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A new mechanism is proposed to explain the "anomaly" in $Z \rightarrow b {\bar b}$ resulting in a prediction of a new, non-sequential fourth family whose masses could all be below $M_W$, thus opening up an exciting porpect for near-future…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pham Quang Hung

A phenomenological theory of fermion masses and mixings is constructed within the framework of a four- family symmetry. It is found that the most favored set of relevant CKM elements are $|V_{us}|\approx 0.222$, $|V_{cb}|\approx 0.044$,…

High Energy Physics - Phenomenology · Physics 2010-11-01 P. Q. Hung

It now appears phenomenologically that the third family of fundamental fermions may be essentially different fron the first two. Particularly the high value (174GeV?) of the top quark mass suggests a special role. In the standard model all…

High Energy Physics - Phenomenology · Physics 2007-05-23 Paul H. Frampton

The phenomenology of an additional U(1) neutral gauge boson Z' coupled to the third family of fermions is discussed. One might expect such a particle to contribute to processes where taus, b and t quarks are produced. Precision data from…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. A. Andrianov , P. Osland , A. A. Pankov , N. V. Romanenko , J. Sirkka

The existence of fourth family follows from the basics of the Standard Model. Because of the high masses of the fourth family quarks, their anomalous decays could be dominant, if certain criteria are met. This will drastically change the…

High Energy Physics - Phenomenology · Physics 2014-11-21 M. Sahin , S. Sultansoy , S. Turkoz

Z' bosons that couple preferentially to the third generation fermions can arise in models with extended weak (SU(2)xSU(2)) or hypercharge (U(1)xU(1)) gauge groups. We show that existing limits on quark-lepton compositeness set by the LEP…

High Energy Physics - Phenomenology · Physics 2011-03-23 Kevin R. Lynch , Meenakshi Narain , Elizabeth H. Simmons , Stephen Mrenna

We present the results of a search for pair production of a fourth-generation charge -1/3 quark (b') in sqrt(s)=1.8 TeV ppbar collisions using 88 pb^(-1) of data obtained with the Collider Detector at Fermilab. We assume that both quarks…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , T. Affolder

We report the most restrictive direct limits on masses of fourth-generation down-type quarks $b^{\prime}$, and quark-like composite fermions ($B$ or $T_{5/3}$), decaying promptly to $t W^{\mp}$. We search for a significant excess of events…

High Energy Physics - Experiment · Physics 2012-08-27 The CDF Collaboration

Some of the motivations for quark and lepton compositeness, and some problems associated with present schemes, are noted. One model is discussed in which quarks and leptons are taken as composites of spin-1/2 fermions $F$ with charges $\pm…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jonathan L. Rosner

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

Results are presented from a search for a fourth generation of quarks produced singly or in pairs in a data set corresponding to an integrated luminosity of 5 inverse femtobarns recorded by the CMS experiment at the LHC in 2011. A novel…

High Energy Physics - Experiment · Physics 2015-03-20 CMS Collaboration

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

We propose an alternative interpretation of the top events discovered at the Tevatron in 1995. Given that the charge of the $b$ quark jet cannot be measured for the whole sample with certainty, the signal can be due to a quark of charge…

High Energy Physics - Phenomenology · Physics 2008-11-26 Darwin Chang , We-Fu Chang , Ernest Ma

We show that a fourth family of quarks with $m_{t'}$ in the range of (400 - 600) GeV provides a rather simple explanation for the several indications of new physics that have been observed involving CP asymmetries of the b-quark. The…

High Energy Physics - Phenomenology · Physics 2010-01-21 Amarjit Soni , Ashutosh Kumar Alok , Anjan Giri , Rukmani Mohanta , Soumitra Nandi

In theories in which the parameters of the low energy theory are not unique, perhaps having different values in different domains of the universe as is possible in some inflationary models, the fermion masses would be distributed with…

High Energy Physics - Phenomenology · Physics 2016-08-25 John F. Donoghue

If $c$ and $t$ quarks are strongly mixed with a weak singlet charge $2/3$ quark, $BR(t\to \ell\nu + X)$ could be suppressed via the $t\to cH^0$ mode, thereby the top quark could still hide below $M_W$, whereas the heavy quark signal…

High Energy Physics - Phenomenology · Physics 2009-10-28 Wei-Shu Hou , Hsuan-Cheng Huang

We present a new model based on the SU(3)xSU(2)xU(1) symmetry, in which there is a new consistent set of chiral fermion fields that renders the model free from anomalies. The new fermions do not share the usual family structure of the…

High Energy Physics - Phenomenology · Physics 2013-07-23 Alexandre Alves , E. Ramirez Barreto , D. A. Camargo , A. G. Dias

Considering the present limits on the masses of fourth family quarks from the Tevatron experiments, the fourth family quarks are expected to have mass larger than the top quark. Due to their expected large mass they could have different…

High Energy Physics - Phenomenology · Physics 2010-03-02 I. T. Cakir , H. Duran Yildiz , O. Cakir , G. Unel

We present a model to explain LHCb's recent measurements of $R_K$ and $R_{K^{\ast}}$ based on an anomaly-free, spontaneously-broken $U(1)_F$ gauge symmetry, without any fermionic fields beyond those of the Standard Model (SM). The model…

High Energy Physics - Phenomenology · Physics 2021-08-24 B. C. Allanach , Joe Davighi

We suggest a model which addresses both the fermion mass hierarchy problem and the family problem in two-layer warped extra dimensions. In this model, 3 family fermions in 4 dimensions (4D) generate from 1 family in two-layer warped 6D by…

High Energy Physics - Phenomenology · Physics 2009-12-10 Zhi-Qiang Guo , Bo-Qiang Ma
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