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Verfasst von:Alonso Álvarez, Gonzalo [VerfasserIn]   i
 Jaeckel, Joerg [VerfasserIn]   i
Titel:Exploring ALPs beyond the canonical
Verf.angabe:Gonzalo Alonso-Álvarez and Joerg Jaeckel
E-Jahr:2017
Jahr:20 Dec 2017
Umfang:41 S.
Fussnoten:Identifizierung der Ressource nach: Last revised 12 Jul 2018 ; Gesehen am 15.12.2020
Titel Quelle:Enthalten in: De.arxiv.org
Ort Quelle:[S.l.] : Arxiv.org, 1991
Jahr Quelle:2017
Band/Heft Quelle:(2017) Artikel-Nummer 1712.07500, 41 Seiten
Abstract:Axion-like particles (ALPs) are interesting dark matter candidates both from the theoretical as well as from the experimental perspective. Usually they are motivated as pseudo-Nambu-Goldstone bosons. In this case one of their most important features is that their coupling to other particles is suppressed by a large scale, the vacuum expectation value of the field breaking the symmetry that gives rise to them. This naturally endows them with very weak interactions but also restricts the maximal field value and therefore the regions where sufficient dark matter is produced. In this paper we investigate deviations from this simplest setup, where the potential and interactions are as expected for a pseudo-Nambu-Goldstone boson, but the kinetic term has singularities. This leads to a significantly increased area in parameter space where such particles can be dark matter and can be probed by current and near future experiments. We discuss cosmological limits and in the course of this give a simple derivation of a formula for isocurvature fluctuations in models with general anharmonic potentials. As an application of this formula we give an update of the isocurvature constraints for QCD axion dark matter models, using the most recent results for the QCD topological susceptibility and the newest Planck data.
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Kostenfrei: Volltext: http://arxiv.org/abs/1712.07500
Datenträger:Online-Ressource
Sprache:eng
Sach-SW:Astrophysics - Cosmology and Nongalactic Astrophysics
 High Energy Physics - Phenomenology
K10plus-PPN:1570670390
Verknüpfungen:→ Sammelwerk

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