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Related papers: A Lepton-specific Universal Seesaw Model with Left…

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To generate the lepton and quark masses in the left-right symmetric models, we can consider a universal seesaw scenario by integrating out heavy fermion singlets which have the Yukawa couplings with the fermion and Higgs doublets. The…

High Energy Physics - Phenomenology · Physics 2011-03-21 Pei-Hong Gu , Manfred Lindner

We study the implications for leptogenesis in a class of left-right symmetric model, where all fermion masses are induced through the Universal Seesaw mechanism. Unlike conventional analyses, we do not use the decays of the neutrino…

High Energy Physics - Phenomenology · Physics 2025-12-24 K. S. Babu , Maximilian Berbig , Srubabati Goswami , Drona Vatsyayan

We propose a low scale renormalizable left-right symmetric theory that successfully explains the observed SM fermion mass hierarchy, the tiny values for the light active neutrino masses and is consistent with the lepton and baryon…

High Energy Physics - Phenomenology · Physics 2022-03-02 A. E. Cárcamo Hernández , Ivan Schmidt

We extend the Type I seesaw and suggest a $new$ seesaw mechanism to generate neutrino masses within the left-right symmetric theories where parity is spontaneously broken. We construct a next to minimal left-right symmetric model where…

High Energy Physics - Phenomenology · Physics 2014-11-21 Joydeep Chakrabortty

A left-right model of quarks and leptons based on the gauge group $SU(3)_c \times SU(2)_L \times SU(2)_R \times U(1)_{B-L}$ is studied. Here the scalar sector consists of only two doublets namely (1,2,1,1) and (1,1,2,1) but familiar…

High Energy Physics - Phenomenology · Physics 2007-05-23 Biswajoy Brahmachari

We present a general framework for models in which the lepton mixing matrix is the product of the maximal mixing matrix U_\omega\ times a matrix constrained by a well-defined Z_2 symmetry. Our framework relies on neither supersymmetry nor…

High Energy Physics - Phenomenology · Physics 2015-06-17 W. Grimus , L. Lavoura

We build a supersymmetric model with $SU(2)_{L}\otimes SU(2)_{R}\otimes U(1)_{(B-L)}$ electroweak gauge symmetry, where $SU(2)_{L}$ is the left-handed currents while $SU(2)_{R}$ is the right-handed currents and $B$ and $L$ are the usual…

High Energy Physics - Phenomenology · Physics 2021-05-14 M. C. Rodriguez

We propose a left-right model of quarks and leptons based on the gauge group $SU(3)_C \times SU(2)_L \times SU(2)_R \times U(1)_{B-L}$, where the scalar sector consists of only two doublets: (1,2,1,1) and (1,1,2,1). As a result, any fermion…

High Energy Physics - Phenomenology · Physics 2009-11-10 Biswajoy Brahmachari , Ernest Ma , Utpal Sarkar

We systematically construct realistic mass matrices for the type-I seesaw mechanism out of more than 20 trillion possibilities. We use only very generic assumptions from extended quark-lepton complementarity, i.e., the leptonic mixing…

High Energy Physics - Phenomenology · Physics 2008-11-26 Florian Plentinger , Gerhart Seidl , Walter Winter

We show how the use of a see-saw mechanism based on a $3 \times 3$ neutrino mass matrix texture can considerably simplify Higgs sectors for quark-lepton symmetric models (and for Standard Model extensions generally). The main theory we…

High Energy Physics - Phenomenology · Physics 2009-10-28 R. Foot , R. R. Volkas

Instead of anchoring the seesaw mechanism with the conventional heavy right-handed neutrino singlet, a small Majorana neutrino mass may be obtained just as well with the addition of a heavy triplet of leptons per family to the minimal…

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

In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the exception of neutrino masses. The hierarchies and apparent regularities among the quark and lepton masses are, however, otherwise a mystery.…

High Energy Physics - Phenomenology · Physics 2022-11-07 Sudip Jana , Sophie Klett , Manfred Lindner

Recently, it was shown in arXiv:1512.06742 that a straightforward implementation of the type I seesaw mechanism in a warped extra dimensional framework is in reality a {\em natural} realization of "inverse" seesaw, i.e., the Standard Model…

High Energy Physics - Phenomenology · Physics 2018-05-02 Kaustubh Agashe , Peizhi Du , Sungwoo Hong

Instead of right-handed neutrino singlets, the standard model is extended to include lepton triplets $(\Sigma^+, \Sigma^0, \Sigma^-)$. Each quark and lepton family may now transform under an anomaly-free $U(1)_X$ gauge symmetry, known…

High Energy Physics - Phenomenology · Physics 2021-03-17 Ernest Ma

Successful leptogenesis within the conventional TeV-scale left-right implementation of type-I seesaw has been shown to require that the mass of the right-handed $W_R^\pm$ boson should have a lower bound much above the reach of the Large…

High Energy Physics - Phenomenology · Physics 2018-04-18 Pei-Hong Gu , Rabindra N. Mohapatra

Stimulated by the phenomenological success of the universal seesaw mass matrix model, where the mass terms for quarks and leptons f_i (i=1,2,3) and hypothetical super-heavy fermions F_i are given by \bar{f}_L m_L F_R +\bar{F}_L m_R f_R +…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yoshio Koide

Observation of non-zero neutrino masses at a scale $\sim 10^{-1} - 10^{-2}$ eV is a major problem in the otherwise highly successful Standard Model. The most elegant mechanism to explain such tiny neutrino masses is the seesaw mechanism…

High Energy Physics - Phenomenology · Physics 2016-02-10 S. Chakdar , K. Ghosh , V. Hoang , P. Q. Hung , S. Nandi

We investigate the collider signatures of the minimal framework for quark-lepton unification at a scale not far from the electroweak symmetry breaking scale. This theory predicts a rich spectrum of new fields, including one vector…

High Energy Physics - Phenomenology · Physics 2026-03-31 Jon Butterworth , Hridoy Debnath , Pavel Fileviez Perez , Peng Wang

We enlarge the lepton sector of the Standard Model by adding to it two right-handed neutrino singlets, and propose a model based on the seesaw mechanism and on the lepton number $\bar L = L_e - L_\mu - L_\tau$. The model is innovative from…

High Energy Physics - Phenomenology · Physics 2009-10-31 L. Lavoura , W. Grimus

We show that solutions for the masses and mixings of the quarks and leptons based on a $U(1)\times Z_2$ horizontal symmetry are possible. The seesaw mechanism is shown to work consistently in the presence of the discrete symmetry. The…

High Energy Physics - Phenomenology · Physics 2009-10-31 Micheal S. Berger , Kim Siyeon
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