4.6 Article

Dynamical study of NTADE and SMHDE models within Rastall gravity

Journal

CHINESE JOURNAL OF PHYSICS
Volume 81, Issue -, Pages -

Publisher

ELSEVIER
DOI: 10.1016/j.cjph.2022.11.009

Keywords

Modified gravity; Dark energy models; Cosmological parameters

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This paper investigates the cosmological implications of Rastall gravity by using the new Tsallis agegraphic dark energy (NTADE) and Sharma-Mittal holographic dark energy (SMHDE) models. The results show that the equation of state parameter for NTADE lies in the phantom region, while for SMHDE it exhibits quintom and quintessence regions dependent on the model parameter delta. The deceleration parameter shows a phase transition from decelerating to accelerating phases for both models. The omega(D) - omega(D)' pair exhibits freezing and thawing regions for NTADE, and freezing region for SMHDE. The (J, s) pair for SMHDE indicates different dark energy eras, including phantom, quintessence, and Chaplygin gas, while the NTADE model only shows Chaplygin gas behavior. It is concluded that SMHDE is a more efficient model as it approaches the Lambda CDM limit and produces results within a stable region according to graphical analysis of the square speed of sound.
This paper is mainly focused to investigate the cosmological implications of Rastall gravity with the help of two dark energy models, i.e., new Tsallis agegraphic dark energy (NTADE) and Sharma-Mittal holographic dark energy (SMHDE). The background of flat FLRW space-time is being considered to develop the dynamical system of equations. To check the viability of these models and to distinguish them, we develop some important cosmological parameters. By constraining the involved model parameters, it is observed that the equation of state (EoS) parameter for the NTADE model lies in the phantom region whereas, for SMHDE, it shows quintom as well as quintessence regions depending on the values of model parameter delta. The deceleration parameter shows the phase transition from decelerating to the accelerating phase for both models. The omega(D) - omega(D)' pair shows freezing and thawing regions for NTADE, and the freezing region for SMHDE. The pair (J, s) for SMHDE indicates a rich behavior as it shows different DE eras, a phantom, the quintessence as well as Chaplygin gas but the NTADE model shows Chaplygin gas behavior only. We conclude that SMHDE is a more efficient model than the NTADE model because it approaches Lambda CDM limit and the results for this model lie in a stable region as shown by graphical analysis of the square speed of sound.

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