<p>In this paper, we investigate the evolution of the FLRW universe by analyzing the constant jerk parameter <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>j</mi> </math></EquationSource> <EquationSource Format="TEX">$j$</EquationSource> </InlineEquation> within the framework of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>f</mi> <mo stretchy="false">(</mo> <mi>T</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$f(T)$</EquationSource> </InlineEquation> gravity. Using a model-independent parametrization approach, we assume <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>j</mi> </math></EquationSource> <EquationSource Format="TEX">$j$</EquationSource> </InlineEquation> as constant and derive an expression for the Hubble parameter as <Equation ID="Equa"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_Equa.gif" Format="GIF" Height="50" Rendition="HTML" Resolution="72" Type="Linedraw" Width="385" /> </MediaObject> <EquationSource Format="MATHML"><math> <mi>H</mi> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> <mo>=</mo> <msub> <mi>H</mi> <mn>0</mn> </msub> <msup> <mrow> <mo>[</mo> <msub> <mi>ξ</mi> <mn>1</mn> </msub> <msup> <mrow> <mo>(</mo> <mi>z</mi> <mo>+</mo> <mn>1</mn> <mo>)</mo> </mrow> <mfrac> <mrow> <mn>3</mn> <mo>+</mo> <msqrt> <mrow> <mn>8</mn> <mi>j</mi> <mo>+</mo> <mn>1</mn> </mrow> </msqrt> </mrow> <mn>2</mn> </mfrac> </msup> <mo>+</mo> <mrow> <mo>(</mo> <mn>1</mn> <mo>−</mo> <msub> <mi>ξ</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> <msup> <mrow> <mo>(</mo> <mi>z</mi> <mo>+</mo> <mn>1</mn> <mo>)</mo> </mrow> <mfrac> <mrow> <mn>3</mn> <mo>−</mo> <msqrt> <mrow> <mn>8</mn> <mi>j</mi> <mo>+</mo> <mn>1</mn> </mrow> </msqrt> </mrow> <mn>2</mn> </mfrac> </msup> <mo>]</mo> </mrow> <mfrac> <mrow> <mn>1</mn> </mrow> <mn>2</mn> </mfrac> </msup> </math></EquationSource> <EquationSource Format="TEX"> \(\begin{aligned} H(z)=H_{0}\left [\xi _{1}\left (z+1\right )^{\frac{3+\sqrt{8j+1}}{2}}+ \left (1{-\xi }_{1}\right )\left (z+1\right )^{\frac{3-\sqrt{8j+1}}{2}} \right ]^{\frac{1}{2}} \end{aligned}\) </EquationSource> </Equation> We estimate model parameters via a Chi-square test coupled with Markov Chain Monte Carlo (MCMC) simulations, based on 52 Observational Hubble Data (OHD) points and 1701 Pantheon+SHOES data points. This method yields the best fit values: <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq6.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="97" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>ξ</mi> <mn>1</mn> </msub> <mo>=</mo> <msubsup> <mn>0.39</mn> <mrow> <mo>−</mo> <mn>0.08</mn> </mrow> <mrow> <mo>+</mo> <mn>0.12</mn> </mrow> </msubsup> </math></EquationSource> <EquationSource Format="TEX">$\xi _{1}={0.39}_{-0.08}^{+0.12}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq7.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="91" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>j</mi> <mo>=</mo> <msubsup> <mn>0.67</mn> <mrow> <mo>−</mo> <mn>0.19</mn> </mrow> <mrow> <mo>+</mo> <mn>0.19</mn> </mrow> </msubsup> </math></EquationSource> <EquationSource Format="TEX">$j={0.67}_{-0.19}^{+0.19}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq8.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="199" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mn>0</mn> </msub> <mo>=</mo> <msubsup> <mn>66.08</mn> <mrow> <mo>−</mo> <mn>2.78</mn> </mrow> <mrow> <mo>+</mo> <mn>2.83</mn> </mrow> </msubsup> <mspace width="0.25em" /> <mi>k</mi> <mi>m</mi> <mo stretchy="false">/</mo> <mi>s</mi> <mo stretchy="false">/</mo> <mi>M</mi> <mi>p</mi> <mi>c</mi> </math></EquationSource> <EquationSource Format="TEX">$H_{0}={66.08}_{-2.78}^{+2.83} \; km/s/Mpc$</EquationSource> </InlineEquation> for OHD dataset and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq9.