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Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect

The long range proximity effect in high-T(c) c-axis Josephson junctions with a high-T(c) barrier of lower T(c) is still a puzzling phenomenon. It leads to supercurrents in junctions with much thicker barriers than would be allowed by the conventional proximity effect. Here we measured the T − x (Tem...

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Autores principales: Kirzhner, Tal, Koren, Gad
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4150101/
https://www.ncbi.nlm.nih.gov/pubmed/25175417
http://dx.doi.org/10.1038/srep06244
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author Kirzhner, Tal
Koren, Gad
author_facet Kirzhner, Tal
Koren, Gad
author_sort Kirzhner, Tal
collection PubMed
description The long range proximity effect in high-T(c) c-axis Josephson junctions with a high-T(c) barrier of lower T(c) is still a puzzling phenomenon. It leads to supercurrents in junctions with much thicker barriers than would be allowed by the conventional proximity effect. Here we measured the T − x (Temperature-doping level) phase diagram of the barrier coherence length ξ(N)(T, x), and found an enhancement of ξ(N) at moderate under-doping and high temperatures. This indicates that a possible origin of the long range proximity effect in the cuprate barrier is the conjectured pre-formed pairs in the pseudogap regime, which increase the length scale over which superconducting correlations survive in the seemingly normal barrier. In more details, we measured the supercurrents I(c) of Superconducting - Normal - Superconducting SNS c-axis junctions, where S was optimally doped Y Ba(2)Cu(3)O(7−δ) below T(c) (90 K) and N was La(2−x)Sr(x)CuO(4) above its T(c) (<25 K) but in the pseudogap regime. From the exponential decay of I(c)(T) ∝ exp[−d/ξ(N)(T)], where d is the barrier thickness, the ξ(N)(T) values were extracted. By repeating these measurements for different barrier doping levels x, the whole phase diagram of ξ(N)(T, x) was obtained.
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spelling pubmed-41501012014-09-02 Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect Kirzhner, Tal Koren, Gad Sci Rep Article The long range proximity effect in high-T(c) c-axis Josephson junctions with a high-T(c) barrier of lower T(c) is still a puzzling phenomenon. It leads to supercurrents in junctions with much thicker barriers than would be allowed by the conventional proximity effect. Here we measured the T − x (Temperature-doping level) phase diagram of the barrier coherence length ξ(N)(T, x), and found an enhancement of ξ(N) at moderate under-doping and high temperatures. This indicates that a possible origin of the long range proximity effect in the cuprate barrier is the conjectured pre-formed pairs in the pseudogap regime, which increase the length scale over which superconducting correlations survive in the seemingly normal barrier. In more details, we measured the supercurrents I(c) of Superconducting - Normal - Superconducting SNS c-axis junctions, where S was optimally doped Y Ba(2)Cu(3)O(7−δ) below T(c) (90 K) and N was La(2−x)Sr(x)CuO(4) above its T(c) (<25 K) but in the pseudogap regime. From the exponential decay of I(c)(T) ∝ exp[−d/ξ(N)(T)], where d is the barrier thickness, the ξ(N)(T) values were extracted. By repeating these measurements for different barrier doping levels x, the whole phase diagram of ξ(N)(T, x) was obtained. Nature Publishing Group 2014-09-01 /pmc/articles/PMC4150101/ /pubmed/25175417 http://dx.doi.org/10.1038/srep06244 Text en Copyright © 2014, Macmillan Publishers Limited. All rights reserved http://creativecommons.org/licenses/by-nc-nd/4.0/ This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivs 4.0 International License. The images or other third party material in this article are included in the article's Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder in order to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by-nc-nd/4.0/
spellingShingle Article
Kirzhner, Tal
Koren, Gad
Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect
title Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect
title_full Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect
title_fullStr Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect
title_full_unstemmed Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect
title_short Pairing and the phase diagram of the normal coherence length ξ(N)(T, x) above T(c) of La(2−x)Sr(x)CuO(4) thin films probed by the Josephson effect
title_sort pairing and the phase diagram of the normal coherence length ξ(n)(t, x) above t(c) of la(2−x)sr(x)cuo(4) thin films probed by the josephson effect
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4150101/
https://www.ncbi.nlm.nih.gov/pubmed/25175417
http://dx.doi.org/10.1038/srep06244
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