A dipole amplifier for electric dipole moments, axion-like particles and a dense dark matter hairs detector

preprint2016arXivOpen access

Abstract

A tool that can constrain, in minutes, beyond-the-standard-model parameters like electric dipole moments (EDM) down to a lower-bound deN<10−37e⋅cmd_\text{e}^{\cal{N}}<10^{-37}\text{e}\cdot\text{cm} in bulk materials, or the coupling of axion-like particles (ALP) to photons down to ∣Gaγγ∣<10−16|G_{aγγ}|<10^{-16}~GeV−1^{-1}, is described. Best limits are den<3⋅10−26e⋅cmd^n_e<3\cdot10^{-26}\text{e}\cdot\text{cm} for neutron EDM and ∣Gaγγ∣<6.6⋅10−11|G_{aγγ}|<6.6\cdot10^{-11}~GeV−1^{-1}. The {\it dipole amplifier} is built from a superconducting loop immersed in a toroidal magnetic field, B⃗\vec{B}. When nuclear magnetic moments in the London penetration depth align with B⃗\vec{B}, the bulk magnetization is always accompanied by an EDM-induced bulk electric field E⃗∝B⃗\vec{E}\propto\vec{B} that generates detectable oscillatory supercurrents with a characteristic frequency ωD∝deNω_{\text{D}}\propto d_\text{e}^{\cal{N}}. Cold dark matter (CDM) ALP are formally similar where ωD∝∣Gaγγ∣na/(2ma)ω_\text{D}\propto |G_{aγγ}|\sqrt{n_a/(2m_a)} with mam_a the ALP mass and nan_a its number density. A space probe traversing a dark matter hair with a dipole amplifier is sensitive enough to detect ALP density variations if ∣Gaγγ∣nh/(2ma)>4.9⋅10−27|G_{aγγ}|\sqrt{n_h/(2m_a)}>4.9\cdot10^{-27} where nhn_h is the ALP number density in the hair.

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