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Related papers: Hints of New Flavor Physics at LEP?

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For a new family-nonuniversal gauge interaction to be accessible at the LHC it will most likely couple preferentially to the third family. By coupling to all members of the third family the production of a new gauge boson (the $X$ with…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. Holdom

A new $U(1)$ gauge boson coupling predominantly to the third family has been considered in connection with recent LEP data. We consider another likely consequence of such a gauge boson, a greatly enhanced $b$ quark decay mode, $b \to s…

High Energy Physics - Phenomenology · Physics 2009-10-28 B. Holdom , M. V. Ramana

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

A new massive gauge boson (X) coupling 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) extracted from Gamma_h/Gamma_ell.…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Holdom

We consider extensions of the Standard Model with an extra U(1) gauge boson which couples to B-(alpha L_e + beta L_mu + gamma L_tau) with alpha + beta + gamma = 3. We show that the extra gauge boson necessarily mixes with the Z leading to…

High Energy Physics - Phenomenology · Physics 2007-05-23 Lay Nam Chang , Oleg Lebedev , Will Loinaz , Tatsu Takeuchi

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

Assuming the existence of a gauge boson $X$ which couples to $B - 3 L_\tau$, we discuss the present experimental constraints on $g_X$ and $m_X$ from $Z \to l^+ l^-$ and $Z \to \bar f f X~(f = q, \nu_\tau, \tau)$. We also discuss the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Ernest Ma , D. P. Roy

We derive limits on a class of new physics effects that are naturally present in grand unified theories based on extended gauge groups, and in particular in $E_6$ and $SO(10)$ models. We concentrate on $i$) the effects of the mixing of new…

High Energy Physics - Phenomenology · Physics 2010-11-01 Enrico Nardi , Esteban Roulet , Daniele Tommasini

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

Spontaneous breaking of inter-family (horizontal) gauge symmetries can be at the origin of the mass hierarchy between the fermion families. The corresponding gauge bosons have flavor-nondiagonal couplings which generically induce the…

High Energy Physics - Phenomenology · Physics 2018-12-14 Zurab Berezhiani , Benedetta Belfatto

Based on a specific model with U(3) family gauge symmetry at $10^3$ TeV scale, we show its experimental signatures to search for. Since the gauge symmetry is introduced with a special purpose, its gauge coupling constant and gauge boson…

High Energy Physics - Phenomenology · Physics 2011-06-27 Yoshio Koide , Yukinari Sumino , Masato Yamanaka

We consider the extended electroweak gauge group SU(2)_1 \times SU(2)_2 \times U(1)_Y where the first and second families of fermions couple to SU(2)_1 while the third family couples to SU(2)_2. Bounds based an precision electroweak…

High Energy Physics - Phenomenology · Physics 2007-05-23 David J. Muller , Satya Nandi

Gauged extensions [$SU(2)_L\otimes U(1)_Y\otimes U(1)_X$] of the standard $SU(2)_L\otimes U(1)_Y$ model obtained without extending the fermion content of the model are studied. Models that are possible when $U(1)_X$ is identified with some…

High Energy Physics - Phenomenology · Physics 2009-10-28 Gautam Dutta , K. B. Vijaykumar , Anjan S. Joshipura

The existence of anomalous electric($\tilde \kappa$) and/or magnetic($\kappa$) dipole moment couplings between the heavy flavor fermions ($c,b,\tau$) and the $Z$ boson can cause significant shifts in the values of several electroweak…

High Energy Physics - Phenomenology · Physics 2009-10-28 Thomas G. Rizzo

This paper describes recent developments in Heavy Flavour physics at LEP, focusing on a new result from the ALEPH Collaboration on the search for flavour oscillations of the Bs meson. The impact of this analysis on the world combination and…

High Energy Physics - Experiment · Physics 2007-05-23 Andrea Sciaba

Standard Model may allow an extended gauge sector with anomaly-free flavored gauge symmetries, such as $L_{i} - L_{j}$, $B_{i} - L_{j}$, and $B - 3L_{i}$, where $i,j=1,2,3$ are flavor indices. We investigate phenomenological implications of…

High Energy Physics - Phenomenology · Physics 2019-07-17 Eung Jin Chun , Arindam Das , Jinsu Kim , Jongkuk Kim

By extending the standard gauge group to SU(3)_c \times SU(2)_L \times U(1)_Y \times U(1)_X with X charges carried only by the third family we accommodate the LEP measurement of R_b and predict a potentially measurable discrepancy in…

High Energy Physics - Phenomenology · Physics 2009-10-28 Paul H. Frampton , Mark B. Wise , Brian D. Wright

If the minimal standard model of quarks and leptons is extended to include just a righthanded partner to nu_tau, then the quantum number B-3L_tau can be added as a gauge symmetry without the appearance of anomalies. A suitable extension of…

High Energy Physics - Phenomenology · Physics 2009-10-30 Ernest Ma

We discuss the phenomenology of a light U(1) gauge boson, $\gamma_B$, that couples only to baryon number. Gauging baryon number at high energies can prevent dangerous baryon-number violating operators that may be generated by Planck scale…

High Energy Physics - Phenomenology · Physics 2008-02-03 Christopher D. Carone , Hitoshi Murayama

I discuss a model of lepton flavor symmetry based on the non-Abelian finite group T(7) and the gauging of B-L, which has a residual Z(3) symmetry in the charged-lepton Yukawa sector, allowing it to be observable at the Large Hadron Collider…

High Energy Physics - Phenomenology · Physics 2011-03-02 Ernest Ma
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