Non-Singular Gravity Without Black Holes

dc.creatorCornish, N. J.
dc.creatorMoffat, J. W.
dc.date1994-06-03
dc.date.accessioned2026-07-07T11:46:22Z
dc.date.available2026-07-07T11:46:22Z
dc.descriptionA non-singular, static spherically symmetric solution to the nonsymmetric gravitational and electromagnetic theory field equations is derived, which depends on the four parameters m, l^2, Q and s, where m is the mass, Q is the electric charge, l^2 is the NGT charge of a body and s is a dimensionless constant. The electromagnetic field invariants are also singularity-free, so that it is possible to construct regular particle-like solutions in the theory. All the curvature invariants are finite, there are no null surfaces in the spacetime and there are no black holes. A new stable, superdense object (SDO) replaces black holes.
dc.description26 pages, UTPT-94-08
dc.identifierhttps://arxiv.org/abs/gr-qc/9406007
dc.identifierhttp://arxiv.org/abs/gr-qc/9406007
dc.identifierJ.Math.Phys.35:6628-6643,1994
dc.identifierdoi:10.1063/1.530697
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/202202
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleNon-Singular Gravity Without Black Holes
dc.typetext

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