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Reference17 articles.
1. W. Heitler: inThe Quantum Theory of Fields, edited byR. Stoops (Interscience Publ., New York, N. Y., 1962), p. 37;N. Nakanishi:Prog. Theor. Phys. Suppl.,51, 1 (1972).
2. J. Schwinger:Quantum Electrodynamics (Dover Publ., Inc., New York, N. Y., 1958), p. 16.
3. J. P. Hsu:Nuovo Cimento B,74, 67 (1983);78, 85 (1983);Phys. Lett. A.,97, 137 (1983). See also Nature Editorial (Nature,303, 129 (1983)) for a discussion of common time in four-dimensional framework. For recent applications of a scalar evolution variable in many-particle systems, seeJ. P. Hsu andT. Y. Shi:Phys. Rev. D,26, 2745 (1982);J. P. Hsu:Nuovo Cimento B,75, 185 (1983);Phys. Rev. D,24, 802 (1981). The idea of having a common time for all observers (or frames) is very simple. For example, the observers in a train (F′-frame) and the observers on the ground (F 0-frame) can use the same clock system in, say, theF 0-frame. To embed this idea in the four-dimensional symmetry framework is not so trivial. SeeJ. P. Hsu andT. N. Sherry:Found. Phys.,10, 57 (1980).
4. J. P. Hsu:Nuovo Cimento A,56, 1 (1980);55, 145 (1980). See also ref. (1,2,5).W. Heitle: inThe Quantum Theory of Fields, edited byR. Stoops (Interscience Publ., New York, N. Y., 1962), p. 37;N. Nakanishi:Prog. Theor. Phys. Suppl.,51, 1 (1972).J. Schwinger:Quantum Electrodynamics (Dover Publ., Inc., New York, N. Y., 1958), p. 16. This is to be compared with the result in the previous work,J. P. Hsu andE. Mac:Nuovo Cimento B,49, 55 (1979).
5. This is to be compared with the result in the previous work,J. P. Hsu andE. Mac:Nuovo Cimento B,49, 55 (1979).
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