Erratum: Covariant Spin Kinetic Theory I: Collisionless Limit, [Y.-C. Liu, K. Mameda, and X.-G. Huang, Chin. Phys. C 44, 094101 (2020)]

Yu-Chen Liu; Kazuya Mameda; Xu-Guang Huang

doi:10.1088/1674-1137/ac009b

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《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 2021, Vol. 45> Issue(8) : 089001 DOI: 10.1088/1674-1137/ac009b

Erratum: Covariant Spin Kinetic Theory I: Collisionless Limit, [Y.-C. Liu, K. Mameda, and X.-G. Huang, Chin. Phys. C 44, 094101 (2020)]

1.
Physics Department and Center for Particle Physics and Field Theory, Fudan University, Shanghai 200433, China
2.
RIKEN Nishina Center for Accelerator-Based Science, Wako 351-0198, Japan
3.
Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Fudan University, Shanghai 200433, China

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- spin Kinetic theory ,
- field theory in curved spacetime ,
- spin polarization

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Yu-Chen Liu, Kazuya Mameda and Xu-Guang Huang. Erratum: Covariant Spin Kinetic Theory I: Collisionless Limit, [ Y.-C. Liu, K. Mameda, and X.-G. Huang, Chin. Phys. C 44, 094101 (2020)][J]. Chinese Physics C. doi: 10.1088/1674-1137/ac009b

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Received: 2021-03-23

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1.
沈阳化工大学材料科学与工程学院沈阳 110142

Erratum: Covariant Spin Kinetic Theory I: Collisionless Limit, [Y.-C. Liu, K. Mameda, and X.-G. Huang, Chin. Phys. C 44, 094101 (2020)]

1. Physics Department and Center for Particle Physics and Field Theory, Fudan University, Shanghai 200433, China
2. RIKEN Nishina Center for Accelerator-Based Science, Wako 351-0198, Japan
3. Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Fudan University, Shanghai 200433, China

Received Date: 2021-03-23
Available Online: 2021-08-15

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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}). $