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Unified Field Theory

Canadian Journal of Mathematics, 1950
Introduction. In a recent unified theory originated by Einstein and Straus [l], the gravitational and electromagnetic fields are represented by a single nonsymmetric tensor gy which is a function of four coordinates xr(r = 1, 2, 3, 4). In addition a non-symmetric linear connection Γjki is assumed for the space and a Hamiltonian function is defined in ...
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Einstein's Unified Field Theory

Proceedings of the Physical Society. Section A, 1952
In this paper it is shown that, under certain assumptions about the metric of the space-time, energy momentum tensor of the total field, when Einstein's field equations are satisfied, vanishes identically. A new version of the unified field theory is suggested, and it is indicated briefly that a genuine energy momentum tensor exists which is conserved ...
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Unified Field Theory

Physics Bulletin, 1976
Ramon Prasad London: Geometrica 1975 pp v + 70 price £2.50 Unified field theory has captured the imagination of many scientists including Weyl, Eddington, Einstein and Schrodinger. This little book presents the author's attempts to extend this work.
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Unified field theories

Reports on Progress in Physics, 1981
In this article we review recent progress in applying quantum gauge field theories to the description of the fundamental forces. We start from the principles of local gauge invariance and spontaneous symmetry breaking to derive the successful Weinberg-Salam model for the weak and electromagnetic interactions and also quantum chromodynamics, the theory ...
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*Unified Field Theories

2013
This chapter touches – symmetry-inspired – theoretical considerations which are mathematically far advanced, but so far are not at all required by deviations between the predictions of the Standard Model or general relativity and experiment. The success of the electro-weak unification within the Glashow-Salam-Weinberg model motivated the search for ...
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Superconformal Unified Field Theory

Physical Review Letters, 1977
We present the gauge theory of the graded conformal group. It contains four real fields with spins 2, $\frac{3}{2}$, 1, and \textonehalf{}. The theory is invariant under local proper conformal, scale, chiral, gravitational, and supersymmetry transformations.
M. Kaku   +2 more
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