Abstract

We derive novel constraints on millicharged dark matter and ultralight axion-like particles using pulsar timing and fast radio burst observations. Millicharged dark matter affects the dispersion measure of the time of arrival of radio pulses in a way analogous to free electrons. Light pseudo-scalar dark matter, on the other hand, causes the polarization angle of radio signals to oscillate. We show that current and future data can set strong constraints in both cases. For dark matter particles of charge $\epsilon e$, these constraints are ${\epsilon}/{m_{\rm milli}} \lesssim 10^{-8}{\rm eV}^{-1}$, for masses $m_{\rm milli}\gtrsim 10^{-6}\,$eV. For axion-like particles, the analysis of signals from pulsars yields constraints in the axial coupling of the order of $g/m_a\lesssim 10^{-13} {\rm GeV}^{-1}/(10^{-22}{\rm eV})$. Both bounds scale as $(\rho/\rho_{\rm dm})^{1/2}$ if the energy density $\rho$ of the components is a fraction of the total dark matter energy density $\rho_{\rm dm}$. We do a detailed study of both effects using data from two samples of pulsars in the galaxy and in globular clusters, as well as data from FRB 121102 and PSR J0437$-$4715. We show that in both cases actual pulsar data constrain a new region of the parameter space for these models, and will improve with future pulsar-timing observations.

Highlights

  • Unraveling the nature of dark matter (DMa) is among the most urgent issues in fundamental physics

  • We present new results for DMa models directly coupled to light from the propagation of radio pulses from pulsars and fast radio bursts (FRBs)

  • We focus on the case of millicharged DMa, i.e., g 1⁄4 0

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Summary

INTRODUCTION

Unraveling the nature of dark matter (DMa) is among the most urgent issues in fundamental physics. We derive stringent constraints on millicharged DMa and axionlike particles (ALPs) based on dispersion measurements (DMs) of radio signals from pulsars and FRBs, and on the modulation of. We give a unified treatment, where the millicharged DMa and ALPs are considered as independent species In the former case, we consider that (a fraction of) the DMa is made of particles with mass mmilli and electric charge q 1⁄4 εe (ε ≪ 1) [11,12,13,14,15,16,17,18]. 4πεejνmilli g 2 εμρλν Fμρ ∂ λ φ; ð2Þ where g is the ALP-photon axial coupling, jν is the ordinary electron current, whereas jνmilli is the current from millicharged particles The role of this term in the propagation of radio waves will be studied, under the.

DISPERSION IN THE TOA
TOA CONSTRAINTS ON MILLICHARGED DMa
POLARIZATION CONSTRAINTS ON ALPS
DISCUSSION
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