Infrared properties of epitaxial La2−xSrxCuO4 thin films in the normal and superconducting states
F. Gao, D. B. Romero, D. B. Tanner, J. Talvacchio, M. G. Forrester
DOI 10.1103/PhysRevB.47.1036 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
The CuO2-plane optical reflectance of superconducting La2−xSrxCuO4 thin films (Tc≃31 K) has been measured over a wide frequency and temperature range. The optical conductivity in the normal state is well described by a temperature-dependent weak-coupling (λ≊0.25) free-carrier term plus an overdamped, weakly temperature-dependent, midinfrared component. The free-carrier plasma frequency is nearly constant, ωpD=6300 cm−1, whereas the relaxation rate varies linearly with temperature above Tc. In the superconducting state, according to our two-component approach, most of the Drude oscillator strength condenses to a δ(ω) function. A two-fluid analysis gives a rapid drop in the quasiparticle damping rate below Tc. A reasonable estimate (∼2750 Å) for the ab-plane London penetration depth is obtained from the superfluid density. We observe that the midinfrared strength increases below Tc, suggesting that some (∼15%) of the free carriers do not condense into superconducting pairs and may have a strong interaction with pair-breaking excitations. Two absorption edges around 80 cm−1 (3.7 kBTc) and 400 cm−1 (18 kBTc) are seen but neither is assigned to the superconducting gap. Comparisons with a one-component picture described by a frequency-dependent scattering rate and effective mass are made and discussed. The far-infrared ab-plane phonons show systematic changes with temperature, which are associated with the structural transition near 250 K.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| La2-xSrxCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 31 | Pressure not reported | onset |
| La2-xSrxCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 29 | Pressure not reported | onset |
| La1.85Sr0.15CuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| YBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | unknown |
Similar papers
Anomalously sharp superconducting transitions in overdoped La2−xSrxCuO4 films
similarity 0.96T. R. Lemberger et al.
Source status unknown — claims are unverified
Optical evidence for strong anisotropy in the normal and superconducting states in Bi2Sr2CaCu2O8+z
similarity 0.96S. Tajima et al.
Source status unknown — claims are unverified
Magnetic penetration depth in superconducting La2−xSrxCuO4 films
similarity 0.96Kathleen M. Paget et al.
Source status unknown — claims are unverified
Superconductor-insulator phase transition in single-crystal La2−xSrxCuO4 films grown by the liquid-phase epitaxy method
similarity 0.96A. T. M. Nazmul Islam et al.
Source status unknown — claims are unverified
Evidence for a common high-temperature superconducting effect in La1.85Sr0.15CuO4 and YBa2Cu3O7
similarity 0.96Y. C. Jean et al.
Source status unknown — claims are unverified
Superconducting and normal-state properties of YBa2(Cu1−xZnx)4O8
similarity 0.96Takayuki Miyatake et al.
Source status unknown — claims are unverified