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="97" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>ξ</mi> <mn>1</mn> </msub> <mo>=</mo> <msubsup> <mn>0.37</mn> <mrow> <mo>−</mo> <mn>0.03</mn> </mrow> <mrow> <mo>+</mo> <mn>0.03</mn> </mrow> </msubsup> </math></EquationSource> <EquationSource Format="TEX">$\xi _{1}={0.37}_{-0.03}^{+0.03}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq10.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="91" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>j</mi> <mo>=</mo> <msubsup> <mn>0.67</mn> <mrow> <mo>−</mo> <mn>0.38</mn> </mrow> <mrow> <mo>+</mo> <mn>0.40</mn> </mrow> </msubsup> </math></EquationSource> <EquationSource Format="TEX">$j={0.67}_{-0.38}^{+0.40}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq11.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="110" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mn>0</mn> </msub> <mo>=</mo> <msubsup> <mn>72.80</mn> <mrow> <mo>−</mo> <mn>0.29</mn> </mrow> <mrow> <mo>+</mo> <mn>0.31</mn> </mrow> </msubsup> </math></EquationSource> <EquationSource Format="TEX">$H_{0}={72.80}_{-0.29}^{+0.31}$</EquationSource> </InlineEquation> <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="85" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>k</mi> <mi>m</mi> <mo stretchy="false">/</mo> <mi>s</mi> <mo stretchy="false">/</mo> <mi>M</mi> <mi>p</mi> <mi>c</mi> </math></EquationSource> <EquationSource Format="TEX">$km/s/Mpc$</EquationSource> </InlineEquation> for Pantheon+SHOES dataset. The value of <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq13.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mn>0</mn> </msub> </math></EquationSource> <EquationSource Format="TEX">$H_{0}$</EquationSource> </InlineEquation> obtained in our analysis closely resembles the value estimated by the Planck Collaboration in 2018, <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq14.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="202" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>67.4</mn> <mo>±</mo> <mn>0.5</mn> <mspace width="0.25em" /> <mi>k</mi> <mi>m</mi> <mo stretchy="false">/</mo> <mi>s</mi> <mo stretchy="false">/</mo> <mi>M</mi> <mi>p</mi> <mi>c</mi> </math></EquationSource> <EquationSource Format="TEX">$H_{0}=67.4\pm 0.5\; km/s/Mpc$</EquationSource> </InlineEquation>. Our analysis of the deceleration parameter <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq15.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>q</mi> </math></EquationSource> <EquationSource Format="TEX">$q$</EquationSource> </InlineEquation> reveals a transition from an early decelerating phase to a present accelerating expansion, with <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq16.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="97" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>q</mi> <mn>0</mn> </msub> <mo>≈</mo> <mo>−</mo> <mn>0.3887</mn> </math></EquationSource> <EquationSource Format="TEX">$q_{0}\approx -0.3887$</EquationSource> </InlineEquation> <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq17.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mo stretchy="false">(</mo> <mi>O</mi> <mi>H</mi> <mi>D</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$(OHD)$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq18.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="97" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>q</mi> <mn>0</mn> </msub> <mo>≈</mo> <mo>−</mo> <mn>0.4139</mn> </math></EquationSource> <EquationSource Format="TEX">$q_{0}\approx -0.4139$</EquationSource> </InlineEquation> <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq19.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="173" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mo stretchy="false">(</mo> <mi>P</mi> <mi>a</mi> <mi>n</mi> <mi>t</mi> <mi>h</mi> <mi>e</mi> <mi>o</mi> <mi>n</mi> <mo>+</mo> <mi>S</mi> <mi>H</mi> <mi>O</mi> <mi>E</mi> <mi>S</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$(Pantheon+SHOES)$</EquationSource> </InlineEquation>. Additionally, we examine dynamic parameter such as energy density, pressure, and equation of state parameter within the model <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq20.