Quantum interference effects in a five-dimensional Kaluza-Klein theory

1987 ◽  
Vol 4 (5) ◽  
pp. 1473-1474 ◽  
Author(s):  
R O Weber
1986 ◽  
Vol 3 (3) ◽  
pp. 425-430 ◽  
Author(s):  
R Parthasarathy ◽  
G Rajassekaran ◽  
R Vasuedevan

1987 ◽  
Vol 4 (5) ◽  
pp. 1327-1331
Author(s):  
R Parthasarathy ◽  
R Nagarajan ◽  
G Rajasekaran

1988 ◽  
Vol 03 (02) ◽  
pp. 187-190
Author(s):  
R.O. WEBER

The unification of non-abelian gauge theories and gravitation in a higher dimensional Kaluza-Klein theory is shown to unify quantum interference effects.


1983 ◽  
Vol 61 (6) ◽  
pp. 844-856 ◽  
Author(s):  
M. W. Kalinowski

This paper is devoted to a five-dimensional unification of Moffat's theory of gravitation and electromagnetism. We found "interference effects" between gravitational and electromagnetic fields which appear to be due to the skew-symmetric part of the metric of Moffat's theory. Our unification, called the nonsymmetric Jordan–Thiry theory, becomes the classical Kaluza–Klein theory if the skew-symmetric part of the metric is zero. The possible generalization to an arbitrary gauge group is discussed.


1985 ◽  
Vol 146 (8) ◽  
pp. 655 ◽  
Author(s):  
I.Ya. Aref'eva ◽  
I.V. Volovich
Keyword(s):  

1987 ◽  
Vol 189 (1-2) ◽  
pp. 96-98 ◽  
Author(s):  
M. Arik ◽  
T. Dereli
Keyword(s):  

1995 ◽  
Vol 04 (05) ◽  
pp. 639-659 ◽  
Author(s):  
ANDREW BILLYARD ◽  
PAUL S. WESSON ◽  
DIMITRI KALLIGAS

The augmentation of general relativity’s spacetime by one or more dimensions is described by Kaluza-Klein theory and is within testable limits. Should an extra dimension be observable and significant, it would be beneficial to know how physical properties would differ from “conventional” relativity. In examining the class of five-dimensional solutions analogous to the four-dimensional Schwarzschild solution, we examine where the origin to the system is located and note that it can differ from the four-dimensional case. Furthermore, we study circular orbits and find that the 5D case is much richer; photons can have stable circular orbits in some instances, and stable orbits can exist right to the new origin in others. Finally, we derive both gravitational and inertial masses and find that they do not generally agree, although they can in a limiting case. For all three examinations, it is possible to obtain the four-dimensional results in one limiting case, that of the Schwarzschild solution plus a flat fifth dimension, and that the differences between 4D and 5D occur when the fifth dimension obtains any sort of significance.


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