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Prog. Theor. Phys. Vol. 31 No. 2 (1964) pp. 311-321

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On the Commutation Relation for the Canonical Energy Density

Toshiei Kimura

Research Institute for Theoretical Physics, Hiroshima University, Takehara, Hiroshima-ken

(Received September 19, 1963)

Abstract:

The interaction Hamiltonian in the interaction representation for an arbitrary spin field coupled to the external gravitational field is obtained by using the method which is the extension of Yang-Feldman's one. The equal time commutator for the canonical energy density is derived directly from the integrability condition of the Schrödinger equation in the interaction representation. It is shown that the presence of ordinary interactions among fields does not alter drastically the form of commutator for free fields and also the relation between the present method and Schwinger's one based on the extended conservation law is discussed.


URL : http://ptp.ipap.jp/link?PTP/31/311/
DOI : 10.1143/PTP.31.311

[ Full Text PDF : FREE ACCESS (585K) ] Citation:


References:

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    See also, P. A. M. Dirac, Rev. Mod. Phys. 34 (1962), 592[APS].
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  11. This formula can be also derived by the straightforward method as shown by
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Citing Article(s) :

  1. Progress of Theoretical Physics Vol. 33 No. 3 (1965) pp. 510-523 :
    An Attempt to Derive the Gravitational Potential
    Toshiei Kimura
  2. Progress of Theoretical Physics Vol. 54 No. 3 (1975) pp. 914-916 :
    A Comment on the First Event of Possible ΔSQ=-1 Process
    Shuzo Ogawa, Yu-ichi Yamamoto and Tsutomu Yanagida