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Manifestly supersymmetric formulation of eleven dimensional supergravity in the framework of light-cone approach is discussed.

High Energy Physics - Theory · Physics 2007-05-23 R. R. Metsaev

We investigate Supersymmetric models where neither R parity nor lepton number is imposed. Neutrino masses can be kept highly suppressed compared to the electroweak scale if the $\mu$-terms in the superpotential are aligned with the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Tom Banks , Yuval Grossman , Enrico Nardi , Yosef Nir

We discuss the general form of quadratic (1,1) supergravity in two dimensions, and show that this theory is equivalent to two scalar supermultiplets coupled to non-trivial supergravity. It is demonstrated that the theory possesses stable…

High Energy Physics - Theory · Physics 2009-10-28 Ahmed Hindawi , Burt A. Ovrut , Daniel Waldram

In recent work arXiv:1412.1715 it was shown how to modify Gell-Mann's proposal for identifying the 48 quarks and leptons of the Standard Model with the 48 spin-1/2 fermions of maximal SO(8) gauged supergravity that remain after the removal…

High Energy Physics - Theory · Physics 2015-07-02 Axel Kleinschmidt , Hermann Nicolai

We consider six-dimensional supergravity with gauge group $SO(10)\times U(1)_A$, compactified on the orbifold $T^2 / \mathbb{Z}_2$. Three quark-lepton generations arise as zero modes of a bulk $\bf16$-plet due to magnetic flux of the…

High Energy Physics - Theory · Physics 2015-10-14 Wilfried Buchmuller , Markus Dierigl , Fabian Ruehle , Julian Schweizer

We present a spontaneously broken N=2 supergravity model that reduces in the flat limit to a globally supersymmetric N=2 system with explicit soft supersymmetry breaking terms. These soft terms generate a mass O(100 GeV) for mirror quarks…

High Energy Physics - Theory · Physics 2010-12-16 L. Girardello , M. Porrati , A. Zaffaroni

In this talk I discuss the motivations for supersymmetry, focussing on models with broken R-parity and lepton number. After describing the main theoretical features of these models, I discuss some of the signals expected at colliders such…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. W. F. Valle

Two applications of the method of differential renormalization to supersymmetric gauge theories are reviewed. The photon propagator in supersymmetric QED is renormalized at one loop and the first supergravity contributions to the anomalous…

High Energy Physics - Phenomenology · Physics 2009-09-25 F. del Aguila , A. Culatti , R. Munoz-Tapia , M. Perez-Victoria

Following up on our earlier work where we showed how to amend a scheme originally proposed by M. Gell-Mann to identify the 48 spin 1/2 fermions of N=8 supergravity that remain after complete breaking of N=8 supersymmetry with the 3x16…

High Energy Physics - Theory · Physics 2018-09-12 Krzysztof A. Meissner , Hermann Nicolai

We investigate supersymmetric models where neither R-parity nor lepton number nor baryon number is imposed. The full high energy theory has an exact horizontal U(1) symmetry that is spontaneously broken. Quarks and Higgs fields carry…

High Energy Physics - Phenomenology · Physics 2014-11-17 Galit Eyal , Yosef Nir

We consider a covariant quantization of the D=11 massless superparticle in the supertwistor framework. D=11 supertwistors are highly constrained, but the interpretation of their bosonic components as Lorentz harmonic variables and their…

High Energy Physics - Theory · Physics 2007-05-23 Igor A. Bandos , Jose A. de Azcarraga , Dmtri P. Sorokin

A grand unified model based on SU(5) and supersymmetry is presented. Pairs of superfields belonging to 15 and 15* representations are newly introduced, while gauge coupling unification is satisfied. Improper mass relations in the minimal…

High Energy Physics - Phenomenology · Physics 2009-10-29 Noriyuki Oshimo

The recently proposed model of neutrino mass with no new physics beyond the TeV energy scale is shown to admit a natural and realistic supersymmetric realization, when combined with another recently proposed model of quark masses in the…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma

We review the structure of maximal $D=11$ and $D=10$ supergravities. Upon dimensional reduction, these theories give rise to the unique maximal supergravities in all lower spacetime dimensions $D<10$. In $D$ dimensions, maximal supergravity…

High Energy Physics - Theory · Physics 2023-11-17 Henning Samtleben

Light-cone gauge manifestly supersymmetric formulation of eleven dimensional supergravity is developed. The formulation is given entirely in terms of light cone scalar superfield, allowing us to treat all component fields on an equal…

High Energy Physics - Theory · Physics 2009-11-10 R. R. Metsaev

We demonstrate that a phenomenologically viable four-dimensional grand unified theory with no proton decay can be constructed. This is done in the framework of the minimal non-supersymmetric SU(5) GUT by introducing new representations and…

High Energy Physics - Phenomenology · Physics 2018-11-22 Bartosz Fornal , Benjamin Grinstein

A model in which quarks and leptons consist of three "more elementary" particles of spin 1/2 is proposed. A gauge field theory with SU(4) symmetry that corresponds to this model predicts the existence of two new bosons.

High Energy Physics - Phenomenology · Physics 2007-05-23 N. G. Marchuk

We recall the obstacles which seemed, long ago, to prevent one from viewing supersymmetry as a possible fundamental symmetry of Nature. Is spontaneous supersymmetry breaking possible ? Where is the spin-1/2 Goldstone fermion of…

High Energy Physics - Phenomenology · Physics 2016-11-23 Pierre Fayet

The complete supersymmetric action for eleven-dimensional supergravity is presented. The action is polynomial in the scalar fermionic pure spinor superfield, and contains only a minor modification to the recently proposed three-point…

High Energy Physics - Theory · Physics 2010-12-06 Martin Cederwall

A remarkable U(1) gauge extension of the supersymmetric standard model was proposed eight years ago. It is anomaly-free, has no mu term, and conserves baryon and lepton numbers automatically. The phenomenology of a specific version of this…

High Energy Physics - Phenomenology · Physics 2010-05-19 Ernest Ma
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