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Related papers: Impact of $\nu$SMEFT operators on low-scale leptog…

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Baryon number is an accidental symmetry of the Standard Model at the Lagrangian level. Its violation is arguably one of the most compelling phenomena predicted by physics beyond the Standard Model. Furthermore, there is a large experimental…

High Energy Physics - Phenomenology · Physics 2026-02-13 Arnau Bas i Beneito , John Gargalionis , Juan Herrero-Garcia , Arcadi Santamaria , Michael A. Schmidt

The gauge-invariant operators up to dimension six in the low-energy effective field theory below the electroweak scale are classified. There are 70 Hermitian dimension-five and 3631 Hermitian dimension-six operators that conserve baryon and…

High Energy Physics - Phenomenology · Physics 2024-03-21 Elizabeth E. Jenkins , Aneesh V. Manohar , Peter Stoffer

We present a low-scale type-I seesaw scenario with discrete flavor and CP symmetries. This scenario not only explains the measured values of the lepton mixing angles, but also makes predictions for leptonic CP violation, and connects the…

High Energy Physics - Phenomenology · Physics 2023-01-03 Garv Chauhan , P. S. Bhupal Dev

Leptogenesis appears to be a viable alternative to account for the baryon asymmetry of the universe through baryogenesis. In this context, we consider a scenario in which the standard model is extended with $S_3$ and $Z_2$ symmetry in…

High Energy Physics - Phenomenology · Physics 2020-06-24 Subhasmita Mishra , Anjan Giri

We study lepton-number-violating interactions at dimension seven in the Standard Model effective field theory that contribute to the meson decays $B \to K \nu \nu$ and $K \to \pi \nu \nu$. Such interactions could washout the baryon…

High Energy Physics - Phenomenology · Physics 2026-01-26 Motoi Endo , Kåre Fridell , Sho Iwamoto , Yushi Mura , Kei Yamamoto

We study how leptogenesis can be implemented in a seesaw model with $S_4$ flavor symmetry, which leads to the neutrino tri-bimaximal mixing matrix and degenerate right-handed (RH) neutrino spectrum. Introducing a tiny soft $S_4$ symmetry…

High Energy Physics - Phenomenology · Physics 2010-12-13 Y. H. Ahn , Sin Kyu Kang , C. S. Kim , T. Phong Nguyen

The extension of the Standard Model by heavy right-handed neutrinos can simultaneously explain the observed neutrino masses via the seesaw mechanism and the baryon asymmetry of the Universe via leptogenesis. If the mass of the heavy…

High Energy Physics - Phenomenology · Physics 2020-07-10 Marco Drewes , Bjorn Garbrecht , Dario Gueter , Juraj Klaric

We present a pragmatic approach to lower down the mass scale of right-handed neutrinos in leptogenesis by introducing a scalar decaying to right-handed neutrinos. The key point of our proposal is that the out-of-equilibrium decays of the…

High Energy Physics - Phenomenology · Physics 2025-07-30 Jun-Yu Tong , Zhao-Huan Yu , Hong-Hao Zhang

Neutrinoless double beta decay, lepton number violating collider processes and the Baryon Asymmetry of the Universe (BAU) are intimately related. In particular lepton number violating processes at low energies in combination with sphaleron…

High Energy Physics - Phenomenology · Physics 2015-05-29 Julia Harz , Wei-Chih Huang , Heinrich Päs

The extension of Majorana neutrino mass mechanism of the neutrinoless double-beta decay ($0\nu\beta\beta$) with the inclusion of right-handed leptonic and hadronic currents is revisited. While only the exchange of light neutrinos is…

High Energy Physics - Phenomenology · Physics 2015-11-11 Dusan Stefanik , Rastislav Dvornicky , Fedor Simkovic , Petr Vogel

In Standard Model Effective Field Theory (SMEFT), invisible neutron decay arises from d = 12 operators. Adding new light particles to the field content of the SM, such as right-handed neutrinos, allows one to construct operators for…

High Energy Physics - Phenomenology · Physics 2026-02-05 J. C. Helo , M. Hirsch , T. Ota

We study the thermal leptogenesis in the $E_6\times U(1)_A$ SUSY GUT model in which realistic masses and mixings of quarks and leptons can be realized. We show that the sufficient baryon number can be produced by the leptogenesis in the…

High Energy Physics - Phenomenology · Physics 2016-03-23 Takuya Ishihara , Nobuhiro Maekawa , Mao Takegawa , Masato Yamanaka

We study lepto-axiogenesis in theories where the right-handed neutrino is light enough that its dynamics affect the determination of the baryon asymmetry. When compared with theories of high-scale lepto-axiogenesis where the Majorana…

High Energy Physics - Phenomenology · Physics 2024-02-19 Patrick Barnes , Raymond T. Co , Keisuke Harigaya , Aaron Pierce

Baryon and lepton number are excellent low-energy symmetries of the Standard Model (SM) that tightly constrain the form of its extensions. In this paper we investigate the possibility that these accidental symmetries are violated in the…

High Energy Physics - Phenomenology · Physics 2025-12-18 Arnau Bas i Beneito , John Gargalionis , Juan Herrero-Garcia , Michael A. Schmidt

We explore an anomaly-free ${\textrm U}(1)$ gauge extended beyond the Standard model (BSM) framework, to account for the baryon asymmetry of the Universe, along with arranging for tiny neutrino mass. Neutrino masses are generated via…

High Energy Physics - Phenomenology · Physics 2023-05-03 Kuldeep Deka , Tanumoy Mandal , Ananya Mukherjee , Soumya Sadhukhan

We study the evolution of a cosmological baryon asymmetry in leptogenesis when the right-handed neutrinos are produced in inflaton decays. By performing a detailed numerical study over a broad range of inflaton-neutrino couplings we show…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. Hahn-Woernle , M. Plumacher

It is usually believed that the observation of the neutrino-antineutrino (${\nu}$-$\bar{\nu}$) oscillations is almost impossible since the oscillation probabilities are expected to be greatly suppressed by the square of tiny ratio of…

High Energy Physics - Phenomenology · Physics 2017-04-05 Chao-Qiang Geng , Da Huang

The degenerate leptogenesis is studied when the degeneracy in two of the heavy right-handed neutrinos [the third one is irrelevant if $\mu -\tau $ symmetry is assumed] is due to $\bar{L}\equiv (L_{e}-L_{\mu}-L_{\tau}) $ discrete symmetry.…

High Energy Physics - Phenomenology · Physics 2010-05-19 Riazuddin

Dirac neutrinos with lepton-number-violating interactions can give rise to a new leptogenesis mechanism. In its simplest renormalizable realization, based on a gauged B-L symmetry spontaneously broken by four units, the decay of a new…

High Energy Physics - Phenomenology · Physics 2013-10-10 Julian Heeck

We discuss the systematic decomposition of the dimension nine neutrinoless double beta decay operator, focusing on mechanisms with potentially small contributions to neutrino mass, while being accessible at the LHC. We first provide a (d=9…

High Energy Physics - Phenomenology · Physics 2015-06-12 Florian Bonnet , Martin Hirsch , Toshihiko Ota , Walter Winter