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1981•Progress of Theoretical PhysicsOpen access

Axially Symmetric and Stationary Solution of New General Relativity

Michiaki Fukui, Kazunori Hayashi

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Abstract

In New General Relativity and axially symmetric and stationary gravitational field equation agrees with that of General Relativity with ω replaced by ω = (1 + x/ λ)1/2ω, provided the integrated orbital angular momentum L and the integrated spin angular momentum S are connected by L = (λ/x −1)S at spatial infinity. Here λ is a new parameter, which might agree with the Einstein constant x.

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In New General Relativity and axially symmetric and stationary gravitational field equation agrees with that of General Relativity with ω replaced by ω = (1 + x/ λ)1/2ω, provided the integrated orbital angular momentum L and the integrated spin angular momentum S are connected by L = (λ/x −1)S at spatial infinity. Here λ is a new parameter, which might agree with the Einstein constant x.

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Available abstract

In New General Relativity and axially symmetric and stationary gravitational field equation agrees with that of General Relativity with ω replaced by ω = (1 + x/ λ)1/2ω, provided the integrated orbital angular momentum L and the integrated spin angular momentum S are connected by L = (λ/x −1)S at spatial infinity. Here λ is a new parameter, which might agree with the Einstein constant x.

Key concepts: Physics, Axial symmetry, Introduction to the mathematics of general relativity, General relativity, Angular momentum, Two-body problem in general relativity, Theoretical motivation for general relativity, Theory of relativity

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