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="124" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>f</mi> <mrow> <mo>(</mo> <mi>T</mi> <mo>)</mo> </mrow> <mo>=</mo> <mi>T</mi> <mo>+</mo> <mi>η</mi> <msup> <mi>T</mi> <mi>β</mi> </msup> </math></EquationSource> <EquationSource Format="TEX">$f\left (T\right )=T+\eta T^{\beta }$</EquationSource> </InlineEquation>, where <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq21.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> <EquationSource Format="TEX">$\eta $</EquationSource> </InlineEquation> and <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq22.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation> are an arbitrary real constant. The equation of state parameter <InlineEquation ID="IEq23"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq23.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>ω</mi> </math></EquationSource> <EquationSource Format="TEX">$\omega $</EquationSource> </InlineEquation> in our model demonstrates a smooth transition from the radiation-dominated era to the matter-dominated era and finally to the dark energy era. The present-day values of <InlineEquation ID="IEq24"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq24.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="99" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>ω</mi> <mn>0</mn> </msub> <mo>≈</mo> <mo>−</mo> <mn>0.6196</mn> </math></EquationSource> <EquationSource Format="TEX">$\omega _{0} \approx -0.6196$</EquationSource> </InlineEquation> <InlineEquation ID="IEq25"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq25.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mo stretchy="false">(</mo> <mi>O</mi> <mi>H</mi> <mi>D</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$(OHD)$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq26"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq26.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="99" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>ω</mi> <mn>0</mn> </msub> <mo>≈</mo> <mo>−</mo> <mn>0.6548</mn> </math></EquationSource> <EquationSource Format="TEX">$\omega _{0} \approx -0.6548$</EquationSource> </InlineEquation> <InlineEquation ID="IEq27"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq27.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="173" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mo stretchy="false">(</mo> <mi>P</mi> <mi>a</mi> <mi>n</mi> <mi>t</mi> <mi>h</mi> <mi>e</mi> <mi>o</mi> <mi>n</mi> <mo>+</mo> <mi>S</mi> <mi>H</mi> <mi>O</mi> <mi>E</mi> <mi>S</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$(Pantheon+SHOES)$</EquationSource> </InlineEquation> suggests that the universe is currently in a quintessence phase, where dark energy behaves as a dynamical component rather than a cosmological constant <InlineEquation ID="IEq28"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq28.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>ω</mi> <mo>=</mo> <mo>−</mo> <mn>1</mn> </math></EquationSource> <EquationSource Format="TEX">$\omega = -1$</EquationSource> </InlineEquation>. This behavior indicates that our model is physically acceptable and aligns with the general features of cosmic evolution. Notably, the strong energy condition (SEC) is violated at present <InlineEquation ID="IEq29"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq29.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mrow> <mo>(</mo> <mi>z</mi> <mo>=</mo> <mn>0</mn> <mo>)</mo> </mrow> </math></EquationSource> <EquationSource Format="TEX">$\left (z =0\right )$</EquationSource> </InlineEquation> and is projected to remain violated in the future <InlineEquation ID="IEq30"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq30.