<p>In a perovskite oxide of <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41598_2025_408_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {ABO}_3\)</EquationSource> </InlineEquation>, the <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41598_2025_408_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {BO}_6\)</EquationSource> </InlineEquation> octahedral rotation and tilting are known to result in a structural distortion and transform the crystalline structure to a lower symmetry phase, such as the tetragonal phase (<i>T</i>-phase) and distorted orthorhombic phase (<i>O</i>-phase). Here, we present the observation of such structural transformation in 6 unit cell (uc) ultrathin films of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41598_2025_408_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {SrRuO}_3\)</EquationSource> </InlineEquation> (SRO) driven by an additional <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41598_2025_408_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {SrTiO}_3\)</EquationSource> </InlineEquation> (STO) capping layer. A series of nominal STO (x uc)/SRO (6 uc) films with x ranging from 0 to 8 were grown on STO (001) substrates using an oxide molecular beam system with adsorption-controlled growth technique for SRO and layer-by-layer growth technique for STO. Systematic high-resolution X-ray diffraction measurements revealed a clear transition from the <i>T</i>-phase for x = 0 to the <i>O</i>-phase for x = 2 and 8, which was accompanied by a change of the structural orientation from (001)-oriented SRO in <i>T</i>-phase to (110)-oriented SRO in <i>O</i>-phase. Our findings highlight the possibility of intriguing interface-driven structural phase and orientation transformations in a perovskite oxide system.</p>

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Evolution of the structural phase and orientation in ultrathin SrRuO3 film with SrTiO3 capping layer

  • Akhilesh Kr. Singh,
  • Song Yang,
  • Uddipta Kar,
  • Guan-Ruei Chen,
  • Shih-Chang Weng,
  • Chia-Hung Hsu,
  • Wei-Li Lee

摘要

In a perovskite oxide of \(\text {ABO}_3\) , the \(\text {BO}_6\) octahedral rotation and tilting are known to result in a structural distortion and transform the crystalline structure to a lower symmetry phase, such as the tetragonal phase (T-phase) and distorted orthorhombic phase (O-phase). Here, we present the observation of such structural transformation in 6 unit cell (uc) ultrathin films of \(\text {SrRuO}_3\) (SRO) driven by an additional \(\text {SrTiO}_3\) (STO) capping layer. A series of nominal STO (x uc)/SRO (6 uc) films with x ranging from 0 to 8 were grown on STO (001) substrates using an oxide molecular beam system with adsorption-controlled growth technique for SRO and layer-by-layer growth technique for STO. Systematic high-resolution X-ray diffraction measurements revealed a clear transition from the T-phase for x = 0 to the O-phase for x = 2 and 8, which was accompanied by a change of the structural orientation from (001)-oriented SRO in T-phase to (110)-oriented SRO in O-phase. Our findings highlight the possibility of intriguing interface-driven structural phase and orientation transformations in a perovskite oxide system.