Abstract <p>We investigate the implications of the modified gravity theory <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(R,L_{m})\)</EquationSource> <!--GravCos2470051Shukla-m3--> </InlineEquation> on the cosmological evolution. By examining the nonlinear model <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="226" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(R,L_{m})={R}/{2}+(\alpha R+1)L_{m}\)</EquationSource> <!--GravCos2470051Shukla-m4--> </InlineEquation>, we explore the impact of a nonminimal coupling between curvature and matter on the cosmic expansion. Using a parametrized deceleration parameter dependent on the redshift <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(z\)</EquationSource> <!--GravCos2470051Shukla-m5--> </InlineEquation>, we analyze the Friedmann–Lemaître–Robertson–Walker (FLRW) universe in the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(R,L_{m})\)</EquationSource> <!--GravCos2470051Shukla-m6--> </InlineEquation> framework. Through observational constraints derived from Cosmic Chronometers (CC), Type Ia Supernovae (SNIa), and Baryon Acoustic Oscillations (BAO), we perform a detailed comparison with the standard <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda\)</EquationSource> <!--GravCos2470051Shukla-m7--> </InlineEquation>CDM model. Our results show that the <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(R,L_{m})\)</EquationSource> <!--GravCos2470051Shukla-m8--> </InlineEquation> model is consistent with observational data, but deviations from the <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq9.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda\)</EquationSource> <!--GravCos2470051Shukla-m9--> </InlineEquation>CDM model emerge in its geometric structure, highlighting the potential of <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5251_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(R,L_{m})\)</EquationSource> <!--GravCos2470051Shukla-m10--> </InlineEquation> gravity in explaining the dark energy and cosmic acceleration.</p>

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Observational Study of the Deceleration Parameter in \(\boldsymbol{f(R,L_{m})}\) Theory of Gravity

  • Bhupendra Kumar Shukla,
  • D. Sofuoğlu,
  • A. Beesham,
  • Ala Ouguergouz,
  • Shashi Narayan Shukla

摘要

Abstract

We investigate the implications of the modified gravity theory \(f(R,L_{m})\) on the cosmological evolution. By examining the nonlinear model \(f(R,L_{m})={R}/{2}+(\alpha R+1)L_{m}\) , we explore the impact of a nonminimal coupling between curvature and matter on the cosmic expansion. Using a parametrized deceleration parameter dependent on the redshift \(z\) , we analyze the Friedmann–Lemaître–Robertson–Walker (FLRW) universe in the \(f(R,L_{m})\) framework. Through observational constraints derived from Cosmic Chronometers (CC), Type Ia Supernovae (SNIa), and Baryon Acoustic Oscillations (BAO), we perform a detailed comparison with the standard \(\Lambda\) CDM model. Our results show that the \(f(R,L_{m})\) model is consistent with observational data, but deviations from the \(\Lambda\) CDM model emerge in its geometric structure, highlighting the potential of \(f(R,L_{m})\) gravity in explaining the dark energy and cosmic acceleration.