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The $U(1)_{B-L}$ gauge symmetry is a promising extension of the standard model of particle physics, which is supposed to be broken at some high energy scale. Associated with the $U(1)_{B-L}$ gauge symmetry breaking, right-handed neutrinos…

High Energy Physics - Phenomenology · Physics 2018-09-28 Nobuchika Okada , Osamu Seto

We propose a simple testable model with mass generation mechanisms for dark matter and neutrino based on the gauged $U(1)_{B-L}$ symmetry and an exact $Z_2$ parity. The $U(1)_{B-L}$ symmetry is spontaneously broken at the TeV scale, by…

High Energy Physics - Phenomenology · Physics 2011-08-08 Shinya Kanemura , Osamu Seto , Takashi Shimomura

Recently we have proposed a renormalizable grand unified theory, based on the SU(5) gauge symmetry, where the neutrino masses are generated through the type I and type III seesaw mechanisms. In this letter we study the supersymmetric…

High Energy Physics - Phenomenology · Physics 2011-11-09 Pavel Fileviez Perez

We analyze the lepton sector of a Left-Right Model based on the gauge group SU(2)_L x SU(2)_R x U(1), concentrating mainly on neutrino properties. Using the seesaw mechanism and a horizontal symmetry, we keep the right-handed symmetry…

High Energy Physics - Phenomenology · Physics 2009-11-11 Ken Kiers , Michael Assis , David Simons , Alexey A. Petrov , Amarjit Soni

Formation of transitory domain walls is quite generic in theories with spontaneous breaking of discrete symmetries. Since these walls are in conflict with cosmology, there has to be some mechanism which makes them disappear. We study one…

High Energy Physics - Phenomenology · Physics 2012-11-07 Debasish Borah

We study the electroweak vacuum stability in Type I seesaw models for 3 generations of neutrinos in scenarios where the right-handed neutrinos have explicit bare mass terms in the Lagrangian and where these are dynamically generated through…

High Energy Physics - Phenomenology · Physics 2016-03-23 John Ng , Alejandro de la Puente

In supersymmetric models without $R$-parity neutrinos naturally become massive and mix with each other. We explore the predictions of a very restricted model with only three free parameters and find that this model naturally yields masses…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ralf Hempfling

The strong CP problem can be solved in Parity symmetric theories with electroweak gauge group containing $SU(2)_L \times SU(2)_R$ broken by the minimal Higgs content. Neutrino masses may be explained by adding the same number of gauge…

High Energy Physics - Phenomenology · Physics 2023-11-20 Lawrence J. Hall , Keisuke Harigaya , Yogev Shpilman

We present a comprehensive analysis of a supersymmetric $SO(10)$ Grand Unified Theory, which is broken to the Standard Model via the breaking of two intermediate symmetries. The spontaneous breaking of the first intermediate symmetry,…

High Energy Physics - Phenomenology · Physics 2024-04-01 Bowen Fu , Stephen F. King , Luca Marsili , Silvia Pascoli , Jessica Turner , Ye-Ling Zhou

In the LHC era the issue of the origin and nature of neutrino mass has attained a new meaning and a renewed importance. The growing success of the Higgs-Weinberg mechanism behind the charged fermion masses paves the way for the question of…

High Energy Physics - Phenomenology · Physics 2020-05-20 Goran Senjanovic , Vladimir Tello

In the Minimal Supersymmetric Standard Model with bilinear R-Parity violation, terms that violate R-Parity and lepton number are introduced in the superpotential, and sneutrino vacuum expectation values are induced. As a result, neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-07 Marco A. Diaz , Roberto A. Lineros , Maximiliano A. Rivera

$\mu\nu$SSM is an $R$-parity violating non-minimal supersymmetric model which uses right chiral neutrino superfields to solve the $\mu$-problem. The $R$-parity violation together with a TeV scale seesaw mechanism using right handed…

High Energy Physics - Phenomenology · Physics 2011-01-25 Pradipta Ghosh

We study gauge symmetry breaking patterns in supersymmetric gauge models defined on $M^4\times S^1$. Instead of utilizing the Scherk-Schwarz mechanism, supersymmetry is broken by bare mass terms for gaugino and squarks. Though the matter…

High Energy Physics - Theory · Physics 2009-11-10 Naoyuki Haba , Kazunori Takenaga , Toshifumi Yamashita

The neutrino masses are generated in grand unified theory (GUT) constrained supersymmetric model with R-parity violation. The neutrinos acquire masses via tree-level neutrino-neutralino mixing as well as via one-loop radiative corrections.…

High Energy Physics - Phenomenology · Physics 2009-11-10 Marek Gozdz , Wieslaw A. Kaminski , Fedor Simkovic

In the context of the left-right symmetric gauge group [SU(6)]$^3\times$ Z$_3$ which unifies nongravitational forces with flavors, we analyze the generational seesaw mechanism. At tree level we get…

High Energy Physics - Phenomenology · Physics 2009-08-26 William A. Ponce , Arnulfo Zepeda , Ricardo Gaitan Lozano

We construct SUSY $SU(3) \otimes SU(2)_{L} \otimes U(1)$ electroweak models with superweak R-parity. The scale of R-parity violation in one of the models is determined by the Majorana mass of neutrino and it is very small that leads to the…

High Energy Physics - Phenomenology · Physics 2009-10-28 N. V. Krasnikov

$R$-parity violating supersymmetric models (RPV SUSY) are becoming increasingly more appealing than its $R$-parity conserving counterpart in view of the hitherto non-observation of SUSY signals at the LHC. In this paper, we discuss RPV…

High Energy Physics - Phenomenology · Physics 2015-10-12 Vasiliki A. Mitsou

The spontaneous breakdown of the scale, the chiral and the superconformal symmetries for a hidden $SU(N)$ gauge group is studied in an effective lagrangean approach. The relevant low-energy degrees of freedom are taken to be the composite…

High Energy Physics - Phenomenology · Physics 2009-10-22 E. A. Dudas

We explore a mechanism of radiative B-L symmetry breaking in analogous to the radiative electroweak symmetry breaking. The breaking scale of B-L symmetry is related to the neutrino masses through the see-saw mechanism. Once we incorporate…

High Energy Physics - Phenomenology · Physics 2009-02-02 Tatsuru Kikuchi , Takayuki Kubo

In R parity violating supersymmetry (conserving baryon number B but violating lepton number L), Majorana neutrino masses may arise at tree level, in one loop, and in two loops. The L violating interactions work together with the B + L…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ernest Ma