Variable Cosmological Term

2003 ◽  
Author(s):  
Irina Dymnikova
Author(s):  
Archana Dixit ◽  
Anirudh Pradhan ◽  
Dinesh Chandra Maurya

In this paper, we have investigated the physical behavior of cosmological models in modified Teleparallel gravity with a general function [Formula: see text] where [Formula: see text] and [Formula: see text] are model parameters and [Formula: see text] is the torsion scalar. We have considered a homogeneous and isotropic Friedman universe filled with perfect fluid. We have derived the deceleration parameter [Formula: see text] in terms of equation of state (EoS) parameter [Formula: see text] and Hubble parameter [Formula: see text]. We have investigated the variation of [Formula: see text] over the observed values of Hubble constant in various observations within the range of redshift [Formula: see text]. Also, we have studied effective energy density [Formula: see text], effective pressure [Formula: see text] and effective EoS parameter [Formula: see text]. We have observed that the second term of [Formula: see text] function behaves just like variable cosmological term [Formula: see text] ([Formula: see text]) at late-time universe and causes the acceleration in expansion and works just like dark energy candidates. Also, we have evaluated the age of the present universe for various stages of matter [Formula: see text] and various [Formula: see text] functions.


2003 ◽  
Vol 20 (16) ◽  
pp. 3797-3814 ◽  
Author(s):  
K A Bronnikov ◽  
A Dobosz ◽  
I G Dymnikova

2015 ◽  
Vol 70 (11) ◽  
pp. 905-911 ◽  
Author(s):  
Carlos Blanco-Pérez ◽  
Antonio Fernández-Guerrero

AbstractWe propose a model of expansion of the universe in which a minimal, ‘quantised’ rate is dependent upon the value of the cosmological constant Λ in Einstein’s field equations, itself not a constant but a function of the size and the entropy of the universe. From this perspective, we offer an expression which relates Hubble’s constant with the cosmological constant.


2001 ◽  
Vol 561 (1) ◽  
pp. L19-L22 ◽  
Author(s):  
K. Kimura ◽  
M. Hashimoto ◽  
K. Sakoda ◽  
K. Arai

2015 ◽  
Vol 360 (1) ◽  
Author(s):  
J. Socorro ◽  
M. D’oleire ◽  
Luis O. Pimentel

2006 ◽  
Vol 21 (06) ◽  
pp. 479-494 ◽  
Author(s):  
JOAN SOLÀ ◽  
HRVOJE ŠTEFANČIĆ

One of the main aims in the next generation of precision cosmology experiments will be an accurate determination of the equation of state (EOS) for the dark energy (DE). If the latter is dynamical, the resulting barotropic index ω should exhibit a nontrivial evolution with the redshift. This is usually interpreted as a sign that the mechanism responsible for the DE is related to some dynamical scalar field, and in some cases this field may behave non-canonically (phantom field). Present observations seem to favor an evolving DE with a potential phantom phase near our time. In the literature, there is a plethora of dynamical models trying to describe this behavior. Here we show that the simplest option, namely a model with a variable cosmological term, Λ = Λ(t), leads in general to a nontrivial effective EOS, with index ωe, which may naturally account for these data features. We prove that in this case there is always a "crossing" of the ωe = -1 barrier near our time. We also show how this effect is modulated (or even completely controlled) by a variable Newton's gravitational coupling G = G(t).


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