Correlation between superconductivity and normal-state properties in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">La</mml:mi></mml:mrow><mml:mrow><mml:mn>1.85</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Sr</mml:mi></mml:mrow><mml:mrow><mml:mn>0.15</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Zn</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>)</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>system
TL;DRAbstract
Superconducting and normal-state properties have been studied in the ${\mathrm{La}}_{1.85}{\mathrm{Sr}}_{0.15}({\mathrm{Cu}}_{1\ensuremath{-}x}{\mathrm{Zn}}_{x}){\mathrm{O}}_{4}$ system with $0\ensuremath{\le}x\ensuremath{\le}0.06$. The value of ${T}_{c}$ decreases rapidly with the Zn content and vanishes as 2.1 at.% of Zn is doped into the Cu sublattice. Metallic resistivity is observed when superconductivity disappears at $x=0.02$. The suppression of ${T}_{c}$ is not caused by the reduction of carrier concentration which should remain constant in the Zn-doped samples, but rather due to the filling of the local Cu ${d}_{{x}^{2}\ensuremath{-}{y}^{2}}$ state. The residual resistivity scales linearly with the Zn content as expected from the impurity scattering due to disorder. Quantitative analysis of the residual resistivity indicates that the mean free path due to disorder is about twice as large as the coherence length when ${T}_{c}$ is suppressed to zero. The implication of this find
Chat with Paper
AI Agents for this Paper
Superconducting and normal-state properties have been studied in the ${\mathrm{La}}_{1.85}{\mathrm{Sr}}_{0.15}({\mathrm{Cu}}_{1\ensuremath{-}x}{\mathrm{Zn}}_{x}){\mathrm{O}}_{4}$ system with $0\ensuremath{\le}x\ensuremath{\le}0.06$. The value of ${T}_{c}$ decreases rapidly with the Zn content and vanishes as 2.1 at.% of Zn is doped into the Cu sublattice. Metallic resistivity is observed when superconductivity disappears at $x=0.02$. The suppression of ${T}_{c}$ is not caused by the reduction of carrier concentration which should remain constant in the Zn-doped samples, but rather due to the filling of the local Cu ${d}_{{x}^{2}\ensuremath{-}{y}^{2}}$ state. The residual resistivity scales linearly with the Zn content as expected from the impurity scattering due to disorder. Quantitative analysis of the residual resistivity indicates that the mean free path due to disorder is about twice as large as the coherence length when ${T}_{c}$ is suppressed to zero. The implication of this find
Keywords
Chat
Click to start Chat