Origin of Symmetries 1991
DOI: 10.1142/9789814329057_0016
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Constraints imposed by CP conservation in the presence of pseudoparticles

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Cited by 392 publications
(672 citation statements)
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“…All bounds are derived assuming that the Peccei-Quinn mechanism [29] is at work. We pay special attention to the role of hadronic and nuclear uncertainties.…”
Section: Jhep02(2016)011mentioning
confidence: 99%
“…All bounds are derived assuming that the Peccei-Quinn mechanism [29] is at work. We pay special attention to the role of hadronic and nuclear uncertainties.…”
Section: Jhep02(2016)011mentioning
confidence: 99%
“…It is then natural to identify the scale M I with the breaking scale f a of a PQ symmetry U(1) PQ [18], which resolves the strong CP problem. Moreover, the µ parameter of MSSM could be obtained as µ ∼ f 2 a /m P ∼ m 3/2 [19].…”
Section: A Simultaneous Solution Of the Strong Cp And µ Problemsmentioning
confidence: 99%
“…The strong CP problem can be elegantly resolved by including a Peccei-Quinn (PQ) symmetry [18] broken spontaneously at an intermediate mass scale, which can be easily generated within the supergravity (SUGRA) extension of MSSM. The PQ field, which breaks the PQ symmetry, corresponds, in this case, to a flat direction in field space lifted by non-renormalizable interactions.…”
Section: Introductionmentioning
confidence: 99%
“…A DM relic particle candidate must be non-relativistic, must be stable on the cosmological time scale, and must interact weakly with other particles. Some of the possible candidates are: WIMPS [16], axions [17,18,19,20,21], MeV-scalar fields [22,23], technicolor candidates [24,25,26], and ultra-light scalar fields [27,28,29,30,31,32]. An ultra-light scalar field is motivated as DM because it can alleviate some of the problems that arise at galactic scale in the standard paradigm of cold DM, namely, the origin of cuspy halos [33] and the overproduction of substructure [34].…”
Section: Introductionmentioning
confidence: 99%