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Given the best-fit results of six neutrino oscillation parameters, we plot the Dirac and Majorana unitarity triangles (UTs) of the 3\times 3 lepton flavor mixing matrix to show their real shapes for the first time. The connections of the…

High Energy Physics - Phenomenology · Physics 2016-06-22 Zhi-zhong Xing , Jing-yu Zhu

Leptonic unitarity triangle (LUT) provides a geometric description of CP violations in the lepton-neutrino sector and is directly measurable in principle. In this work, we reveal that the angles in the LUT have definite physical meaning,…

High Energy Physics - Phenomenology · Physics 2014-04-02 Hong-Jian He , Xun-Jie Xu

$\mu-\tau$ reflection symmetry is an attractive flavour symmetry in lepton mixing, which accommodates maximal values of atmospheric mixing angle ($\theta_{23}=\pi/4$) and Dirac CP phase ($\delta=\pi/2/3\pi/2$). Another significance of this…

High Energy Physics - Phenomenology · Physics 2025-10-16 Chandan Kumar Borah , Chandan Duarah

We present a geometric description of lepton flavor mixing and CP violation in matter by using the language of leptonic unitarity triangles. The exact analytical relations for both sides and inner angles are established between every…

High Energy Physics - Phenomenology · Physics 2011-09-13 He Zhang , Zhi-zhong Xing

We study a $\mu - \tau$ reflection symmetry in neutrino sector realized at the GUT scale in the context of the seesaw model. In our scenario, the exact $\mu - \tau$ reflection symmetry realized in the basis where the charged lepton and…

High Energy Physics - Phenomenology · Physics 2015-05-13 Y. H. Ahn , Sin Kyu Kang , C. S. Kim , T. Phong Nguyen

Given the Dirac neutrino mass term, we explore the constraint conditions which allow the corresponding mass matrix to be invariant under the \mu-\tau reflection transformation, leading us to the phenomenologically favored predictions…

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

We consider an exact mu-tau reflection symmetry in neutrino sectorrealized at the GUT scale in the context of the seesaw model with and without supersymmetry. Assuming the two lighter heavy Majorana neutrinos are degenerate at the GUT…

High Energy Physics - Phenomenology · Physics 2008-11-11 Y. H. Ahn , Sin Kyu Kang , C. S. Kim , T. Phong Nguyen

We discuss minimal non-supersymmetric models of resonant leptogenesis, based on an approximate flavour symmetries. As an illustrative example, we consider a resonant tau-leptogenesis model, compatible with universal right-handed neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-05 Frank F. Deppisch , Apostolos Pilaftsis

We point out that the observed neutrino mixing pattern at low energies is very likely to originate from the 3 times 3 lepton flavor mixing matrix U which possesses the exact mu-tau permutation symmetry |U_{mu i}| = |U_{tau i}| (for i=1,2,3)…

High Energy Physics - Phenomenology · Physics 2015-06-22 Shu Luo , Zhi-zhong Xing

We study the impact of minimal non-supersymmetric models of resonant leptogenesis on charged lepton flavour violation and the neutrino mixing angle theta(13). Possible low-scale flavour realisations of resonant tau-, mu- and e-leptogenesis…

High Energy Physics - Phenomenology · Physics 2011-04-22 Frank F. Deppisch , Apostolos Pilaftsis

In this paper, we have studied the consequences of the $\mu$-$\tau$ reflection symmetry for leptogenesis in the type-I seesaw model with diagonal Dirac neutrino mass matrix. We have first obtained the phenomenologically allowed values of…

High Energy Physics - Phenomenology · Physics 2024-05-13 Zhen-hua Zhao , Yan Shao , Hong-Yu Shi

After the observation of non-zero $\theta_{13}$ the goal has shifted to observe $CP$ violation in the leptonic sector. Neutrino oscillation experiments can, directly, probe the Dirac $CP$ phases. Alternatively, one can measure $CP$…

High Energy Physics - Phenomenology · Physics 2016-05-04 Surender Verma , Shankita Bhardwaj

We construct a left-right symmetric (LRS) model in five dimensions which accounts naturally for the lepton flavor parameters. The fifth dimension is described by an orbifold, S_1/Z_2 times Z'_2, with a typical size of order TeV^{-1}. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 Gilad Perez

The $\mu-\tau$ reflection symmetry of the lepton mixing matrix accommodates maximal atmospheric mixing ($\theta_{23}=\pi/4$) as well as maximal Dirac CP phase ($\delta=\pm \pi/2$) for the Dirac case. In the standard parametrization of the…

High Energy Physics - Phenomenology · Physics 2021-04-02 Chandan Duarah

At the Tevatron, the most promising channel to detect supersymmetry is three leptons plus missing energy, where the leptons are $e$'s and/or $\mu$'s. This final state appears from the production of chargino and second lighetst neutralino.…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Accomando , R. Arnowitt , B. Dutta

A supersymmetric see-saw model obeying the flavor symmetry L_mu - L_tau, which naturally predicts quasi-degenerate neutrinos, is investigated. Breaking of the symmetry is introduced in the Dirac mass matrix because it is the most economic…

High Energy Physics - Phenomenology · Physics 2010-04-05 Toshihiko Ota , Werner Rodejohann

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

We conjecture that there exists a remarkable correlation among the three elements in the first row of the $3\times 3$ lepton flavor mixing matrix $U$: $|U^{}_{e1}|^2 = 2 \left(|U^{}_{e2}|^2 + |U^{}_{e3}|^2\right)$, which holds even though…

High Energy Physics - Phenomenology · Physics 2026-03-03 Zhi-zhong Xing

We study minimal scenarios of resonant leptogenesis near the electroweak phase transition. These models offer a number of testable phenomenological signatures for low-energy experiments and future high-energy colliders. Our study extends…

High Energy Physics - Phenomenology · Physics 2009-11-11 Apostolos Pilaftsis , Thomas E. J. Underwood

The precision of the neutrino oscillation parameters measurements has improved and will continue to improve as the next-generation experiments become online. Beyond the more precise measurements of the mixing angles and phases used to…

High Energy Physics - Phenomenology · Physics 2026-01-27 Mathieu Guigue , Lorenzo Restrepo
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