Cu nuclear quadrupole resonance and far-infrared reflectance of superconducting (Y1−yCay)Ba2Cu3O6
A. J. Vega, M. K. Crawford, E. M. McCarron, W. E. Farneth
DOI 10.1103/PhysRevB.40.8878 · Physical Review B
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Abstract
Cu63 and Cu65 nuclear-quadrupole-resonance spectra of a series of materials of composition (Y1−yCay)Ba2Cu3O6+δ with 0<y<0.5 and δ≪1 are reported. For y>0.1 these materials are superconducting with Tc around 45 K. For y values below 0.25 the spectra consist of two components. One signal is identical to that of Cu(1) in YBa2Cu3O6, showing that the chain sites are not affected by the hole doping that accompanies substitution of Ca for Y. The other signal, which can be assigned to Cu(2) sites, is identical for all superconducting samples in the series and is not observed when y<0.1. Relaxation times indicate that the Cu(1) nuclei are in insulating environments, while the Cu(2) sites are conducting. Thus the conductivity is highly anisotropic. This is also demonstrated by far-infrared reflectance spectra. As Ca is added to YBa2Cu3O6, there is a gradual decrease in the strength of the Eu (ab plane) modes due to free-carrier screening. The A2u (c-axis) modes, on the other hand, remain unscreened at low frequencies.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| (Y1-yCay)Ba2Cu3O6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 45 | Pressure not reported | unknown |
| (Y0.8Ca0.2)Ba2Cu3O6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 50 | Pressure not reported | unknown |
| (Y1-yCay)Ba2Cu3O6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 50 | Pressure not reported | onset |
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