Abstract

The $\mu$eV-mass axion is one of the most promising candidates for cold dark matter, and remains to be a well-motivated solution to the CP problem of Quantum Chromodynamics (QCD) via the Peccei-Quinn mechanism. In this paper, we propose a novel method to detect the dark-matter axions in our galaxy via the resonant emission $|{\rm e}\rangle \to |{\rm g}\rangle + \gamma + \gamma^{\prime}_{} + a$ (or absorption $a + |{\rm e}\rangle \to |{\rm g}\rangle + \gamma + \gamma^{\prime}_{}$) in an atomic system with superradiance, where $|{\rm e}\rangle$ and $|{\rm g}\rangle$ stand for the excited and ground energy levels of atoms, respectively. A similar process via $|{\rm e}\rangle \to |{\rm g}\rangle + \gamma + a$ (or $a + |{\rm e}\rangle \to |{\rm g}\rangle + \gamma$) is also put forward to probe the axion-electron coupling. For the nominal experimental setup assuming a background-free environment, most of the parameter space for typical QCD axion models can be covered with parahydrogen molecules or ytterbium atoms. However, the background in a realistic experimental setup remains to be a major issue that needs to be solved in future studies. Searching for better atomic or molecular candidates may be required for a bigger signal-to-noise ratio.

Highlights

  • More than forty years ago, Peccei and Quinn (PQ) proposed an appealing solution to the charge-parity (CP) problem of quantum chromodynamics (QCD) by introducing a dynamical scalar field and imposing a global Uð1ÞPQ symmetry on the whole Lagrangian [1,2]. It was Weinberg [3] and Wilczek [4] who shortly discovered that a Nambu-Goldstone boson, i.e., the axion, arose from the spontaneous breaking of the PQ symmetry at some high-energy scale

  • The original model with the PQ symmetry spontaneously broken at the electroweak scale ΛEW ≡ 102 GeV has been ruled out, the “invisible” axion models, such as the KSVZ model [5,6] and the DFSZ model [7,8], are still attracting a lot of attention

  • Apart from providing a solution to the strong CP problem, these models indicate that axions can be a good candidate for cold dark matter in our Universe [9,10,11,12,13] and can be detected in realistic experiments [14,15,16,17]

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Summary

INTRODUCTION

More than forty years ago, Peccei and Quinn (PQ) proposed an appealing solution to the charge-parity (CP) problem of quantum chromodynamics (QCD) by introducing a dynamical scalar field and imposing a global Uð1ÞPQ symmetry on the whole Lagrangian [1,2]. Out that the QCD axions within a particular mass region 1 μeV ≲ ma ≲ 104 μeV survive all the experimental constraints and can make up the entire cold dark matter For this reason, many interesting ideas have been proposed to test the QCD axion models in this region [22,23,24,25,26,27,28,29,30,31,32,33,34,35]. In order to increase the rate, we can use two triggering laser beams corresponding to the photon modes of γ1 and γ2 to help stimulate the atomic transitions. On this point, our method is different from the one suggested in Ref.

ATOMIC SUPERRADIANCE
TRANSITION AMPLITUDE
TRANSITION RATE
AXION-ELECTRON COUPLING
CONCLUSIONS
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