2019
DOI: 10.48550/arxiv.1906.02291
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Current-voltage characteristics in Ag/Au nanostructures at resistive transitions

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Cited by 3 publications
(11 citation statements)
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“…The four-probe R for 23, 67 (I : 2, 3 and V : 6, 7) and 23, 58 channels were recorded simultaneously in the same thermal cycle, while that for 12, 78 with 45 • rotated lead configuration was measured in a separate cool down. The resistance of the as-prepared films varies from 0.4 − 1.5 Ω across the different regions of the film with corresponding resistivity ≈ 4 − 15 × 10 −8 Ω-m [25]. As evident from Fig.…”
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confidence: 73%
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“…The four-probe R for 23, 67 (I : 2, 3 and V : 6, 7) and 23, 58 channels were recorded simultaneously in the same thermal cycle, while that for 12, 78 with 45 • rotated lead configuration was measured in a separate cool down. The resistance of the as-prepared films varies from 0.4 − 1.5 Ω across the different regions of the film with corresponding resistivity ≈ 4 − 15 × 10 −8 Ω-m [25]. As evident from Fig.…”
mentioning
confidence: 73%
“…When the sweep rate is decreased, the ERA remains robust but the T C increases considerably, indicating the nanostructure film exists in an out-of-equilibrium state. Our earlier experiments [24,25] indicated that T C in the Ag/Au nanostructures also change with ageing, which may complicate unambiguous determination of the effect of the sweep rate alone. A small 'dip' in R immediately following the peak, observed most clearly for cycles h3−h5, has also been observed at the superconductor to normal transitions in Au 0.7 In 0.3 rings [21] and high-T C Bi 2 Sr 2 CaCu 2 O 8−y films [10] that associates the resistance anomaly to the fluctuation regime [7].…”
Section: Resistance Of mentioning
confidence: 97%
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