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Related papers: Nearly Invariance of Jarlskog Determinant due to P…

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We consider future experiments to detect CP violation in neutrino oscillations and discuss how to test that all asymmetries are indeed described in terms of the single leptonic Jarlskog invariant as predicted in the absence of new physics…

High Energy Physics - Phenomenology · Physics 2008-12-18 Guido Altarelli , Davide Meloni

We consider the effects of Planck scale on four flavour neutrino mixings. The gravational interaction at $M_{x}=M_{\rm planck}$, we find that for degenerate neurino mass order, the Planck scale effects changes the mixing angle…

High Energy Physics - Phenomenology · Physics 2021-06-15 Bipin Singh Koranga , Vivek Kumar Nautiyal

Neutrino mixing lead to a non zero contribution to the cosmological constant. We consider non renormalization $1/M_{x}$ interaction term as a perturbation of the neutrino mass matrix. We find that for the degenerate neutrino mass spectrum.…

High Energy Physics - Phenomenology · Physics 2009-11-04 Bipin Singh Koranga

Current experimental data on neutrino oscillations are consistent with the tri-bimaximal mixing. If future experimental data will determine a non-zero $V_{e3}$ and/or find CP violations in neutrino oscillations, there is the need to modify…

High Energy Physics - Phenomenology · Physics 2008-11-26 Xiao-Gang He , A. Zee

This work explores how the generalized uncertainty principle, a theoretical modification of the Heisenberg uncertainty principle inspired by quantum gravity, affects neutrino flavor oscillations. By extending the standard two-flavor…

High Energy Physics - Phenomenology · Physics 2025-09-18 Kartik Joshi , Sanjib Dey , Satyajit Jena

CP violation in the lepton mass matrix will be probed with good precision in upcoming experiments. The amount of CP violation present in oscillations can be quantified in numerous ways and is typically parameterized by the complex phase…

High Energy Physics - Phenomenology · Physics 2021-05-20 Peter B. Denton , Rebekah Pestes

We point out that there is a unique parametrization of quark flavor mixing in which every angle is close to the Cabibbo angle \theta_C \simeq 13^\circ with the CP-violating phase \phi_q around 1^\circ, implying that they might all be…

High Energy Physics - Phenomenology · Physics 2015-06-04 Jean-Marc Gerard , Zhi-zhong Xing

Neutrino mixing parameters are subject to quantum corrections and hence are scale dependent. This means that the mixing parameters associated to the production and detection of neutrinos need not coincide since these processes are…

High Energy Physics - Phenomenology · Physics 2022-06-14 K. S. Babu , Vedran Brdar , André de Gouvêa , Pedro A. N. Machado

Bayesian analysis results require a choice of prior distribution. In long-baseline neutrino oscillation physics, the usual parameterisation of the mixing matrix induces a prior that privileges certain neutrino mass and flavour state…

