Results 61 to 70 of about 30,921 (232)
Ring Division Algebras, Self-Duality and Supersymmetry [PDF]
, 2000 Latex,PH.D ...
Khaled Abdel-Khalek
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Component d = 6 Born-Infeld theory with N = (2, 0) → N = (1, 0) supersymmetry breaking
Journal of High Energy Physics, 2019 The formalism of nonlinear realizations is used to construct a theory with 1/2 partial breaking of global supersymmetry with the N = (1, 0), d = 6 abelian vector multiplet as a Goldstone superfield.
Nikolay Kozyrev
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Journal of High Energy Physics, 2018 In N=5 $$ \mathcal{N}=5 $$, 6, 8 supergravities there are hidden symmetries of equations of motion, described by duality groups SU(1, 5), SO*(12), E 7(7) respectively.
Renata Kallosh +3 more
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Duality, Entropy and ADM Mass in Supergravity [PDF]
, 2009 We consider the Bekenstein-Hawking entropy-area formula in four dimensional extended ungauged supergravity and its electric-magnetic duality property.
Cerchiai, Bianca L. +3 more
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3D dualities and supersymmetry enhancement from domain walls [PDF]
Journal of High Energy Physics, 2019 Abstract We test recently proposed IR dualities and supersymmetry enhancement by studying the supersymmetry on domain walls. In the SU(3) Wess-Zumino model studied in [1, 2], we show that domain walls exhibit supersymmetry enhancement. This model was conjectured to be dual to an $$ \mathcal{N} $$
Martin Roček +2 more
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Three dimensional canonical singularity and five dimensional N $$ \mathcal{N} $$ = 1 SCFT
Journal of High Energy Physics, 2017 We conjecture that every three dimensional canonical singularity defines a five dimensional N $$ \mathcal{N} $$ = 1 SCFT. Flavor symmetry can be found from singularity structure: non-abelian flavor symmetry is read from the singularity type over one ...
Dan Xie, Shing-Tung Yau
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T-duality and the Worldvolume Solitons of Five-Branes and KK-Monopoles [PDF]
, 1997 We show that the fluxes of the various six-dimensional "gauge" theories are associated to below threshold bound states of D-branes with the NS-5-branes and KK-monopoles which preserve half of bulk supersymmetry. We then present the supergravity solutions
Bergshoeff +12 more
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Communications on Pure and Applied Mathematics, Volume 78, Issue 12, Page 2247-2304, December 2025.Abstract We consider a planar Coulomb gas ensemble of size N$N$ with the inverse temperature β=2$\beta =2$ and external potential Q(z)=|z|2−2clog|z−a|$Q(z)=|z|^2-2c \log |z-a|$, where c>0$c>0$ and a∈C$a \in \mathbb {C}$. Equivalently, this model can be realised as N$N$ eigenvalues of the complex Ginibre matrix of size (c+1)N×(c+1)N$(c+1) N \times (c+1)
Sung‐Soo Byun +2 more
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de Sitter Excited State in Heterotic E8×E8${\rm E}_8 \times {\rm E}_8$ Theory
Fortschritte der Physik, Volume 73, Issue 12, December 2025.Abstract A novel duality sequence is devised to study late‐time cosmology in the heterotic E8×E8${\rm E}_8 \times {\rm E}_8$ setup of Horava and Witten with dynamical walls that are moving towards each other. Remarkably, the dimensionally reduced 4‐dimensional theory does not violate NEC and no bouncing or ekpyrotic phase is observed.
Suddhasattwa Brahma +5 more
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JT gravity from non-Abelian T-duality
Journal of High Energy PhysicsWe study the geometries obtained by performing super non-Abelian T-duality of the Principal Chiral Model on OSp(1|2). While the initial model represents an appropriate 3D supergravity background, interpretable as the superspace version of AdS3, the T ...
Daniele Bielli +2 more
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