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Related papers: Lower Bounds on U_{e3}

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The neutrino mixing matrix U is in general of the form U=U_e^+ U_nu, where U_e arises from the diagonalization of charged leptons and U_nu is from the neutrino sector. We discuss the possibility that U_nu is nearly diagonal (in the…

High Energy Physics - Phenomenology · Physics 2010-04-05 Guido Altarelli , Ferruccio Feruglio , Isabella Masina

In the absence of a tree-level scalar-field mass, renormalization-group methods permit the explicit summation of leading-logarithm contributions to all orders of the perturbative series within the effective potential for $SU(2)\times U(1)$…

High Energy Physics - Phenomenology · Physics 2009-11-10 V. Elias , R. B. Mann , D. G. C. McKeon , T. G. Steele

The R-symmetry formalism is applied for the supersymmetric SU(3)_C X SU(3)_L X U(1)_X (3-3-1) model with right-handed neutrinos. For this kind of models, we study generalization of the MSSM relation among R-parity, spin and matter-parity.…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. V. Dong , D. T. Huong , M. C. Rodriguez , H. N. Long

We study the neutrino sector in a minimal $SU(3)_L\times U(1)_X$ model, in which its mass is generated at one-loop level with the charged lepton mass, and hence there exists a strong correlation between the charged-lepton mass and the…

High Energy Physics - Phenomenology · Physics 2016-04-20 Hiroshi Okada , Nobuchika Okada , Yuta Orikasa

We consider an effective theory with an $SU(2)\times U(1)\times A_{4}\times Z_{2}\times Z_{4}$ symmetry and investigate the possibility of a linking TeV-leptogenesis with a reactor angle $|U_{e3}|$ through spontaneous $A_{4}$ symmetry…

High Energy Physics - Phenomenology · Physics 2010-05-25 Y. H. Ahn , Chian-Shu Chen

The quasi-degeneracy of heavier sterile neutrino masses in the Neutrino Minimal Standard Model ($\nu$MSM) facilitates the production of lepton asymmetry below the electroweak scale. The first order loop corrections to this mass-difference…

High Energy Physics - Phenomenology · Physics 2010-06-22 Ananda Roy

One of the outstanding issues in neutrino physics is the experimental determination of the neutrino mass hierarchy: Is the order of the neutrino masses ``normal'' - m_1^2<m_2^2<m_3^2 - or is it inverted - m_3^2<m_1^2<m_2^2, with m_2^2-m_1^2…

High Energy Physics - Phenomenology · Physics 2007-05-23 Andre de Gouvea , James Jenkins

In the presence of extra neutrino states at high scales, the low-energy effective $3\times 3$ leptonic mixing matrix (LMM) is in general nonunitary. We revisit the question of what is our current knowledge of individual LMM matrix elements…

High Energy Physics - Phenomenology · Physics 2024-03-06 Daniel Aloni , Avital Dery

We show that the assumption of type II seesaw mechanism for small neutrino masses coupled with $b-\tau$ mass unification in a minimal SUSY SO(10) model leads not only to a natural understanding of large atmospheric mixing angle…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. S. Goh , R. N. Mohapatra , Siew-Phang Ng

Recent developments in thermal leptogenesis are reviewed. Neutrino mixing data favor a simple picture where the matter-anti matter asymmetry is generated by the decays of the heavy RH neutrinos mildly close to thermal equilibrium and,…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Di Bari

The MNS matrix structure emerging as a result of recent neutrino measurements strongly suggests two large mixing angles (solar and atmospheric) and one small angle (|U_e3| << 1). Especially when combined with the neutrino mass hierarchy,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Richard F. Lebed , Daniel R. Martin

If the neutrino mass spectrum turns out to be m^{}_3 < m^{}_1 < m^{}_2, one may choose to relabel it as m^{\prime}_1 < m^{\prime}_2 < m^{\prime}_3 such that all the masses of fundamental fermions with the same electrical charges are in…

High Energy Physics - Phenomenology · Physics 2018-01-17 Zhi-zhong Xing , Jing-yu Zhu

We propose a model which uses the seesaw mechanism and the lepton number $\bar L = L_e - L_\mu - L_\tau$ to achieve the neutrino mass spectrum $m_1 = m_2$ and $m_3 = 0$, together with a lepton mixing matrix $U$ with $U_{e3} = 0$. In this…

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

Current solar and atmospheric neutrino oscillation data seem to favor a bimaximal pattern for neutrino mixings where the matrix elements U_{e2} and U_{\mu 3} are of order one, while U_{e3} is much smaller. We show that such a pattern can be…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr

We study the effects of breaking S3 symmetry in the neutrino mass matrix for the masses and mixing matrix of neutrinos. At zeroth order the model gives degenerate neutrino masses and accommodates tribimaximal mixing. We introduce…

High Energy Physics - Phenomenology · Physics 2012-02-16 S. Dev , Radha Raman Gautam , Lal Singh

In short-baseline experiments such as LSND and MiniBooNE, an excess of electron neutrinos has been observed, originating from a muon neutrino beam. To address this anomaly, in the line of many works, we investigate various neutrino mixing…

High Energy Physics - Phenomenology · Physics 2026-03-06 Priya , Simran Arora , B. C. Chauhan

Correlations between light neutrino observables are arguably the strongest predictions of lepton avour models based on (discrete) symmetries, except for the very few cases which unambiguously predict the full set of leptonic mixing angles.…

High Energy Physics - Phenomenology · Physics 2016-11-22 Julia Gehrlein , Alexander Merle , Martin Spinrath

Within the framework of R-parity violating minimal supergravity model, at least three relatively large lepton-number violating $\l'$ type trilinear couplings at the GUT scale, not directly related to neutrino physics, can naturally generate…

High Energy Physics - Phenomenology · Physics 2009-11-11 Amitava Datta , Jyoti Prasad Saha , Anirban Kundu , Abhijit Samanta

If neutrino masses have a radiative origin, their smallness can be naturally understood even when lepton number violation occurs near the weak scale. We analyze a specific model of this type wherein the neutrino masses arise as two--loop…

High Energy Physics - Phenomenology · Physics 2009-11-07 K. S. Babu , C. Macesanu

If lepton masses and mixings are explained by a flavour symmetry in seesaw model which leads to U_{e3}=0 at leading order, we find that, under reasonable assumptions, a future observation of low energy leptonic CP violation implies, barring…

High Energy Physics - Phenomenology · Physics 2009-11-05 Yin Lin