Ionic size effect due to a nonclassical percolation process on the superconductor-insulator transition inR1−xPrxBa2Cu3O7−δ(R=rare earth)
Author:
Publisher
American Physical Society (APS)
Subject
Condensed Matter Physics,Electronic, Optical and Magnetic Materials
Link
http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevB.76.024514/fulltext
Reference36 articles.
1. Suppression of superconductivity inGd1−xPrxBa2Cu3O7−yandR0.8Pr0.2Ba2Cu3O7−ysystems
2. Evidence for pair‐breaking in (R1−xPrx)Ba2Cu3O7−y(R=Er, Y, Dy, Gd, Eu) systems
3. Ion-size effect onTcin (R1−xPrx)Ba2Cu3O7−ysystems (R=Nd, Eu, Gd, Dy, Y, Er, and Yb)
4. Suppression of superconductivity in the oxide systemsR1−xPrxBa2Cu3O7−y(R=Sm, Gd, and Tm)
5. Evidence against hole filling by Pr inYBa2Cu3O7
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1. Doping of Sm3Ba5Cu8O19 Compound with Praseodymium;Journal of Low Temperature Physics;2020-01-13
2. Critical current density in (YBa2Cu3O7−δ)1−–(PrBa2Cu3O7−δ) melt-textured composites;Physica C: Superconductivity and its Applications;2018-06
3. Fluctuation-induced conductivity and phase separation in composite samples (YBa2Cu3O7-δ)1−y–(PrBa2Cu3O7-δ)y;Phase Transitions;2015-09-22
4. Splitting of the pairing transition and coherence transition in R1−xCexBa2Cu3O7−δ(R = Y, Er, Ho and Gd);Superconductor Science and Technology;2012-01-20
5. Percolative nanostructure and superconductivity in the mixed crystalline cuprate Nd1 −xPrxBa2Cu3O7 − δ;Journal of Physics: Condensed Matter;2010-11-05
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