1996
DOI: 10.1103/physrevd.53.5185
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GIM violation and new dynamics of the third generation

Abstract: In strong dynamical schemes for electroweak symmetry breaking the third generation must be treated in a special manner, owing to the heavy top quark. This potentially leads to new flavor physics involving the members of the third generation in concert with the adjoining generations, with potential novel effects in b-flavored and charm physics. We give a general discussion and formulation of this kind of physics, abstracted largely from top-color models which we elaborate in detail. We identify sensitive channe… Show more

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Cited by 209 publications
(290 citation statements)
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References 58 publications
(80 reference statements)
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“…These new particles treat the third generation fermions differently from those in the first and second generations. The couplings of the gauge boson Z ′ relevant to our calculation can be written as [11,12]:…”
mentioning
confidence: 99%
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“…These new particles treat the third generation fermions differently from those in the first and second generations. The couplings of the gauge boson Z ′ relevant to our calculation can be written as [11,12]:…”
mentioning
confidence: 99%
“…To obtain the top quark condensation and not form the bottom quark condensation, there must be tan θ ′ ≪ 1 [9,11].…”
mentioning
confidence: 99%
“…To completely avoid the problems, such as triviality and unnaturaless arising from the elementary Higgs in the SM, various kinds of dynamical models are proposed and among which T C2 models and flavor-universal T C2 models are very interesting because they can explain the large top quark mass and provide possible dynamics of elecroweak symmetry breaking(EWSB) [3]. A common feature of these models is that the SM gauge groups are extended at energy well above the weak scale.…”
mentioning
confidence: 99%
“…The flavor-diagonal couplings of the non-universal gauge boson Z ′ to fermions, which are related our calculation, can be written as [3,7]:…”
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confidence: 99%
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