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Lepton mixing, which requires physics beyond the Standard Model, is surprisingly compatible with a minimal, symmetryless and unbiased approach, called anarchy. This contrasts with highly involved flavor symmetry models. On the other hand,…

High Energy Physics - Phenomenology · Physics 2013-02-08 Julian Heeck , Werner Rodejohann

We present a TeV-scale left-right ultraviolet completion of type-I seesaw for neutrino masses based on the $SU(2)_L\times SU(2)_R\times U(1)_{B-L}$ gauge group without parity, which leads to "large" light-heavy neutrino mixing while keeping…

High Energy Physics - Phenomenology · Physics 2013-12-04 P. S. Bhupal Dev , Chang-Hun Lee , R. N. Mohapatra

We investigate the low-energy phenomenology of the Type-I seesaw mechanism within a 3+3 framework containing three active and three sterile neutrinos. Using the exact seesaw relation as a bridge between the high-scale sterile-sector…

High Energy Physics - Phenomenology · Physics 2026-03-30 Suka Sriyansu Pattanaik , Sasmita Mishra

We discuss a neutrino mass model based on the S_4 flavor symmetry within the minimal seesaw framework, in which only two right-handed neutrinos are introduced and transform as 2 under S_4. Although the model contains less free parameters…

High Energy Physics - Phenomenology · Physics 2015-03-19 Rui-Zhi Yang , He Zhang

In this paper, we make an attempt to combine the neutrino trimaximal (TM1 and TM2) mixings and $\mu$-$\tau$ reflection symmetry in the type-I seesaw model. Such a scenario is highly restrictive and predictive: in addition to three…

High Energy Physics - Phenomenology · Physics 2022-05-16 Zhen-hua Zhao

We propose a minimal predictive inverse seesaw model based on two right-handed neutrinos and two additional singlets, leading to the same low energy neutrino mass matrix as in the Littlest Seesaw (LS) (type I) model. In order to implement…

High Energy Physics - Phenomenology · Physics 2020-03-02 A. E. Cárcamo Hernández , S. F. King

In addition to three active neutrinos, one or more light sterile neutrinos have been conjectured to account for the LSND, MiniBooNE and reactor antineutrino anomalies (at the sub-eV mass scale) or for warm dark matter in the Universe (at…

High Energy Physics - Phenomenology · Physics 2013-05-30 Zhi-zhong Xing

The atmospheric and solar neutrino oscillation data suggest hierarchical neutrino masses with at least one large mixing. The simplest see-saw models for reconciling the two features are U(1) extensions of the SM with flavour dependent gauge…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. P. Roy

With just the Standard Model Higgs doublet, there are only three types of seesaw models that generate light Majorana neutrino masses at tree level after electroweak spontaneous symmetry breaking. However, if there exist additional TeV…

High Energy Physics - Phenomenology · Physics 2024-08-13 Alessio Giarnetti , Juan Herrero-Garcia , Simone Marciano , Davide Meloni , Drona Vatsyayan

We consider the seesaw mechanism of neutrino mass generation in the light of our present knowledge of the neutrino masses and mixing. We analyse the seesaw mechanism constrained by the following assumptions: (1) minimal seesaw with no Higgs…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Kh. Akhmedov , G. C. Branco , M. N. Rebelo

A model of neutrino oscillations is presented that has only three degrees of freedom and is consistent with existing data. The model is a subset of the renormalizable sector of the Standard-Model Extension (SME), and it offers an…

High Energy Physics - Phenomenology · Physics 2008-11-26 Teppei Katori , Alan Kostelecky , Rex Tayloe

Light sterile neutrinos of mass about an eV with mixing $\tilde U_{ls}$ of a few percent to active neutrinos may solve some anomalies shown in experimental data related to neutrino oscillation. How to have light sterile neutrinos is one of…

High Energy Physics - Phenomenology · Physics 2015-06-17 Xiao-Gang He , Wei Liao

Models of neutrino masses are discussed capable of explaining in a natural way the maximal mixing between $\nu_{\mu}$ and $\nu_{\tau}$ observed by the Super-Kamiokande collaboration. For three generations of leptons two classes of such…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Jezabek , Y. Sumino

As neutrino experiments are starting to probe the detailed structure of the neutrino mass matrix, we present sumrules relating its matrix elements for a class of models with approximate $L_e-L_{\mu}-L_{\tau}$ symmetry and the observables in…

High Energy Physics - Phenomenology · Physics 2015-06-25 H. S. Goh , R. N. Mohapatra , S. -P. Ng

Models of leptogenesis often invoke the out-of-equilibrium decays of heavy right-handed neutrinos in order to create a baryon asymmetry of the universe through the electroweak phase transition. Their presumed existence argues strongly for…

High Energy Physics - Phenomenology · Physics 2011-02-16 Ernest Ma , Subir Sarkar , Utpal Sarkar

The linear seesaw (LSS) model provides a natural framework for generating small neutrino masses at low energy scales, thereby offering promising testability prospects. However, in generic LSS models, the exact mass degeneracy (before the…

High Energy Physics - Phenomenology · Physics 2025-12-24 Yan Shao , Zhen-hua Zhao

A natural extension of the standard model to accommodate massive neutrinos is to introduce one Higgs triplet and three right-handed Majorana neutrinos, leading to a 6 \times6 neutrino mass matrix. We show that three light Majorana neutrinos…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei Chao , Shu Luo , Zhi-zhong Xing , Shun Zhou

The seesaw mechanism can play a key role in the generation of the leptonic mixing in unified models. We consider an unified model with a family symmetry and extended seesaw, and obtain viable fermion masses and mixing (leptonic mixing is…

High Energy Physics - Phenomenology · Physics 2015-05-14 Ivo de Medeiros Varzielas

It has been observed that simultaneous explanation of the solar and atmospheric neutrino deficits and the reported evidence for $\nu_{\mu}\to \nu_{e}$ oscillation from the Los Alamos Liquid Scintillator Detector (LSND) requires at least one…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. C. Gibbons , R. N. Mohapatra , S. Nandi , A. Raychaudhuri