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相关论文: More on deviation from bi-maximal neutrino mixing

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The unprecedented precision now being achieved in the measurement of the Pontecorvo--Maki--Nakagawa--Sakata (PMNS) lepton mixing matrix opens a new window onto the underlying structure of the neutrino mass matrix and the possibly associated…

高能物理 - 唯象学 · 物理学 2026-04-02 Alessio Giarnetti , Simone Marciano , Davide Meloni

The present article is an endeavor to look into some fruitful frameworks based on "Bi-maximal" neutrino mixing, from a model independent stand. The possibilities involving the correction or attenuation of the original BM mixing matrix,…

高能物理 - 唯象学 · 物理学 2016-03-28 Subhankar Roy , N. Nimai Singh

The PMNS neutrino mixing matrix U_{PMNS} is in general a product of two unitary matrices U_{lep} and U_{\nu} arising from the diagonalization of the charged lepton and neutrino mass matrices, U_{PMNS} = U^{\dagger}_{lep} U_{\nu}. Assuming…

高能物理 - 唯象学 · 物理学 2014-11-17 P. H. Frampton , S. T. Petcov , W. Rodejohann

Taking into account the latest neutrino oscillation data, we study texture zeros of the lepton mass matrices. Assuming the Dirac neutrino mass matrix M_D, the charged-lepton mass matrix M_l and the mass matrix of heavy right-handed Majorana…

高能物理 - 唯象学 · 物理学 2013-02-01 Harald Fritzsch , Shun Zhou

We estimate the PMNS (Pontecorvo-Maki-Nakagawa-Sakata) matrix in terms of neutrino and charged lepton mixing given as $U_{\rm PMNS}=V_{\rm lep}^\dagger(\tilde\theta_{13}) U_\nu(\tilde\theta_{23}, \tilde\theta_{12})$, based on a new…

高能物理 - 唯象学 · 物理学 2014-04-17 HoSeong La , Thomas J. Weiler

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…

高能物理 - 唯象学 · 物理学 2010-04-05 Guido Altarelli , Ferruccio Feruglio , Isabella Masina

Current experimental data allow the zero value for one neutrino mass, either m_1 = 0 or m_3 = 0. This observation implies that a realistic neutrino mass texture can be established by starting from the limit (a) m_1 = m_2 = 0 and m_3 \neq 0…

高能物理 - 唯象学 · 物理学 2008-11-26 Aik Hui Chan , Harald Fritzsch , Shu Luo , Zhi-zhong Xing

We develop a formalism for constructing the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) matrix and neutrino masses using an expansion that originates when a sequence of heavy right handed neutrinos are integrated out, assuming a seesaw mechanism…

高能物理 - 唯象学 · 物理学 2015-06-04 Benjamin Grinstein , Michael Trott

In this article, we derive the tiny neutrino masses and mixings from the democratic and diagonal texture approach, which consistent with the recent experimental oscillation data. The unitary rotation matrices, which diagonalize the neutrino…

高能物理 - 唯象学 · 物理学 2023-05-16 Itishree Sethi , Biswaranjan Behera , Mitesh Kumar Behera

In the model-independent context, where the neutrino mass matrix is assumed to be diagonalized by means of a unitary matrix that possess the Tri-Bi-Maximal (TBM) flavor mixing pattern. We present an analysis where the TBM deviation is…

高能物理 - 唯象学 · 物理学 2023-05-02 E. Barradas-Guevara , O. Félix-Beltrán , F. Gonzalez-Canales

Current neutrino data are consistent with the so-called tribimaximal mixing scenario, which predicts \sin^2 \theta_{12}=1/3, zero U_{e3} and maximal \theta_{23}. This implies a special form of the neutrino mass matrix. Introducing small…

高能物理 - 唯象学 · 物理学 2014-11-18 F. Plentinger , W. Rodejohann

We point out two simple but instructive possibilities to construct the charged lepton and neutrino mass matrices, from which the nearly bi-maximal neutrino mixing with large T violation can naturally emerge. The two lepton mixing scenarios…

高能物理 - 唯象学 · 物理学 2014-11-17 Zhi-zhong Xing

Assuming that the neutrino mass matrix is diagonalized by the tribimaximal mixing matrix, we explore the textures for the charged lepton mass matrix that render an $U_{PMNS}$ lepton mixing matrix consistent with data. In particular we are…

高能物理 - 唯象学 · 物理学 2014-06-10 J. Alberto Acosta , Alfredo Aranda , Manuel A. Buen-Abad , Alma D. Rojas

The three active light neutrinos are used to explain the neutrino oscillations. The inherently bi-large mixing neutrino mass matrix and the Fritzsch type, bi-small mixing charged lepton mass matrix are assumed. By requiring the maximal…

高能物理 - 唯象学 · 物理学 2014-11-17 Chun Liu , Jeonghyeon Song

I review the construction of a model for lepton masses based on the flavour symmetry group A4 x U(1) reproducing the so-called tri-bimaximal lepton mixing scheme, in eccelent agreement with current data. The model predicts a neutrino…

高能物理 - 唯象学 · 物理学 2009-04-25 Ferruccio Feruglio

Tri/bi-maximal mixing (TBM) is a specific lepton mixing ansatz, which describes the trend of the current neutrino oscillation data, in particular the recent SNO and KAMLAND results. The significant feature of TBM in this respect is…

高能物理 - 唯象学 · 物理学 2007-05-23 P. F. Harrison , W. G. Scott

In the limit of an approximate $\mu-\tau$ symmetry in the neutrino mass matrix, we explore deviations to the Tri-Bi-Maximal mixing pattern in the neutrino sector. We consider two different ansatzes for the corrected pattern to predict the…

高能物理 - 唯象学 · 物理学 2019-05-22 Diana C. Rivera-Agudelo , S. L. Tostado , Abdel Pérez-Lorenzana

Current data indicates that lepton mixing is very close to the tri-bimaximal mixing scenario. In general, however, one expects deviations from any mixing scenario. We discuss several examples to perturb tri-bimaximal mixing, namely soft…

高能物理 - 唯象学 · 物理学 2009-04-13 Werner Rodejohann

On the basis of a seesaw-type mass matrix model for quarks and leptons, $M_f \simeq m_L M_F^{-1} m_R$, where $m_L\propto m_R$ are universal for $f=u,d,\nu$ and $e$ (up-quark-, down-quark-, neutrino- and charged lepton-sectors), and $M_F$…

高能物理 - 唯象学 · 物理学 2014-11-17 Yoshio Koide

It has recently been shown that the phenomenologically successful pattern of cobimaximal neutrino mixing ($\theta_{13} \neq 0$, $\theta_{23} = \pi/4$, and $\delta_{CP} = \pm \pi/2$) may be achieved in the context of the non-Abelian discrete…

高能物理 - 唯象学 · 物理学 2017-10-25 Ernest Ma , G. Rajasekaran
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