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This work explores the neutrino phenomenology of the scotoseesaw model under non-holomorphic $A_4$ modular flavor symmetry providing a non-SUSY framework for realization of the modular symmetry. To prevent mixing between the beyond standard…

High Energy Physics - Phenomenology · Physics 2026-01-13 Salah Nasri , Labh Singh , Tapender , Surender Verma

We show that soft supersymmetry breaking terms involving the heavy sneutrinos can lead to sneutrino-antisneutrino mixing and to new sources of CP violation, which are present even if a single generation is considered. These terms are…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yuval Grossman , Tamar Kashti , Yosef Nir , Esteban Roulet

I suggest a minimal extension of the SM with $U(1)_{B-L}\otimes Z_{2}$. It can simultaneously accommodate the tiny neutrino mass, cold dark mater and baryon asymmetry besides the SM. All of the new physics arise from the $U(1)_{B-L}$…

High Energy Physics - Phenomenology · Physics 2017-04-27 Wei-Min Yang

In the standard lore, the baryon asymmetry of the present universe is attributed to the leptogenesis from the sterile right-handed neutrino with heavy Majorana mass decaying into the Standard Model's leptons at the very early universe --…

High Energy Physics - Phenomenology · Physics 2026-05-06 Juven Wang

CP violation and the violation of baryon-minus-lepton number B-L do not necessarily have to occur simultaneously in order to accomplish successful leptogenesis. Instead, it suffices if new CP-violating interactions at high energies result…

High Energy Physics - Phenomenology · Physics 2023-02-07 Valerie Domcke , Kohei Kamada , Kyohei Mukaida , Kai Schmitz , Masaki Yamada

We investigate the CP asymmetry for a hybrid texture of the neutrino mass matrix predicted by $Q_8$ family symmetry in the context of the type-I seesaw mechanism and examine its consequences for leptogenesis. We, also, calculate the…

High Energy Physics - Phenomenology · Physics 2011-03-22 S. Dev , Surender Verma

We present a scenario of nonthermal leptogenesis following supersymmetric hybrid inflation, in the case where inflaton decay to both heavy right handed neutrino and SU(2)_L triplet superfields is kinematically disallowed. Lepton asymmetry…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thomas Dent , George Lazarides , Roberto Ruiz de Austri

We propose a novel scenario to explain the matter-antimatter asymmetry by twofold leptogenesis, wherein heavy Majorana neutrinos exhibit temperature-dependent masses and engage in $CP$-violating decays. This scenario envisages two distinct…

High Energy Physics - Phenomenology · Physics 2024-02-14 YeolLin ChoeJo , Kazuki Enomoto , Yechan Kim , Hye-Sung Lee

We review the current status of the data on neutrino masses and lepton mixing and the prospects for measuring the CP-violating phases in the lepton sector. The possible connection between low energy CP violation encoded in the Dirac and…

High Energy Physics - Phenomenology · Physics 2018-03-05 C. Hagedorn , R. N. Mohapatra , E. Molinaro , C. C. Nishi , S. T. Petcov

We investigate the possibility that dark matter and the baryon asymmetry of the Universe are generated by the same mechanism, following an idea initially proposed by V.A. Kuzmin and recently discussed by R. Kitano and I. Low. In our model,…

High Energy Physics - Phenomenology · Physics 2009-11-11 Nicolas Cosme , Laura Lopez Honorez , Michel H. G. Tytgat

Supersymmetric scenarios incorporating thermal leptogenesis as the origin of the observed matter-antimatter asymmetry generically predict abundances of the primordial elements which are in conflict with observations. In this paper we…

High Energy Physics - Phenomenology · Physics 2011-07-28 Andrea De Simone , Mathias Garny , Alejandro Ibarra , Christoph Weniger

The energy levels of the left and the right handed neutrinos is split in the background of gravitational waves generated during inflation which in presence of lepton number violating interactions gives rise to a net lepton asymmetry at…

General Relativity and Quantum Cosmology · Physics 2009-11-11 Subhendra Mohanty , A. R. Prasanna , G. Lambiase

The observation of neutrino masses leads to the possibility of leptonic mixing and CP violation. One of the simplest extensions of the Standard Model giving rise to neutrino masses consists of the introduction of one righthanded neutrino…

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

We propose a model with an $U(1)_{B-L}$ gauge symmetry, in which small neutrino masses, dark matter and the matter-antimatter asymmetry in the Universe can be simultaneously explained. In particular, the neutrino masses are generated…

High Energy Physics - Phenomenology · Physics 2018-02-19 Chao-Qiang Geng , Hiroshi Okada

Soft leptogenesis is a mechanism which generates the matter-antimatter asymmetry of the Universe via the out-of-equilibrium decays of heavy sneutrinos in which soft supersymmetry breaking terms play two important roles: they provide the…

High Energy Physics - Phenomenology · Physics 2015-05-05 Rathin Adhikari , Arnab Dasgupta , Chee Sheng Fong , Raghavan Rangarajan

We consider leptogenesis in a minimal S_3 extension of the standard model with an additional Z_2 symmetry in the leptonic sector. It is found that the CP phase appearing in the neutrino mixing is the same as that for the CP asymmetries…

High Energy Physics - Phenomenology · Physics 2016-09-06 Takeshi Araki , Jisuke Kubo , Emmanuel A. Paschos

We propose a unified explanation for the origin of dark matter and baryon number asymmetry on the basis of a non-supersymmetric model for neutrino masses. Neutrino masses are generated in two distinct ways, that is, a tree-level seesaw…

High Energy Physics - Phenomenology · Physics 2008-11-26 Daijiro Suematsu

The current laws of physics do not explain the observed imbalance of matter and antimatter in the universe. Sakharov proposed that an explanation would require the violation of CP symmetry between matter and antimatter. The only CP…

