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New Astronomy
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Tsallis HDE with an IR cutof as Ricci horizon in a fat FLRW universe
Umesh Kumar Sharma
⁎
,a
, Vandna Srivastava
b
a
Department of Mathematics, Institute of Applied Sciences and Humanities, GLA University Mathura-281406, UP, India
b
Department of Mathematics, Applied Sciences, MIET, Meerut-250005, UP, India
ARTICLE INFO
Keywords:
Phantom
Quintessence
k-essence
THDE
PACS:
98.80.-k
ABSTRACT
The THDE (Tsallis HDE) model using an IR cut of as Ricci horizon has been investigated in the context of a fat
Friedmann-Lema
^
tre-Robertson-Walker Universe by describing an accelerated expansion stage which Universe is
experiencing. Evolution of Universe from decelerated (earlier) to the accelerated (current) phase exhibits by
deceleration parameter (DP) attained in the model of THDE. The good behavior of cosmos is represented by
Tsallis parameter δ and the EoS parameter’s values as phantom era ( < 1
T
) and the quintessence era
( 1
T
). Stability of the THDE model has been suggested by squared sound speed v
s
2
. Additionally, for the
THDE model the relation between phantom, quintessence and k-essence scalar felds has been analysed which
helps to annotate the accelerated phase of the expanded Universe.
1. Introduction
Diferent observations (like measurements of CMB temperature and
polarization anisotropies from the Planck satellite, SNeIa luminosity
distance measurements and measurements of the clustering of the LSS)
from diferent survey provide a noteworthy description of the Universe
Aghanim (2018); Scolnicv (2018); Alam (2017). These observations are
pointing to ΛCDM model which describes the spatially fat Universe
comprising of two dark components :- Dark Energy (DE) and Dark
Matter (DM) Sahni (2004). DE represents about 70% of the total energy
consist of a component which is known for its numerousness and stand
responsible for the acceleration of the current scenario of expanded
Universe and about 5% baryons (the visible matter). Remaining about
25% is associated to DM. Although the nature and cosmological prop-
erties are unrevealed but still researchers accepted the dark energy as a
key to unveil the lining of Universe. CC-cosmological constant (or the
vacuum energy) has been introduced to explain the efects of DE with a
constant equation of state (EoS) parameter ω = where vacuum energy
plays an important role. With the predictions of ΛCDM model for which
observational data are remarkably consistent. Two fundamental pro-
blem arises in front of cosmologists: 1- Fine tuning: (required by vacuum
energy) which gives the comparison between observational cosmolo-
gical constant and fundamental Plank Scale. Fundamental Plank scale is
greater than the observed value 10
123
ρ
p
.
2- Coincidence Problem: Although with the expansion of Universe
evolutionary of two densities of DE and DM is diferent but coincidently
their amount exists in same magnitude. Requirement of the proportion
of DM and DE densities is equal or tending to unity leads to various
dynamic dark energy models have been stated in the literature. Some
references . Barbieri et al. (2005); Heckman et al. (2019); Higgs (2015);
Benisty et al. (2019); Nunes and Pan (2016); Kamenshchik et al. (2001);
Freese and Lewis (2002); Hlozek et al. (2015); . Visinelli and
Vagnozzi (2019); Ratra and PJE (1988); Peracaula et al. (2018);
Wetterich (1988); Bento et al. (2002); Li (2004); PJE and
Vilenkin (1999); Caldwell et al. (1998); Capozziello et al. (2018);
Benisty and Guendelman (2018); Rinaldi (2015); Cicoli et al. (2012);
Di et al. (2020) are included for some recent and infuential approaches
to explain DE and cosmic acceleration alternatively which could alle-
viate or even solve two problems.
On modifying standard HDE as = S A (δ is non-extensive para-
meter and γ is a constant). Tsallis HDE Tavayef et al. (2018), a new dark
energy model has been recently proposed taking Tsallis entropy as its
foundation Tsallis and LJL (2013) and holographic principle(i.e. Finite
number of degrees of freedom in a system which is bounded and related
to the area of its boundary) and energy density = BL
D
2 4
where B is a
(not known) parameter and L is an I R cut-of. With the value = 1 and
=
G
1
4
( = = = h k c 1
B
in units) power-law distribution of probability
neutralizes and in the system of the ordinary probability distribution
the Bekenstein entropy is recouped Vershynina (2019). In
Zadeh et al. (2018a), the researchers investigated the dynamics in both
interacting and non-interacting cases in FRW fat Universe. Inside
Brans-Dicke gravity theory and Brane cosmology Ghafari et al. (2018,
2019), THDE and its outgrowths with an IR cutof as Hubble horizon is
analysed. Sheykhi Sheykhi (2018) by considering an IR cut of to be the
https://doi.org/10.1016/j.newast.2020.101519
Received 4 August 2020; Accepted 3 October 2020
⁎
Corresponding author.
E-mail addresses: sharma.umesh@gla.ac.in (U.K. Sharma), vandna.rathor@miet.ac.in (V. Srivastava).
New Astronomy 84 (2021) 101519
Available online 09 October 2020
1384-1076/ © 2020 Elsevier B.V. All rights reserved.
T