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Related papers: Radiative Neutrino Masses in a SUSY GUT Model

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A radiatively-induced neutrino mass matrix with a simple structure is proposed on the basis of an SU(5) SUSY GUT model with R-parity violation. The model has matter fields $\bar{5}'_{L}+5'_{L}$ in addition to the ordinary matter fields…

High Energy Physics - Phenomenology · Physics 2017-08-23 Yoshio Koide

Within the framework of an SU(5) SUSY GUT model, a possible general form of the neutrino mass matrix induced by R-parity violation is investigated. The model has matter fields \bar{5}'_{L}+5'_{L} in addition to the ordinary matter fields…

High Energy Physics - Phenomenology · Physics 2009-11-10 Yoshio Koide

Within the framework of an SU(5) SUSY GUT model, a mechanism which effectively induces R-parity-violating terms below the unification energy scale M_X is proposed. The model has matter fields \bar{5}_{L(+)}+10_{L(-)} and Higgs fields…

High Energy Physics - Phenomenology · Physics 2014-11-17 Yoshio Koide , Joe Sato

The radiatively induced neutrino mass matrix is investigated on the basis of an SU(5) SUSY model. In order to evade the proton decay, an ansatz based on a discrete symmetry $Z_2$ is assumed: although, at the unification scale, we have two…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide , Joe Sato

In minimal SUSY GUT models the $R$-parity breaking terms are severely constrained by SU(5) gauge invariance. We consider the particular case where the explicit $R$-parity breaking occurs only via dimension 2 terms of the superpotential.…

High Energy Physics - Phenomenology · Physics 2009-10-28 Ralf Hempfling

In order to evade the proton decay which appears when the Zee model is embedded into a SUSY GUT scenario with R-parity violation, a new idea based on a discrete Z_2 symmetry is proposed. Under the symmetry Z_2, the quark and lepton mass…

High Energy Physics - Phenomenology · Physics 2009-09-29 Yoshio Koide , Ambar Ghosal

A mechanism of radiatively generating neutrino masses is implemented in an SU(2)_L x U(1)_Y x SU(2)'_L x U(1)'_Y model, where the first and second families respect SU(2)_L x U(1)_Y while SU(2)'_L x U(1)'_Y is specific for the third family.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yutaka Okamoto , Masaki Yasue

Gravity-mediated SUSY breaking models with R-parity conservation give rise to dark matter in the universe. I review neutralino dark matter in the minimal supergravity model (mSUGRA), models with non-universal soft SUSY breaking terms…

High Energy Physics - Phenomenology · Physics 2015-05-13 Howard Baer

An overview is given of the experimental neutrino mixing results and types of neutrino models proposed, with special attention to the general features of various GUT models involving intra-family symmetries and horizontal flavor symmetries.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Carl H. Albright

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 talk, RPV scenarios where…

High Energy Physics - Phenomenology · Physics 2015-07-31 Vasiliki A. Mitsou

Supersymmetric SU(5) GUT augmented with anomaly free U(1)_F flavor symmetry is presented. Very economical field content and U(1)_F charge assignment are obtained by specific construction. In particular, three families of 10+5* chiral…

High Energy Physics - Phenomenology · Physics 2015-03-13 Zurab Tavartkiladze

We compute one loop neutrino masses in the R-parity violating Minimal Supersymmetric Model, including the bilinear R-parity violating masses in the mass insertion approximation. To the order we calculate, our results are independent of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Sacha Davidson , Marta Losada

An R-parity violating SUSY model with lepton-number violating couplings $\lambda'_{i33}$, i=2,3 can generate a neutrino mass spectrum that explains the recent results from neutrino oscillation experiments. These R-parity violating couplings…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , T. Han , S. Hesselbach , D. Marfatia

We implement a symmetry violation guideline into a two-Higgs-doublet model embedded with three right-handed neutrinos, and exploit the generic Yukawa structures of the model via a hypothetical symmetry restoration of a global…

High Energy Physics - Phenomenology · Physics 2020-04-22 Shao-Ping Li , Xin-Qiang Li

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

$R$-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

CP violation, fermion masses and mixing angles including that of neutrinos are studied in an SUSY SO(10)$\times \Delta (48)\times$ U(1) model. The nonabelian SU(3) discrete family symmetry $\Delta(48)$ associated with a simple scheme of…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. C. Chou , Y. L. Wu

We study a prediction on neutrino observables in a non-supersymmetric renormalizable $SO(10)$ GUT model that contains a ${\bf 10}$ complex scalar field and a ${\bf 126}$ scalar field whose Yukawa couplings with ${\bf 16}$ matter fields…

High Energy Physics - Phenomenology · Physics 2023-04-19 Naoyuki Haba , Yasuhiro Shimizu , Toshifumi Yamada

We analyse the fermion masses and mixings in the flipped SU(5) model. The fermion mass matrices are evolved from the GUT scale down to $m_W$ by solving the renormalization group equations for the Yukawa couplings. The constraints imposed by…

High Energy Physics - Phenomenology · Physics 2010-11-01 G. K. Leontaris , J. D. Vergados

The electroweak unification group $G\equiv SU(2)_L\times U(1)_e\times U(1)_\mu\times U(1)_\tau$ in which each fermion multiplet has its own $U(1)$ factor was proposed in 1986 to get the neutrino mass matrix. In this paper, the gauge group G…

High Energy Physics - Phenomenology · Physics 2019-06-26 Fayyazuddin
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