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Evolution of the pseudogap state in weakly praseodymium-doped single crystals with a specified topology of planar defects
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10.1063/1.2400687
/content/aip/journal/ltp/32/12/10.1063/1.2400687
http://aip.metastore.ingenta.com/content/aip/journal/ltp/32/12/10.1063/1.2400687

Figures

Image of FIG. 1.
FIG. 1.

Temperature dependence of the resistivity for single crystals K1 (1) and K2 (2); the arrows indicate points of deviation from the linear dependence; the inset shows a schematic illustration of the bridge used in the resistive studies; b,c—transitions to the superconducting state for the same crystals, as obtained from the resistive (b) and magnetic (c) measurements; d—temperature dependence of in the region of the superconducting transition of two samples.

Image of FIG. 2.
FIG. 2.

Temperature dependence of the excess conductivity in the plane for single crystals K1 (1) and K2 (2). Approximation of the experimental curves by Eq. (3) is shown by the dashed curves, and in inset “b” by straight lines with slope (3D regime) and (2D regime). The arrows indicate the points of the 2D-3D crossover.

Tables

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Table I.

Parameters of the experimetal samples.

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/content/aip/journal/ltp/32/12/10.1063/1.2400687
2006-12-01
2014-04-21
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Evolution of the pseudogap state in weakly praseodymium-doped Y1−zPrzBa2Cu3O7−δ single crystals with a specified topology of planar defects
http://aip.metastore.ingenta.com/content/aip/journal/ltp/32/12/10.1063/1.2400687
10.1063/1.2400687
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