Abstract <p>This paper proposes a new scalar field cosmological model aimed at studying the late-time acceleration of the universe, based on a parametrization of the deceleration parameter. The main objective is to constrain fundamental cosmological parameters by integrating the latest measurements of the Hubble parameter from various observational datasets, including BAO, BAO <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570055Beesham-m1--> </InlineEquation> R19, CC <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570055Beesham-m2--> </InlineEquation> SC <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570055Beesham-m3--> </InlineEquation> BAO, and CC <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570055Beesham-m4--> </InlineEquation> SC <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570055Beesham-m5--> </InlineEquation> BAO <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570055Beesham-m6--> </InlineEquation> R19 from recent galaxy surveys. With a redshift range covering <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(0.106&lt;z&lt;2.33\)</EquationSource> <!--GravCos2570055Beesham-m7--> </InlineEquation>, and incorporating the newest Hubble constant measurements from Riess et al. in 2019, we acquire best-fit parameter values for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(H_{0}\)</EquationSource> <!--GravCos2570055Beesham-m8--> </InlineEquation> and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(r_{d}\)</EquationSource> <!--GravCos2570055Beesham-m9--> </InlineEquation>. It is noteworthy that within late-time observations of <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(H_{0}\)</EquationSource> <!--GravCos2570055Beesham-m10--> </InlineEquation>, we observe a significant discrepancy, reproducing the reported <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(H_{0}\)</EquationSource> <!--GravCos2570055Beesham-m11--> </InlineEquation> tension. While our model is in good agreement with both the joint analysis and analysis with R19, discrepancies arise when BAO and BAO with R19 datasets are gradually included. Our model provides an excellent fit to the observed data and is consistent with the standard <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\Lambda\)</EquationSource> <!--GravCos2570055Beesham-m12--> </InlineEquation>CDM paradigm at higher redshifts. However, the most interesting aspect is the prediction of future super-accelerated expansion, in contrast to the de Sitter phase predicted by the <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\Lambda\)</EquationSource> <!--GravCos2570055Beesham-m13--> </InlineEquation>CDM model. The unique behavior of the jerk parameter also hints at new dynamics as ccompared to traditional cosmological models.</p>

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Scalar Field Dark Energy Model Via Observational Constraints

  • Aroonkumar Beesham,
  • Alfred Mvunyelwa Msomi,
  • Sfundo Cebolenkosi Gumede

摘要

Abstract

This paper proposes a new scalar field cosmological model aimed at studying the late-time acceleration of the universe, based on a parametrization of the deceleration parameter. The main objective is to constrain fundamental cosmological parameters by integrating the latest measurements of the Hubble parameter from various observational datasets, including BAO, BAO \(+\) R19, CC \(+\) SC \(+\) BAO, and CC \(+\) SC \(+\) BAO \(+\) R19 from recent galaxy surveys. With a redshift range covering \(0.106<z<2.33\) , and incorporating the newest Hubble constant measurements from Riess et al. in 2019, we acquire best-fit parameter values for \(H_{0}\) and \(r_{d}\) . It is noteworthy that within late-time observations of \(H_{0}\) , we observe a significant discrepancy, reproducing the reported \(H_{0}\) tension. While our model is in good agreement with both the joint analysis and analysis with R19, discrepancies arise when BAO and BAO with R19 datasets are gradually included. Our model provides an excellent fit to the observed data and is consistent with the standard \(\Lambda\) CDM paradigm at higher redshifts. However, the most interesting aspect is the prediction of future super-accelerated expansion, in contrast to the de Sitter phase predicted by the \(\Lambda\) CDM model. The unique behavior of the jerk parameter also hints at new dynamics as ccompared to traditional cosmological models.