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In the context of Calabi-Yau string models we explore the origin of characteristic pattern of quark-lepton masses and the CKM matrix. The discrete $R$-symmetry $Z_K \times Z_2$ is introduced and the $Z_2$ is assigned to the $R$-parity. The…

High Energy Physics - Phenomenology · Physics 2009-10-28 N. Haba , C. Hattori , M. Matsuda , T. Matsuoka

We propose a simple $SU(5)$ model that connects the neutrino mass generation mechanism to the observed disparity between the masses of charged leptons and down-type quarks. The model is built out of $5$-, $10$-, $15$-, $24$-, and…

High Energy Physics - Phenomenology · Physics 2020-01-22 Ilja Doršner , Shaikh Saad

Within the framework of a local SU(3) family symmetry model, we report a general analysis of the mechanism for neutrino mass generation and mixing, including light sterile neutrinos. In this scenario, ordinary heavy fermions, top and bottom…

High Energy Physics - Phenomenology · Physics 2014-12-23 Albino Hernandez-Galeana

This work considers the remarkable suggestion that the three families of quarks and leptons may be unified, together with the Higgs and gauge fields of the Standard Model (SM), into a single "particle", namely the $\textbf{248}$ vector…

High Energy Physics - Phenomenology · Physics 2020-10-12 Alfredo Aranda , Francisco J. de Anda , Stephen F. King

In supersymmetry, there are gauge invariant dimension 5 proton decay operators which must be suppressed by a mass scale much larger than the Planck mass. It is natural to expect that this suppression should be explained by a mechanism that…

High Energy Physics - Phenomenology · Physics 2009-11-07 Mitsuru Kakizaki , Masahiro Yamaguchi

The quark and charged lepton masses and the angles and phase of the CKM mixing matrix are nicely reproduced in a model which assumes SU(3)xSU(3) flavour symmetry broken by the v.e.v.'s of fields in its bi-fundamental representation. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 I. Masina , C. A. Savoy

A unified form of mass matrix is proposed for neutrinos, charged leptons, up quarks and down quarks. Some constraints for the parameters involved are tent% atively postulated. Then, the predictions are neatly consistent with available…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. Krolikowski

We propose a predictive model based on the $SU(3)_{C}\otimes SU(3)_{L}\otimes U(1)_{X}$ gauge group supplemented by the $A_{4}\otimes Z_{3}\otimes Z_{4}\otimes Z_{6}\otimes Z_{16}$ discrete group, which successfully describes the SM fermion…

High Energy Physics - Phenomenology · Physics 2016-05-03 A. E. Cárcamo Hernández , R. Martinez

The necessity of the fourth family follows from the SM basics. According to flavor democracy the Dirac masses of the fourth SM family fermions are almost equal with preferable value 450 GeV, which corresponds to common (for all fundamental…

High Energy Physics - Phenomenology · Physics 2014-11-18 S. Sultansoy

The combination of precise determinations of $V_{us}$ and $V_{ud}$ hints towards a violation of the CKM first row unitarity at about $3\sigma$ level. Conversely, the recent measurement of the $W$-boson mass by the CDF Collaboration exhibits…

High Energy Physics - Phenomenology · Physics 2023-07-28 Benedetta Belfatto , Sokratis Trifinopoulos

The first fermion family might play a special role in understanding the physics of flavour. This possibility is suggested by the observation that the up-down splitting within quark families increases with the family number: $ m_u\sim m_d$,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Z. G. Berezhiani , R. Rattazzi

Vectorial partners of the Standard Model quarks and leptons are predicted in many dynamical models of electroweak symmetry breaking. The most easily accessible of these new particles, either due to mass or couplings, are typically expected…

High Energy Physics - Phenomenology · Physics 2023-08-23 Alexander Belyaev , R. Sekhar Chivukula , Benjamin Fuks , Elizabeth H. Simmons , Xing Wang

We propose a radiatively induced quark and lepton mass model in the first and second generation with extra $U(1)$ gauge symmetry and vector-like fermions. Then we analyze the allowed regions which simultaneously satisfy the FCNCs for the…

High Energy Physics - Phenomenology · Physics 2016-08-31 Takaaki Nomura , Hiroshi Okada

Reliable values of quark and lepton masses are important for model building at a fundamental energy scale, such as the Fermi scale M_Z \approx 91.2 GeV and the would-be GUT scale \Lambda_GUT \sim 2 \times 10^16 GeV. Using the latest data…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-zhong Xing , He Zhang , Shun Zhou

We study two-site deconstructions of the $SU(2)_L$ gauge group factor of the SM. Models based on this approach can explain the hierarchies of the quark masses and CKM mixing between third and light families if these fields are localised on…

High Energy Physics - Phenomenology · Physics 2024-08-12 Bernat Capdevila , Andreas Crivellin , Javier M. Lizana , Stefan Pokorski

The extension of the standard model with pairs of the vector-like families is studied. The quark mixing matrices for the left- and right-handed charged currents, as well as those for the flavour changing neutral currents, the Z and Higgs…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yu. F. Pirogov , O. V. Zenin

We discuss the lattice formulation of gauge theories with fermions in arbitrary representations of the color group, and present the implementation of the RHMC algorithm for simulating dynamical Wilson fermions. A first dataset is presented…

High Energy Physics - Lattice · Physics 2010-01-21 Luigi Del Debbio , Agostino Patella , Claudio Pica

A search for pair-produced heavy vector-like charge-2/3 quarks, T, in pp collisions at a center-of-mass energy of 7 TeV, is performed with the CMS detector at the LHC. Events consistent with the flavor-changing-neutral-current decay of a T…

High Energy Physics - Experiment · Physics 2012-08-27 CMS Collaboration

The Exceptional Supersymmetric (SUSY) Standard Model predicts three families of Higgs doublets plus three Higgs singlets, where one family develops vacuum expectation values (VEVs), while the remaining two which do not are called Inert. The…

High Energy Physics - Phenomenology · Physics 2011-05-05 J. P. Hall , S. F. King , R. Nevzorov , S. Pakvasa , M. Sher

There are strong arguments favoring the Flavor Democracy hypothesis (or the Democratic Mass Matrix approach) within the Standard Model framework. However, the large mass of the top quark ($m_t >> m_b, m_\tau$) poses an obstacle to the…

High Energy Physics - Phenomenology · Physics 2026-03-06 Burak Dagli , Saleh Sultansoy , Ismail Toy