2020
DOI: 10.1007/jhep01(2020)054
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A landscape for the cosmological constant and the Higgs mass

Abstract: The cosmological constant and the Higgs mass seem unnaturally small and anthropically selected. We show that both can be efficiently scanned in Quantum Field Theories with a large enough number of vacua controllable thanks to approximated Z 2 symmetries (even for Coleman-Weinberg potentials). We find that vacuum decay in a landscape implies weaker bounds than previously estimated. Special vacua where one light scalar is accidentally light avoid catastrophic vacuum decay if its self-cubic is absent. This is wha… Show more

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Cited by 9 publications
(6 citation statements)
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References 42 publications
(80 reference statements)
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“…We now consider the same phenomenon in more general theories with scalars, as a multiverse with many vacua mostly comes from scalar vacuum expectation values. As a quantum field theory example, 2 N vacua can arise if each of N scalars s has 2 different vacuum expectation values that minimise the potential [60,61].…”
Section: Dark Matter As Multiverse Relics?mentioning
confidence: 99%
“…We now consider the same phenomenon in more general theories with scalars, as a multiverse with many vacua mostly comes from scalar vacuum expectation values. As a quantum field theory example, 2 N vacua can arise if each of N scalars s has 2 different vacuum expectation values that minimise the potential [60,61].…”
Section: Dark Matter As Multiverse Relics?mentioning
confidence: 99%
“…It is easy to always approximately decouple the landscape to the point of making detection prospects of the multitude of vacua almost non-existent. However it is useful to keep in mind that the more standard string theory (or field theory [47,48]) landscape is not the only option. The landscape can also be entirely contained in our patch of the Universe, either in the form of a scanning field coupled to the Higgs, as is the case for the Relaxion [30], or of feebly interacting copies of the Standard Model, as was proposed in Nnaturalness [31].…”
Section: Early History Of the Universementioning
confidence: 99%
“…It is easy to always approximately decouple the landscape to the point of making detection prospects of the multitude of vacua almost non-existent. However it is useful to keep in mind that the more standard string theory (or field theory [46,47]) landscape is not the only option. The landscape can also be entirely contained in our patch of the Universe, either in the form of a scanning field coupled to the Higgs, as is the case for the Relaxion [29], or of feebly interacting copies of the Standard Model, as was proposed in Nnaturalness [30].…”
Section: General Features Of Cosmological Naturalnessmentioning
confidence: 99%