ID: hep-th/9811010

N=8 SCFT and M Theory on AdS_4 x RP^7

November 2, 1998

View on ArXiv
Changhyun Ahn, Hoil Kim, Bum-Hoon Lee, Hyun Seok Yang
High Energy Physics - Theory

We study M theory on $AdS_4 \times \RP^7$ corresponding to 3 dimensional ${\cal N}=8$ superconformal field theory which is the strong coupling limit of 3 dimensional super Yang-Mills theory. For SU(N) theory, a wrapped M5 brane on $\RP^5$ can be interpreted as baryon vertex. For $SO(N)/Sp(2N)$ theory, by using the property of (co-)homology of $\RP^7$, we classify various wrapping branes and consider domain walls and the baryon vertex.

Similar papers 1

SO(2N) (0,2) SCFT and M Theory on $AdS_7 \times {RP}^4$

August 30, 1998

93% Match
Changhyun Ahn, Hoil Kim, Hyun Seok Yang
High Energy Physics - Theory

We study M theory on $AdS_7 \times \RP^4$ corresponding to 6 dimensional SO(2N) $(0, 2)$ superconformal field theory on a circle which becomes 5 dimensional super Yang-Mills theory at low energies. For SU(N) (0,2) theory, a wrapped D4 brane on $\S^4$ which is connected to a D4 brane on the boundary of $AdS_7$ by N fundamental strings can be interpreted as baryon vertex. For SO(2N) (0,2) theory, by using the property of homology of $\RP^4$, we classify various wrapping branes....

Find SimilarView on arXiv

N=2 SCFT and M Theory on AdS_4 x Q^{1,1,1}

August 25, 1999

89% Match
Changhyun Ahn
High Energy Physics - Theory

Coincident M2 branes at a conical singularity are related to M theory on AdS_4 x X_7 for an appropriate 7 dimensional Sasaki-Einstein manifold X_7. For X_7=Q^{1,1,1}=(SU(2) x SU(2) x SU(2))/(U(1) x U(1)) which was found sometime ago, the infrared limit of the theory on N M2 branes was constructed recently. It is the SU(N) x SU(N) x SU(N) gauge theories with three series of chiral fields A_i, i=1,2 transforming in the (N, \bar{N},1) representation, B_j, j=1,2 transforming in t...

Find SimilarView on arXiv

On N=8 Supergravity on $AdS_5$ and N=4 Superconformal Yang-Mills theory

February 27, 1998

88% Match
Sergio Ferrara, Christian Fronsdal, Alberto Zaffaroni
High Energy Physics - Theory

We discuss the spectrum of states of IIB supergravity on $AdS_5\times S^5$ in a manifest $SU(2,2/4)$ invariant setting. The boundary fields are described in terms of N=4 superconformal Yang-Mills theory and the proposed correspondence between supergravity in $AdS_5$ and superconformal invariant singleton theory at the boundary is formulated in an N=4 superfield covariant language.

Find SimilarView on arXiv

M5-branes and Wilson Surfaces in AdS$_{7}$/CFT$_{6}$ Correspondence

April 3, 2014

87% Match
Hironori Mori, Satoshi Yamaguchi
High Energy Physics - Theory

We study AdS$_{7}$/CFT$_{6}$ correspondence between M-theory on AdS$_{7} \times S^{4}$ and the 6D $\mathcal{N} = (2,0)$ superconformal field theory. In particular we focus on Wilson surfaces. We use the conjecture that the (2,0) theory compactified on $S^{1}$ is equivalent to the 5D maximal super Yang-Mills (MSYM) and Wilson surfaces wrapping this $S^1$ correspond to Wilson loops in 5D MSYM. The Wilson loops in 5D MSYM obtained by the localization technique result in the Cher...

Find SimilarView on arXiv

Orbifolds AdS_7xS^4 and Six Dimensional (0, 1) SCFT

April 14, 1998

87% Match
Changhyun Ahn, Kyungho Oh, Radu Tatar
High Energy Physics - Theory

We analyze the relation between the large N limit of 6 dimensional superconformal field theories with eight supercharges and M theory on orbifolds of AdS_7xS^4. We use the known spectrum of Kaluza-Klein harmonics of supergravity on AdS_7xS^4 and we take their orbifold projection to get information about the chiral primary operators of 6 dimensional SCFT which is realized on the worldvolume of M5 brane sitting at the orbifold singularities.

Find SimilarView on arXiv

Four-Dimensional SCFTs from M5-Branes

March 1, 2012

86% Match
Ibrahima Bah, Christopher Beem, ... , Wecht Brian
High Energy Physics - Theory

We engineer a large new set of four-dimensional N=1 superconformal field theories by wrapping M5-branes on complex curves. We present new supersymmetric AdS_5 M-theory backgrounds which describe these fixed points at large N, and then directly construct the dual four-dimensional CFTs for a certain subset of these solutions. Additionally, we provide a direct check of the central charges of these theories by using the M5-brane anomaly polynomial. This is a companion paper which...

Find SimilarView on arXiv

Baryons and Domain Walls in an N = 1 Superconformal Gauge Theory

August 12, 1998

85% Match
Steven S. Gubser, Igor R. Klebanov
High Energy Physics - Theory

Coincident D3-branes placed at a conical singularity are related to string theory on $AdS_5\times X_5$, for a suitable five-dimensional Einstein manifold $X_5$. For the example of the conifold, which leads to $X_5=T^{1,1}=(SU(2)\times SU(2))/U(1)$, the infrared limit of the theory on $N$ D3-branes was constructed recently. This is ${\cal N}=1$ supersymmetric $SU(N)\times SU(N)$ gauge theory coupled to four bifundamental chiral superfields and supplemented by a quartic superpo...

Find SimilarView on arXiv

Branes, Orbifolds and the Three Dimensional ${\cal N} = 2$ SCFT in the Large N limit

June 4, 1998

85% Match
Changhyun Ahn, Kyungho Oh, Radu Tatar
High Energy Physics - Theory

We study the correspondence between the large $N$ limit of ${\cal N} = 2$ three dimensional superconformal field theories and M theory on orbifolds of $AdS_4 \times {\bf S^7}$. We identify the brane configuration which gives $C^3/Z_3$ as a background for the M theory in terms of a Brane Box Model or a (p, q) web model. By taking the orbifold projection on the known spectrum of Kaluza-Klein harmonics of supergravity, we obtain information about the chiral primary operators a...

Find SimilarView on arXiv

N = 2 SCFTs: An M5-brane perspective

January 6, 2010

85% Match
Bin Chen, Eoin Ó. Colgáin, ... , Yavartanoo Hossein
High Energy Physics - Theory

Inspired by the recently discovered holographic duality between N=2 SCFTs and half-BPS M-theory backgrounds, we study probe M5-branes. Though our main focus is supersymmetric M5-branes whose worldvolume has an AdS_n factor, we also consider some other configurations. Of special mention is the identification of AdS_5 and AdS_3 probes preserving supersymmetry, with only the latter supporting a self-dual field strength.

Find SimilarView on arXiv

M Theory on AdS_p x S^{11-p} and Superconformal Field Theories

March 5, 1998

85% Match
Ofer Aharony, Yaron Oz, Zheng Yin
High Energy Physics - Theory

We study the large N limit of the interacting superconformal field theories associated with N M5 branes or M2 branes using the recently proposed relation between these theories and M theory on AdS spaces. We first analyze the spectrum of chiral operators of the 6d (0,2) theory associated with M5 branes in flat space, and find full agreement with earlier results obtained using its DLCQ description as quantum mechanics on a moduli space of instantons. We then perform a similar ...

Find SimilarView on arXiv