Cosmological solutions of the Friedmann type in the tensor-scalar theory of gravitation

Astrophysics ◽  
1994 ◽  
Vol 36 (4) ◽  
pp. 349-354
Author(s):  
G. G. Haroutyunian ◽  
V. V. Papoyan
1991 ◽  
Vol 14 (2) ◽  
pp. 305-308 ◽  
Author(s):  
Aroonkumar Beesham

The scale covariant theory of gravity admits the possibility of a time varying gravitational constant but contains a gauge function for which there is no independent equation. The circumstances under which explicit forms for a gauge function may be derived within the context of Friedmann-Robertson-Walker cosmological models are investigated and several forms are derived.


1965 ◽  
Vol 33 (2) ◽  
pp. 162-163
Author(s):  
A. L. Harvey

1971 ◽  
Vol 4 (2) ◽  
pp. 205-216 ◽  
Author(s):  
H. O. Girotti ◽  
D. Wisnivesky

2018 ◽  
Vol 1 ◽  
pp. 67-81 ◽  
Author(s):  
S.V. Chervon ◽  
◽  
A.S. Kubasov ◽  
K. A. Bolshakova ◽  
◽  
...  

1995 ◽  
Vol 225 (2) ◽  
pp. 237-240 ◽  
Author(s):  
Marcelo S. Berman ◽  
M. M. Som

1969 ◽  
Vol 47 (20) ◽  
pp. 2161-2164 ◽  
Author(s):  
Peter Rastall

The scalar theory of gravitation is known to be in agreement with observed planetary motions if the Sun is assumed to be stationary with respect to the preferred coordinate systems of the theory. We now assume that the Sun is moving, and we find that, unless its speed is improbably small, there are observable effects on the planetary orbits. The difficulty can be overcome if one assumes that the Newtonian charts are determined by the distribution of matter.


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