<p>Increasing the critical temperature of superconducting materials, particularly the goal of achieving room temperature, remains one of the significant challenges in the field. Addressing this challenge requires a comprehensive understanding of the factors influencing critical temperature. Specifically, it is hypothesized that increasing the interlayer distance between&#xa0;<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1792_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(CuO_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> planes, along with a corresponding reduction in the surface area of these planes or an increase in the <i>c/a</i> ratio of the crystal lattice constants, could elevate the critical temperature of high-temperature cuprate superconductors. In this study, we investigate the relationship between critical temperature and the <i>c/a</i> ratio at various doping levels of the single <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1792_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(CuO_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>&#xa0;layer cuprate superconductor <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1792_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="113" /> </InlineMediaObject> <EquationSource Format="TEX">\(Hg{Ba}_{2}Cu{O}_{4+\delta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>H</mi> <mi>g</mi> <msub> <mrow> <mi mathvariant="italic">Ba</mi> </mrow> <mn>2</mn> </msub> <mi>C</mi> <mi>u</mi> <msub> <mi>O</mi> <mrow> <mn>4</mn> <mo>+</mo> <mi>δ</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> (Hg-1201), which exhibits the highest known critical temperature, under both atmospheric and high-pressure conditions. Our results indicate no significant correlation between critical temperature and the <i>c/a</i> ratio under atmospheric pressure. However, under applied external pressure, we show a generally decreasing critical temperature as a function of the <i>c/a</i> ratio. These findings suggest that parameters related to the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1792_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(CuO_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>u</mi> <msub> <mi>O</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>&#xa0;planes in Hg-1201 and other high-temperature cuprate superconductors are insufficient to explain the variations in critical temperature. Furthermore, we conclude that charge reservoirs, carrier dynamics, and inter-electronic orbital interactions significantly influence the fluctuations in critical temperature.</p>

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Investigation of the Dependence of the Superconducting Critical Temperature of Hg-1201 on the Crystal Lattice c/a Ratio Under Ambient and High-Pressure Conditions

  • Abdullo Ahadov,
  • Davron Dzhuraev

摘要

Increasing the critical temperature of superconducting materials, particularly the goal of achieving room temperature, remains one of the significant challenges in the field. Addressing this challenge requires a comprehensive understanding of the factors influencing critical temperature. Specifically, it is hypothesized that increasing the interlayer distance between  \(CuO_2\) C u O 2 planes, along with a corresponding reduction in the surface area of these planes or an increase in the c/a ratio of the crystal lattice constants, could elevate the critical temperature of high-temperature cuprate superconductors. In this study, we investigate the relationship between critical temperature and the c/a ratio at various doping levels of the single \(CuO_2\) C u O 2  layer cuprate superconductor \(Hg{Ba}_{2}Cu{O}_{4+\delta }\) H g Ba 2 C u O 4 + δ (Hg-1201), which exhibits the highest known critical temperature, under both atmospheric and high-pressure conditions. Our results indicate no significant correlation between critical temperature and the c/a ratio under atmospheric pressure. However, under applied external pressure, we show a generally decreasing critical temperature as a function of the c/a ratio. These findings suggest that parameters related to the \(CuO_2\) C u O 2  planes in Hg-1201 and other high-temperature cuprate superconductors are insufficient to explain the variations in critical temperature. Furthermore, we conclude that charge reservoirs, carrier dynamics, and inter-electronic orbital interactions significantly influence the fluctuations in critical temperature.