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dc.contributor.authorMyrzakulov, Yerlan
dc.contributor.authorDonmez, O.
dc.contributor.authorKoussour, M.
dc.contributor.authorAlizhanov, D.
dc.contributor.authorBekchanov, S.
dc.contributor.authorRayimbaev, J.
dc.date.accessioned2026-03-27T12:12:53Z
dc.date.available2026-03-27T12:12:53Z
dc.date.issued2024
dc.identifier.issn22126864
dc.identifier.otherDOI 10.1016/j.dark.2024.101614
dc.identifier.urihttp://repository.enu.kz/handle/enu/30879
dc.description.abstractIn 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.isoenru
dc.publisherPhysics of the Dark Universeru
dc.relation.ispartofseriesVolume 46 Article number 101614;
dc.titleLate-time cosmology in f(Q,Lm) gravity: Analytical solutions and observational fitsru
dc.typeArticleru


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