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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

Leptophobic Z^\prime gauge boson appears naturally in many grand unified theories, such as flipped SU(5) or string-inspired E_6 models. This elusive particle easily escapes the direct/indirect detections because it does not couple to…

High Energy Physics - Phenomenology · Physics 2014-11-18 Seungwon Baek , Jong Hun Jeon , C. S. Kim

As described previously, a new massive gauge boson (X) coupling only to the third family produces a tantalizing pattern of deviations away from the standard model. These include increasing Gamma_b/Gamma_h and decreasing the alpha_s(M_Z)…

High Energy Physics - Phenomenology · Physics 2016-09-01 B. Holdom

We review the model-independent description of the couplings of the top quark to the Higgs and gauge bosons in theories beyond the Standard Model. Then we examine these couplings in the case of arbitrary heavy vector-like quarks mixing with…

High Energy Physics - Phenomenology · Physics 2015-06-15 J. A. Aguilar-Saavedra , M. Perez-Victoria

We investigate the implications of a seesaw type mass matrix, i.e., $M_f\simeq m_L M_F^{-1} m_R$, for quarks and leptons $f$ under the assumption that the matrices $m_L$ and $m_R$ are common to all flavors (up-/down- and quark-/lepton-…

High Energy Physics - Phenomenology · Physics 2010-11-01 Y. Koide , H. Fusaoka

New class of models are constructed in which the third family quarks, but not leptons, experience a new SU(2) or U(1) gauge force. Anomaly cancellation enforces the introduction of spectator quarks so that the top and bottom masses are…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. -J. He , T. M. P. Tait , C. -P. Yuan

It is proposed that all flavor mixing is caused by the mixing of the three quark and lepton families with vectorlike fermions in 5 + 5-bar multiplets of SU(5). This simple assumption implies that both V_{CKM} and U_{MNS} are generated by a…

High Energy Physics - Phenomenology · Physics 2015-06-11 S. M. Barr , Heng-Yu Chen

The ATLAS and CMS collaborations at the LHC have performed analyses on the existing data sets, studying the case of one vector-like fermion or multiplet coupling to the standard model Yukawa sector. In the near future, with more data…

High Energy Physics - Phenomenology · Physics 2015-02-03 Giacomo Cacciapaglia , Aldo Deandrea , Naveen Gaur , Daisuke Harada , Yasuhiro Okada , Luca Panizzi

We show that the recent measurements of $B_s-\bar{B}_s$ mass difference, $\Delta m_s$, by D{\O} and CDF collaborations give very strong constraints on MSSM scenario with large flavor mixing in the LL and/or RR sector of down-type squark…

High Energy Physics - Phenomenology · Physics 2009-11-11 Seungwon Baek

Motivated by the very recent measurements performed at the LHCb and the Tevatron of the $B_s^0-\bar B_s^0$ mixing, in this paper we revisit it in a family non-universal $Z^{\prime}$ model, to check if a simultaneous explanation for all the…

High Energy Physics - Phenomenology · Physics 2015-06-04 Xin-Qiang Li , Yan-Min Li , Gong-Ru Lu , Fang Su

Vector-like quarks have been of interest for a plethora of experimentally motivated reasons and have come under increased investigation recently due to their inclusion to the Standard Model (SM) appreciably improving global fits to several…

High Energy Physics - Phenomenology · Physics 2022-07-12 Shyam Balaji

The Littlest Higgs model contains a new vector-like heavy quark in the up sector. There are two interesting features of its existence. One is that it extends the $3\times3$ CKM matrix in the Standard Model to a $4\times3$ matrix and the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jae Yong Lee

We present a quantitative analysis of the flavor physics of a SUSY SO(10) model proposed by Chang, Masiero, and Murayama, linking b -> s transitions to the large observed atmospheric neutrino mixing. We consider B_s-B_s-bar mixing and tau…

High Energy Physics - Phenomenology · Physics 2009-09-29 Sebastian Jager

In models with partially composite quarks, the couplings of quarks to the Z boson generically receive non-universal corrections that are not only constrained by electroweak precision tests but also lead to flavour-changing neutral currents…

High Energy Physics - Phenomenology · Physics 2015-06-15 David M. Straub

We explore the phenomenology of charged Higgs bosons ($H^\pm$) and Vector-Like Quarks (VLQs), specifically the top-like $T$, within the Two Higgs Doublet Model Type-II (2HDM-II). We consider both a singlet VLQ $(T)$ and a doublet $(TB)$…

High Energy Physics - Phenomenology · Physics 2024-09-25 Rachid Benbrik , Mohammed Boukidi , Stefano Moretti

We consider a model where the standard model is extended by the addition of a vector-like isosinglet down-type quark b'. We perform a chi square fit to the flavor physics data and obtain the preferred central values along with errors of all…

High Energy Physics - Phenomenology · Physics 2016-03-23 Ashutosh Kumar Alok , Subhashish Banerjee , Dinesh Kumar , S. Uma Sankar

The investigation of mixing phenomena and lifetime in neutral B meson systems provides an important testing ground for standard model flavour dynamics. Spectroscopic parameters has been used to calculate the pseudoscalar decay constant and…

High Energy Physics - Phenomenology · Physics 2008-11-25 Bhavin Patel , Ajay Kumar Rai , P. C. Vinodkumar

We propose a mass matrix model that gives a unified description of quark and lepton with the same texture form based on a flavor 2 <-> 3 symmetry. The model is in contrast with the conventional picture that the mass matrix forms in the…

High Energy Physics - Phenomenology · Physics 2009-11-11 Koichi Matsuda , Hiroyuki Nishiura

Neutral mesons exhibit a phenomenon called flavour mixing. As a consequence of a second order weak process the flavour eigenstates corresponding to the meson and its anti-meson are superpositions of two mass eigenstates. A meson produced in…

High Energy Physics - Phenomenology · Physics 2013-09-03 Wouter Hulsbergen

An SU(2) vectorlike singlet quark with a charge either +2/3 (t') or -1/3 (b') is predicted in many extensions of the Standard Model. The mixing of these quarks with the top or bottom lead to Flavor Changing Yukawa Interactions and Neutral…

High Energy Physics - Phenomenology · Physics 2015-03-18 Aarti Girdhar , Biswarup Mukhopadhyaya , Monalisa Patra