<p>This study investigates the properties of AlB<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>-type YB<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> and YGa<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> compounds using density-functional theory, focusing on elastic constants, electronic structure, mechanical behavior, and electron–phonon (<Emphasis Type="BoldItalic">e</Emphasis>-<Emphasis Type="BoldItalic">ph</Emphasis>) coupling. The results, aligned with theoretical predictions, are compared with MgB<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> to assess their superconducting potential. YGa<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> has larger structural dimensions but lower phonon frequencies due to gallium’s higher atomic mass. YB<InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>, on the other hand, shows a higher critical temperature (5.59 K), attributed to its stronger <Emphasis Type="BoldItalic">e</Emphasis>-<Emphasis Type="BoldItalic">ph</Emphasis> coupling and higher density of states at the Fermi level. Shorter B-B bonds in YB<InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> enhance its band structure and raise the Fermi energy. Both compounds are mechanically stable, with YB<InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> exhibiting higher shear resistance and stronger covalent bonding. Additionally, YB<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> has a higher Debye temperature (779.75 K) and sound velocities, indicating superior mechanical properties. These findings underscore YB<InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>’s promise as a superconductor with favorable <Emphasis Type="BoldItalic">e</Emphasis>-<Emphasis Type="BoldItalic">ph</Emphasis> interactions compared to YGa<InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7017_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{\varvec{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>.</p>

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The Physical and Superconducting Properties of Hexagonal YGa\(_2\) and YB\(_2\): A Comparative Ab-Initio Study

  • Cihan Parlak,
  • Gürcan Yıldırım

摘要

This study investigates the properties of AlB \(_{\varvec{2}}\) 2 -type YB \(_{\varvec{2}}\) 2 and YGa \(_{\varvec{2}}\) 2 compounds using density-functional theory, focusing on elastic constants, electronic structure, mechanical behavior, and electron–phonon (e-ph) coupling. The results, aligned with theoretical predictions, are compared with MgB \(_{\varvec{2}}\) 2 to assess their superconducting potential. YGa \(_{\varvec{2}}\) 2 has larger structural dimensions but lower phonon frequencies due to gallium’s higher atomic mass. YB \(_{\varvec{2}}\) 2 , on the other hand, shows a higher critical temperature (5.59 K), attributed to its stronger e-ph coupling and higher density of states at the Fermi level. Shorter B-B bonds in YB \(_{\varvec{2}}\) 2 enhance its band structure and raise the Fermi energy. Both compounds are mechanically stable, with YB \(_{\varvec{2}}\) 2 exhibiting higher shear resistance and stronger covalent bonding. Additionally, YB \(_{\varvec{2}}\) 2 has a higher Debye temperature (779.75 K) and sound velocities, indicating superior mechanical properties. These findings underscore YB \(_{\varvec{2}}\) 2 ’s promise as a superconductor with favorable e-ph interactions compared to YGa \(_{\varvec{2}}\) 2 .