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mrow> <mo>(</mo> <mi>z</mi> <mo>&lt;</mo> <mn>0</mn> <mo>)</mo> </mrow> </math></EquationSource> <EquationSource Format="TEX">$\left (z &lt; 0\right )$</EquationSource> </InlineEquation>, driving the observed accelerated expansion of the universe. Also, this study offers insights into the impact of a constant jerk parameter on cosmic evolution and expansion dynamics within the framework of modified gravity, with a specific focus on the <InlineEquation ID="IEq31"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4428_Article_IEq31.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>f</mi> <mrow> <mo>(</mo> <mi>T</mi> <mo>)</mo> </mrow> </math></EquationSource> <EquationSource Format="TEX">$f\left (T\right )$</EquationSource> </InlineEquation> gravity model.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Exploring cosmological effects of a constant jerk parameter in FLRW universe within \(f(T)\) gravity

  • Syed Mudassir Syed Iqbal,
  • G. U. Khapekar

摘要

In this paper, we investigate the evolution of the FLRW universe by analyzing the constant jerk parameter j $j$ within the framework of f ( T ) $f(T)$ gravity. Using a model-independent parametrization approach, we assume j $j$ as constant and derive an expression for the Hubble parameter as H ( z ) = H 0 [ ξ 1 ( z + 1 ) 3 + 8 j + 1 2 + ( 1 ξ 1 ) ( z + 1 ) 3 8 j + 1 2 ] 1 2 \(\begin{aligned} H(z)=H_{0}\left [\xi _{1}\left (z+1\right )^{\frac{3+\sqrt{8j+1}}{2}}+ \left (1{-\xi }_{1}\right )\left (z+1\right )^{\frac{3-\sqrt{8j+1}}{2}} \right ]^{\frac{1}{2}} \end{aligned}\) We estimate model parameters via a Chi-square test coupled with Markov Chain Monte Carlo (MCMC) simulations, based on 52 Observational Hubble Data (OHD) points and 1701 Pantheon+SHOES data points. This method yields the best fit values: ξ 1 = 0.39 0.08 + 0.12 $\xi _{1}={0.39}_{-0.08}^{+0.12}$ , j = 0.67 0.19 + 0.19 $j={0.67}_{-0.19}^{+0.19}$ , H 0 = 66.08 2.78 + 2.83 k m / s / M p c $H_{0}={66.08}_{-2.78}^{+2.83} \; km/s/Mpc$ for OHD dataset and ξ 1 = 0.37 0.03 + 0.03 $\xi _{1}={0.37}_{-0.03}^{+0.03}$ , j = 0.67 0.38 + 0.40 $j={0.67}_{-0.38}^{+0.40}$ , H 0 = 72.80 0.29 + 0.31 $H_{0}={72.80}_{-0.29}^{+0.31}$ k m / s / M p c $km/s/Mpc$ for Pantheon+SHOES dataset. The value of H 0 $H_{0}$ obtained in our analysis closely resembles the value estimated by the Planck Collaboration in 2018, H 0 = 67.4 ± 0.5 k m / s / M p c $H_{0}=67.4\pm 0.5\; km/s/Mpc$ . Our analysis of the deceleration parameter q $q$ reveals a transition from an early decelerating phase to a present accelerating expansion, with q 0 0.3887 $q_{0}\approx -0.3887$ ( O H D ) $(OHD)$ and q 0 0.4139 $q_{0}\approx -0.4139$ ( P a n t h e o n + S H O E S ) $(Pantheon+SHOES)$ . Additionally, we examine dynamic parameter such as energy density, pressure, and equation of state parameter within the model f ( T ) = T + η T β $f\left (T\right )=T+\eta T^{\beta }$ , where η $\eta $ and β $\beta $ are an arbitrary real constant. The equation of state parameter ω $\omega $ in our model demonstrates a smooth transition from the radiation-dominated era to the matter-dominated era and finally to the dark energy era. The present-day values of ω 0 0.6196 $\omega _{0} \approx -0.6196$ ( O H D ) $(OHD)$ and ω 0 0.6548 $\omega _{0} \approx -0.6548$ ( P a n t h e o n + S H O E S ) $(Pantheon+SHOES)$ suggests that the universe is currently in a quintessence phase, where dark energy behaves as a dynamical component rather than a cosmological constant ω = 1 $\omega = -1$ . This behavior indicates that our model is physically acceptable and aligns with the general features of cosmic evolution. Notably, the strong energy condition (SEC) is violated at present ( z = 0 ) $\left (z =0\right )$ and is projected to remain violated in the future ( z < 0 ) $\left (z < 0\right )$ , driving the observed accelerated expansion of the universe. Also, this study offers insights into the impact of a constant jerk parameter on cosmic evolution and expansion dynamics within the framework of modified gravity, with a specific focus on the f ( T ) $f\left (T\right )$ gravity model.