2019
DOI: 10.1103/physrevd.99.055010
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Solutions to axion electrodynamics in various geometries

Abstract: Recently there has been a surge of new experimental proposals to search for ultra-light axion dark matter with axion mass, ma 1 µeV. Many of these proposals search for small oscillating magnetic fields induced in or around a large static magnetic field. Lately, there has been interest in alternate detection schemes which search for oscillating electric fields in a similar setup. In this paper, we explicitly solve Maxwell's equations in a simplified geometry and demonstrate that in this mass range, the axion in… Show more

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Cited by 59 publications
(74 citation statements)
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“…Since we are in free space we have µ = 1, = 1, ρ f = 0, and J f = 0. A full analytic solution can be obtained with the theory of retarded potentials for the axion charge and current terms [59,60] as in equations (2.13) and (2.14), because in our approach the axion-Maxwell equations are decoupled. This gives an electric field of…”
Section: Free Spacementioning
confidence: 99%
“…Since we are in free space we have µ = 1, = 1, ρ f = 0, and J f = 0. A full analytic solution can be obtained with the theory of retarded potentials for the axion charge and current terms [59,60] as in equations (2.13) and (2.14), because in our approach the axion-Maxwell equations are decoupled. This gives an electric field of…”
Section: Free Spacementioning
confidence: 99%
“…Using further that the external B-field is generated by a current j e with ∇ × B ext = j e one can rewrite this expression as 2 [17] (up to a missing factor 1/4π). There, they have been derived as solutions of the Maxwell's equations with the method of retarded Green's functions, confirming the equivalence of the two methods.…”
Section: Zero-velocity Axionsmentioning
confidence: 99%
“…We discuss the effect of gradient terms, and show that in the limit of a homogeneous axion field, we recover the results of Refs. [17,18], which were obtained by solving the classical Maxwell's equations to leading order in g aγ and imposing the relevant boundary conditions. In section 3, we provide an explicit example by applying our method to the case of an infinitely long solenoid.…”
Section: Introductionmentioning
confidence: 99%
“…The Lagrangian (1) implies that a time-dependent background density of ADM modifies Maxwell's equations. In particular, in the presence of a static magnetic field B 0 , ADM generates an oscillating magnetic field, B a , as if sourced by an effective AC current density parallel to B 0 [8], J eff = g aγγ 2ρ DM B 0 cos(m a t).…”
Section: Introductionmentioning
confidence: 99%