4.7 Article

Rich structure of nonthermal relativistic CMB spectral distortions from high energy particle cascades at redshifts z ≲ 2 x 105

Journal

PHYSICAL REVIEW D
Volume 99, Issue 4, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.99.043520

Keywords

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Funding

  1. Science and Engineering Research Board (SERB) of Department of Science and Technology, Government of India [ECR/2015/000078]
  2. MPG-DST
  3. Max-Planck-Gesellschaft

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It is generally assumed that for energy injection before recombination, all of the injected energy is dissipated as heat in the baryon-photon plasma, giving rise to the y-type, i-type, and mu-type distortions in the cosmic microwave background (CMB) spectrum. We show that this assumption is incorrect when the energy is injected in the form of energetic (i.e., energy much greater than the background CMB temperature) particles. We evolve the electromagnetic cascades, from the injection of high energy particles, in the expanding Universe and follow the nonthermal component of CMB spectral distortions resulting from the interaction of the electromagnetic shower with the background photons, electrons, and ions. The electromagnetic shower loses a substantial fraction of its energy to the CMB spectral distortions before the energy of the particles in the shower has degraded to low enough energies that they can thermalize with the background plasma. This spectral distortion is the result of the interaction of nonthermal energetic electrons in the shower with the CMB and thus has a shape that is substantially different from the y-type or i-type distortions. The shape of the final nonthermal relativistic (ntr-type) CMB spectral distortion depends upon the initial energy spectrum of the injected electrons, positrons, and photons and thus has information about the energy injection mechanism, e.g., the decay or annihilation channel of the decaying or annihilating dark matter particles. The shape of the spectral distortion is also sensitive to the redshift of energy injection. Our calculations open up a new window into the energy injection at z less than or similar to 2 x 10(5) which is not degenerate with, and can be distinguished from the low redshift thermal y-type distortions.

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