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Related papers: Giant Magnons on CP^3 by Dressing Method

200 papers

A novel, nonperturbative, way to generate chiral symmetry breaking within the linear sigma model for 3 flavours is discussed. After spontaneous chiral symmetry breaking in the vacuum at the tree level the scalar nonet obtains mass, while…

High Energy Physics - Phenomenology · Physics 2009-10-30 Nils A. Tornqvist

A 5D SU(7) family unification model with two spinor representations of SO(14) is presented. The fifth dimension is compactified on $S^1/Z_2\times Z_2'$. The orbifolding is used to obtain 4D SO(10) chiral fermions. The 4D grand unification…

High Energy Physics - Phenomenology · Physics 2009-11-07 Kyuwan Hwang , Jihn E. Kim

We present a Grand Unified model based on SO(10) with a Delta(27) family symmetry. Fermion masses and mixings are fitted and agree well with experimental values. An extended seesaw mechanism plays a key role in the generation of the…

High Energy Physics - Phenomenology · Physics 2009-10-29 Federica Bazzocchi , Ivo de Medeiros Varzielas

We study the large N limit of SO(N) and Sp(N) Chern-Simons gauge theory on S^3 and identify its closed string dual as topological strings on an orientifold of the small resolution of the conifold. Applications to large N dualities for N=1…

High Energy Physics - Theory · Physics 2007-05-23 S. Sinha , C. Vafa

It is shown that type I seesaw models based on the standard model Lagrangian extended with three heavy Majorana right-handed fields do not have leptogenesis in leading order, if the symmetries of mass matrices are also the residual symmetry…

High Energy Physics - Phenomenology · Physics 2010-04-29 R. Gonzalez Felipe , H. Serodio

We consider the Pseudo-Gap (PG) state of high-$T_c$ superconductors in form of a composite order parameter fluctuating between 2$p_F$-charge ordering and superconducting (SC) pairing. In the limit of linear dispersion and at the hotspots,…

Superconductivity · Physics 2015-05-25 T. Kloss , X. Montiel , C. Pépin

The residual symmetry approach, along with a complex extension for some flavor invariance, is a powerful tool to uncover the flavor structure of the $3\times3$ neutrino Majorana mass matrix $M_\nu$ towards gaining insights into neutrino…

High Energy Physics - Phenomenology · Physics 2016-12-21 Rome Samanta , Probir Roy , Ambar Ghosal

We do not know why there are three fermion families in the Standard Model (SM), nor can we explain the observed pattern of fermion masses and mixing angles. Standard grand unified theories based on the SU(5) and SO(10) groups fail to shed…

High Energy Physics - Phenomenology · Physics 2020-12-16 Renato M. Fonseca

We present a complete, calculable, and phenomenologically viable model of dynamical supersymmetry breaking. The model is a simple extension of the so called 3-2 model, with gauge group SU(3)xSU(2)xG_SM and the MSSM fields directly coupled…

High Energy Physics - Phenomenology · Physics 2015-06-05 Francesco Caracciolo , Andrea Romanino

We perform a first-principles semi-classical computation of the one-loop corrections to the dispersion relation and S-matrix of Giant Magnons in AdS_5 x S^5 string theory. The results agree exactly with expectations based on the strong…

High Energy Physics - Theory · Physics 2009-04-30 Heng-Yu Chen , Nick Dorey , Rui F. Lima Matos

We present a 3-3-1 model as a subgroup of SU(4)PS X SU(4)L+R gauge symmetry with symmetry-breaking pattern SU(4)->SU(3) X U(1) for both SU(4) groups. A Pleitez-Frampton type of 3C-3L-1X model is obtained with charged heavy leptons and…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sutapa Sen , Aparna Dixit

We consider an inverse seesaw mechanism of neutrino mass generation in which the Standard Model is extended by $3+3$ (heavy) sterile states, and endowed with a flavour symmetry $G_f$, $G_f=\Delta (3 \, n^2)$ or $G_f=\Delta (6 \, n^2)$, and…

High Energy Physics - Phenomenology · Physics 2022-03-23 C. Hagedorn , J. Kriewald , J. Orloff , A. M. Teixeira

We construct the first three family N=1 supersymmetric string model with Standard Model gauge group SU(3)_C x SU(2)_L x U(1)_Y from an orientifold of type IIA theory on T^6/(Z_2 x Z_2) and D6-branes intersecting at angles. In addition to…

High Energy Physics - Theory · Physics 2008-11-26 Mirjam Cvetic , Gary Shiu , Angel M. Uranga

We review the role of R symmetries in models of supersymmetric unification in four and more dimensions, and in string theory. We show that, if one demands anomaly freedom and fermion masses, only R symmetries can forbid the supersymmetric…

High Energy Physics - Phenomenology · Physics 2015-06-12 Mu-Chun Chen , Maximilian Fallbacher , Michael Ratz

We investigate the spectrum of supersymmetric grand unification models based on the gauge groups SU(5), SO(10) and E6, paying particular attention to the first and second generation. We demonstrate how the measurement of the first or second…

High Energy Physics - Phenomenology · Physics 2015-06-11 D. J. Miller , A. P. Morais , P. N. Pandita

Flavour symmetries appropriate for describing a neutrino spectrum with degenerate solar pair and a third massive or massless neutrino are discussed. We demand that the required residual symmetries of the leptonic mass matrices be subgroups…

High Energy Physics - Phenomenology · Physics 2014-08-27 Anjan S. Joshipura , Ketan M. Patel

Based on the SO(3) gauge symmetry for three family leptons and general see-saw mechanism, we present a simple scheme that allows three nearly degenerate Majorana neutrino masses needed for hot dark matter. The vacuum structure of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yue-Liang Wu

In the present paper we extend to the massive case the procedure of divergences subtraction, previously introduced for the massless nonlinear sigma model (D=4). Perturbative expansion in the number of loops is successfully constructed. The…

High Energy Physics - Theory · Physics 2015-05-19 Ruggero Ferrari

In this paper we find giant magnon and single spike string solutions in a sector of the gamma-deformed conifold. We examine the dispersion relations and find a behavior analogous to the undeformed case. The transcendental functional…

High Energy Physics - Theory · Physics 2009-11-10 H. Dimov , M. Michalcik , R. C. Rashkov

We build a supersymmetric version with $SU(3)_C\otimes SU(2)_L\otimes U(1)_{Y^\prime}\otimes U(1)_{B-L}$ gauge symmetry, where $Y^\prime$ is a new charge and $B$ and $L$ are the usual baryonic and leptonic numbers. The model has three…

High Energy Physics - Phenomenology · Physics 2017-06-14 J. C. Montero , V. Pleitez , M. C. Rodriguez , B. L. Sánchez-Vega