LINEARITY, NON SELF-INTERACTING SPHERICALLY SYMMETRICAL GRAVITATIONAL-FIELDS, THE SPHERELAND EQUIVALENCE PRINCIPLE AND HAMILTONIAN BUBBLES

Citation
Ei. Guendelman et Ai. Rabinowitz, LINEARITY, NON SELF-INTERACTING SPHERICALLY SYMMETRICAL GRAVITATIONAL-FIELDS, THE SPHERELAND EQUIVALENCE PRINCIPLE AND HAMILTONIAN BUBBLES, General relativity and gravitation, 28(2), 1996, pp. 117-128
Citations number
16
Categorie Soggetti
Physics
ISSN journal
00017701
Volume
28
Issue
2
Year of publication
1996
Pages
117 - 128
Database
ISI
SICI code
0001-7701(1996)28:2<117:LNSSSG>2.0.ZU;2-6
Abstract
For a large class of spherically symmetric gravitational fields, when matter is dropped in a spherically symmetric way, it is possible to de compose this matter into free-falling shells such that their associate d 2+1-dimensional (i.e. surface) energy-momentum tensor is conserved, that is, is not affected by the environment. Further 'non-interacting' features can be found for this class of gravitational fields as can b e seen by the fact that Einstein's equations are linear in this case. Matter of a shell falling in one of these fields obeys energy momentum conservation from the point of view of the 2+1-dimensional world-shee t of the shell. This means that in the case of a test particle moving in one of these free falling sheets, the motion follows a 2+1-dimensio nal geodesic equation, or what is the same, its dynamics is governed b y a 'sphereland equivalence principle'. As a result of this, a shell f alling in such a gravitational field can be treated as a closed system which can be described by a 2+1-dimensionally defined Hamiltonian.