Phonon Raman scattering inY1−xPrxBa2Cu4O8(x=0–1) and (Y1−xPrx)2Ba4Cu7O15−δ(x=0–0.6)
Author:
Publisher
American Physical Society (APS)
Link
http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevB.53.3590/fulltext
Reference40 articles.
1. A review of the superconducting and normal state properties of Y1−xPrxBa2Cu3O7
2. Transport and structural properties ofPr1−xCaxBa2Cu3O7−δthin films grown by pulsed-laser deposition
3. Anisotropic optical spectrum of untwinnedPrBa2Cu3O7: Persistence of the charge-transfer insulating state of theCuO2plane against hole doping
4. Synthesis of a new “124” compound, PrBa2Cu4O8
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1. Scandium and gallium substitution effects in the (Y1−xScx)Ba2Cu4O8 and (Y1−xGax)Ba2Cu4O8 superconducting oxides;Materials Chemistry and Physics;2010-01
2. Effect of Fe substitution in the structure and superconducting properties of the (Y0.8Pr0.2)Ba2Cu4−xFexO8 system;Physica C: Superconductivity;2003-03
3. Sol–gel chemistry approach in the preparation of precursors for the substituted superconducting oxides;Journal of Non-Crystalline Solids;2002-12
4. Synthesis and characterization of Pr0.9Ca0.1Ba2Cu4O8 by an aqueous solution method;Solid State Ionics;2001-05
5. Raman scattering inYBa2Cu4O8andPrBa2Cu4O8: Indications of pseudogap effects in nonsuperconductingPrBa2Cu4O8;Physical Review B;2000-03-01
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