Abstract

The most sensitive haloscopes that search for axion dark matter through the two photon electromagnetic anomaly, convert axions into photons through the mixing of axions with a large DC magnetic field. In this work we apply Poynting theorem to the resulting axion modified electrodynamics and identify two possible Poynting vectors, one similar to the Abraham Poynting vector and the other to the Minkowski Poynting vector in electrodynamics. The latter picks up the extra non-conservative terms while the former does not. To understand the source of energy conversion and power flow in the detection systems, we apply the two Poynting theorems to axion modified electrodynamics, for both the resonant cavity and broadband low-mass axion detectors. We show that both Poynting theorems give the same sensitivity for a resonant cavity axion haloscope, but predict markedly different sensitivity for a low-mass broadband capacitive haloscope. Hence we ask the question, can understanding which one is the correct one for axion dark matter detection, be considered under the framework of the Abraham-Minkowski controversy? In reality, this should be confirmed by experiment when the axion is detected. However, many electrodynamic experiments have ruled in favour of the Minkowski Poynting vector when considering the canonical momentum in dielectric media. In light of this, we show that the axion modified Minkowski Poynting vector should indeed be taken seriously for sensitivity calculation for low-mass axion haloscope detectors in the quasi static limit, and predict orders of magnitude better sensitivity than the Abraham Poynting vector equivalent.

Highlights

  • To gain a significant sensitivity, it is widely considered that the best way to search for the axion is when the first background photonic degree of freedom is a large direct current (DC) magnetic field, which generates a second photon that can be detected

  • In a circuit where the direction of the electric field E1 in a capacitor is parallel to the applied DC magnetic field, B⃗ 0, Eq (37) still holds for the capacitor, with an effective form factor of unity, which can be shown by substituting Eq (44) into (38), and we can use this fact to help calculate the sensitivity of a low-mass capacitor experiment

  • By applying the Poynting theorem to axion modified electrodynamics, we have shown how the sensitivity of a resonant cavity and reactive broadband axion haloscope may be calculated

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Summary

INTRODUCTION

The force on a particle with complex electric polarizability is known not to be derivable from a scalar potential as its curl is nonzero Such forces are nonconservative and nondissipative, and their inclusion has been described both classically and quantum mechanically [96,97], in particular the quantizing of electrodynamics in dielectric and dispersive media [98–100]. It was shown that there exists a similar nonconservative curl force term in axion modified electrodynamics [62,112] This occurs when the axion mixes with a DC background magnetic field, which converts the axion mass to the energy of the second photonic degree of freedom [62,112]. In this work we apply the Minkowski and Abraham Poynting theorem equivalents to axion modified electrodynamics and compare the difference, where the former picks up the extra curl force term, while the latter does not

THE EFFECTIVE AXION CURRENT AND CHARGE DENSITY
Time dependent form
Harmonic phasor form
CALCULATION OF POWER GENERATED IN A DC MAGNETIC FIELD AXION HALOSCOPE USING POYNTING THEOREM
Axion modified Minkowski Poynting theorem
Abraham or Minkowski Poynting theorem in axion modified electrodynamics?
RESONANT CAVITY HALOSCOPE
Cavity dissipated power
Sensitivity from the Abraham Poynting theorem
Sensitivity from the Minkowski Poynting theorem
LOW-MASS BROADBAND AXION HALOSCOPES UNDER DC MAGNETIC FIELD
Capacitor under DC magnetic field
Sensitivity assuming the Abraham Poynting theorem
Sensitivity assuming the Minkowski Poynting theorem
DISCUSSION AND CONCLUSIONS
Axion modified Abraham Poynting theorem
Abraham Poynting theorem
Minkowski Poynting theorem
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