Abstract <p>Deposition modes for thin films of FeSe<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\({}_{0.5}\)</EquationSource> <!--BPhysMGU2570033Petrov-m7--> </InlineEquation>Te<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\({}_{0.5}\)</EquationSource> <!--BPhysMGU2570033Petrov-m8--> </InlineEquation> on an amorphous substrate made of K-208 glass, containing cerium oxide (CeO<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq9.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\({}_{2}\)</EquationSource> <!--BPhysMGU2570033Petrov-m9--> </InlineEquation>), have been found. The transition temperature of the film, <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="63" /> </InlineMediaObject> <EquationSource Format="TEX">\(T_{\textrm{C}}=9.5\)</EquationSource> <!--BPhysMGU2570033Petrov-m10--> </InlineEquation> K, to the superconducting state turned out to be higher than that on borosilicate glass from Fischer Scientific, which does not contain CeO<InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq9.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\({}_{2}\)</EquationSource> <!--BPhysMGU2570033Petrov-m11--> </InlineEquation>, but lower than the superconducting transition temperature of the target, <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="89" /> </InlineMediaObject> <EquationSource Format="TEX">\(T_{\textrm{C}}(M)=14\)</EquationSource> <!--BPhysMGU2570033Petrov-m12--> </InlineEquation> K. This behavior contrasts with the well-known properties of thin films in the FeSe and FeSe<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq13.gif" Format="GIF" Height="8" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\({}_{x}\)</EquationSource> <!--BPhysMGU2570033Petrov-m13--> </InlineEquation>Te<InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq14.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\({}_{1-x}\)</EquationSource> <!--BPhysMGU2570033Petrov-m14--> </InlineEquation> family on crystalline substrates. Based on the measurement results, the vortex activation energy (<i>U</i>), the critical current density (<InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq15.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(j_{\textrm{C}}\)</EquationSource> <!--BPhysMGU2570033Petrov-m15--> </InlineEquation>), the upper critical field (<InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq16.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{C2}\)</EquationSource> <!--BPhysMGU2570033Petrov-m16--> </InlineEquation>), and the irreversibility field (<InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11972_2025_8783_Article_IEq17.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{\textrm{irr}}\)</EquationSource> <!--BPhysMGU2570033Petrov-m17--> </InlineEquation>) have been obtained.</p>

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FeSe\({}_{\mathbf{0.5}}\)Te\({}_{\mathbf{0.5}}\) Films on Glass with CeO\({}_{\mathbf{2}}\) Doping

  • A. V. Petrov,
  • O. V. Snigirev,
  • E. A. Ovchenkov,
  • Yu. V. Blinova,
  • N. V. Porokhov,
  • A. R. Shevchenko,
  • D. A. Chareev,
  • A. G. Maresov

摘要

Abstract

Deposition modes for thin films of FeSe \({}_{0.5}\) Te \({}_{0.5}\) on an amorphous substrate made of K-208 glass, containing cerium oxide (CeO \({}_{2}\) ), have been found. The transition temperature of the film, \(T_{\textrm{C}}=9.5\) K, to the superconducting state turned out to be higher than that on borosilicate glass from Fischer Scientific, which does not contain CeO \({}_{2}\) , but lower than the superconducting transition temperature of the target, \(T_{\textrm{C}}(M)=14\) K. This behavior contrasts with the well-known properties of thin films in the FeSe and FeSe \({}_{x}\) Te \({}_{1-x}\) family on crystalline substrates. Based on the measurement results, the vortex activation energy (U), the critical current density ( \(j_{\textrm{C}}\) ), the upper critical field ( \(H_{C2}\) ), and the irreversibility field ( \(H_{\textrm{irr}}\) ) have been obtained.