Abstract

We investigate the properties of a stochastic gravitational wave background produced by a first-order electroweak phase transition in the regime of extreme supercooling. We study a scenario whereby the percolation temperature that signifies the completion of the transition, T_mathrm{p}, is as low as a few MeV (nucleosynthesis temperature), while most of the true vacuum bubbles are formed much earlier at the nucleation temperature, T_mathrm{n}sim 50 GeV. This implies that the gravitational wave spectrum is mainly produced by the collisions of large bubbles and characterised by a large amplitude and a peak frequency as low as f sim 10^{-9}{-}10^{-7} Hz. We show that such a scenario can occur in (but not limited to) a model based on a non-linear realisation of the electroweak gauge group, so that the Higgs vacuum configuration is altered by a cubic coupling. In order to carefully quantify the evolution of the phase transition of this model over such a wide temperature range we go beyond the usual fast transition approximation, taking into account the expansion of the Universe as well as the behaviour of the nucleation probability at low temperatures. Our computation shows that there exists a range of parameters for which the gravitational wave spectrum lies at the edge between the exclusion limits of current pulsar timing array experiments and the detection band of the future Square Kilometre Array observatory.

Highlights

  • Cosmological phase transitions (PTs) are predicted by many particle physics models with important consequences on the dynamics of the Universe

  • The peak frequency of a stochastic gravitational waves (GWs) background produced by a PT near the electroweak scale, TEW ∼ 100 GeV, is expected to lie in the millihertz range which coincides with the projected sensitivity of the future eLISA space-based interferometer [12]

  • The characteristic frequency and amplitude of the spectrum are derived from the dynamics of the PT and depend on a few key parameters: the duration of the transition, the size of colliding bubbles, the bubble-walls velocity and the fraction of vacuum energy transferred into the bubble walls

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Summary

Introduction

Cosmological phase transitions (PTs) are predicted by many particle physics models with important consequences on the dynamics of the Universe. The peak frequency of a stochastic GW background produced by a PT near the electroweak scale, TEW ∼ 100 GeV, is expected to lie in the millihertz range which coincides with the projected sensitivity of the future eLISA space-based interferometer [12] This motivated a series of investigations into the production of GWs in various BSM models, see e.g. A barrier exists between the two different phases of the Higgs field from the electroweak scale down to zero temperature, allowing a significant amount of supercooling This model exhibits a range of parameters for which the PT is long-lasting, meaning that most of the true vacuum bubbles are nucleated around T ∼ 50 GeV but collide well below the electroweak scale, as low as T ∼ [0.1, 10] GeV. We discuss our results and approximations in the conclusion

A non-linearly realised electroweak gauge group
Prolonged electroweak phase transition
Decay probability
Bubble dynamics and energy
Equation of state
Numerical solutions
Gravitational wave production
Conclusion
Findings
Finite temperature potential
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