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dc.contributor.authorMyrzakulov, Y.
dc.contributor.authorDonmez, O.
dc.contributor.authorKoussour, M.
dc.contributor.authorMuminov, S.
dc.contributor.authorOstemir, D.
dc.contributor.authorRayimbaev, J.
dc.date.accessioned2026-03-27T07:27:31Z
dc.date.available2026-03-27T07:27:31Z
dc.date.issued2025
dc.identifier.issn1434-6052
dc.identifier.otherdoi.org/10.1140/epjc/s10052-025-14112-1
dc.identifier.urihttp://repository.enu.kz/handle/enu/30844
dc.description.abstractWe are experiencing a golden age of experimental cosmology, with exact and accurate observations being used to constrain various gravitational theories like never before. Alongside these advancements, energy conditions play a crucial theoretical role in evaluating and refining new proposals in gravitational physics. We investigate the energy conditions (WEC, NEC, DEC, and SEC) for two f (Q, Lm) gravity models using the FLRW metric in a flat geometry. Model 1, f (Q, Lm) = −αQ + 2Lm + β, features linear parameter dependence, satisfying most energy conditions while selectively violating the SEC to explain cosmic acceleration. The EoS parameter transitions between quintessence, a cosmological constant, and phantom energy, depending on α and β. Model 2, f (Q, Lm) = −αQ +λ(2Lm)2 +β, introduces nonlinearities, ensuring stronger SEC violations and capturing complex dynamics like dark energy transitions. While Model 1 excels in simplicity, Model 2’s robustness makes it ideal for accelerated expansion scenarios, highlighting the potential of f (Q, Lm) gravity in explaining cosmic phenomena.ru
dc.language.isoenru
dc.publisherThe European Physical Journal Cru
dc.relation.ispartofseries85:376;
dc.titleEnergy conditions in f( Q, Lm) gravityru
dc.typeArticleru


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