Pair-breaking effects in high-temperature superconductors
C. Bandte, P. Hertel, J. Appel
DOI 10.1103/PhysRevB.45.8026 · Physical Review B
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Abstract
We assume strong dynamic pair breaking to be responsible for some of the superconducting properties of the high-Tc materials. Using the theory of superconductors containing paramagnetic impurities, we solve the equation for the temperature-dependent energy gap with a frequency-dependent self-energy, whose ω dependence is obtained by two independent ways: a ‘‘direct’’ procedure using the experimental data of the Raman scattering intensity in the superconducting state and an ‘‘indirect’’ procedure relating the self-energy in the superconducting state to that of the normal state via the dynamical scattering rate. We assume ‘‘marginal-Fermi-liquid’’ behavior for the frequency dependence of the self energy. We obtain a non-BCS-like temperature dependence of the gap Δ(T), which remains nearly constant below Tc and drops almost discontinuously to zero at Tc, with a ratio 2Δ(0)/kTc of up to 8. These results are used to give a qualitative explanation of experimental findings, such as tunneling, infrared, photoemission, and Raman spectroscopy. In addition, the direct procedure predicts gapless superconductivity.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| YBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| YBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| DyBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| (Sm0.5Y0.5)Ba2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| (Sm0.5Ho0.5)Ba2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi2Sr2CaCu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi2Sr2CaCu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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