Eddy magnetization from the chiral Barnett effect

Kenji Fukushima, Shi Pu, and Zebin Qiu
Phys. Rev. A 99, 032105 – Published 11 March 2019

Abstract

We discuss the spin, the angular momentum, and the magnetic moment of rotating chiral fermions using a kinetic theory. We find that, in addition to the chiral vortical contribution along the rotation axis, finite circular spin polarization is induced by the spin-momentum correlation of chiral fermions, which is canceled by a change in the orbital angular momentum. We point out that the eddy magnetic moment is nonvanishing due to the g factors, exhibiting the chiral Barnett effect.

  • Figure
  • Received 7 September 2018

DOI:https://doi.org/10.1103/PhysRevA.99.032105

©2019 American Physical Society

Physics Subject Headings (PhySH)

Nuclear PhysicsParticles & Fields

Authors & Affiliations

Kenji Fukushima1, Shi Pu1,2, and Zebin Qiu1

  • 1Department of Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
  • 2Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, China

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Issue

Vol. 99, Iss. 3 — March 2019

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