High Energy Physics - Experiment · Physics 2025-12-16 The T2K Collaboration , K. Abe , S. Abe , R. Akutsu , H. Alarakia-Charles , Y. I. Alj Hakim , S. Alonso Monsalve , L. Anthony , S. Aoki , K. A. Apte , T. Arai , T. Arihara , S. Arimoto , Y. Ashida , E. T. Atkin , N. Babu , V. Baranov , G. J. Barker , G. Barr , D. Barrow , P. Bates , L. Bathe-Peters , M. Batkiewicz-Kwasniak , N. Baudis , V. Berardi , L. Berns , S. Bhattacharjee , A. Blanchet , A. Blondel , P. M. M. Boistier , S. Bolognesi , S. Bordoni , S. B. Boyd , C. Bronner , A. Bubak , M. Buizza Avanzini , J. A. Caballero , F. Cadoux , N. F. Calabria , S. Cao , S. Cap , D. Carabadjac , S. L. Cartwright , M. P. Casado , M. G. Catanesi , J. Chakrani , A. Chalumeau , D. Cherdack , P. S. Chong , A. Chvirova , J. Coleman , G. Collazuol , F. Cormier , A. A. L. Craplet , A. Cudd , D. D'ago , C. Dalmazzone , T. Daret , P. Dasgupta , C. Davis , Yu. I. Davydov , P. de Perio , G. De Rosa , T. Dealtry , C. Densham , A. Dergacheva , R. Dharmapal Banerjee , F. Di Lodovico , G. Diaz Lopez , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , K. E. Duffy , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , J. Elias , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , L. Feng , D. Ferlewicz , A. J. Finch , M. D. Fitton , C. Forza , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , J. García-Marcos , A. C. Germer , L. Giannessi , C. Giganti , M. Girgus , V. Glagolev , M. Gonin , R. González Jiménez , J. González Rosa , E. A. G. Goodman , K. Gorshanov , P. Govindaraj , M. Grassi , M. Guigue , F. Y. Guo , D. R. Hadley , S. Han , D. A. Harris , R. J. Harris , T. Hasegawa , C. M. Hasnip , S. Hassani , N. C. Hastings , Y. Hayato , I. Heitkamp , D. Henaff , Y. Hino , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , M. C. F. Hooft , K. Hosokawa , J. Hu , A. K. Ichikawa , K. Ieki , M. Ikeda , T. Ishida , M. Ishitsuka , H. Ito , S. Ito , A. Izmaylov , N. Jachowicz , S. J. Jenkins , C. Jesús-Valls , M. Jia , J. J. Jiang , J. Y. Ji , T. P. Jones , P. Jonsson , S. Joshi , M. Kabirnezhad , A. C. Kaboth , H. Kakuno , J. Kameda , S. Karpova , V. S. Kasturi , Y. Kataoka , T. Katori , A. Kawabata , Y. Kawamura , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , S. King , V. Kiseeva , J. Kisiel , A. Klustová , L. Kneale , H. Kobayashi , L. Koch , S. Kodama , M. Kolupanova , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , Y. Kudenko , Y. Kudo , A. Kumar Jha , R. Kurjata , V. Kurochka , T. Kutter , L. Labarga , M. Lachat , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , A. Langella , D. H. Langridge , J. -F. Laporte , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , D. Leon Silverio , S. Levorato , S. V. Lewis , B. Li , C. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , K. K. Mahtani , M. Mandal , S. Manly , A. D. Marino , D. G. R. Martin , D. A. Martinez Caicedo , L. Martinez , M. Martini , T. Matsubara , R. Matsumoto , V. Matveev , C. Mauger , K. Mavrokoridis , N. McCauley , K. S. McFarland , C. McGrew , J. McKean , A. Mefodiev , G. D. Megias , L. Mellet , C. Metelko , M. Mezzetto , S. Miki , V. Mikola , E. W. Miller , A. Minamino , O. Mineev , S. Mine , J. Mirabito , M. Miura , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , A. Muñoz , L. Munteanu , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , K. D. Nakamura , A. Nakano , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , D. T. Nguyen , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , Y. Noguchi , T. Nosek , F. Nova , P. Novella , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , R. Okazaki , W. Okinaga , K. Okumura , T. Okusawa , N. Onda , N. Ospina , L. Osu , N. Otani , Y. Oyama , V. Paolone , J. Pasternak , D. Payne , M. Pfaff , L. Pickering , B. Popov , A. J. Portocarrero Yrey , M. Posiadala-Zezula , Y. S. Prabhu , H. Prasad , F. Pupilli , B. Quilain , P. T. Quyen , E. Radicioni , B. Radics , M. A. Ramirez , R. Ramsden , P. N. Ratoff , M. Reh , G. Reina , C. Riccio , D. W. Riley , E. Rondio , S. Roth , N. Roy , A. Rubbia , L. Russo , A. Rychter , W. Saenz , K. Sakashita , S. Samani , F. Sánchez , E. M. Sandford , Y. Sato , T. Schefke , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , T. Sekiya , D. Seppala , D. Sgalaberna , A. Shaikhiev , M. Shiozawa , Y. Shiraishi , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , A. J. Speers , R. Spina , A. Srivastava , P. Stowell , Y. Stroke , I. A. Suslov , A. Suzuki , S. Y. Suzuki , M. Tada , S. Tairafune , A. Takeda , Y. Takeuchi , K. Takeya , H. K. Tanaka , H. Tanigawa , V. V. Tereshchenko , N. Thamm , C. Touramanis , N. Tran , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , M. Varghese , I. Vasilyev , G. Vasseur , E. Villa , U. Virginet , T. Vladisavljevic , T. Wachala , S. -i. Wada , D. Wakabayashi , H. T. Wallace , J. G. Walsh , L. Wan , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , K. Yamamoto , T. Yamamoto , C. Yanagisawa , Y. Yang , T. Yano , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , R. Zaki , A. Zalewska , J. Zalipska , G. Zarnecki , J. Zhang , X. Y. Zhao , H. Zheng , H. Zhong , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

