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相关论文: The top quark mass in the minimal top condensation…

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I discuss the properties of the minimal supersymmetric extension of the standard model, in the case in which there is a dynamical breakdown of the electroweak symmetry induced by the formation of condensates of the third generation of…

高能物理 - 唯象学 · 物理学 2007-05-23 C. E. M. Wagner

The electroweak symmetry may be broken by a composite Higgs which arises naturally as a bound state of the top quark if the standard model gauge fields and fermions propagate in extra dimenions. The top quark mass and the Higgs mass can be…

高能物理 - 唯象学 · 物理学 2009-10-31 Hsin-Chia Cheng

The condition of unification of gauge couplings in the minimal supersymmetric standard model provides successful predictions for the weak mixing angle as a function of the strong gauge coupling and the supersymmetric threshold scale. In…

高能物理 - 唯象学 · 物理学 2009-09-25 M. Carena , S. Pokorski , M. Olechowski , C. E. M. Wagner

Recently, a new class of realistic models for electroweak symmetry breaking have been constructed, without supersymmetry. These theories have naturally light Higgs bosons and perturbative new physics at the TeV scale. We describe these…

高能物理 - 唯象学 · 物理学 2011-01-13 Nima Arkani-Hamed , Andrew G. Cohen , Thomas Gregoire , Jay G. Wacker

It is shown, using dispersion relations techniques for bound states, that the presence of a large top-Yukawa coupling lowers the Higgs mass from the condensate-model value of twice the top mass (~350 Gev) to 100-200 Gev consistent with the…

高能物理 - 唯象学 · 物理学 2007-05-23 Bipin R. Desai , Alexander R. Vaucher

In the two Higgs doublet model, perturbativity breaks down below the Planck scale: For top mass values 170-180 GeV, the Yukawa coupling reaches the pole below 1000 TeV, if the ratio of vev's v_u/v_d is below 1. We discuss top condensate…

高能物理 - 唯象学 · 物理学 2007-05-23 R. Bonisch

We describe a deconstructed Higgsless model in which electroweak symmetry breaking results largely from a Higgsless mechanism while the top quark mass is generated by a topcolor mechanism. The top quark mass arises from a Yukawa coupling to…

高能物理 - 唯象学 · 物理学 2010-09-15 R. Sekhar Chivukula , Neil D. Christensen , Baradhwaj Coleppa , Elizabeth H. Simmons

In the scenarios with heavy top squarks, mass parameters of the Higgs field must be fine-tuned due to a large logarithmic correction to the soft scalar mass. We consider a new possibility that the top Yukawa coupling is small above TeV…

高能物理 - 唯象学 · 物理学 2009-11-11 Tatsuo Kobayashi , Hiroaki Nakano , Haruhiko Terao

In the standard electroweak model, the measured top quark mass requires a sizeable Yukawa coupling to the fundamental scalar. This large coupling alone might induce a dynamical breaking of the electroweak symmetry as well as…

高能物理 - 唯象学 · 物理学 2009-10-28 D. Delepine , J. -M. Gerard , R. Gonzalez Felipe

I analyze the predictions for the strong gauge coupling, $\alpha_3(M_Z) $, and the top quark and light Higgs masses in the framework of gauge and bottom-tau Yukawa coupling unification in the minimal supersymmetric standard model. These…

高能物理 - 唯象学 · 物理学 2007-05-23 M. Carena

Electroweak symmetry can be naturally broken by observed quark and gauge fields in various extra-dimensional configurations. No new {\it fundamental} fields are required below the quantum gravitational scale ($\sim$ 10 - 100 TeV). We…

高能物理 - 唯象学 · 物理学 2009-10-31 Hsin-Chia Cheng , Bogdan A. Dobrescu , Christopher T. Hill

The principles of finiteness and reduction of couplings can be applied to achieve Gauge-Yukawa Unification. It is found that the observed top-bottom hierarchy and the top quark mass naturally follow if there exists Gauge-Yukawa Unification…

高能物理 - 理论 · 物理学 2016-09-06 Jisuke Kubo , Myriam Mondragon , George Zoupanos

Strong gauge and top-Yukawa couplings predicted in the presence of extra dimensions lead to a trickle-down effect of the top-coupling through the renormalization group equations for the quark Yukawa matrices. The matrix elements for the u…

高能物理 - 唯象学 · 物理学 2007-05-23 Bipin R. Desai , Alexander R. Vaucher

We show that if the Standard Model gauge fields and fermions propagate in extra dimenions, a composite Higgs field with the correct quantum number can arise naturally as a bound state due to the strong gauge interactions in higher…

高能物理 - 唯象学 · 物理学 2009-10-31 Hsin-Chia Cheng

An overview of top physics and phenomenology at a high-energy linear collider is presented. A comprehensive study of top quark physics is possible at such a facility. The unique threshold production of top pairs would provide measurements…

高能物理 - 唯象学 · 物理学 2007-05-23 Raymond Frey

`Little Higgs' models, in which the Higgs particle arises as a pseudo-Goldstone boson, have a natural mechanism of electroweak symmetry breaking associated with the large value of the top quark Yukawa coupling. The mechanism typically…

高能物理 - 唯象学 · 物理学 2009-11-10 Maxim Perelstein , Michael E. Peskin , Aaron Pierce

The top quark may get its mass not from a fundamental scalar but a Nambu-Jona-Lasinio mechanism involving a strongly coupled gauge sector that triggers top-quark condensation. Forbidding a large hierarchy in the gap equation implies that…

高能物理 - 唯象学 · 物理学 2009-10-30 James D. Wells

We propose a new mechanism in which all of the electroweak symmetry breaking is driven by a natural top quark condensate, produced by topcolor interactions at a multi-TeV scale. The scheme allows the observed top quark mass, and acceptable…

高能物理 - 唯象学 · 物理学 2009-10-30 Bogdan A. Dobrescu , Christopher T. Hill

The one-loop evolution of Yukawa couplings in the minimal supersymmetric left-right model (MSUSYLR) model with a wide variation of the right handed breaking scale $M_R$ from 1 TeV to $10^{18}$ GeV is studied assuming that all third…

高能物理 - 唯象学 · 物理学 2010-01-06 Biswajoy Brahmachari

The top-quark Yukawa coupling is too large to permit radiative electroweak symmetry breaking to occur for small values of y, the Higgs self-coupling, to leading-logarithm order. However, a large y solution leading to a viable Higgs mass of…

高能物理 - 唯象学 · 物理学 2008-11-26 V. Elias , R. B. Mann , D. G. C. McKeon , T. G. Steele
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