Friedmann cosmological models with bulk viscosity in a scale covariant theory

2007 ◽  
Vol 310 (3-4) ◽  
pp. 269-271 ◽  
Author(s):  
N. Ibotombi Singh ◽  
Anita Sorokhaibam
1977 ◽  
Vol 16 (6) ◽  
pp. 1643-1663 ◽  
Author(s):  
V. Canuto ◽  
P. J. Adams ◽  
S.-H. Hsieh ◽  
E. Tsiang

Author(s):  
Shri Ram ◽  
S. Chandel ◽  
M.K. Verma

In this paper, we obtain an anisotropic Bianchi type-II space-time with dark matter and the modified holographic Ricci dark energy in the scale-covariant theory of gravitation. Exact solutions of the field equations are obtained by assuming (I) a negative constant value of the deceleration parameter (II) the component σ<sup>1</sup><sub>1</sub> of the shear tensor σ<sup>j</sup><sub>i</sub> is proportional to the mean Hubble parameter and (III) the gauge function Φ is proportional to a power function of the average scale factor. We have also discussed some important physical aspects of the model which is in agreement with the modern cosmological observations.


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.


1974 ◽  
Vol 63 ◽  
pp. 273-282
Author(s):  
I. D. Novikov

Observations primarily of the microwave background radiation show that the Universe expands isotropically with a high degree of accuracy at the present time and that the matter distribution is homogeneous on a large scale. Thus, the Friedmann cosmological models are a good approximation today for the expanding Universe. This is valid for at least some period of time in the past too. But how did the Universe expand and what was the matter distribution close to the starting point, near the cosmological singularity?


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