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We study meson decays mediated by the heavy gauge bosons of the Pati-Salam model of quark-lepton unification. We consider the scenarios in which the tau lepton is associated with the third, second, and first generation of quarks. The most…

High Energy Physics - Phenomenology · Physics 2009-10-28 G. Valencia , S. Willenbrock

A general discussion of the Cabibbo-Kobayashi-Maskawa (CKM) matrix is given and the importance stressed of determining the matrix elements as an essential part of understanding CP violation in and beyond the Standard Model. The status of…

High Energy Physics - Phenomenology · Physics 2009-11-07 Frederick J. Gilman

We examine the problem of three generation quark flavor mixing in realistic, superstring derived standard--like models, constructed in the free fermionic formulation. We study the sources of family mixing in these models and discuss the…

High Energy Physics - Phenomenology · Physics 2010-11-01 Alon E. Faraggi , Edi Halyo

We reconsider an universal mass matrix model which has a seesaw-invariant structure with four-zero texture common to all quarks and leptons. The CKM quark and MNS lepton mixing matrices of the model are analyzed analytically.We show that…

High Energy Physics - Phenomenology · Physics 2014-11-18 Koichi Matsuda , Hiroyuki Nishiura

Heavy-meson semileptonic decays calculations on the lattice are reviewed. The focus is upon obtaining reliable matrix elements. Errors that depend upon the lattice spacing, $a$, are an important source of systematic error. Full $O(a)$…

High Energy Physics - Lattice · Physics 2009-10-28 James Simone

We study the effect from a sequential fourth generation quark on penguin-dominated two-body nonleptonic B meson decays in the next-to-leading order perturbative QCD formalism. With an enhancement of the color-suppressed tree amplitude and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei-Shu Hou , Hsiang-nan Li , Satoshi Mishima , Makiko Nagashima

We investigate the quark structure of D and B mesons in the framework of a constituent quark model. To this end, we assume a scalar confining and a one gluon exchange (OGE) potential. The parameters of the model are adopted to reproduce the…

High Energy Physics - Phenomenology · Physics 2010-11-01 Stefan Resag , Michael Beyer

Metastable quarks of 4th generation are predicted in the framework of heterotic string phenomenology. Their presence in heavy stable hadrons are usually strongly constrained; however their hidden compositions in Heavy doubly charged baryons…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Belotsky , D. Fargion , M. Yu. Khlopov , R. V. Konoplich , M. G. Ryskin , K. I. Shibaev

We study the properties of singular values of mixing matrices embedded within an experimentally determined interval matrix. We argue that any physically admissible mixing matrix needs to have the property of being a contraction. This…

High Energy Physics - Phenomenology · Physics 2018-09-24 K. Bielas , W. Flieger , J. Gluza , M. Gluza

We explore a scenarios where topcolor-like dynamics operates in the presence of fourth generation matter fields. Using the Minimal Walking Technicolor as a concrete basis for model building, we construct explicit models and confront them…

High Energy Physics - Phenomenology · Physics 2011-02-08 Hidenori S. Fukano , Kimmo Tuominen

A brief review of the current state of observed deviations of theoretical predictions from experimental data in semileptonic decays of $B$ and $B_c$ mesons is given. A theoretical analysis of these decays is carried out, taking into account…

High Energy Physics - Phenomenology · Physics 2023-07-19 Aidos Issadykov , Mikhail A. Ivanov

The coupling constants of the order $p^2$ low-energy weak effective lagrangian can be determined from the $K\to\pi$ and $K\to 0$ weak matrix elements, choosing degenerate quark masses for the first of these. However, for typical values of…

High Energy Physics - Lattice · Physics 2009-10-31 Maarten Golterman , Elisabetta Pallante

Possible anomalous single productions of the fourth standard model generation up and down type quarks at CERN Large Hadron Collider are studied. Namely, $p p \to u_4 (d_4) X$ with subsequent $u_4\to bW^{+}$ process followed by leptonic…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Ciftci

We give an overview of recent progress in the study of fermion mass and flavor mixing phenomena. Mass matrix ansatze are considered within the SM and SUSY GUTs where some predictive frameworks based on SU(5) and SO(10) are reviewed. We…

High Energy Physics - Phenomenology · Physics 2009-11-11 N. Chamoun , S. Khalil

Defining, in the framework of quantum field theory, their mass eigenstates through their matricial propagator, we show why the mixing matrices of non-degenerate coupled systems should not be parametrized as unitary. This is how, for…

High Energy Physics - Phenomenology · Physics 2008-11-26 Quentin Duret , Bruno Machet

Existence of the fourth family follows from the basics of the Standard Model and the actual mass spectrum of the third family fermions. We discuss possible manifestations of the fourth SM family at existing and future colliders. The LHC and…

High Energy Physics - Phenomenology · Physics 2013-05-29 M. Sahin , S. Sultansoy , S. Turkoz

The features of a model interpreting the light scalar mesons as diquark-antidiquark bound states and the consequences of its natural extension to include heavy quarks are briefly reviewed.

High Energy Physics - Phenomenology · Physics 2009-11-11 L. Maiani , F. Piccinini , A. D. Polosa , V. Riquer

In the light of several recent analyses pointing towards texture 4-zero Fritzsch-like quark mass matrices as the only viable structures for quark mass matrices, this work adopts a model independent approach to reconstruct an alternate and…

High Energy Physics - Phenomenology · Physics 2017-08-31 Rohit Verma

We obtain constraints on possible structures of mass matrices in the quark sector by using as experimental restrictions the determined values of the quark masses at the $M_Z$ energy scale, the magnitudes of the quark mixing matrix elements…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Chaturvedi , V. Gupta , G. Sanchez-Colon

A composite model of fermions is proposed to explain the "anomaly" in $Z \rightarrow b {\bar b}$ and, to a lesser extent, in $Z \rightarrow c {\bar c}$. It contains a {\em nonsequential} fourth family whose mass of one member (the charge…

High Energy Physics - Phenomenology · Physics 2008-02-03 P. Q. Hung