期刊
PHYSICAL REVIEW LETTERS
卷 128, 期 9, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.128.092301
关键词
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资金
- RCF at BNL
- NERSC Center at LBNL
- Open Science Grid consortium
- Office of Nuclear Physics within the U.S. DOE Office of Science
- U.S. National Science Foundation
- Ministry of Education and Science of the Russian Federation
- Chinese Academy of Science
- Ministry of Science and Technology of China
- Chinese Ministry of Education
- Higher Education Sprout Project by the Ministry of Education at NCKU
- National Research Foundation of Korea
- National Science Centre of Poland
- Ministry of Science, Education and Sports of the Republic of Croatia
- RosAtom of Russia
- German Bundesministerium fur Bildung, Wissenschaft, Forschung and Technologie (BMBF)
- Helmholtz Association
- Japan Society for the Promotion of Science (JSPS)
- National Natural Science Foundation of China
- Czech Science Foundation
- Ministry of Education, Youth and Sports of the Czech Republic
- Hungarian National Research, Development and Innovation Office
- New National Excellency Programme of the Hungarian Ministry of Human Capacities
- Department of Atomic Energy
- Department of Science and Technology of the Government of India
- Ministry of Education, Culture, Sports, Science, and Technology (MEXT)
The chiral magnetic effect is a phenomenon of charge separation caused by the imbalanced chirality of quarks in quantum chromodynamics. Experimental measurements are challenging due to background interference, but the sensitivity of the effect to specific planes can help determine the signal. In this study, measurements in Au + Au collisions at the Relativistic Heavy-Ion Collider indicate that the charge separation is consistent with zero in peripheral collisions, while some indication of a finite chiral magnetic effect signal is observed in midcentral collisions, but significant residual background effects may still be present.
The chiral magnetic effect (CME) refers to charge separation along a strong magnetic field due to imbalanced chirality of quarks in local parity and charge-parity violating domains in quantum chromodynamics. The experimental measurement of the charge separation is made difficult by the presence of a major background from elliptic azimuthal anisotropy. This background and the CME signal have different sensitivities to the spectator and participant planes, and could thus be determined by measurements with respect to these planes. We report such measurements in Au + Au collisions at a nucleon-nucleon center-of-mass energy of 200 GeV at the Relativistic Heavy-Ion Collider. It is found that the charge separation, with the flow background removed, is consistent with zero in peripheral (large impact parameter) collisions. Some indication of finite CME signals is seen in midcentral (intermediate impact parameter) collisions. Significant residual background effects may, however, still be present.
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