Quantum gravity "foam", among its various generic Lorentz non-invariant effects, would cause neutrino mixing. It is shown here that, if the foam is manifested as a nonrenormalizable effect at scale M, the oscillation length generically…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ram Brustein , David Eichler , Stefano Foffa

We find that the precision and accuracy of current experimental data on the moduli of nine Cabibbo-Kobayashi-Maskawa (CKM) quark flavor mixing matrix elements allow us to numerically determine the it correct size of the Jarlskog invariant…

High Energy Physics - Phenomenology · Physics 2023-10-26 Shu Luo , Zhi-zhong Xing

With the help of a block parametrization of the canonical seesaw flavor textures in terms of the Euler-like rotation angles and CP-violaing phases, we derive a general and explicit expression for the Jarlskog invariant of CP violation in…

High Energy Physics - Phenomenology · Physics 2023-08-09 Zhi-zhong Xing

The results previously obtained from the model-independent application of a generalized hidden horizontal $\mathbb{Z}_2$ symmetry to the neutrino mass matrix are updated using the latest global fits for the neutrino oscillation parameters.…

High Energy Physics - Phenomenology · Physics 2014-09-17 Andrew D. Hanlon , Wayne W. Repko , Duane A. Dicus

In the quark sector, Jarlskog rephasing invariant parameter $J_{CP}$ has important implications for the CP violation as well as phase structure of the quark mass matrices. In fact all CP violating effects in this sector are proportional to…

High Energy Physics - Phenomenology · Physics 2018-04-05 Madan Singh

We propose a phenomenological model of lepton mixing and CP violation based on the flavor democracy of charge leptons and the mass degeneracy of neutrinos. A nearly bi-maximal flavor mixing pattern, which is favored by current data on…

High Energy Physics - Phenomenology · Physics 2007-05-23 Harald Fritzsch , Zhi-zhong Xing

It is hypotesized that neutrinos are massles and mixed among three (muon, electron and tau) flavors with a mixing length proportional to (E_nu/E_Planck)^-2. It is suggested that this hypothesis mostly reconciles the standard solar models…

Astrophysics · Physics 2007-05-23 David Eichler , Zakir F. Seidov

We consider the implications of a violation of the equivalence principle or of Lorentz invariance in the neutrino sector for the T-asymmetry $\Delta P_T \equiv P(\nu_{\alpha} \to \nu_{\beta}) - P(\nu_{\beta} \to \nu_{\alpha})$ in a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yvonne Y. Y. Wong

At present there is good agreement between the neutrino mass-squared difference determined from the solar neutrino data and the anti-neutrino mass-squared difference determined from the KamLAND reactor anti-neutrino experiment. However, the…

High Energy Physics - Phenomenology · Physics 2009-12-11 Bipin Singh koranga , Mohan Narayan , S Uma Sankar

We discuss a simple model of lepton mixing and CP violation based on the flavor democracy of charge leptons and the mass degeneracy of neutrinos. A nearly bi-maximal flavor mixing pattern, which is favored by current data on atmospheric and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Harald Fritzsch , Zhi-zhong Xing

In this paper, we show that the ratio of the effective Jarlskog invariant $\widetilde{\cal J}$ for leptonic CP violation in three-flavor neutrino oscillations in matter to its counterpart ${\cal J}$ in vacuum $\widetilde{\cal J}/{\cal J}…

High Energy Physics - Phenomenology · Physics 2020-01-08 Xin Wang , Shun Zhou