2018
DOI: 10.3389/fspas.2018.00040
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Cosmological Aspects of Higgs Vacuum Metastability

Abstract: The current central experimental values of the parameters of the Standard Model give rise to a striking conclusion: metastability of the electroweak vacuum is favoured over absolute stability. A metastable vacuum for the Higgs boson implies that it is possible, and in fact inevitable, that a vacuum decay takes place with catastrophic consequences for the Universe. The metastability of the Higgs vacuum is especially significant for cosmology, because there are many mechanisms that could have triggered the decay… Show more

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Cited by 116 publications
(135 citation statements)
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“…The study of a quantized scalar field in de Sitter space is a mature endeavour [1][2][3][4] possessing well-known difficulties when the field is light [5][6][7][8]. Light spectator scalars in de Sitter space are not just of formal interest, but rather they can have a variety of cosmological implications such as generation of dark matter [9][10][11] or triggering electroweak vacuum decay [12][13][14]. The stochastic approach presented in Refs.…”
Section: Introductionmentioning
confidence: 99%
“…The study of a quantized scalar field in de Sitter space is a mature endeavour [1][2][3][4] possessing well-known difficulties when the field is light [5][6][7][8]. Light spectator scalars in de Sitter space are not just of formal interest, but rather they can have a variety of cosmological implications such as generation of dark matter [9][10][11] or triggering electroweak vacuum decay [12][13][14]. The stochastic approach presented in Refs.…”
Section: Introductionmentioning
confidence: 99%
“…Attacking this problem fully numerically is an interesting option, but goes beyond the scope of this work. 13 In our simulations this happens less than one e-fold after the time where the full potential crosses zero,…”
Section: )mentioning
confidence: 69%
“…H E < 0. 13 At each time N of the evolution we compute the number of e-folds N AdS necessary to fall in AdS with initial conditions given by h = h cl (N ). We say that h cl (N ) ∈ AdS if N AdS < N − N , (3.5) where N − N is the number of e-folds left before the end of inflation when the Higgs starts its classical dynamics at the value h cl (N ).…”
Section: )mentioning
confidence: 99%
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“…However, this part will contribute to the effective potential through the φ dependent loop logarithms. The UV limit of the de Sitter effective potential for the theory (4.1) at one loop level takes the form 3 [40]…”
Section: Yukawa Theory In Curved Spacetimementioning
confidence: 99%