev. Lett. 60 (1988) 1229 [INSPIRE].
3. M.A. Vasiliev, Nonlinear equations for symmetric massless higher spin fields in (A)dS
d, Phys. Lett. B 567 (2003) 139 [hep-th/0304049] [INSPIRE].
4. A. Sagnotti, Notes on strings and higher spins, J. Phys. A 46 (2013) 214006 [arXiv:1112.4285] [INSPIRE].
5. M.R. Gaberdiel and R. Gopakumar, Stringy symmetries and the higher spin square, J. Phys. A 48 (2015) 185402 [arXiv:1501.07236] [INSPIRE].
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