4.7 Article

Probing axionlike particles via cosmic microwave background polarization

Journal

PHYSICAL REVIEW D
Volume 103, Issue 6, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.103.063508

Keywords

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Funding

  1. World Premier International Research Center Initiative (WPI Initiative), MEXT, Japan
  2. Program of Excellence in Photon Science
  3. Advanced Leading Graduate Course for Photon Science
  4. Japan Society for the Promotion of Science (JSPS) KAKENHI [JP18K13537, JP19J21974, JP20K14497, JP20J20248]

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The study suggests that ALPs can rotate the linear polarization of photons and convert the cosmic microwave background E mode to the B mode through the ALP-photon coupling. By deriving the relationship between ALP dynamics and rotation angle, the current and future sensitivities of CMB observations to the ALP-photon coupling were calculated. Neglected fluctuations of the ALP field at the observer have been found to induce significant isotropic rotation of the CMB polarization.
Axionlike particles (ALPs) rotate the linear polarization of photons through the ALP-photon coupling and convert the cosmic microwave background (CMB) E mode to the B mode. We derive the relation between the ALP dynamics and the rotation angle by assuming that the ALP phi has a quadratic potential, V = m(2)phi(2)/2. We compute the current and future sensitivities of CMB observations to the ALP-photon coupling g, which can reach g = 4 x 10(-21) GeV-1 for 10(-32) eV less than or similar to m less than or similar to 10(-28) eV and extensively exceed the other searches for any mass m less than or similar to 10(-25) eV. We find that the fluctuation of the ALP field at the observer, which has been neglected in previous studies, can induce significant isotropic rotation of the CMB polarization. The measurements of isotropic and anisotropic rotation allow us to put bounds on relevant quantities, such as the ALP mass m and the ALP density parameter Omega(phi). In particular, if LiteBIRD detects anisotropic rotation, we obtain the lower bound on the tensor-to-scalar ratio as r > 5 x 10(-9).

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