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We discuss leptonic mixing and CP violation at low and high energies, emphasizing possible connections between leptogenesis and CP violation at low energies, in the context of lepton flavour models. Furthermore we analyse weak basis…

High Energy Physics - Phenomenology · Physics 2009-11-10 Gustavo C. Branco , M. N. Rebelo

Neutrinos are the fundamental particles, blind to all kind of interactions except the weak and gravitational. Hence, they can propagate very long distances without any deviation. This characteristic property can thus provide an ideal…

High Energy Physics - Phenomenology · Physics 2020-05-20 Rudra Majhi , Soumya C , Rukmani Mohanta

We searched for a sidereal modulation in the MINOS far detector neutrino rate. Such a signal would be a consequence of Lorentz and CPT violation as described by the Standard-Model Extension framework. It also would be the first detection of…

High Energy Physics - Experiment · Physics 2014-11-21 MINOS Collaboration , P. Adamson , D. J. Auty , D. S. Ayres , C. Backhouse , G. Barr , W. L. Barrett , M. Bishai , A. Blake , G. J. Bock , D. J. Boehnlein , D. Bogert , C. Bower , S. Budd , S. Cavanaugh , D. Cherdack , S. Childress , B. C. Choudhary , J. A. B. Coelho , J. H. Cobb , S. J. Coleman , L. Corwin , J. P. Cravens , D. Cronin-Hennessy , I. Z. Danko , J. K. de Jong , N. E. Devenish , M. V. Diwan , M. Dorman , C. O. Escobar , J. J. Evans , E. Falk , G. J. Feldman , M. V. Frohne , H. R. Gallagher , R. A. Gomes , M. C. Goodman , P. Gouffon , R. Gran , N. Grant , K. Grzelak , A. Habig , D. Harris , P. G. Harris , J. Hartnell , R. Hatcher , A. Himmel , A. Holin , X. Huang , J. Hylen , J. Ilic , G. M. Irwin , Z. Isvan , D. E. Jaffe , C. James , D. Jensen , T. Kafka , S. M. S. Kasahara , G. Koizumi , S. Kopp , M. Kordosky , Z. Krahn , A. Kreymer , K. Lang , G. Lefeuvre , J. Ling , P. J. Litchfield , L. Loiacono , P. Lucas , W. A. Mann , M. L. Marshak , N. Mayer , A. M. McGowan , R. Mehdiyev , J. R. Meier , M. D. Messier , D. G. Michael , J. L. Miller , W. H. Miller , S. R. Mishra , J. Mitchell , C. D. Moore , L. Mualem , S. Mufson , J. Musser , D. Naples , J. K. Nelson , H. B. Newman , R. J. Nichol , W. P. Oliver , M. Orchanian , J. Paley , R. B. Patterson , T. Patzak , G. Pawloski , G. F. Pearce , R. Pittam , R. K. Plunkett , J. Ratchford , T. M. Raufer , B. Rebel , P. A. Rodrigues , C. Rosenfeld , H. A. Rubin , V. A. Ryabov , M. C. Sanchez , N. Saoulidou , J. Schneps , P. Schreiner , V. K. Semenov , P. Shanahan , W. Smart , A. Sousa , M. Strait , N. Tagg , R. L. Talaga , J. Thomas , M. A. Thomson , G. Tinti , R. Toner , G. Tzanakos , J. Urheim , P. Vahle , B. Viren , A. Weber , R. C. Webb , C. White , L. Whitehead , S. G. Wojcicki , D. M. Wright , T. Yang , M. Zois , R. Zwaska

Tests of CPT and Lorentz symmetry using neutral-meson oscillations are studied within a formalism that allows for indirect CPT and T violation of arbitrary size and is independent of phase conventions. The analysis is particularly…

High Energy Physics - Phenomenology · Physics 2009-09-25 Alan Kostelecky

Using a generalized procedure for obtaining the equation of motion of a propagating fermionic particle, we examine previous claims for a lightlike preferred axis embedded in the framework of Lorentz-invariance violation with preserved…

High Energy Physics - Phenomenology · Physics 2011-07-19 Alex E. Bernardini

We have studied mixing and masses of three left handed Majorana neutrinos in the model, which assumes exactly degenerate neutrino masses at some "neutrino unification" scale. Such a simple theoretical ansatz naturally leads to…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. N. Ioannisian , N. A. Kazarian

