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Prog. Theor. Phys. Vol. 55 No. 4 (1976) pp. 1259-1275
Canonical Quantization of Massless Tensor Field in General Covariant Gauge
Toshiei Kimura
Research Institute for Theoretical Physics, Hiroshima University, Takehara, Hiroshima-ken 725
(Received September 13, 1975)
Abstract:
In order to find a massive tensor field theory which tends to massless limit smoothly, canonical quantization of massless tensor field is carried out in general covariant gauges. To specify a gauge, three auxiliary fields are introduced. Generally there appears a gauge independent parameter b which plays an important role in the quantization procedure. When b ≠1 four-dimensional commutation relations among fields can be derived through a straightforward extension of the method devised for quantum electrodynamics. There exists a massive tensor theory which connects with massless one, although Lagrangian does not coincide with the Fierz-Pauli one when the auxiliary vector fields are absent. When b = 1 it is necessary to introduce scalar fields in addition to the vector fields and to follow the method of Dirac's new Poisson bracket. In this case another gauge independent parameter β appears in propagator for graviton and affects the interaction between matters. It is shown that in the case with b = 1 and β= ∞, there exists not only a massless tensor theory consistent with experimental facts but also a massive theory which tends to the massless one smoothly.
URL :
http://ptp.ipap.jp/link?PTP/55/1259/
DOI : 10.1143/PTP.55.1259
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Citing Article(s) :
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Progress of Theoretical Physics Vol. 59 No. 3 (1978) pp. 972-985
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Progress of Theoretical Physics Vol. 59 No. 6 (1978) pp. 2175-2177
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Progress of Theoretical Physics Vol. 60 No. 3 (1978) pp. 857-867
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