Abstract:We study the matter creation cosmology as an alternative theory to explain the dark energy phenomena. We discuss the matter-dominated Universe in a flat Friedmann-Robertson-Walker line element by adopting the thermodynamics of open systems, in which the matter creation irreversible processes may take place at a cosmological scale. We propose a new form of the matter creation rate, Γ = 3α H 0 + 3β H + 3γäȧ , which generalizes some of the previous models in the literature. Exact solutions of the field equations … Show more
“…Here, while the Universe is passing from deceleration to acceleration for t = 0, q > 0 so the constrain for the parameters is obtained as b a < 1 2 . Also, t 0 showing the age of the Universe, in this study is considered as t 0 = 13.8Gyr relying on SN Ia+OHD (SN:Supernovae, OHD:Observational Hubble Data) [34]. On the other hand, for the deceleration parameter there is the value of q 0 = q(t 0 ) = − 0.73 according to SN Ia observational data [35].…”
In this study, Tsallis Holographic Dark Energy (THDE) was studied in the framework of $f(R, T)$ gravitational theory by taking into consideration the homogeneous and anisotropic Bianchi-I spacetime. The Hubble horizon was chosen as $IR$ cutoff of the system. To obtain solutions of field equations, THDE density and a form of Hubble parameter were used. Additionally, various physical parameters such as energy of state parameter, deceleration parameter and scale factor have been discussed. The characteristics and parameters of the model have been also examined by plotting their evolution graphics. Furthermore, statefinder parameters, which are effective tools for separating dark energy models, have been explored. By the illustration of trajectory in $r-s$ plane, it is found that this model behaves like Chaplygin gas at initial stage, then ranging in quintessence region it finally approaches to $\Lambda$ Cold Dark Matter. Lastly, from the evolutions of $r-q$ and $s-q$ planes it is seen that the model evolves to the De Sitter expansion point.
“…Here, while the Universe is passing from deceleration to acceleration for t = 0, q > 0 so the constrain for the parameters is obtained as b a < 1 2 . Also, t 0 showing the age of the Universe, in this study is considered as t 0 = 13.8Gyr relying on SN Ia+OHD (SN:Supernovae, OHD:Observational Hubble Data) [34]. On the other hand, for the deceleration parameter there is the value of q 0 = q(t 0 ) = − 0.73 according to SN Ia observational data [35].…”
In this study, Tsallis Holographic Dark Energy (THDE) was studied in the framework of $f(R, T)$ gravitational theory by taking into consideration the homogeneous and anisotropic Bianchi-I spacetime. The Hubble horizon was chosen as $IR$ cutoff of the system. To obtain solutions of field equations, THDE density and a form of Hubble parameter were used. Additionally, various physical parameters such as energy of state parameter, deceleration parameter and scale factor have been discussed. The characteristics and parameters of the model have been also examined by plotting their evolution graphics. Furthermore, statefinder parameters, which are effective tools for separating dark energy models, have been explored. By the illustration of trajectory in $r-s$ plane, it is found that this model behaves like Chaplygin gas at initial stage, then ranging in quintessence region it finally approaches to $\Lambda$ Cold Dark Matter. Lastly, from the evolutions of $r-q$ and $s-q$ planes it is seen that the model evolves to the De Sitter expansion point.
“…A covariant formulation of the irreversible thermodynamics was developed in [73]. In fact, irreversible thermodynamics and thermodynamics of open systems is a widely studied field, since it is useful in various applications [74][75][76][77][78][79][80][81][82][83][84].…”
We explore the possibility of gravitationally generated particle production in the scalar-tensor representation of f (R, T ) gravity. Due to the explicit nonminimal curvature-matter coupling in the theory, the divergence of the matter energy-momentum tensor does not vanish. We explore the physical and cosmological implications of this property by using the formalism of irreversible thermodynamics of open systems in the presence of matter creation/annihilation. The particle creation rates, pressure, temperature evolution and the expression of the comoving entropy are obtained in a covariant formulation and discussed in detail. Applied together with the gravitational field equations, the thermodynamics of open systems lead to a generalization of the standard ΛCDM cosmological paradigm, in which the particle creation rates and pressures are effectively considered as components of the cosmological fluid energy-momentum tensor. We also consider specific models, and compare the scalar-tensor f (R, T ) cosmology with the ΛCDM scenario and the observational data for the Hubble function. The properties of the particle creation rates, of the creation pressures, and entropy generation through gravitational matter production are further investigated in both the low and high redshift limits.
“…The second type is BV [34,47], which is similar to both bulk viscous models [10][11][12][13][14] and CCDM models [15][16][17][18][19][20][21][22][23][24][25][26]. In BV (bulk-viscous-cosmology-like) models, the acceleration equation includes an extra driving term, whereas the Friedmann equation does not [34,47].…”
Section: Introductionmentioning
confidence: 99%
“…An accelerated expansion of the late universe [1,2] has been widely accepted as a new paradigm. To explain the accelerated expansion, astrophysicists have proposed several cosmological models [3]: e.g., ΛCDM (Lambda cold dark matter) models, Λ(t)CDM models (i.e., a timevarying Λ(t) cosmology) [4][5][6][7][8][9], bulk viscous models [10][11][12][13][14], and the creation of CDM (CCDM) models [15][16][17][18][19][20][21][22][23][24][25][26], as well as other scenarios . The evolution of the universe has been recently examined from a thermodynamic viewpoint, using such models [41][42][43][44][45][46][47][48][49][50][51][52][53][54][55][56][57][58][59].…”
Cosmological adiabatic particle creation results in the generation of irreversible entropy. The evolution of the irreversible entropy is examined in a flat Friedmann-Robertson-Walker universe at late times, using a dissipative model with a power-law term (proportional to the power of the Hubble parameter H). In a dissipative universe, the irreversible entropy included in the Hubble volume is found to be proportional to H −1 , unlike for the Bekenstein-Hawking entropy on the horizon of the universe. In addition, the evolution of the horizon entropy is examined, extending the previous analysis of a non-dissipative universe [Phys. Rev. D 100, 123545 (2019)]. In the present model, the generalized second law of thermodynamics is always satisfied, whereas the maximization of entropy is satisfied under specific conditions. The dissipative universe should be constrained by the entropy maximization as if the universe behaves as an ordinary, isolated macroscopic system.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.