Weak and electromagnetic interactions
Author:
Publisher
Springer Science and Business Media LLC
Subject
Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics
Link
http://link.springer.com/content/pdf/10.1007/BF02726525.pdf
Reference7 articles.
1. B. D’Espagnat, J. Prentki andA. Salam:Nucl. Phys.,5, 447 (1958). This paper will here by referred to as ESP. Similar ideas have been suggested byG. Takeda: to be published. In ESP theQ space is designated asM space.
2. J. Schwinger:Ann. of Phys.,2, 407 (1957).
3. This was first done bySchwinger (ref. (1)). The difference between our work and Schwinger’s is that here the charged Bose fields arise naturally from the 3-dimensional charge-gauge and there is little arbitrariness in writing down the interaction Lagrangian.
4. Mathematically the work in this Section in completely analogous with that ofYang andMills (Phys. Rev.,96, 191 (1954)); andR. Shaw (Cambridge dissertation, unpublished (1954)).Yang andMills were considering the possibility of a generalized gauge transformation in three-dimensional isotopic rather than charge-space.
5. This has actually been checked to the lowest order byS. Kamefuchi. We are indebted for a private communication. He has also checked that an effective mass will appear for theA ± fields if parity-violating terms are added.
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