We construct supersymmetric field theories on Sp × S1 for p = 1,…,5. These spaces are the boundaries of the anti-de Sitter space in (p + 2)-dimensions. Thesetheories are invariant under the super extension of the anti-de Sitter group in (p + 2)-dimensions, whose bosonic subalgebra is SO(p + 1,2) asterisk in circle SO(N), for N = 1,2,4,8. The anti-de Sitter group SO(p + 1,2) acts as the conformal group on Sp × S1. We conjecture that these theories describe the super p-branes propagating in AdSp + 2 × SN−1. The internal space is always one of the parallelizable spheres, namely S1, S3 or S7
Generalizing the "The Membrane at the End of the Universe", a 1987 paper "Supersingletons" by Blenco...
We demonstrate the existence of singleton supermult iplets in Osp(N,4) for all N. These represent ex...
We present a geometric formulation of super p-brane theories in which the Wess-Zumino term is (p + 1...
We construct supersymmetric field theories on Sp × S1 for p = 1,…,5. These spaces are the boundaries...
We consider the inclusion of brane charges in AdS/sub 5/ superalgebras that contain the maximal cent...
Building on the superspace formulation for four-dimensional N = 2 matter-coupled supergravity develo...
We extend the results of arXiv:1401.1645 on the generalized conformal Sp(2n)-structure of infinite m...
We quantize the superstring on the AdS2 × S2 background with Ramond-Ramond flux using a PSU(1,1\2)/U...
The AdS/CFT transformation relates two nonlinear realizations of (super)conformal groups: their real...
We briefly review how to obtain N = 1, 2 Poincaré supergravity theories in four dimensions from the ...
We introduce some (anti-) M/D-branes through turning on the corresponding field strengths of the 11-...
AbstractWe consider partial spontaneous breaking of N=1 AdS4 supersymmetry OSp(1|4) down to N=1, d=3...
Conformal symmetry relates the metric on AdS(2) x S-1 to that of S-3. This implies that under a suit...
We quantize the N = 8 supersymmetric singleton field theory which is formulated on the boundary of t...
Abstract We study a one-parameter family of N $$ \mathcal{N} $$ = 2 anti-de Sitter vacua with U(1)2 ...
Generalizing the "The Membrane at the End of the Universe", a 1987 paper "Supersingletons" by Blenco...
We demonstrate the existence of singleton supermult iplets in Osp(N,4) for all N. These represent ex...
We present a geometric formulation of super p-brane theories in which the Wess-Zumino term is (p + 1...
We construct supersymmetric field theories on Sp × S1 for p = 1,…,5. These spaces are the boundaries...
We consider the inclusion of brane charges in AdS/sub 5/ superalgebras that contain the maximal cent...
Building on the superspace formulation for four-dimensional N = 2 matter-coupled supergravity develo...
We extend the results of arXiv:1401.1645 on the generalized conformal Sp(2n)-structure of infinite m...
We quantize the superstring on the AdS2 × S2 background with Ramond-Ramond flux using a PSU(1,1\2)/U...
The AdS/CFT transformation relates two nonlinear realizations of (super)conformal groups: their real...
We briefly review how to obtain N = 1, 2 Poincaré supergravity theories in four dimensions from the ...
We introduce some (anti-) M/D-branes through turning on the corresponding field strengths of the 11-...
AbstractWe consider partial spontaneous breaking of N=1 AdS4 supersymmetry OSp(1|4) down to N=1, d=3...
Conformal symmetry relates the metric on AdS(2) x S-1 to that of S-3. This implies that under a suit...
We quantize the N = 8 supersymmetric singleton field theory which is formulated on the boundary of t...
Abstract We study a one-parameter family of N $$ \mathcal{N} $$ = 2 anti-de Sitter vacua with U(1)2 ...
Generalizing the "The Membrane at the End of the Universe", a 1987 paper "Supersingletons" by Blenco...
We demonstrate the existence of singleton supermult iplets in Osp(N,4) for all N. These represent ex...
We present a geometric formulation of super p-brane theories in which the Wess-Zumino term is (p + 1...