Bulk-modulus anomalies at the superconducting transition of single-phase Y<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Ba</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>7</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
Аннотация
We report sound-velocity measurements on polycrystalline single-phase Y${\mathrm{Ba}}_{2}$${\mathrm{Cu}}_{3}$${\mathrm{O}}_{7}$ with a ${T}_{c}$ of 90 K. The sound velocity is found to increase as the temperature is reduced from room temperature in contrast to the decrease observed in ${\mathrm{La}}_{1.85}$${\mathrm{Sr}}_{0.15}$Cu${\mathrm{O}}_{4}$. At ${T}_{c}$ there is no discontinuity in the sound velocity within experimental resolution, as expected from thermodynamic arguments and the small value of $\frac{d{T}_{c}}{\mathrm{dP}}$. As the temperature is lowered below ${T}_{c}$ the sound velocity increases at a greater rate. A similar increase below ${T}_{c}$ is observed in ${\mathrm{La}}_{1.85}$${\mathrm{Sr}}_{0.15}$Cu${\mathrm{O}}_{4}$. The magnitude of the sound-velocity increase below ${T}_{c}$ is much larger than observed in conventional superconductors.
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