High Energy Physics - Experiment · Physics 2021-01-26 K. Abe , R. Akutsu , A. Ali , C. Alt , C. Andreopoulos , L. Anthony , M. Antonova , S. Aoki , A. Ariga , Y. Asada , Y. Ashida , E. T. Atkin , Y. Awataguchi , S. Ban , M. Barbi , G. J. Barker , G. Barr , C. Barry , M. Batkiewicz-Kwasniak , A. Beloshapkin , F. Bench , V. Berardi , S. Berkman , L. Berns , S. Bhadra , S. Bienstock , A. Blondel , S. Bolognesi , B. Bourguille , S. B. Boyd , D. Brailsford , A. Bravar , D. Bravo Berguño , C. Bronner , A. Bubak , M. Buizza Avanzini , J. Calcutt , T. Campbell , S. Cao , S. L. Cartwright , M. G. Catanesi , A. Cervera , A. Chappell , C. Checchia , D. Cherdack , N. Chikuma , G. Christodoulou , J. Coleman , G. Collazuol , L. Cook , D. Coplowe , A. Cudd , A. Dabrowska , G. De Rosa , T. Dealtry , P. F. Denner , S. R. Dennis , C. Densham , F. Di Lodovico , N. Dokania , S. Dolan , O. Drapier , J. Dumarchez , P. Dunne , L. Eklund , S. Emery-Schrenk , A. Ereditato , P. Fernandez , T. Feusels , A. J. Finch , G. A. Fiorentini , G. Fiorillo , C. Francois , M. Friend , Y. Fujii , R. Fujita , D. Fukuda , R. Fukuda , Y. Fukuda , K. Gameil , C. Giganti , T. Golan , M. Gonin , A. Gorin , M. Guigue , D. R. Hadley , J. T. Haigh , P. Hamacher-Baumann , M. Hartz , T. Hasegawa , N. C. Hastings , T. Hayashino , Y. Hayato , A. Hiramoto , M. Hogan , J. Holeczek , N. T. Hong Van , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , T. Ishii , M. Ishitsuka , K. Iwamoto , A. Izmaylov , B. Jamieson , S. J. Jenkins , C. Jesús-Valls , M. Jiang , S. Johnson , P. Jonsson , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , D. Karlen , S. P. Kasetti , Y. Kataoka , T. Katori , Y. Kato , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kim , J. Kim , S. King , J. Kisiel , A. Knight , A. Knox , T. Kobayashi , L. Koch , T. Koga , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , H. Kubo , Y. Kudenko , N. Kukita , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , M. Lamoureux , M. Laveder , M. Lawe , M. Licciardi , T. Lindner , R. P. Litchfield , S. L. Liu , X. Li , A. Longhin , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , S. Manly , L. Maret , A. D. Marino , J. F. Martin , T. Maruyama , T. Matsubara , K. Matsushita , V. Matveev , K. Mavrokoridis , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , C. Metelko , M. Mezzetto , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , J. Morrison , Th. A. Mueller , L. Munteanu , S. Murphy , Y. Nagai , T. Nakadaira , M. Nakahata , Y. Nakajima , A. Nakamura , K. G. Nakamura , K. Nakamura , S. Nakayama , T. Nakaya , K. Nakayoshi , C. Nantais , T. V. Ngoc , K. Niewczas , K. Nishikawa , Y. Nishimura , T. S. Nonnenmacher , F. Nova , P. Novella , J. Nowak , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , K. Okumura , T. Okusawa , S. M. Oser , R. A. Owen , Y. Oyama , V. Palladino , J. L. Palomino , V. Paolone , W. C. Parker , P. Paudyal , M. Pavin , D. Payne , G. C. Penn , L. Pickering , C. Pidcott , G. Pintaudi , E. S. Pinzon Guerra , C. Pistillo , B. Popov , K. Porwit , M. Posiadala-Zezula , A. Pritchard , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , P. N. Ratoff , E. Reinherz-Aronis , C. Riccio , E. Rondio , S. Roth , A. Rubbia , A. C. Ruggeri , A. Rychter , K. Sakashita , F. Sánchez , C. M. Schloesser , K. Scholberg , J. Schwehr , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , R. Shah , A. Shaikhiev , F. Shaker , A. Shaykina , M. Shiozawa , W. Shorrock , A. Shvartsman , A. Smirnov , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , J. Steinmann , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , M. Tajima , A. Takeda , Y. Takeuchi , H. K. Tanaka , H. A. Tanaka , S. Tanaka , L. F. Thompson , W. Toki , C. Touramanis , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , W. Uno , M. Vagins , S. Valder , Z. Vallari , D. Vargas , G. Vasseur , C. Vilela , W. G. S. Vinning , T. Vladisavljevic , V. V. Volkov , T. Wachala , J. Walker , J. G. Walsh , Y. Wang , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , R. J. Wilson , K. Wood , C. Wret , Y. Yamada , K. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , S. Yen , N. Yershov , M. Yokoyama , T. Yoshida , M. Yu , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos , A. Zykova

Baryogenesis via leptogenesis provides an appealing mechanism to explain the observed baryon asymmetry of the Universe. Recent refinements in the understanding of the dynamics of leptogenesis include detailed studies of the effects of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Enrico Nardi

The addition of gauge singlet fermions to the Standard Model Lagrangian renders the neutrinos massive and allows one to explain all that is experimentally known about neutrino masses and lepton mixing. At the same time, the gauge singlet…

High Energy Physics - Phenomenology · Physics 2010-12-02 Wei-Chih Huang
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