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Related papers: B-L Cosmic strings and Baryogenesis

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We show that in supersymmetric models with gauged B-L symmetry, there is a new source for cosmological lepton asymmetry. The Higgs bosons responsible for B-L gauge symmetry breaking decay dominantly into right-handed sneutrinos \tilde{N}…

High Energy Physics - Phenomenology · Physics 2010-01-05 K. S. Babu , Yanzhi Meng , Zurab Tavartkiladze

The extension of the Standard model (SM) with three heavy right handed neutrinos, a complex scalar and the gauged $U(1)_{\rm B-L}$ symmetry (the minimal $B-L$ model) is considered the most compelling minimal one: the presence and the…

High Energy Physics - Phenomenology · Physics 2021-01-19 Gongjun Choi , Tsutomu T. Yanagida , Norimi Yokozaki

The Standard Model (SM) of particle physics is a precise model of electroweak interactions, however there is growing tension between the SM and observations (neutrino oscillations, dark matter, dark energy, baryogenesis, among others).…

High Energy Physics - Phenomenology · Physics 2016-08-23 Zachary Burell

We put forward a new proposal for generating the baryon asymmetry of the universe by making use of the dynamics of a $\mathrm{U}(1)$ scalar field coupled to dark matter. High dark matter densities cause the $\mathrm{U}(1)$ symmetry to break…

High Energy Physics - Phenomenology · Physics 2017-11-22 Jeremy Sakstein , Mark Trodden

In the type-I seesaw mechanism for neutrino masses, there exists a $B-L$ symmetry, whose breaking leads to the lepton number violating mass of the heavy Majorana neutrinos. This would imply the existence of a new neutral scalar associated…

High Energy Physics - Phenomenology · Physics 2018-02-16 P. S. Bhupal Dev , Rabindra N. Mohapatra , Yongchao Zhang

We explore a mechanism of radiative B-L symmetry breaking in analogous to the radiative electroweak symmetry breaking. The breaking scale of B-L symmetry is related to the neutrino masses through the see-saw mechanism. Once we incorporate…

High Energy Physics - Phenomenology · Physics 2008-11-26 Tatsuru Kikuchi , Takayuki Kubo

The difference between baryon number B and lepton number L is the only anomaly-free global symmetry of the Standard Model, easily promoted to a local symmetry by introducing three right-handed neutrinos, which automatically make neutrinos…

High Energy Physics - Phenomenology · Physics 2014-11-11 Julian Heeck

The electroweak symmetry is unbroken in the core of cosmic strings originating from a symmetry breaking at an energy higher than the electroweak scale $\eta_{EW}$. The dynamics of such strings may generate a baryon asymmetry below the…

High Energy Physics - Phenomenology · Physics 2010-11-01 R. Brandenberger , A. -C. Davis , M. Trodden

Cosmological B-L breaking is a natural and testable mechanism to generate the initial conditions of the hot early universe. If B-L is broken at the grand unification scale, the false vacuum phase drives hybrid inflation, ending in tachyonic…

High Energy Physics - Phenomenology · Physics 2015-06-15 Wilfried Buchmuller , Valerie Domcke , Kohei Kamada , Kai Schmitz

We consider realizations of a gauged B-L symmetry in the context of the Dark Dimension scenario, where the SM lives on a codimension one brane in 5d spacetime. The B-L can naturally be a bulk gauge symmetery leading to a global symmetry on…

High Energy Physics - Theory · Physics 2026-03-04 Miguel Montero , Cumrun Vafa , Irene Valenzuela

Baryogenesis appears to require lepton number violation. This is naturally realized in extensions of the standard model containing right-handed neutrinos. We discuss the generation of a baryon asymmetry by the out-of-equilibrium decay of…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Plumacher

We calculate the effects of a light, very weakly-coupled boson $X$ arising from a spontaneously broken $U(1)_{B-L}$ symmetry on $\Delta N_{\rm eff}$ as measured by the CMB and $Y_p$ from BBN. Our focus is the mass range $1 \; {\rm eV}…

High Energy Physics - Phenomenology · Physics 2024-04-30 Haidar Esseili , Graham D. Kribs

We propose a new model where the Dirac mass term for neutrinos, the Majorana mass term for right-handed neutrinos, and the other new fermion masses arise via the spontaneous breakdown of the $U(1)_{B-L}$ gauge symmetry. The anomaly-free…

High Energy Physics - Phenomenology · Physics 2014-07-10 Shinya Kanemura , Toshinori Matsui , Hiroaki Sugiyama

We study the cosmology of a modified majoron model motivated by the need to protect a global $U(1)$ symmetry from gravity-induced hard explicit breaking (by $d \leq 4$ operators) at the Planck scale. The model extends the Standard Model by…

High Energy Physics - Phenomenology · Physics 2026-02-24 Tathagata Ghosh , Kousik Loho , Sudip Manna

In the presence of anomaly induced sphaleron process, only a B-L asymmetry can be partially converted to the baryon asymmetry while any B+L asymmetry would be completely erased. Thus in any successful baryogenesis theories, B-L is usually…

High Energy Physics - Phenomenology · Physics 2008-11-26 Pei-Hong Gu , Utpal Sarkar

Interactions of heavy Majorana neutrinos in the thermal phase of the early universe may be the origin of the cosmological matter-antimatter asymmetry. This mechanism of baryogenesis implies stringent constraints on light and heavy Majorana…

High Energy Physics - Phenomenology · Physics 2009-11-10 W. Buchmuller , P. Di Bari , M. Plumacher

It has been considered that baryogenesis models without a generation of $B$-$L$ asymmetry such as the GUT baryogenesis do not work since the asymmetry is washed out by the electroweak sphalerons. Here, we point out that helical…

High Energy Physics - Phenomenology · Physics 2018-07-05 Kohei Kamada

The quest for a common origin of neutrino mass and baryogenesis is one of the longstanding goals in particle physics. A minimal gauge extension of the Standard Model by $U(1)_{\rm B-L}$ symmetry provides a unique scenario to explain the…

High Energy Physics - Phenomenology · Physics 2026-03-18 Anirban Biswas , Sougata Ganguly

It is shown that the requirement of preservation of baryon asymmetry does not rule out a scale for leptogenesis as low as 10 TeV. The conclusions are compatible with see-saw mechanism if for example the pivot mass scale for neutrinos is…

High Energy Physics - Phenomenology · Physics 2009-11-10 Narendra Sahu , Urjit A. Yajnik

The seesaw mechanism with three heavy Majorana right-handed neutrinos provides an elegant explanation for neutrino masses and, combined with leptogenesis, can generate the baryon asymmetry of the universe (BAU). Naturally embedded in a…

High Energy Physics - Phenomenology · Physics 2025-05-06 Juan Herrero-Garcia , Giacomo Landini , Tsutomu T. Yanagida