Results 31 to 40 of about 333 (139)
Supersymmetry Laser Arrays with High‐Order Exceptional Point
Advanced Photonics Research, Volume 4, Issue 9, September 2023., 2023 The concept of supersymmetry and parity‐time symmetry broken are combined to build a laser array, working at visible range, with mode control capability, small volume, expandability, and simplicity. It also works as a high‐order sensing device for weak perturbation.
Guodong Liu +9 more
wiley +1 more source
On the Role of Torsion and Higher Forms in Off‐Shell Supergravity
Fortschritte der Physik, Volume 71, Issue 8-9, September 2023., 2023 Abstract The presence of a nonvanishing totally antisymmetric (super)torsion, equivalent to an axial vector, and higher forms in the “new minimal” and “old minimal” off‐shell formulations of N=1$\mathcal {N}=1$, D=4$D=4$ supergravity is elaborated. The geometric superspace approach and study both the geometric Lagrangian and the off‐shell closure of ...
Lucrezia Ravera
wiley +1 more source
Optical Transitions and Nonreciprocity in Spatio‐Temporally Periodic Layers of Spherical Particles
Advanced Optical Materials, Volume 11, Issue 12, June 19, 2023., 2023 High‐refractive‐index dielectric particles, arranged periodically in space and also modulated periodically in time, exhibit intriguing nonreciprocal optical properties, which result from strong inelastic scattering occurring in the triple‐resonance regime.
Emmanouil Panagiotidis +3 more
wiley +1 more source
Sparticle spectroscopy and electroweak symmetry breaking with gauge-mediated supersymmetry breaking [PDF]
Nuclear Physics B, 1997 The phenomenology associated with gauge-mediated supersymmetry breaking is presented. A renormalization group analysis of the minimal model is performed in which the constraints of radiative electroweak symmetry breaking are imposed. The resulting superpartner and Higgs boson spectra are highly correlated and depend on only a few parameters ...
Dimopoulos, Savas +2 more
openaire +2 more sources
On the BPS Sector in AdS3/CFT2 Holography
Fortschritte der Physik, Volume 71, Issue 4-5, May 2023., 2023 Abstract The BPS sector in AdS3/CFT2$AdS_3/CFT_2$ duality has been fertile ground for the exploration of gauge/gravity duality, from the match between black hole entropy and the CFT elliptic genus to the construction of large families of geometrical microstates and the identification of the corresponding states in the CFT.
Emil J. Martinec +2 more
wiley +1 more source
Supersymmetry breaking in disordered systems and relation to functional renormalization and replica-symmetry breaking [PDF]
Journal of Physics: Condensed Matter, 2005 In this article, we study an elastic manifold in quenched disorder in the limit of zero temperature. Naively it is equivalent to a free theory with elasticity in Fourier-space proportional to k^4 instead of k^2, i.e. a model without disorder in two space-dimensions less.
Kay Jörg Wiese
openalex +5 more sources
Mixed mediation of supersymmetry breaking with anomalous U(1) gauge symmetry [PDF]
Journal of High Energy Physics, 2011 Models with anomalous U(1) gauge symmetry contain various superfields which can have nonzero supersymmetry breaking auxiliary components providing the origin of soft terms in the visible sector, e.g. the U(1) vector superfield, the modulus or dilaton superfield implementing the Green-Schwarz anomaly cancellation mechanism, U(1)-charged but standard ...
Kiwoon Choi +3 more
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MINIMALITY AND SUPERSYMMETRY - DYNAMICAL SYMMETRY BREAKING THROUGH PREONS
Le Journal de Physique Colloques, 1982 No abstract ...
Jogesh C. Pati
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Supersymmetry breaking and moduli stabilization with anomalous U(1) gauge symmetry [PDF]
Journal of High Energy Physics, 2006 32 pages; references are ...
Kiwoon Choi, Kwang-Sik Jeong
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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
wiley +1 more source