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After the publication of the paper, we found two incorrect signs in Eqs. (11) and (13). The correct form of Eq. (11) should be
$ \frac{\hbar}{2} \Delta_ \mu {\cal{P}}- { \Pi}^ \nu \tilde{\cal{S}}_{\mu\nu} = m {\cal{A}}_ \mu + \frac{\hbar^2}{8} \tilde{R}_{\nu\rho\sigma\mu}\partial_p^\nu {\cal{S}}^{\rho\sigma} \,, $
(1) and the correct form of Eq. (13) should be
$ \frac{\hbar}{2} \Delta_ \mu {\cal{F}}-{ \Pi}^ \nu {\cal{S}}_{ \mu \nu} = \frac{\hbar^2}{16} (R_{ \mu \nu \rho\sigma} \partial^ \nu_p {\cal{S}}^{ \rho\sigma} + 2 R^{\nu\rho} \partial^p_ \nu {\cal{S}}_{ \rho \mu}). $
(2)
Erratum: Covariant Spin Kinetic Theory I: Collisionless Limit, [Y.-C. Liu, K. Mameda, and X.-G. Huang, Chin. Phys. C 44, 094101 (2020)]
- Received Date: 2021-03-23
- Available Online: 2021-08-15
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