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0342387628
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The distribution (2) was derived [10] for the first time for a system that is physically very much different from disordered interface: long ballistic double-barrier structure with symmetric uniform tunnel barriers. The reasons for coincidence between the two systems are not completely clear.
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0032500145
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0343692877
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22
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0343257133
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note
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c where the junction dc I-V curves are almost linear while the junction electrodes are still superconducting. This procedure may easily give a few percent error.
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24
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0342822417
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note
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The two latter curves may be readily calculated from the current-phase relation for a single channel [24,25] by its averaging with the respective weight (1),(2) and then maximizing the current over the Josephson phase difference.
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28
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0343692873
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note
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3, indicating that the aluminum oxide structure is highly disordered.
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29
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0343257130
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note
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Results of previous experiments with large-area, multimode Josephson junctions in the MAR regime could be interpreted as evidence of either a small number of high-transparency pinholes [29] or percolation paths through localized states [30]. In both cases, the samples were much less uniform than our junctions, so that apparently such explanations were adequate.
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0001697625
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32
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0004210024
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