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Plasma dark matter direct detection

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arxiv 1512.06471 v1 pith:ZHNDJS4E submitted 2015-12-21 astro-ph.GA hep-ph

classification astro-ph.GAhep-ph
keywords darkmatterrecoilsdetectiondirectelectronmodulationplasma
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abstract

Dark matter in spiral galaxies like the Milky Way may take the form of a dark plasma. Hidden sector dark matter charged under an unbroken $U(1)'$ gauge interaction provides a simple and well defined particle physics model realising this possibility. The assumed $U(1)'$ neutrality of the Universe then implies (at least) two oppositely charged dark matter components with self-interactions mediated via a massless "dark photon" (the $U(1)'$ gauge boson). In addition to nuclear recoils such dark matter can give rise to keV electron recoils in direct detection experiments. In this context, the detailed physical properties of the dark matter plasma interacting with the Earth is required. This is a complex system, which is here modelled as a fluid governed by the magnetohydrodynamic equations. These equations are numerically solved for some illustrative examples, and implications for direct detection experiments discussed. In particular, the analysis presented here leaves open the intriguing possibility that the DAMA annual modulation signal is due primarily to electron recoils (or even a combination of electron recoils and nuclear recoils). The importance of diurnal modulation (in addition to annual modulation) as a means of probing this kind of dark matter is also emphasised.

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  1. First direct detection constraint on mirror dark matter kinetic mixing using LUX 2013 data

    hep-ex 2019-08 conditional novelty 6.0 of 10

    A search of 95 live-days of LUX 2013 data finds no mirror dark matter electron recoils, giving 90% confidence upper limits on kinetic mixing for mirror electron temperatures 0.1-0.9 keV and excluding temperatures abov...

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