Isotope effect in La2−xSrxCuO4 superconductors
Maria Ronay, M. A. Frisch, T. R. McGuire
DOI 10.1103/PhysRevB.45.355 · Physical Review B
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Abstract
A ‘‘nonzero’’ isotope effect for x=0.15, and an ‘‘anomalous’’ isotope effect, with the oxygen isotope-effect exponent αO larger than the theoretical value of 0.5 for x=0.12, were reported in the past for the La2−xSrxCuO4 system. In view of the importance of understanding the mechanisms of high-temperature superconductivity, a reinvestigation of the isotope effect with more precise materials synthesis and isotope characterization is called for. We synthesized in flowing O218, or in flowing O216, copper-rich and stoichiometric versions of the La2−xSrxCuO4 materials at x=0.125 and x=0.15. We characterized the materials with x-ray diffraction, high-sensitivity, high-temperature mass spectrometry, and magnetic measurements. We found that in the stoichiometric materials, both at x=0.125 and x=0.15, the oxygen isotope-effect exponent, αO≃0.4. The copper-rich samples at x=0.125 have a larger isotope shift than the stoichiometric ones, due to a larger amount of the La1.67Sr0.33Cu2O5 nonsuperconducting second phase in the containing18 material, than in the containing16 material, which leaves the superconducting phase with a lower strontium concentration, which further lowers Tc. For the copper-rich x=0.15 material we found an oxygen isotope-effect exponent αO=0.08.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| La1.87Sr0.125Cu1.07O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 28.8 | Pressure not reported | unknown |
| La1.87Sr0.125Cu1.07O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 26.4 | Pressure not reported | unknown |
| La1.88Sr0.125Cu0.97O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30.1 | Pressure not reported | unknown |
| La1.88Sr0.125Cu0.97O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 28.4 | Pressure not reported | unknown |
| La1.85Sr0.15Cu1.07O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 36.6 | Pressure not reported | unknown |
| La1.85Sr0.15Cu1.07O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 36.3 | Pressure not reported | unknown |
| La1.85Sr0.15Cu0.97O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 33.25 | Pressure not reported | unknown |
| La1.85Sr0.15Cu0.97O4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 31.75 | Pressure not reported | unknown |
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