Abstract

We discuss the axion dark matter (DM) condensate and the consequences the interactions of dark matter would have on the spectrum of collective modes. We find that DM self-interactions change the spectrum of excitations from a quadratic to a linearlike dispersion with velocity ${v}_{s}$ which is set by the interactions, but dominated by gravity. For typical DM densities and interactions we find ${v}_{s}\ensuremath{\sim}{10}^{\ensuremath{-}12}c$. This soundlike mode corresponds to DM density oscillations just like in any other Bose liquid, hence we call it dark sound (DS). The DS mode is well defined and describes stable density oscillations at intermediate length scales $k\ensuremath{\ge}{k}_{\mathrm{min}}\ensuremath{\sim}{10}^{4}\text{ }\text{ }{\mathrm{lyr}}^{\ensuremath{-}1}$. In the extreme long-wavelength limit gravity dominates and leads to Jeans instability of the sound mode at the scale of clump formation $k\ensuremath{\le}{k}_{\mathrm{min}}$. We also discuss the possible observable consequences of the DS, including quantized DS modes inside clumps, their characteristic energy, and noise features that might facilitate the observation of DM.

Highlights

  • Dark matter (DM) [1] makes a vivid gravitational imprint on visible matter, but the rest of its nature is yet to be understood

  • (v) We find that coupling of DM to sources like photons has the potential to stabilize clumps and induce a gap in the dark sound (DS) mode

  • In this paper we discussed the axion DM density oscillations that result in DS modes

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Summary

INTRODUCTION

Dark matter (DM) [1] makes a vivid gravitational imprint on visible matter, but the rest of its nature is yet to be understood. Significant attention in the field is devoted to the notion that the BEC of bosonic DM is subject to attractive interactions If this is the case a homogeneous ground state is not possible and the BEC state forms clumps with no infinite-range phase coherence. For the fluctuations of the axion field away from its mean value we have a finite hδa 2ðr; tÞi; δaðr; tÞ 1⁄4 aðr; tÞ − hai, and the size of these fluctuations will be controlled by the characteristic energy of DM that, presumably, is set by the decoupling energy of dark sector. VI we summarize the results and provide an outlook for possible observable consequences of DS in our search for DM signatures

Axion interactions
The axion condensate
The meaning of the condensed phase
Condensation solution
The dark sound mode
CLUMPY DARK MATTER
Gravity dominates at galactic densities
Form of the clumps
Dark sound normal modes
Numerical simulations
Estimates
Shape of the axion signal
Localized clump modes and specific heat
Summary
Comparison with related approaches
Outlook
Relativistic complex scalar with attractive interaction
Findings
Sine-Gordon model
Full Text
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