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Metal-bosonic insulator-superconductor transition in boron-doped granular diamond

In a variety of superconductors, mostly in two-dimensional (2D) and one-dimensional (1D) systems, the resistive superconducting transition R(T) demonstrates in many cases an anomalous narrow R(T) peak just preceding the onset of the superconducting state R=0 at T(c). The amplitude of this R(T) peak...

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Bibliographic Details
Published in:Physical review letters 2013-02, Vol.110 (7), p.077001-077001, Article 077001
Main Authors: Zhang, Gufei, Zeleznik, Monika, Vanacken, Johan, May, Paul W, Moshchalkov, Victor V
Format: Article
Language:English
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Summary:In a variety of superconductors, mostly in two-dimensional (2D) and one-dimensional (1D) systems, the resistive superconducting transition R(T) demonstrates in many cases an anomalous narrow R(T) peak just preceding the onset of the superconducting state R=0 at T(c). The amplitude of this R(T) peak in 1D and 2D systems ranges from a few up to several hundred percent. In three-dimensional (3D) systems, however, the R(T) peak close to T(c) is rarely observed, and it reaches only a few percent in amplitude. Here we report on the observation of a giant (∼1600%) and very narrow (∼1  K) resistance peak preceding the onset of superconductivity in heavily boron-doped diamond. This anomalous R(T) peak in a 3D system is interpreted in the framework of an empirical model based on the metal-bosonic insulator-superconductor transitions induced by a granularity-correlated disorder in heavily doped diamond.
ISSN:0031-9007
1079-7114
DOI:10.1103/physrevlett.110.077001