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Related papers: Non-Anomalous Discrete R-symmetry Decrees Three Ge…

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We show that large leptonic mixing occurs most naturally in the framework of the Sandard Model just by adding a fourth generation. One can then construct a small $Z_4$ discrete symmetry, instead of the large $S_{4L}\times S_{4R}$, which…

High Energy Physics - Phenomenology · Physics 2010-02-03 Joaquim I. Silva-Marcos

In this work we explore the possibility to fix the number of new non-sequential chiral-type generations of fermions that could be added to the standard model by combining the condition that arise from the anomalies cancellation with the…

High Energy Physics - Phenomenology · Physics 2020-08-11 Elmer Ramirez Barreto , David Romero Abad

We construct supersymmetric composite models of quarks and leptons from type IIA T^6/(Z_2 x Z_2) orientifolds with intersecting D6-branes. In case of T^6 = T^2 x T^2 x T^2 with no tilted T^2, a composite model of the supersymmetric SU(5)…

High Energy Physics - Theory · Physics 2009-11-10 Noriaki Kitazawa

We discuss local \R-symmetry as a potentially powerful new model building tool. We first review and clarify that a $U(1)$ \R-symmetry can only be gauged in local and not in global supersymmetry. We determine the anomaly-cancellation…

High Energy Physics - Phenomenology · Physics 2011-02-19 A. H. Chamseddine , Herbi Dreiner

The new quantum number is introduced. It is shown that the conservation of -number results in the conservation of difference between baryon and lepton numbers. The problem of quark-lepton symmetry is discussed. It is shown that the nature…

High Energy Physics - Phenomenology · Physics 2007-05-23 N. A. Korkhmazyan , N. N. Korkhmazyan

We propose a model of generations that has exactly three generations. This model has several attractive features: There is a simple mechanism to produce the CKM quark mixings and their neutrino analogs. There are definite predictions for…

High Energy Physics - Phenomenology · Physics 2007-05-23 O. W. Greenberg

In models with dynamical electroweak symmetry breaking, this breaking is normally communicated to quarks and leptons by a set of vector bosons with masses generated via sequential breaking of a larger gauge symmetry. In reasonably…

High Energy Physics - Phenomenology · Physics 2014-11-20 Thomas A. Ryttov , Robert Shrock

We explore the recently proposed gauge symmetry \( SU(3)_C \otimes SU(3)_L \otimes SU(3)_R \otimes U(1)_X \), which naturally embeds both the Left-Right symmetric model and the 3-3-1 model as subgroups. Within this unified framework, we…

High Energy Physics - Phenomenology · Physics 2025-06-23 Richard H. Benavides , Yithsbey Giraldo , Eduardo Rojas

The supersymmetric extension of the standard model suffers from a problem of baryon-number violation. Discrete (and global) symmetries introduced to protect the proton are unstable under gravitational effects. We add a gauged $U(1)_X$ to…

High Energy Physics - Phenomenology · Physics 2009-10-28 A. H. Chamseddine , Herbi Dreiner

Given the particle content of the standard model without and with a right-handed neutrino, the requirement that all anomalies cancel singles out a set of possible global symmetries which can be gauged. I review this topic and propose a new…

High Energy Physics - Phenomenology · Physics 2009-10-31 Ernest Ma

Anomalies can be elegantly analyzed by means of the Dai-Freed theorem. In this framework it is natural to consider a refinement of traditional anomaly cancellation conditions, which sometimes leads to nontrivial extra constraints in the…

High Energy Physics - Theory · Physics 2020-04-03 Iñaki García-Etxebarria , Miguel Montero

The lack of experimental evidence for supersymmetry motivates R-parity violating realizations of the MSSM. Dropping R-parity, alternative symmetries have to be imposed in order to stabilize the proton. We determine the possible discrete R…

High Energy Physics - Phenomenology · Physics 2013-05-30 Herbi K. Dreiner , Marja Hanussek , Christoph Luhn

The first part of this talk presents the general complexion of baryon and lepton number non-conservation that may arise in the context of quark-lepton unification. The second part presents the status of grand unification with and without…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jogesh C. Pati

The Minimal Supersymmetric Standard Model (MSSM) is plagued by two major fine-tuning problems: the mu-problem and the proton decay problem. We present a simultaneous solution to both problems within the framework of a U(1)'-extended MSSM…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hye-Sung Lee , Konstantin T. Matchev , Ting T. Wang

We present two models where the familiar leptonic symmetry $L_e-L_\mu-L_\tau$ is a gauge symmetry. We show how anomaly cancellation constrains the allowed theories, with one of them requiring a fourth sequential chiral standard model…

High Energy Physics - Phenomenology · Physics 2023-07-19 Satyabrata Mahapatra , Rabindra N. Mohapatra , Narendra Sahu

We consider supersymmetric extensions of the standard model in which the usual $R$ or matter parity gets replaced by another $R$ or non-$R$ discrete symmetry that explains the observed longevity of the nucleon and solves the $\mu$ problem…

High Energy Physics - Phenomenology · Physics 2015-01-14 Mu-Chun Chen , Michael Ratz , Volodymyr Takhistov

Quark-lepton symmetric models are a class of gauge theories motivated by the similarities between the quarks and leptons. In these models the gauge group of the standard model is extended to include a ``color'' group for the leptons.…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. Foot , H. Lew , R. R. Volkas

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

In family unification models, all three families of quarks and leptons are grouped together into an irreducible representation of a simple gauge group, thus unifying the Standard Model gauge symmetries and a gauged family symmetry. Large…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr , Bumseok Kyae

Spontaneously broken Abelian gauge symmetries can explain the fermion mass hierarchies of the minimal supersymmetric standard model. In most cases it is assumed that the $U(1)_H$ symmetry is anomalous. However, non-anomalous models are also…

High Energy Physics - Phenomenology · Physics 2007-05-23 Enrico Nardi