Thermal-difference reflectance spectroscopy of the high-temperature cuprate superconductors
M. J. Holcomb, C. L. Perry, J. P. Collman, W. A. Little
DOI 10.1103/PhysRevB.53.6734 · Physical Review B
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Abstract
The temperature-dependent thermal-difference reflectance (TDR) spectra of thin-film samples of Tl2Ba2Ca2Cu3O10, (BiPb)2Sr2Ca2Cu3O10, Tl2Ba2CaCu2O8, and YBa2Cu3O7 have been measured for photon energies between 0.3 and 4.5 eV at temperatures above and below each material’s superconducting critical temperature. The amplitude of the characteristic optical structure near the screened plasma frequency of each sample in the normal-state TDR spectrum varies approximately linearly with temperature, T, indicating that the temperature-dependent optical scattering rate in these materials scales with temperature as T2. From the TDR spectra collected above and below the critical temperature of each sample, the superconducting to normal-state reflectance ratio, RS/RN, has been obtained. In all of these spectra, there are significant deviations from unity in RS/RN at photon energies on the order of 2.0 eV. This optical structure cannot be accounted for using the conventional Mattis-Bardeen description of the optical properties of a superconductor or its strong-coupling extension where electron-pairing interactions are limited to energies less than 0.1 eV. However, both the temperature and energy dependence of the structure in the RS/RN spectra may be adequately described within Eliashberg theory with an electron-boson coupling function which consists of both a low-energy component (<0.1 eV) and a high-energy component located between 1.6 and 2.1 eV. © 1996 The American Physical Society.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Tl2Ba2Ca2Cu3O10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| BiPb2Sr2Ca2Cu3O10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Tl2Ba2CaCu2O8 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 |
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