Advances in Superconductivity VIII 1996
DOI: 10.1007/978-4-431-66871-8_22
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Giant Resistive Peak Close to The Superconducting Transition in Bi2Sr2CaCu2O8 Single Crystals

Abstract: A remarkable resistivity anomaly near the superconducting transition temperature is observed in the ab-plane of as-grown Bi 2 Sr 2 CaCu 2 0 8 (Bi-2212) single crystals. The resistivity at the peak is much large than the normal state resistivity areund 100 K. The peak vanished gradually with increasing the applied magnetic field or transport current. The I-V curves of the samples exhibit also a peak close the transition steps, vanishing gradually with increasing magnetic field. The observed phenomena can be int… Show more

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Cited by 1 publication
(4 citation statements)
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“…The experimental data for ρ(T, B) obtained for the underdoped YBCO film are qualitatively similar to those observed before in HTSC [1,2,3]. The anomalous resistive the opposite happens, where a minimum starts to develop with its width increasing with an increasing applied current.…”
Section: Discussionsupporting
confidence: 85%
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“…The experimental data for ρ(T, B) obtained for the underdoped YBCO film are qualitatively similar to those observed before in HTSC [1,2,3]. The anomalous resistive the opposite happens, where a minimum starts to develop with its width increasing with an increasing applied current.…”
Section: Discussionsupporting
confidence: 85%
“…According to the resistive model, the broadening required for the peak to be eliminated from ρ(T ) should be material-independent provided that the ratio ∆ρ/ρ B = (ρ P − ρ B )/ρ B (where ρ P is the peak's resistivity and ρ B is the resistivity measured in a magnetic field B at the peak's temperature in the absence of the peak) does not change. The experimental data in Refs [1,2,3,4] show that this is not the case. Table 1 lists the data for ∆ρ/ρ B , ∆T c (B * ), and the magnetic field B * at which the peak disappears, for different superconducting materials.…”
Section: Two-dimensional Resistor Modelmentioning
confidence: 99%
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