Electronic Raman scattering in the single-CuO2 layered superconductor Tl2Ba2CuO6+δ
L. V. Gasparov, P. Lemmens, M. Brinkmann, N. N. Kolesnikov, G. Güntherodt
DOI 10.1103/PhysRevB.55.1223 · Physical Review B
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Abstract
Electronic Raman scattering in Tl2Ba2CuO6+δ (Tl-2201) has been investigated in order to test whether the scattering cross section in high-temperature superconductors depends on the number of CuO2 planes, i.e., sheets or specific details of the Fermi surface. The polarized Raman spectra have been measured in different scattering geometries for temperatures above and below Tc. The spectral features of Tl-2201 with one CuO2 plane per unit cell are found to be similar to Tl2Ba2Ca2Cu3O10 with three CuO2 planes and those of other high-temperature superconductors with several CuO2 planes per unit cell. The peak in the B1g symmetry component of the scattering intensity is found at 460 cm−1(Tc=90nK), or 430 cm−1(Tc=80nK). The B1g peak positions scale with Tc, and correspond to 2Δ/kBTc=7.6±0.4. The temperature dependence of the B1g scattering component of Tl-2201 (Tc=80 and 90 K) reveals a deviation from BCS behavior. The experimental data are in qualitative agreement with the calculations of Devereaux and Einzel based on the dx2−y2-wave symmetry of the order parameter used in the description of the Raman-scattering cross section.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Tl2Ba2CuO6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | unknown |
| Tl2Ba2CuO6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 80 | Pressure not reported | unknown |
| Tl2Ba2Ca2Cu3O10 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 |
| Nd2-xCexCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Nb3Sn Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| V3Si 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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