Klas⇒ kovariantnykh kommutatopov dlya polei s tselym spinomJ im ≠ i dlyam=0, bee nyeobkhodimosti vvedeniya indefiiitnoi{cyrillic, short} metpiki

We show that it is possible to give covariant commutators for a field of integer spin J, for nonzero and for zero mass, as particular cases of a more general commutator. We calculate this explicitly for spin 1 and 2. We generate the decompositions of the momentum amplitude for a field of integer spi...

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Autor principal: Weder, R.
Otros Autores: Zandron, O.
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: Società Italiana di Fisica 1971
Acceso en línea:Registro en Scopus
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100 1 |a Weder, R. 
245 1 0 |a Klas⇒ kovariantnykh kommutatopov dlya polei s tselym spinomJ im ≠ i dlyam=0, bee nyeobkhodimosti vvedeniya indefiiitnoi{cyrillic, short} metpiki 
260 |b Società Italiana di Fisica  |c 1971 
270 1 0 |m Weder, R.; Departmento de Física, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, Buenos Aires, Argentina 
506 |2 openaire  |e Política editorial 
504 |a Gupta, S.N., (1950) Proc. Phys. Soc., 63, p. 681 
504 |a Dürr, H.P., Rudolph, E., (1970) Nuovo Cimento, 65 A, p. 423 
504 |a Moses, H.E., (1966) Nuovo Cimento, 42 A, p. 757 
504 |a N. N. Bogliubov and D. V. Shirkov: Introduction to the Theory of Quantized Fields (New York, 1959); Bollini, C.G., (1957) Nuovo Cimento, 6, p. 1034 
504 |a See also for example J. D. Bjorken and S. D. Drell: Relativistic Quantum Fields (New York, 1965); Coester, F., Jauch, J.M., (1950) Phys. Rev., 78, p. 149 
504 |a J. G. Valatin: Dan. Mat. Fys. Medd., 26, No. 13 (1951) 
520 3 |a We show that it is possible to give covariant commutators for a field of integer spin J, for nonzero and for zero mass, as particular cases of a more general commutator. We calculate this explicitly for spin 1 and 2. We generate the decompositions of the momentum amplitude for a field of integer spin J, by decomposing the momentum amplitude of a vector field Aμ in three directions in such a way that the condition of zero divergence is satisfied. In the nonzero-mass case, as is well known, quantum conditions are given on the (2 J + 1) independent components; in this way the usual commutators are obtained. In the massless case only two of the components appear as gauge invariants, and for this reason quantum conditions are given only on these two components, since the others are physically irrelevant. Moreover, the commutators thus obtained are compatible with the field equations and with the subsidiary conditions, and the energy is automatically positive definite, without it being necessary to introduce an indefinite metric. © 1971 Società Italiana di Fisica.  |l eng 
593 |a Departmento de Física, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, Buenos Aires, Argentina 
700 1 |a Zandron, O. 
773 0 |d Società Italiana di Fisica, 1971  |g v. 2  |h pp. 455-466  |k n. 2  |p Nuov Cim A  |x 03693546  |w (AR-BaUEN)CENRE-2203  |t Il Nuovo Cimento A 
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