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Related papers: Baryon and Lepton Number Assignment in $E_6$ Model…

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We study assignments of the hypercharge and baryon minus lepton number for particles in the $E_6$ grand unification model. It is shown that there are three assignments of hypercharge and three assignments of baryon minus lepton number which…

High Energy Physics - Phenomenology · Physics 2009-11-10 J. Harada

The baryogenesis is reanalyzed based on the model by A.G.Cohen et al., in which the lepton number, generated by the neutrinos' scattering from the bubble walls appearing in the development of the electroweak phase transition, is converted…

High Energy Physics - Phenomenology · Physics 2019-08-15 Azusa Yamaguchi , Akio Sugamoto

One of the most puzzling questions in particle physics concerns the status of the baryon (B) and lepton (L) quantum numbers. On the theoretical side, most new physics scenarios naturally lead to their non-conservation and some amount of…

High Energy Physics - Phenomenology · Physics 2013-03-12 Gauthier Durieux , Jean-Marc Gérard , Fabio Maltoni , Christopher Smith

We study the possibility of generating the observed baryon asymmetry via leptogenesis in the decay of heavy Standard Model singlet fermions which carry lepton number, in a framework without Majorana masses above the electroweak scale. Such…

High Energy Physics - Phenomenology · Physics 2009-12-14 M. C. Gonzalez-Garcia , J. Racker , N. Rius

Models where the baryon (B) and lepton (L) numbers are local gauge symmetries that are spontaneously broken at a low scale are revisited. We find new extensions of the Standard Model which predict the existence of fermions that carry both…

High Energy Physics - Phenomenology · Physics 2013-06-05 Michael Duerr , Pavel Fileviez Perez , Mark B. Wise

We present a new scenario for the baryon number violation that may take place in models with large extra dimensions. Our idea is interesting because leptogenesis with a low reheating temperature requires an alternative source of the B+L…

High Energy Physics - Phenomenology · Physics 2009-11-07 Tomohiro Matsuda

In the context of many leptogenesis and baryogenesis scenarios, B-L (baryon minus the lepton number) is converted into B (baryon number) by non-perturbative B+L violating operators in the SU(2)_L sector. We correct a common misconversion of…

High Energy Physics - Phenomenology · Physics 2009-03-27 Daniel J H Chung , Bjorn Garbrecht , Sean Tulin

We propose a new mechanism for baryogenesis. We study the effective potential of left-right extension of the standard model and show that there can be a first order phase transition at the left-right symmetry breaking and hence $(B-L)$…

High Energy Physics - Phenomenology · Physics 2009-10-28 Avijit Ganguly , Jitendra C. Parikh , Utpal Sarkar

In the canonical seesaw mechanism of neutrino mass, lepton number is only multiplicatively conserved, which enables the important phenomenon of leptogenesis to occur, as an attractive explanation of the present baryon asymmetry of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernest Ma

It is shown that wave function renormalization can introduce an important contribution to the generation of baryon and lepton number asymmetries by heavy particle decay. These terms, omitted in previous analyses, are of the same order of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jiang Liu , Gino Segre

Proton decay experiments typically constrain baryon number violation to the scale of grand unified theories. From a phenomenological point of view, this makes direct probing of the associated new resonances, such as the X and Y bosons, out…

High Energy Physics - Phenomenology · Physics 2025-08-29 Amit Bhoonah , Francis Burk , Da Liu , Tong Ou , Deepak Sathyan

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 W. Buchmuller , M. Plumacher

In this talk I will present the work that we did in \cite{1}\cite{2}\cite{3}\cite{4}\cite{5} related to observed lepton universality violation by Babar, Belle and LHCb in R($D^{(*)}$) and $R_{K^{(*)}}$ as well as the reported deviation in…

High Energy Physics - Phenomenology · Physics 2019-09-04 Lobsang Dhargyal

We consider a baryogenesis scenario, where the difference of baryon (B) and lepton (L) number is conserved in such a way that the B-L asymmetry in the standard model sector is compensated by an asymmetry of opposite sign stored in the dark…

High Energy Physics - Phenomenology · Physics 2010-11-26 Florian Bauer , Marc-Thomas Eisele , Mathias Garny

A well-motivated framework to naturally introduce neutrino masses is the B-L model, a U(1) extension of the standard model related to the baryon minus lepton gauged number. Besides three right-handed neutrinos, that are included to cancel…

High Energy Physics - Phenomenology · Physics 2011-06-23 Lorenzo Basso

Electroweak baryogenesis provides a very attractive scenario to explain the origin of the baryon asymmetry. The mechanism of electroweak baryogenesis makes use of the baryon number anomaly and relies on physics that can be tested…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Carena , M. Quiros , M. Seco , C. E. M. Wagner

The electroweak sphaleron process breaks the baryon number conservation within the realms of the Standard Model of particle physics (SM). Recently, it is pointed out that its decoupling may provide the out-of-equilibrium condition required…

High Energy Physics - Phenomenology · Physics 2024-06-18 Muzi Hong , Kohei Kamada , Jun'ichi Yokoyama

We study baryogenesis through lepton number violation in left-right symmetric models. In these models the lepton number and CP violating interactions of the triplet higgs scalars can give rise to lepton number asymmetry through…

High Energy Physics - Phenomenology · Physics 2010-11-01 Patrick J. O'Donnell , Utpal Sarkar

We argue that simpler fermionic contents, responsible for the extension of the standard model with gauged lepton and baryon charges, can be constructed by assuming existence of so-called leptoquarks (j,k) with exotic electric charges…

High Energy Physics - Phenomenology · Physics 2017-05-25 P. V. Dong , H. N. Long

During a large period of time, the anomalous baryon number violating interactions are in equilibrium, when the $(B+L)$ asymmetry is washed out. If there is any lepton number violation during this period, that will also erase the $(B-L)$…

High Energy Physics - Phenomenology · Physics 2007-05-23 Utpal Sarkar
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