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| dc.contributor.author | Myrzakulov, Yerlan | |
| dc.contributor.author | Donmez, O. | |
| dc.contributor.author | Koussour, M. | |
| dc.contributor.author | Alizhanov, D. | |
| dc.contributor.author | Bekchanov, S. | |
| dc.contributor.author | Rayimbaev, J. | |
| dc.date.accessioned | 2026-03-27T12:12:53Z | |
| dc.date.available | 2026-03-27T12:12:53Z | |
| dc.date.issued | 2024 | |
| dc.identifier.issn | 22126864 | |
| dc.identifier.other | DOI 10.1016/j.dark.2024.101614 | |
| dc.identifier.uri | http://repository.enu.kz/handle/enu/30879 | |
| dc.description.abstract | In this study, we examined the late-time cosmic expansion of the universe within the framework of f(Q,Lm) gravity, where Q denotes the non-metricity and Lm represents the matter Lagrangian. We analyzed a linear f(Q,Lm) model of the form f(Q,Lm)=−αQ+2Lm+β. Using MCMC methods, we constrained the model parameters H0, α, and β with various datasets, including H(z), Pantheon+SH0ES, and BAO data. For the H(z) dataset, we found H0=67.90±0.66, α=0.1072−0.0069+0.0054, and β=−1988.2±1.0. For the Pantheon+SH0ES dataset, H0=70.05±0.68, α=0.0916−0.0033+0.0028, and β=−1988.3±1.0. For the BAO dataset, H0=68.1±1.0, α=0.1029−0.0052+0.0041, and β=−1988.24±0.99. Moreover, the energy density remains positive and approaches zero in the distant future, and the deceleration parameter indicates a transition from deceleration to acceleration, with transition redshifts of zt=0.60, zt=0.78, and zt=0.66 for the respective datasets. These findings align with previous observational studies and contribute to our understanding of the universe's expansion dynamics. | ru |
| dc.language.iso | en | ru |
| dc.publisher | Physics of the Dark Universe | ru |
| dc.relation.ispartofseries | Volume 46 Article number 101614; | |
| dc.title | Late-time cosmology in f(Q,Lm) gravity: Analytical solutions and observational fits | ru |
| dc.type | Article | ru |