<p>In this work, we investigate the thermodynamic properties of a non-rotating hairy Bardeen black hole, highlighting deviations from the predictions of standard general relativity due to the presence of additional parameters. Specifically, we analyze the influence of the electric charge <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>Q</mi> </math></EquationSource> <EquationSource Format="TEX">$Q $</EquationSource> </InlineEquation>, the coupling constant <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation>, and the model parameter <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> <EquationSource Format="TEX">$\eta $</EquationSource> </InlineEquation> on the black hole’s mass, temperature, sparsity parameter and entropy. While the overall qualitative behavior of these quantities remains consistent, we find that both <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>Q</mi> </math></EquationSource> <EquationSource Format="TEX">$Q $</EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> <EquationSource Format="TEX">$\eta $</EquationSource> </InlineEquation> tend to decrease the mass and temperature, whereas <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation> exerts an opposite effect by increasing them. Furthermore, using the entropic force approach, we derive a novel expression for the black hole entropy, which encapsulates the modifications to the underlying gravitational interaction. We then examine how the parameters <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>Q</mi> </math></EquationSource> <EquationSource Format="TEX">$Q $</EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation>, and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> <EquationSource Format="TEX">$\eta $</EquationSource> </InlineEquation> affect the circular motion of photons. Our results show that the radius of stable circular orbits increases with <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>Q</mi> </math></EquationSource> <EquationSource Format="TEX">$Q $</EquationSource> </InlineEquation> and <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> <EquationSource Format="TEX">$\eta $</EquationSource> </InlineEquation>, while the radius of unstable circular orbits decreases with <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>Q</mi> </math></EquationSource> <EquationSource Format="TEX">$Q $</EquationSource> </InlineEquation> and increases with <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation>. Additionally, the critical impact parameter is found to grow with increasing <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>Q</mi> </math></EquationSource> <EquationSource Format="TEX">$Q $</EquationSource> </InlineEquation>, but diminish with increasing <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation>. We also study the variations in the Keplerian frequency of photons orbiting the black hole under the influence of these parameters. For small radial distances <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq16.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>r</mi> </math></EquationSource> <EquationSource Format="TEX">$r $</EquationSource> </InlineEquation>, the charge <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>Q</mi> </math></EquationSource> <EquationSource Format="TEX">$Q $</EquationSource> </InlineEquation> reduces the frequency, while for intermediate and large <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq16.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>r</mi> </math></EquationSource> <EquationSource Format="TEX">$r $</EquationSource> </InlineEquation>, it causes an increase. A similar trend is observed for the model parameter <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> <EquationSource Format="TEX">$\eta $</EquationSource> </InlineEquation> for small values of <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq20.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>r</mi> </math></EquationSource> <EquationSource Format="TEX">$r$</EquationSource> </InlineEquation>, whereas the coupling constant <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2025_4499_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation> produces the opposite effect across these regimes. At the end of the paper, we derive the modified Friedmann equation from the entropy of the studied black hole.</p>

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Non-rotating hairy Bardeen black hole: thermodynamic properties, entropic force, and circular photon motion

  • Abdelhakim Benkrane

摘要

In this work, we investigate the thermodynamic properties of a non-rotating hairy Bardeen black hole, highlighting deviations from the predictions of standard general relativity due to the presence of additional parameters. Specifically, we analyze the influence of the electric charge Q $Q $ , the coupling constant β $\beta $ , and the model parameter η $\eta $ on the black hole’s mass, temperature, sparsity parameter and entropy. While the overall qualitative behavior of these quantities remains consistent, we find that both Q $Q $ and η $\eta $ tend to decrease the mass and temperature, whereas β $\beta $ exerts an opposite effect by increasing them. Furthermore, using the entropic force approach, we derive a novel expression for the black hole entropy, which encapsulates the modifications to the underlying gravitational interaction. We then examine how the parameters Q $Q $ , β $\beta $ , and η $\eta $ affect the circular motion of photons. Our results show that the radius of stable circular orbits increases with Q $Q $ and η $\eta $ , while the radius of unstable circular orbits decreases with Q $Q $ and increases with β $\beta $ . Additionally, the critical impact parameter is found to grow with increasing Q $Q $ , but diminish with increasing β $\beta $ . We also study the variations in the Keplerian frequency of photons orbiting the black hole under the influence of these parameters. For small radial distances r $r $ , the charge Q $Q $ reduces the frequency, while for intermediate and large r $r $ , it causes an increase. A similar trend is observed for the model parameter η $\eta $ for small values of r $r$ , whereas the coupling constant β $\beta $ produces the opposite effect across these regimes. At the end of the paper, we derive the modified Friedmann equation from the entropy of the studied black hole.