We propose a new approach to explore CPT violation of neutrino oscillation through a fluctuating matter based on time-dependent geometric quantities. By mapping the neutrino oscillation onto a Poincare sphere structure, we obtain an…

Quantum Physics · Physics 2016-06-14 Zisheng Wang , Hui Pan

The conditions to induce appreciable CP-and T-odd effects in neutrino oscillations are discussed. The propagation in matter leads to fake CP-and CPT-odd asymmetries, besides a Bohm-Aharonov type modification of the interference pattern. We…

High Energy Physics - Phenomenology · Physics 2014-11-17 J. Bernabéu , M. C. Bañuls

Recent experimental data provides evidence for neutrino masses and leads to the possibility of leptonic mixing and CP violation. In this work special attention is dedicated to CP violation in the leptonic sector both at low and at high…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. N. Rebelo

Recently there has been a renewed activity in the physics of violations of Lorentz invariance in the neutrino sector. Flavor dependent Lorentz violation, which generically changes the pattern of neutrino oscillations, is extremely tightly…

High Energy Physics - Phenomenology · Physics 2013-04-05 Luca Maccione , Stefano Liberati , David M. Mattingly

If massive neutrinos are Majorana particles, then the lepton number should be violated in nature and neutrino-antineutrino oscillations $\nu^{}_\alpha \leftrightarrow \overline{\nu}^{}_\beta$ (for $\alpha, \beta = e, \mu, \tau$) will…

High Energy Physics - Phenomenology · Physics 2021-12-02 Yilin Wang , Shun Zhou

An attractive explanation for non-zero neutrino masses and small matter antimatter asymmetry of the present Universe lies in "leptogenesis". At present the {\it size} of the lepton asymmetry is precisely known, while the {\it sign} is not…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kaushik Bhattacharya , Narendra Sahu , Utpal Sarkar , Santosh K. Singh

The detectability of the fermion-potentials appearing in a unified model of fermions is discussed from the viewpoint of an effective field theory. Although the fermion-potentials are effectively represented as terms similar to the…

General Physics · Physics 2013-02-21 Kimihide Nishimura

Precise tests of Lorentz invariance can be executed using neutrino oscillations, which can provide sensitive measurements of suppressed signals of new physics. This talk describes the neutrino sector of the Standard-Model Extension, which…

High Energy Physics - Phenomenology · Physics 2009-09-30 Jorge S. Diaz

We reconsider the extrinsic and possible intrinsic CPT violation in neutrino oscillations, and point out an identity, i.e., $A^{\rm CP}_{\alpha \beta} = A^{\rm CPT}_{\beta \alpha} + A^{\rm T}_{\alpha \beta}$, among the CP, T, and CPT…

High Energy Physics - Phenomenology · Physics 2015-03-03 Tommy Ohlsson , Shun Zhou

We propose a simple ansatz for neutrino phenomenology, in which the relevant lepton mass matrices take the universal Fritzsch-like form and the seesaw relation holds under a particular condition. There exist six textures of this nature, but…

High Energy Physics - Phenomenology · Physics 2009-11-10 Zhi-zhong Xing , Shun Zhou

Searches for Lorentz and CPT violation using neutrino oscillations and the prospects for future tests using neutrino time-of-flight measurements and beta-decay experiments are presented.

High Energy Physics - Phenomenology · Physics 2017-08-23 Jorge S. Diaz

We propose a method by which one could use modified antimatter gravity experiments in order to perform a high-precision test of antimatter charge neutrality. The proposal is based on the application of a strong, external, vertically…

High Energy Physics - Phenomenology · Physics 2022-11-14 U. D. Jentschura

In the context of Standard Model Extensions (SMEs), we analyse four general classes of Super Symmetry (SuSy) and Lorentz Symmetry (LoSy) breaking, leading to {observable} imprints at our energy scales. The photon dispersion relations show a…

High Energy Physics - Phenomenology · Physics 2016-12-05 Luca Bonetti , Luís R. dos Santos Filho , José A. Helayël-Neto , Alessandro D. A. M. Spallicci

A symmetry violation model is considered for a system that can spontaneously choose between identical states which differ from each other only in weak properties (R-L). Such mirror symmetry allows reproduction of observed qualitative…

High Energy Physics - Phenomenology · Physics 2016-01-20 Igor T. Dyatlov
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