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Related papers: Lepton number violation in 331 models

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Lepton number violation and its relation to neutrino masses is investigated in several versions of the $SU(3)_c\otimes SU(3)_L\otimes U(1)_x$ model. Spontaneous and explicit violation and conservation of the lepton number are considered. In…

High Energy Physics - Phenomenology · Physics 2015-03-06 Richard H. Benavides , Luis N. Epele , Huner Fanchiotti , Carlos García Canal , William A. Ponce

The $SU(3)_c\otimes SU(3)_L\otimes U(1)_N$ model of Pisano and Pleitez extends the Standard Model in a particularly nice way, so that for example the anomalies cancel only when the number of generations is divisible by three. The original…

High Energy Physics - Phenomenology · Physics 2009-07-28 R. Foot , O. F. Hernandez , F. Pisano , V. Pleitez

If there exist only three light neutrinos below the weak scale, the neutrino masses can arise by breaking the lepton number L. One example is the Zee mechanism for the neutrino masses. We study phenomenological implications of neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jihn E. Kim , Jae Sik Lee

Lepton family number violation processes arise in the $SU(6)_L \otimes U(1)_Y$ model due to the presence of an extra neutral gauge boson, Z$'$, with family changing couplings, and due to the fact that this model demands the existence of…

High Energy Physics - Phenomenology · Physics 2009-10-31 U. Cotti , R. Gaitan , A. Hernandez , W. Ponce , A. Zepeda

Models based on the extended symmetry gauge $SU(3)_c \otimes SU(3)_L \otimes U(1)_Y$ can be build up with a leptonic sector consistent of five triplets in different $SU(3)_L$ representations where additional heavy fermions are included.…

High Energy Physics - Phenomenology · Physics 2013-10-02 J. M. Cabarcas , J. Duarte , J. -Alexis Rodriguez

We survey 129 lepton number violating effective operators, consistent with the minimal Standard Model gauge group and particle content, of mass dimension up to and including eleven. Upon requiring that each one radiatively generates the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Andre de Gouvea , James Jenkins

In light of the recent $R_{K^{(*)}}$ data on neutral current flavour anomalies in $B \to K^{(*)} \ell^+ \ell^-$ decays, we re-examine their quantitative interpretation in terms of an extended 331 gauge theory framework. We achieve this by…

High Energy Physics - Phenomenology · Physics 2022-08-29 Andrea Addazi , Giulia Ricciardi , Simone Scarlatella , Rahul Srivastava , José W. F. Valle

We study the phenomenology of d=7 1-loop neutrino mass models. All models in this particular class require the existence of several new $SU(2)_L$ multiplets, both scalar and fermionic, and thus predict a rich phenomenology at the LHC. The…

High Energy Physics - Phenomenology · Physics 2018-11-02 R. Cepedello , M. Hirsch , J. C. Helo

The $SU(3)_C X SU(3)_L X U(1)_X$ gauge model with the minimal scalar sector (two Higgs triplets) is studied in detail. One of the vacuum expectation values $u$ is a source of lepton-number violations and a reason for the mixing among the…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. V. Dong , H. N. Long , D. T. Nhung , D. V. Soa

We perform a detailed study of the $\text{b} \to \text{c} \tau \nu$ and $\text{b} \to \text{s} l^+ l^-$ processes in a minimal flipped 331 model based on the $SU(3)_C\times SU(3)_L\times U(1)_N$ gauge symmetry. The non universal $SU(3)_L…

High Energy Physics - Phenomenology · Physics 2023-04-07 P. N. Thu , N. T. Duy , A. E. Carcamo Hernandez , D. T. Huong

We propose two models based on the $SU(3)_C \times SU(3)_L \times U(1)_X$ gauge symmetry, each incorporating distinct inverse seesaw mechanisms for generating neutrino masses at the radiative level. Therefore, neutrino masses are suppressed…

High Energy Physics - Phenomenology · Physics 2024-10-30 V. H. Binh , Cesar Bonilla , A. E. Cárcamo Hernández , D. T. Huong , Vishnudath K. N. , H. N. Long , P. N. Thu , Iván Schmidt

The Majorana nature of neutrinos is strongly motivated from the theoretical and phenomenological point of view. A plethora of neutrino mass models, known collectively as Seesaw models, exist that could generate both a viable neutrino mass…

High Energy Physics - Phenomenology · Physics 2018-06-04 Yi Cai , Tao Han , Tong Li , Richard Ruiz

The sources of lepton flavour and lepton number violation in the left-right symmetric models are reviewed and the most sensitive processes to these violations are discussed. Both the non-SUSY and SUSY versions of the theories are…

High Energy Physics - Phenomenology · Physics 2007-05-23 Martti Raidal

One of the most important and unanswered problems in particle physics is the origin of the three generations of quarks and leptons. The standard Model does not provide any hint regarding its sequential charge assignments, which remain a…

High Energy Physics - Phenomenology · Physics 2024-04-10 Claudio Corianò , Dario Melle

We perform a quantitative study of neutrino phenomenology in the framework of minimal supergravity (mSUGRA) with grand unified theory (GUT)-scale tri-linear lepton number violation. We show that only two non-zero GUT scale lepton number…

High Energy Physics - Phenomenology · Physics 2009-09-17 B. C. Allanach , C. H. Kom

Lepton-number violation (LNV), in general, implies nonzero Majorana masses for the Standard Model neutrinos. Since neutrino masses are very small, for generic candidate models of the physics responsible for LNV, the rates for almost all…

High Energy Physics - Phenomenology · Physics 2019-10-30 André de Gouvêa , Wei-Chih Huang , Johannes König , Manibrata Sen

The number of leptons may or may not be a conserved quantity. The Standard Model predicts that it is (in perturbative processes), but there is the well known possibility that new physics violates lepton number in one or two units. The first…

High Energy Physics - Phenomenology · Physics 2020-12-30 Renato M. Fonseca

If observed, charged lepton flavour violation is a clear sign of new physics - beyond the Standard Model minimally extended to accommodate neutrino oscillation data. After a brief review of several charged lepton flavour violation…

High Energy Physics - Phenomenology · Physics 2016-12-20 Ana M. Teixeira

We study a model with $U(1)$ gauged lepton number symmetry in which the active neutrino masses are generated at two-loop level through the spontaneous breaking of the lepton number symmetry. To cancel gauge anomalies some exotic leptons are…

High Energy Physics - Phenomenology · Physics 2017-06-06 Takaaki Nomura , Hiroshi Okada

We review a recently proposed framework in which the neutrino mass is a signal of supersymmetry breaking and is suppressed dynamically. In addition, we briefly comment on some possible consequences of general lepton-number violation in…

High Energy Physics - Phenomenology · Physics 2009-10-28 Nir Polonsky
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