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

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

Abstract
HTML
Reference
Related

PDF

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

[1]	Kai-Wen Li , Xiu-Lei Ren , Li-Sheng Geng , Bing-Wei Long . Leading order relativistic hyperon-nucleon interactions in chiral effective field theory. Chinese Physics C, 2018, 42(1): 014105. doi: 10.1088/1674-1137/42/1/014105
[2]	Yan-Ling Li , Yong-Liang Ma , Mannque Rho . Nuclear axial currents from scale-chiral effective field theory. Chinese Physics C, 2018, 42(9): 094102. doi: 10.1088/1674-1137/42/9/094102
[3]	Taejin Lee . Covariant open string field theory on multiple Dp-branes. Chinese Physics C, 2018, 42(11): 113105. doi: 10.1088/1674-1137/42/11/113105
[4]	S. Parsamehr . Gaupta-Bleuler triplet for massless spin-3/2 field in de Sitter space. Chinese Physics C, 2017, 41(9): 093106. doi: 10.1088/1674-1137/41/9/093106
[5]	Yue-Liang Wu . Maximal symmetry and mass generation of Dirac fermions and gravitational gauge field theory in six-dimensional spacetime. Chinese Physics C, 2017, 41(10): 103106. doi: 10.1088/1674-1137/41/10/103106
[6]	S. Parsamehr , M. Mohsenzadeh . Gauge theory of massless spin-(3/2) field in de Sitter space-time. Chinese Physics C, 2016, 40(11): 113102. doi: 10.1088/1674-1137/40/11/113102
[7]	SHI Tan , JI Fu-Hao , YE Mao , WAN Wei-Shi , QIAO Shan . Design of a multi-channel spin polarimeter. Chinese Physics C, 2015, 39(3): 039001. doi: 10.1088/1674-1137/39/3/039001
[8]	LI Fang-Qiong , ZHAO Peng-Wei , LIANG Hao-Zhao . Perturbative pseudospin symmetry limit with linear spin-orbit potential. Chinese Physics C, 2011, 35(9): 825-828. doi: 10.1088/1674-1137/35/9/007
[9]	WANG Ping . New quantization conditions for field theory without divergence. Chinese Physics C, 2011, 35(3): 223-227. doi: 10.1088/1674-1137/35/3/003
[10]	GUO Feng-Kun . Heavy quark spin symmetry and heavy flavor hadronic molecules. Chinese Physics C, 2010, 34(9): 1294-1297. doi: 10.1088/1674-1137/34/9/027
[11]	. Lowest-lying spin-1/2 and spin-3/2 baryon magnetic moments in chiral perturbation theory. Chinese Physics C, 2010, 34(9): 1307-1311. doi: 10.1088/1674-1137/34/9/030
[12]	MEI Hua , CHEN Hong , YAO Jiang-Ming . Single-particle resonance states of ¹²²Zr in relativistic mean-field theory combined with real stabilization method. Chinese Physics C, 2009, 33(S1): 101-104. doi: 10.1088/1674-1137/33/S1/033
[13]	BAO Ai-Dong , YAO Hai-Bo , WU Shi-Shu . Topological approach to examine the singularity of the axial-vector current in an Abelian gauge field theory (QED). Chinese Physics C, 2009, 33(3): 177-180. doi: 10.1088/1674-1137/33/3/003
[14]	YAO Jiang-Ming , MENG Jie , Pena Arteaga , Ring Peter . Restoration of rotational symmetry in deformed relativistic mean-field theory. Chinese Physics C, 2009, 33(S1): 21-23. doi: 10.1088/1674-1137/33/S1/007
[15]	GAO Yuan , DONG Jian-Min , ZHANG Hong-Fei , ZUO Wei , LI Jun-Qing . Properties and structure of N=Z nuclei within relativistic mean field theory. Chinese Physics C, 2009, 33(10): 848-853. doi: 10.1088/1674-1137/33/10/006
[16]	YAO Jiang-Ming , . Towards Lambda-nucleon coupling constants in relativistic mean field theory. Chinese Physics C, 2009, 33(S1): 64-66. doi: 10.1088/1674-1137/33/S1/021
[17]	Marc Richard , Xavier Artru , Mokhtar Elchikh , Jacques Soffer , Oleg Teryaev . Model-independent constraints on spin observables. Chinese Physics C, 2009, 33(12): 1153-1158. doi: 10.1088/1674-1137/33/12/017
[18]	ZHANG Li-Hua , ZHAO Yu-Min . Number of spin I states for bosons. Chinese Physics C, 2009, 33(S1): 137-139. doi: 10.1088/1674-1137/33/S1/043
[19]	ZHANG PengFei , RUAN TuNan . Spin Operators in the Quantum Field Theory. Chinese Physics C, 2000, 24(8): 775-779.
[20]	Jing Sicong , Ruan Jie . Bjorken-Johnson-Low Technique and a Perturbative Study on Chiral Anomaly in Pure Abelian Coset Gauge Field Theory. Chinese Physics C, 1991, 15(S2): 141-152.

Access

Get Citation

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

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 2021-03-23

Article Metric

Article Views(1118)
PDF Downloads(26)
Cited by(0)

Policy on re-use

To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.

通讯作者: 陈斌, bchen63@163.com

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

Abstract:

HTML

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}). $