Non-Singular Gravity Without Black Holes

Details Non-Singular Gravity Without Black Holes Non-Singular Gravity Without Black Holes

1994-06-03

arxiv.org/abs/gr-qc/9406007v1

J.Math.Phys.35:6628-6643,1994

Astronomy and Astrophysics

Astrophysics

General Relativity and Quantum Cosmology

26 pages, UTPT-94-08

Scientific paper

10.1063/1.530697

A 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.

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