1995
DOI: 10.1016/0550-3213(95)00049-x
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Decoherence of Friedmann-Robertson-Walker geometries in the presence of massive vector fields with U(1) or SO(3) global symmetries

Abstract: Retrieval of classical behaviour in quantum cosmology is usually discussed in the framework of midisuperspace models in the presence of scalar fields and the inhomogeneous modes corresponding either to gravitational or scalar fields. In this work, we propose an alternative model to study the decoherence of homogeneous and isotropic geometries where the scalar field is replaced by a massive vector field with a global internal symmetry. We study here the cases with U(1) and SO(3) global internal symmetries. The … Show more

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Cited by 26 publications
(20 citation statements)
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References 48 publications
(126 reference statements)
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“…[49]. Massive vector fields with global U (1) and SO(3) symmetries seem to be particularly suitable to generalize these results, given that the reduced matrix density and Wigner functional of the corresponding midisuperspace model [50] exhibit properties that closely resemble the localization process induced by the back-reaction of the massive long wavelength modes discussed in [49].…”
Section: Physical Spacetimementioning
confidence: 99%
“…[49]. Massive vector fields with global U (1) and SO(3) symmetries seem to be particularly suitable to generalize these results, given that the reduced matrix density and Wigner functional of the corresponding midisuperspace model [50] exhibit properties that closely resemble the localization process induced by the back-reaction of the massive long wavelength modes discussed in [49].…”
Section: Physical Spacetimementioning
confidence: 99%
“…Inhomogeneous modes of dilaton and Yang-Mills elds could together drive decoherence due to their coupling. Decoherence could be also driven by massive v ector elds [18].…”
Section: Discussionmentioning
confidence: 99%
“…For the case where the dilaton has no potential, the corresponding WDW equation (18) where is a separation constant. The solution of (15) is then given by [16]: We shall now consider the situation where the dilaton potential is non-vanishing.…”
Section: Solutions Of the Wheeler-dewitt Equationmentioning
confidence: 99%
“…The wave functionals are taken to be functionals of scalar and vector potential configurations on an initial or final surface of constant time, as appropriate. 5 They are assumed to obey the operator form of the constraints π 0 = 0 and D · π = 0:…”
Section: Application To a Nagtmentioning
confidence: 99%