2019
DOI: 10.1103/physrevd.99.115010
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Phase transitions and gravitational wave tests of pseudo-Goldstone dark matter in the softly broken U(1) scalar singlet model

Abstract: We study phase transitions in a softly broken U (1) complex singlet scalar model in which the dark matter is the pseudo-scalar part of a singlet whose direct detection coupling to matter is strongly suppressed. Our aim is to find ways to test this model with the stochastic gravitational wave background from the scalar phase transition. We find that the phase transition which induces vacuum expectation values for both the Higgs boson and the singlet -necessary to provide a realistic dark matter candidate -is al… Show more

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Cited by 33 publications
(15 citation statements)
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References 58 publications
(63 reference statements)
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“…In the model with a global U(1) group explicitly broken down to Z 2 symmetry, ref. [50] shows that all phase transitions leading to the correct vacuum are of the second order. Furthermore, ref.…”
Section: Jhep07(2020)082 Introductionmentioning
confidence: 94%
“…In the model with a global U(1) group explicitly broken down to Z 2 symmetry, ref. [50] shows that all phase transitions leading to the correct vacuum are of the second order. Furthermore, ref.…”
Section: Jhep07(2020)082 Introductionmentioning
confidence: 94%
“…[11,12]), the global U(1) symmetry is explicitly broken down to a Z 2 symmetry by the DM mass term. In this case, the electroweak phase transition is of second order [13]. If the U(1) symmetry is explicitly broken to Z 3 [14] or to nothing, the resulting cubic terms of the general model can induce, in part of the parameter space, strong first-order phase transitions [15][16][17] JHEP10(2020)080…”
Section: Introductionmentioning
confidence: 99%
“…Such a situation can be circumvented if one can effectively suppress DM-nucleon scattering at zero momentum transfer without reducing DM annihilation at the freeze-out epoch. An appealing approach to achieve this is provided by Higgs-portal pseudo-Nambu-Goldstone boson (pNGB) DM models [7][8][9][10][11][12][13][14][15][16][17][18][19][20], where the DM candidate is a pNGB protected by a global symmetry which is softly broken by quadratic mass terms. The pNGB nature makes the tree-level DM-nucleon scattering amplitude vanish in the zero momentum transfer limit [7].…”
Section: Introductionmentioning
confidence: 99%