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Related papers: Flavor changing neutral currents in $SU(3)\otimes …

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Contributions of flavour-changing neutral currents in the 3 3 1 model with right-handed neutrinos to mass difference of the neutral meson system $\Delta m_P (P = K, D, B)$ are calculated. Using the Fritzsch anzats on quark mixing, we show…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hoang Ngoc Long , Vo Thanh Van

We carry out a general analysis of tree level flavor changing neutral currents in the context of 331 models, considering arbitrary quark and gauge boson mixing matrices. The results are applied to definite textures of quark mass matrices,…

High Energy Physics - Phenomenology · Physics 2010-02-22 J. M. Cabarcas , D. Gomez Dumm , R. Martinez

Flavor changing neutral currents coming from a new non-universal neutral Gauge-Boson and from the non-unitary quark mixing matrix for the $SU(3)_c\otimes SU(3)_L\otimes U(1)_X$ model with right handed neutrinos are studied. By imposing as…

High Energy Physics - Phenomenology · Physics 2014-11-20 Richard H. Benavides , Yithsbey Giraldo , William A. Ponce

We show that in the minimal 3-3-1 model the flavor changing neutral currents (FCNCs) do not impose necessarily strong constraints on the mass of the $Z^\prime$ of the model if we also consider the neutral scalar contributions to such…

High Energy Physics - Phenomenology · Physics 2013-12-12 A. C. B. Machado , J. C. Montero , V. Pleitez

We investigate a family-nonuniversal Abelian extension of hypercharge, which significantly alters the phenomenological features of the standard model. Anomaly cancellation requires that the third quark family transforms differently from the…

High Energy Physics - Phenomenology · Physics 2024-10-22 N. T. Duy , D. T. Huong , Duong Van Loi , Phung Van Dong

Flavour changing neutral currents arise in the $SU(3)_c\otimes SU(4)_L\otimes U(1)_X$ extension of the standard model because anomaly cancellation among the fermion families requires one generation of quarks to transform differently from…

High Energy Physics - Phenomenology · Physics 2009-10-06 Jorge L. Nisperuza , Luis A. Sanchez

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 a model in which the third family fermions are subjected to an SU(2) interaction different from the first two family fermions. Constrained by the Z-pole data, the heavy gauge boson mass is bounded from below to be about 1.7 TeV…

High Energy Physics - Phenomenology · Physics 2009-10-31 Ehab Malkawi , C. -P. Yuan

We propose the local $(B-L)_{\mu\tau}$ model, which minimally retains the local $B-L$ extension for the sake of neutrino phenomenologies, and at the same time presents an invisible gauge boson $Z'$ with mass $\sim {\cal O}(10)$ MeV to…

High Energy Physics - Phenomenology · Physics 2019-11-15 Zhaofeng Kang , Yoshihiro Shigekami

In models with an extra U(1)' gauge boson family non-universal couplings to the weak eigenstates of the standard model fermions generally induce flavor-changing neutral currents. This phenomenon leads to interesting results in various B…

High Energy Physics - Phenomenology · Physics 2009-09-15 Vernon Barger , Cheng-Wei Chiang , Jing Jiang , Paul Langacker

An electroweak model of SU(3) $\times$ U(1) gauge group is studied. {}From the group theoretical constraint, the symmetry breaking of this model to the standard model occurs at 1.7~TeV or lower. Hence the mass of the new neutral gauge boson…

High Energy Physics - Phenomenology · Physics 2011-07-19 Daniel Ng

We discuss a model in which the third generation fermions undergo a different $SU(2)$ weak interaction from the first two generation fermions. In general, a flavor changing neutral current interaction is expected. Constrained by the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ehab Malkawi , Tim Tait , C. --P. Yuan

We investigate, in detail, a model in which the third family fermions are subjected to an SU(2) dynamics different from the first two families. Constrained by the precision Z-pole data, the heavy gauge boson mass is bounded from below to be…

High Energy Physics - Phenomenology · Physics 2016-08-25 Ehab Malkawi , C. -P. Yuan

We analyze the effect of flavor changing neutral currents within 331 models. In particular, we concentrate in the so-called "economical" models, which have a minimal scalar sector. Taking into account the experimental measurements of…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. M. Cabarcas , D. Gomez Dumm , R. Martinez

For a model with a fourth family of quarks, new sources of flavor changing neutral currents are identified by confronting the unitary 4x4 quark mixing matrix with the experimental measured values of the familiar 3x3 quark mixing matrix. By…

High Energy Physics - Phenomenology · Physics 2010-04-15 Johana A. Herrera , Richard H. Benavides , William A. Ponce

There are theoretical and phenomenological motivations that there may exist additional heavy Z' bosons with family non-universal couplings. Flavor mixing in the quark and lepton sectors will then lead to flavor changing couplings of the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Paul Langacker , Michael Plumacher

We investigate the possibility of having sizable effects from flavor changing neutral currents at the tree level in a particular class of Two Higgs Doublet Models. Constraints from existing experimental information are discussed. Some…

High Energy Physics - Phenomenology · Physics 2007-05-23 Laura Reina

We show that the economical 3-3-1 model poses a very high new physics scale of the order of 1000~TeV due to the constraint on the flavor-changing neutral current. The implications of the model for neutrino masses, inflation, leptogenesis,…

High Energy Physics - Phenomenology · Physics 2018-09-21 P. V. Dong , D. Q. Phong , D. V. Soa , N. C. Thao

In 3-3-1 models anomaly cancellation requires that one of the three families of quarks transforms as triplet by $\text{SU}(3)_\text{L}$ with the other two transforming necessarily as anti-triplet. This is an important feature of the model…

High Energy Physics - Phenomenology · Physics 2023-08-23 Vinícius Oliveira , C. A. de S. Pires

This work is devoted for gauge boson sector of the recently proposed model based on SU(3)_C X SU(3)_L X U(1)_X group with minimal content of leptons and Higgses. The limits on the masses of the bilepton gauge bosons and on the mixing angle…

High Energy Physics - Phenomenology · Physics 2014-08-25 V. T. N. Huyen , T. T. Lam , H. N. Long , V. Q. Phong
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