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Electroweak Symmetry Breaking via Top Condensation Seesaw
High Energy Physics - Phenomenology · Submitted 9 Dec 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim 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.
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The abstract, sentence by sentence
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 T and S parameters, by invoking a seesaw mechanism involving mixing of the top with an additional isosinglet quark.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | 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. | contribution 0.99 | 0.70 | 0.69 | asserted 0.58 |
| s1 | The scheme allows the observed top quark mass, and acceptable T and S parameters, by invoking a seesaw mechanism involving mixing of the top with an additional isosinglet quark. | method 0.58 | 0.58 | 0.17 | asserted 0.73 |
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The paper
Original abstract
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 T and S parameters, by invoking a seesaw mechanism involving mixing of the top with an additional isosinglet quark.
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References
How the literature uses it
36 arXiv papers cite this in 44 sentences
Papers citing it · 22 sentences without a confident label
Cites it as background 22 papers
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In Top Seesaw models [ref] , an additional $SU(2)_L$-singlet vector-like quark $T$ with the same electric charge as the top quark is introduced.
Explaining the $R_{K^{(*)}}$ anomalies and the CDF $M_W$ in Flavorful Top Seesaw Models with Gauged $U(1)_{L(-R)}$ · The $U(3)_L/U(2)_L$ Top Seesaw model · 0.98
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Moreover the mixing of vector-like quarks with the third generation and in particular the top quark is a common feature in little Higgs models [ref] and composite Higgs models based on top condensation [ref] .
Bounds and Decays of New Heavy Vector-like Top Partners · Introduction · 0.87
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Another possibility is that the Higgs doublet is a bound state of the top quark with a vectorlike quark, as in the top seesaw model [ref] .
Quark and lepton masses from top loops · Conclusions · 0.81
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