Some theoretical and experimental aspects of axion physics
In the first part of the thesis, we revisit the Dine-Fischler-Srednicki-Zhitnisky axion model in light of the recent Higgs LHC results and electroweak precision data. This model is an extension of the two-Higgs-doublet model incorporating a PQ symmetry which leads to a physically acceptable axion. F...
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Zusammenfassung: | In the first part of the thesis, we revisit the
Dine-Fischler-Srednicki-Zhitnisky axion model in light of the recent Higgs LHC
results and electroweak precision data. This model is an extension of the
two-Higgs-doublet model incorporating a PQ symmetry which leads to a physically
acceptable axion. For generic values of the couplings, the model reproduces the
minimal Standard Model, with a massless axion and all the other degrees of
freedom at a very high scale. However, in some scenarios, the extra Higgses
could be relatively light. We use the oblique corrections, in particular
$\Delta\rho$, to constrain the mass spectrum in this case. Finally, we also
work out the non-linear parametrization of the DFSZ model in the generic case
where all scalars except the lightest Higgs and the axion have masses at or
beyond the TeV scale.
In the second part, we study the relevance of a cold axion background (CAB)
as a responsible for the dark matter in the Universe and examine its
consequences through its effects on photon and cosmic ray propagation. We study
the axion-photon system under the joint influence of two backgrounds: an
external magnetic field and a CAB. Their effect consists in producing a
three-way mixing of the axion with the two polarizations of the photon. We
determine the proper frequencies and eigenvectors as well as the corresponding
photon ellipticity and induced rotation of the polarization plane that depend
both on the magnetic field and the local density of axions. We also comment on
the possibility that some of the predicted effects could be measured in optical
table-top experiments.
Circularly polarized photons are energy eigenstates, with a modified
dispersion relation. This enables the emission of a photon by a charged
particle, which is forbidden in regular QED. We study the energy loss of a
cosmic ray due and compute the energy flux of photons emitted in this way. |
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DOI: | 10.48550/arxiv.1512.03311 |