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Higgs sector of the Standard model (SM) is replaced by quantum flavor dynamics (QFD), the gauged flavor $SU(3)_f$ symmetry with scale $\Lambda$. Anomaly freedom requires addition of three $\nu_R$. The approximate QFD Schwinger-Dyson…

High Energy Physics - Phenomenology · Physics 2021-04-07 Petr Beneš , Jiří Hošek , Adam Smetana

The four light neutrino scenario, which explains the atmosphere, solar and LSND neutrino experiments, is studied in the framework of the seesaw mechanism. By taking both the Dirac and Majorana mass matrix of neutrinos to be singular, the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Chun Liu , Jeonghyeon Song

If new sequential leptons $E^\pm$ and $N^0$ exist, the LEP bound implies $m_E$, $m_N > M_Z/2$. The heaviness of the neutral lepton breaks away from the pattern of the first three generations. The minimal model is to have 4 left-handed…

High Energy Physics - Phenomenology · Physics 2009-10-22 Wei-Shu Hou , Gwo-Guang Wong

The three electroweak doublet neutrinos $\nu_{e,\mu,\tau}$ of the Standard Model may acquire small seesaw masses, using either three Majorana fermion singlets $N$ or three Majorana fermion triplets $(\Sigma^+,\Sigma^0,\Sigma^-)$. It is…

High Energy Physics - Phenomenology · Physics 2010-04-15 Rathin Adhikari , Jens Erler , Ernest Ma

Hierarchical masses of quarks and leptons are addressed by imposing horizontal symmetries. In supersymmetric Standard Models, the same symmetries play a role in suppressing flavor violating processes induced by supersymmetric particles.…

High Energy Physics - Phenomenology · Physics 2021-10-27 Yuichiro Nakai , Matthew Reece , Motoo Suzuki

In order to analyze some low energy experimental anomalies, we charge with a non-universal $U(1)'$ gauge symmetry the standard model fermions, taking as a starting point the well-known scotogenic model. In order to have non-trivial…

High Energy Physics - Phenomenology · Physics 2018-12-11 Dario J. Blandon , Diego A. Restrepo , William A. Ponce , Eduardo Rojas

While the $S_3$ scalar leptoquark presents a possible tree-level explanation of the $b \to s \ell \ell$ flavour anomalies, it suffers from two conceptual problems which are often disregarded by model-builders. Firstly, the quantum numbers…

High Energy Physics - Phenomenology · Physics 2021-01-05 Joe Davighi , Matthew Kirk , Marco Nardecchia

The 331 model, an extension of the standard electroweak theory to $SU(3)_L\times U(1)_X$, naturally predicts three families of quarks and leptons via the requirement of anomaly cancellation. This is accomplished by making one of the quark…

High Energy Physics - Phenomenology · Physics 2010-11-01 James T. Liu

We consider supersymmetry breaking models in which the MSSM is extended to include an additional chiral adjoint field for each gauge group with which the the MSSM gauginos acquire Dirac masses. We investigate a framework in which the…

High Energy Physics - Phenomenology · Physics 2009-09-29 Z. Chacko , Patrick J. Fox , Hitoshi Murayama

Beyond Standard Model physics frequently connects flavor symmetry with a discrete group. If the discrete symmetry arises spontaneously from a gauge theory, one can maintain compatibility with quantum gravity and avoid anomalies. We provide…

High Energy Physics - Phenomenology · Physics 2018-12-18 Bradley L. Rachlin , Thomas W. Kephart

Models of spontaneous CP violation can solve the Strong CP problem without the need of an anomalous Peccei-Quinn symmetry. In this work we review the Nelson-Barr approach, quantifying a peculiar coincidence between unrelated mass scales…

High Energy Physics - Phenomenology · Physics 2022-05-10 Alessandro Valenti

Superconformal anomalies provide an elegant and economical way to understand the soft breaking parameters in SUSY models; however, implementing them leads to the several undesirable features including: tachyonic sleptons and electroweak…

High Energy Physics - Phenomenology · Physics 2008-12-18 R. N. Mohapatra , N. Setzer , S. Spinner

By extending the minimal scotogenic model with a spontaneously broken global symmetry $U(1)'$ and a preserved $\mathbb{Z}_2$ symmetry, we build a seesaw model for generating neutrino masses at three-loop level. The new particles have masses…

High Energy Physics - Phenomenology · Physics 2023-11-28 Asmaa Abada , Nicolás Bernal , Antonio E. Cárcamo Hernández , Sergey Kovalenko , Téssio B. de Melo , Takashi Toma

We propose a new $\mathrm{SU}(3)_C \otimes \mathrm{SU}(2)_{L}\otimes \mathrm{U}(1)_{Y}\otimes \mathrm{U}(1)_{X}$ gauge model which is non universal respect to the three fermion families of the Standard Model. We introduce additional one…

High Energy Physics - Phenomenology · Physics 2018-08-22 R. Martinez , S. F. Mantilla

We present a Left-Right symmetric model that provides an explanation for the mass hierarchy of the charged fermions within the framework of the Standard Model. This explanation is achieved through the utilization of both tree-level and…

High Energy Physics - Phenomenology · Physics 2024-01-01 Cesar Bonilla , A. E. Cárcamo Hernández , Sergey Kovalenko , H. Lee , R. Pasechnik , Ivan Schmidt

We consider leptogenesis in a left-right-symmetric seesaw scenario in which neutrino mass generation and leptogenesis are dominated by the type-II seesaw term. Motivated by grand unification, we assume that the neutrino Dirac mass matrix is…

High Energy Physics - Phenomenology · Physics 2021-09-29 Thomas Rink , Werner Rodejohann , Kai Schmitz

The flavor structure of quarks and leptons is not yet fully understood, but it hints a more fundamental theory of non-universal generations. We therefore propose a simple extension of the Standard Model by flipping (i.e., enlarging) the…

High Energy Physics - Phenomenology · Physics 2024-07-09 Duong Van Loi , Phung Van Dong , N. T. Duy , Nguyen Huy Thao

We discuss the phenomenology of a three-family supersymmetric Standard-like Model derived from the orientifold construction, in which the ordinary chiral states are localized at the intersection of branes at angles. In addition to the…

High Energy Physics - Phenomenology · Physics 2009-09-17 Mirjam Cvetic , Paul Langacker , Gary Shiu

The standard model can be interpreted as the leading order of a Low-Energy Effective Theory (LEET) invariant under a higher non linearly realized symmetry $S_{nat}\supset SU(2)_W \times U(1)_Y$ equipped with a systematic power counting.…

High Energy Physics - Phenomenology · Physics 2009-01-06 V. Bernard , M. Oertel , E. Passemar , J. Stern

We study the generation of small neutrino masses in an extra-dimensional model, where right-handed neutrinos are allowed to propagate in the extra dimension, while the Standard Model particles are confined to a brane. Motivated by the fact…

High Energy Physics - Phenomenology · Physics 2010-09-14 Mattias Blennow , Henrik Melbeus , Tommy Ohlsson , He Zhang