Observational constraints on Tsallis holographic dark energy with Ricci horizon cutoff

被引:5
|
作者
Mangoudehi, Zahra Feizi [1 ]
机构
[1] Univ Guilan, Dept Phys, Rasht, Iran
关键词
THDE; Ricci cutoff; Observational constraints; Nonlinear interaction term; Deceleration parameter; Turning point; Stability; Jerk parameter; O M diagnostic; Age of the Universe; PROBE WMAP OBSERVATIONS; COSMOLOGICAL CONSTANT; MODEL; AGE;
D O I
10.1007/s10509-022-04154-2
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
In this research, we are interested in constraining the nonlinear interacting and noninteracting Tsallis holographic dark energy (THDE) with Ricci horizon cutoff by employing three observational datasets. To this aim, the THDE with Ricci horizon considering the noninteraction and nonlinear interaction terms will be fitted by the SNe Ia, SNe Ia+H(z), and SNe Ia+H(z)+GRB samples to investigate the Hubble (H(z)), dark-energy equation of state (omega(DE)), effective equation of state (omega(eff)), and deceleration (q) parameters. Investigating the H(z) parameter illustrates that our models are in good consistency with respect to observations. Also, it can reveal the turning point for both noninteracting and nonlinear interacting THDE with Ricci cutoff in the late-time era. Next, the analysis of the omega(DE) for our models displays that the dark energy can experience the phantom state at the current time. However, this lies in the quintessence regime in the early era and approaches the cosmological constant in the late-time epoch. Similar results will be given for the omega(eff) parameter with the difference that the omega(eff) will experience the quintessence region at the current redshift. In addition to the mentioned parameters, the study of the q parameter indicates that the models satisfy an acceptable transition phase from the matter- to the dark energy-dominated era. After that, the classical stability (v(s)(2)) will be analyzed for our models. The v(s)(2) shows that the noninteracting and nonlinear interacting THDE with Ricci cutoff will be stable in the past era but unstable in the present and progressive epochs. Then, we will employ the Jerk (J) and O M parameters to distinguish between our models and the lambda C DM model. Finally, we will calculate the age of the Universe for the THDE and nonlinear interacting THDE with Ricci as the IR cutoff.
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页数:16
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