| The equivalence between B—W and K—G and R—S equations |
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| 引用本文： | 黄时中,阮图南,吴 宁,郑志鹏.The equivalence between B—W and K—G and R—S equations[J].中国物理 B,2003,12(1):25-32. |
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| 作者姓名： | 黄时中 阮图南 吴 宁 郑志鹏 |
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| 作者单位： | (1)Department of Modern Physics, University of Science and Technology of China, Hefei 230027, China; (2)Department of Physics, Anhui Normal University, Wuhu 241000, China; (3)Institute of High Energy Physics, Chinese Academy of Sciences,Beijing 100039, China |
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| 基金项目： | Project supported by the National Natural Science Foundation of China (Grant Nos 19947001, 90103010 and 19991480), the Doctoral Program Foundation of Institution of Higher Education of China (Grant No 97035807), the Beijing Positive-Negative Electron Collision National Laboratory of China, the Center for Theoretical Nuclear Physics of Lanzhou Heavy Ion Accelerator National Laboratory of China, and the Natural Science Foundation of Anhui Province, China (Grant No 2001KJ109). |
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| 摘 要： | The equivalence between the Bargmann--Wigner (B-W) equations and the
Klein--Gordon (K-G) equations for integral spin, and the Rarita--Schwinger (R-S) equations for half integral spin is established by explicit derivation, starting from the lowest spin cases. It is demonstrated that all the constraints or subsidiary conditions imposed on the K-G or R-S equations are included in the B-W equations.
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| 关 键 词： | 高能物理 B－W方程 K－G方程 R－S方程 |
| 收稿时间： | 5/7/2002 12:00:00 AM |
The equivalence between B-W and K-G band R-S equations |
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| Huang Shi-Zhong,Ruan Tu-Nan,Wu Ning and Zheng Zhi-Peng.The equivalence between B-W and K-G band R-S equations[J].Chinese Physics B,2003,12(1):25-32. |
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| Authors: | Huang Shi-Zhong Ruan Tu-Nan Wu Ning and Zheng Zhi-Peng |
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| Institution: | Department of Physics, Anhui Normal University, Wuhu 241000, China; Department of Modern Physics, University of Science and Technology of China, Hefei 230027, China; Institute of High Energy Physics, Chinese Academy of Sciences,Beijing 100039, China |
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| Abstract: | The equivalence between the Bargmann--Wigner (B-W) equations and the
Klein--Gordon (K-G) equations for integral spin, and the Rarita--Schwinger (R-S) equations for half integral spin is established by explicit derivation, starting from the lowest spin cases. It is demonstrated that all the constraints or subsidiary conditions imposed on the K-G or R-S equations are included in the B-W equations. |
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| Keywords: | higher spins Bargmann--Wigner equations Klein--Gordon equations Rarita--Schwinger equations |
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