scholarly journals Generalized Vaidya solutions in bimetric gravity

2020 ◽  
Vol 37 (14) ◽  
pp. 145010 ◽  
Author(s):  
Marcus Högås ◽  
Mikica Kocic ◽  
Francesco Torsello ◽  
Edvard Mörtsell
Keyword(s):  
2015 ◽  
Vol 748 ◽  
pp. 37-44 ◽  
Author(s):  
Yashar Akrami ◽  
S.F. Hassan ◽  
Frank Könnig ◽  
Angnis Schmidt-May ◽  
Adam R. Solomon
Keyword(s):  

2012 ◽  
Vol 30 (1) ◽  
pp. 015004 ◽  
Author(s):  
Valentina Baccetti ◽  
Prado Martín-Moruno ◽  
Matt Visser

2021 ◽  
Vol 10 (5) ◽  
pp. 2515-2525
Author(s):  
N.P. Gaikwad ◽  
P.V. Lepse ◽  
B.K. Bishi ◽  
N.K. Ashtankar

We have deduced that bulk viscous Bianchi type I barotropic fluid cosmological model with varying $\Lambda$ and functional relation on hubble parameter by solving the field equations bimetric theory of gravitation. It is observed that our model has exponentially accelerating expansion at late time starting with decelerating expansion which agreed the observation of Perlmutter (1998), Knop (2003), Tegmark (2004) and Spergel (2006). In the beginning, our model has more than three spatial-dimensions then it switched over to three-dimensional spatial geometry at late epoch of time and it is agreed with Borkar et al. (2013). Other geometrical and physical behavior of the model have been studied.


2009 ◽  
Vol 80 (10) ◽  
Author(s):  
Manuel Hohmann ◽  
Mattias N. R. Wohlfarth

2003 ◽  
Vol 12 (04) ◽  
pp. 697-712 ◽  
Author(s):  
M. A. CLAYTON ◽  
J. W. MOFFAT

Predictions of the CMB spectrum from a bimetric gravity theory (BGT)1 are presented. The initial inflationary period in BGT is driven by a vanishingly small speed of gravitational waves vg in the very early universe. This initial inflationary period is insensitive to the choice of scalar field potential and initial values of the scalar field. After this initial period of inflation, vg will increase rapidly and the effects of a potential will become important. We show that a quadratic potential introduced into BGT yields an approximately flat spectrum with inflation parameters: ns=0.98, nt=-0.027, αs=-3.2×10-4 and αt=-5.0×10-4, with r ≥ 0.014.


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