2018
DOI: 10.1016/j.physletb.2017.11.017
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Low temperature electroweak phase transition in the Standard Model with hidden scale invariance

Abstract: We discuss a cosmological phase transition within the Standard Model which incorporates spontaneously broken scale invariance as a low-energy theory. In addition to the Standard Model fields, the minimal model involves a light dilaton, which acquires a large vacuum expectation value (VEV) through the mechanism of dimensional transmutation. Under the assumption of the cancellation of the vacuum energy, the dilaton develops a very small mass at 2-loop order. As a result, a flat direction is present in the classi… Show more

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Cited by 32 publications
(20 citation statements)
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References 42 publications
(36 reference statements)
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“…It is however of importance for models in which the barrier becomes weaker at low temperature, see e.g. [33,34,56]. Another observation from Table 1 is that the two quantities (R H p ) −1 and α α+1 (which will be important in the next section) approach 1 for lower and lower values of κ.…”
Section: Numerical Solutionsmentioning
confidence: 86%
See 2 more Smart Citations
“…It is however of importance for models in which the barrier becomes weaker at low temperature, see e.g. [33,34,56]. Another observation from Table 1 is that the two quantities (R H p ) −1 and α α+1 (which will be important in the next section) approach 1 for lower and lower values of κ.…”
Section: Numerical Solutionsmentioning
confidence: 86%
“…2 was mainly introduced as a case of study to illustrate the dynamics of a supercooled and long-lasting PT. We expect other theories to present similar features, especially a class of scale-invariant models with very light scalar particles [33][34][35].…”
Section: Gravitational Wave Productionmentioning
confidence: 99%
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“…In Ref. [21], the possibility of a first order QCD transition with electroweak symmetry breaking after QCD confinement has been considered and analyzed in some detail; see also Re.f [22] 3 .…”
mentioning
confidence: 99%
“…3 Re.f [22] maintains that M ⊙ PBHs form, as it implicitly assumes that no supercooling takes place according to its adopted underlying theory. Instead, we choose to implement the first order QCD transition through initially suppressed quark Yukawa couplings, assuming electroweak symmetry is broken, thereby avoiding possible difficulties related to vacuum energy domination.…”
mentioning
confidence: 99%