Abstract <p>In the context of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(F(T,T_{G})\)</EquationSource> <!--GravCos2570011Pradhan-m3--> </InlineEquation> gravity, we examine the reconstruction scenario of the Tsallis holographic dark energy (THDE) model where <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(T\)</EquationSource> <!--GravCos2570011Pradhan-m4--> </InlineEquation> stands for the torsion scalar, and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(T_{G}\)</EquationSource> <!--GravCos2570011Pradhan-m5--> </InlineEquation> stands for the teleparallel Gauss–Bonnet term. The Hubble constant <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{0}\)</EquationSource> <!--GravCos2570011Pradhan-m6--> </InlineEquation> and the deceleration value <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq7.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(q\)</EquationSource> <!--GravCos2570011Pradhan-m7--> </InlineEquation> are two crucial elements that govern the expansion history of the Universe in power-law cosmology. Using the Markov Chain Monte Carlo (MCMC) technique with the likelihood function, we obtain the sets of constraints as <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq8.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="122" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{0}=70.93^{+0.0024}_{-0.0037}\)</EquationSource> <!--GravCos2570011Pradhan-m8--> </InlineEquation> km/s/Mpc, <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq9.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="132" /> </InlineMediaObject> <EquationSource Format="TEX">\(q=-0.3384^{+0.0027}_{0.0026}\)</EquationSource> <!--GravCos2570011Pradhan-m9--> </InlineEquation> for the Pantheon data and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq10.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="152" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{0}=70.76732^{+0.0030}_{-0.00088}\)</EquationSource> <!--GravCos2570011Pradhan-m10--> </InlineEquation> km/s/Mpc, <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq11.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="132" /> </InlineMediaObject> <EquationSource Format="TEX">\(q=-0.6478^{+0.0093}_{0.0075}\)</EquationSource> <!--GravCos2570011Pradhan-m11--> </InlineEquation> by using the joint data (OHD <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq12.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570011Pradhan-m12--> </InlineEquation> BAO <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq12.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(+\)</EquationSource> <!--GravCos2570011Pradhan-m13--> </InlineEquation> Pantheon), respectively. We find that the considered data fit well with the power-law cosmology at late times. We also use the bulk-viscosity component to solve the modified Einstein’s field equations, <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq14.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="199" /> </InlineMediaObject> <EquationSource Format="TEX">\(\xi=\xi_{0}+\xi_{1}H+\xi_{2}(\dot{H}+H^{2})\)</EquationSource> <!--GravCos2570011Pradhan-m14--> </InlineEquation>. We determine the universe’s current age to be <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq15.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(13.618\)</EquationSource> <!--GravCos2570011Pradhan-m15--> </InlineEquation> Gyr, which is in line with the WMAP data. We additionally discussed the <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12267_2025_5265_Article_IEq16.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(Om(z)\)</EquationSource> <!--GravCos2570011Pradhan-m16--> </InlineEquation> parameter of the derived model.</p>

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Reconstruction of the \(\boldsymbol{F(T,T_{G})}\) Tsallis Holographic Dark Energy Model Based on Observational Constraints

  • Anirudh Pradhan,
  • Archana Dixit,
  • Sanjeev Gupta,
  • S. Krishnannair

摘要

Abstract

In the context of \(F(T,T_{G})\) gravity, we examine the reconstruction scenario of the Tsallis holographic dark energy (THDE) model where \(T\) stands for the torsion scalar, and \(T_{G}\) stands for the teleparallel Gauss–Bonnet term. The Hubble constant \(H_{0}\) and the deceleration value \(q\) are two crucial elements that govern the expansion history of the Universe in power-law cosmology. Using the Markov Chain Monte Carlo (MCMC) technique with the likelihood function, we obtain the sets of constraints as \(H_{0}=70.93^{+0.0024}_{-0.0037}\) km/s/Mpc, \(q=-0.3384^{+0.0027}_{0.0026}\) for the Pantheon data and \(H_{0}=70.76732^{+0.0030}_{-0.00088}\) km/s/Mpc, \(q=-0.6478^{+0.0093}_{0.0075}\) by using the joint data (OHD \(+\) BAO \(+\) Pantheon), respectively. We find that the considered data fit well with the power-law cosmology at late times. We also use the bulk-viscosity component to solve the modified Einstein’s field equations, \(\xi=\xi_{0}+\xi_{1}H+\xi_{2}(\dot{H}+H^{2})\) . We determine the universe’s current age to be \(13.618\) Gyr, which is in line with the WMAP data. We additionally discussed the \(Om(z)\) parameter of the derived model.