GAUGE FIXING AND OBSERVABLES IN GENERAL RELATIVITY
The conventional group of four-dimensional diffeomorphisms is not realizeable as a canonical transformation group in phase space. Yet there is a larger field-dependent symmetry transformation group which does faithfully reproduce 4-D diffeomorphism symmetries. Some properties of this group were firs...
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Published in | Modern physics letters A Vol. 18; no. 33n35; pp. 2475 - 2482 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
World Scientific Publishing Company
20.11.2003
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Subjects | |
Online Access | Get full text |
ISSN | 0217-7323 1793-6632 |
DOI | 10.1142/S0217732303012714 |
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Summary: | The conventional group of four-dimensional diffeomorphisms is not
realizeable as a canonical transformation group in phase space. Yet
there is a larger field-dependent symmetry transformation group which
does faithfully reproduce 4-D diffeomorphism symmetries. Some properties
of this group were first explored by Bergmann and Komar. More recently
the group has been analyzed from the perspective of projectability under
the Legendre map. Time translation is not a realizeable symmetry, and is
therefore distinct from diffeomorphism-induced symmetries. This issue is
explored further in this paper. It is shown that time is not "frozen".
Indeed, time-like diffeomorphism invariants must be time-dependent.
Intrinsic coordinates of the type proposed by Bergmann and Komar are
used to construct invariants. Lapse and shift variables are retained as
canonical variables in this approach, and therefore will be subject to
quantum fluctuations in an eventual quantum theory. Concepts and
constructions are illustrated using the relativistic classical and
quantum free particle. In this example concrete time-dependent
invariants are displayed and fluctuation in proper time is manifest. |
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ISSN: | 0217-7323 1793-6632 |
DOI: | 10.1142/S0217732303012714 |