Quantization of Interacting Fields in QED

Wang Renchuan; Zhu Dongpei

Chinese Physics C> 1994, Vol. 18> Issue(S4) : 357-366

Quantization of Interacting Fields in QED

Wang Renchuan ¹ ,
Zhu Dongpei ²

1. Center for Fundamental Physics, University of Science and Technology of China, Hefei, Anhui;
2. Department of Modem Physics, University of Science and Technology of China, Hefei, Anhui

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Abstract：
We propose a new quantization scheme with which and by the equation of motion the quantization problem of both independent and dependent interacting fields in QED can be solved simultaneously. When the external gauge field A_μ^ex)≠0 (i.e., the Fermion field ψ/(x) and the electromagnetic field A_μ(x) are independent of each other) our scheme gives the same result as the usual quantization approach. When the external gauge field is absent the usual quantization conditions fail since it is not compatible with equation of motion, meanwhile our scheme is still valid. These results are demonstrated with solvable QED in 1+1 dimension.
- dependent interacting fields ,
- quantization ,
- QED

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Wang Renchuan and Zhu Dongpei. Quantization of Interacting Fields in QED[J]. Chinese Physics C, 1994, 18(S4): 357-366.

Wang Renchuan and Zhu Dongpei. Quantization of Interacting Fields in QED[J]. Chinese Physics C, 1994, 18(S4): 357-366. shu

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Received: 1993-08-25

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Supported by the National Science Foundation and the Grant No. LWTZ-1298 of Chinese Academy of Sciences.

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Quantization of Interacting Fields in QED

Wang Renchuan ^1,
Zhu Dongpei ^2,

1. Center for Fundamental Physics, University of Science and Technology of China, Hefei, Anhui;
2. Department of Modem Physics, University of Science and Technology of China, Hefei, Anhui

Received Date: 1993-08-25

Fund Project: Supported by the National Science Foundation and the Grant No. LWTZ-1298 of Chinese Academy of Sciences.

Abstract: We propose a new quantization scheme with which and by the equation of motion the quantization problem of both independent and dependent interacting fields in QED can be solved simultaneously. When the external gauge field A_μ^ex)≠0 (i.e., the Fermion field ψ/(x) and the electromagnetic field A_μ(x) are independent of each other) our scheme gives the same result as the usual quantization approach. When the external gauge field is absent the usual quantization conditions fail since it is not compatible with equation of motion, meanwhile our scheme is still valid. These results are demonstrated with solvable QED in 1+1 dimension.