Results 31 to 40 of about 30,767 (198)
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de Wit, Bernard, Louis, Jan
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A new duality between N $$ \mathcal{N} $$ = 8 superconformal field theories in three dimensions
We propose a new duality between two 3d N $$ \mathcal{N} $$ = 8 superconformal Chern-Simons-matter theories: the U(3)1 × U(3)−1 ABJM theory and a theory consisting of the product between the (SU(2)3 × SU(2)− 3)/ℤ2 BLG theory and a free N $$ \mathcal{N} $$
Nathan B. Agmon +2 more
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Supersymmetry and Dualities in Various Dimensions [PDF]
In these lectures we review how some of the recent developments in string theory are closely related to generic properties of supersymmetry. Lectures given at the Nato Advanced Study Institute on "Strings, Branes and Dualities", Cargese, May 26 - June 14, 1997.
de Wit, Bernard, Louis, Jan
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Duality in the Presence of Supersymmetry Breaking [PDF]
We study Seiberg duality for N=1 supersymmetric QCD with soft supersymmetry-breaking terms. We generate the soft terms through gauge mediation by coupling two theories related by Seiberg duality to the same supersymmetry-breaking sector.
Aharony +32 more
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Dualities of adjoint SQCD and supersymmetry enhancement
Abstract We propose a new dual description of four-dimensional $$ \mathcal{N} $$ N = 1 SU(N) gauge theory with one adjoint (X) and Nf fundamental matters with a superpotential W = TrXp+1. The dual theory consists of the $$ \mathcal{D} $$ D p[SU(N)] Argyres-Douglas
Kazunobu Maruyoshi +2 more
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Instantons on Young diagrams with matters
We present the unrefined instanton partition functions of various 5d gauge theories with matter beyond the fundamental representation as sums over Young diagrams.
Yanyan Chen +3 more
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R^2 Corrections and Non-perturbative Dualities of N=4 String ground states [PDF]
We compute and analyse a variety of four-derivative gravitational terms in the effective action of six- and four-dimensional type II string ground states with N=4 supersymmetry.
Gregori, A. +5 more
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N = (4,4) Supersymmetry and T-Duality [PDF]
A sigma model with four-dimensional target space parametrized by chiral and twisted chiral N =(2,2) superfields can be extended to N =(4,4) supersymmetry off-shell, but this is not true for a model of semichiral fields, where the N = (4,4) supersymmetry can only be realized on-shell. The two models can be related to each other by T-duality.
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The action with manifest E7 type symmetry
We generalize Cremmer-Julia 1st order action of N = 8 $$ \mathcal{N}=8 $$ supergravity with manifest E 7(7) symmetry to cases of N = 6 $$ \mathcal{N}=6 $$ with manifest SO∗(12) and N = 5 $$ \mathcal{N}=5 $$ with manifest SU(1, 5) duality symmetries ...
Renata Kallosh
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Unity of Supersymmetry Breaking Models [PDF]
We examine the models with gauge group U(1)^{k-1}\times\prod_{i=1}^k SU(n_i), which are obtained from decomposing the supersymmetry breaking model of Affleck, Dine and Seiberg containing an antisymmetric tensor field. We note that all of these models are
Affleck +21 more
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