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Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals
We performed a detailed investigation of the superconducting properties of polycrystalline Pr(1−x)Ce(x)Pt(4)Ge(12) pellets. We report the effect of Ce substitution, for x = 0.07, on magnetic field phase diagram H-T. We demonstrate that the upper critical field is well described by the Ginzburg–Landa...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7558182/ https://www.ncbi.nlm.nih.gov/pubmed/32927868 http://dx.doi.org/10.3390/nano10091810 |
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author | Romano, Paola Avitabile, Francesco Nigro, Angela Grimaldi, Gaia Leo, Antonio Shu, Lei Zhang, Jian Di Bartolomeo, Antonio Giubileo, Filippo |
author_facet | Romano, Paola Avitabile, Francesco Nigro, Angela Grimaldi, Gaia Leo, Antonio Shu, Lei Zhang, Jian Di Bartolomeo, Antonio Giubileo, Filippo |
author_sort | Romano, Paola |
collection | PubMed |
description | We performed a detailed investigation of the superconducting properties of polycrystalline Pr(1−x)Ce(x)Pt(4)Ge(12) pellets. We report the effect of Ce substitution, for x = 0.07, on magnetic field phase diagram H-T. We demonstrate that the upper critical field is well described by the Ginzburg–Landau model and that the irreversibility field line has a scaling behaviour similar to cuprates. We also show that for magnetic fields lower than 0.4 T, the activation energy follows a power law of the type 𝐻(−1/2), suggesting a collective pinning regime with a quasi-2D character for the Ce-doped compound with x = 0.07. Furthermore, by means of a point contact Andreev reflection spectroscopy setup, we formed metal/superconductor nano-junctions as small as tens of nanometers on the PrPt(4)Ge(12) parent compound (x = 0). Experimental results showed a wide variety of conductance features appearing in the dI/dV vs. V spectra, all explained in terms of a modified Blonder–Tinkham–Klapwijk model considering a superconducting order parameter with nodal directions as well as sign change in the momentum space for the sample with x = 0. The numerical simulations of the conductance spectra also demonstrate that s-wave pairing and anisotropic s-waves are unsuitable for reproducing experimental data obtained at low temperature on the un-doped compound. Interestingly, we show that the polycrystalline nature of the superconducting PrPt(4)Ge(12) sample can favour the formation of an inter-grain Josephson junction in series with the point contact junction in this kind of experiments. |
format | Online Article Text |
id | pubmed-7558182 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-75581822020-10-29 Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals Romano, Paola Avitabile, Francesco Nigro, Angela Grimaldi, Gaia Leo, Antonio Shu, Lei Zhang, Jian Di Bartolomeo, Antonio Giubileo, Filippo Nanomaterials (Basel) Article We performed a detailed investigation of the superconducting properties of polycrystalline Pr(1−x)Ce(x)Pt(4)Ge(12) pellets. We report the effect of Ce substitution, for x = 0.07, on magnetic field phase diagram H-T. We demonstrate that the upper critical field is well described by the Ginzburg–Landau model and that the irreversibility field line has a scaling behaviour similar to cuprates. We also show that for magnetic fields lower than 0.4 T, the activation energy follows a power law of the type 𝐻(−1/2), suggesting a collective pinning regime with a quasi-2D character for the Ce-doped compound with x = 0.07. Furthermore, by means of a point contact Andreev reflection spectroscopy setup, we formed metal/superconductor nano-junctions as small as tens of nanometers on the PrPt(4)Ge(12) parent compound (x = 0). Experimental results showed a wide variety of conductance features appearing in the dI/dV vs. V spectra, all explained in terms of a modified Blonder–Tinkham–Klapwijk model considering a superconducting order parameter with nodal directions as well as sign change in the momentum space for the sample with x = 0. The numerical simulations of the conductance spectra also demonstrate that s-wave pairing and anisotropic s-waves are unsuitable for reproducing experimental data obtained at low temperature on the un-doped compound. Interestingly, we show that the polycrystalline nature of the superconducting PrPt(4)Ge(12) sample can favour the formation of an inter-grain Josephson junction in series with the point contact junction in this kind of experiments. MDPI 2020-09-10 /pmc/articles/PMC7558182/ /pubmed/32927868 http://dx.doi.org/10.3390/nano10091810 Text en © 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Romano, Paola Avitabile, Francesco Nigro, Angela Grimaldi, Gaia Leo, Antonio Shu, Lei Zhang, Jian Di Bartolomeo, Antonio Giubileo, Filippo Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals |
title | Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals |
title_full | Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals |
title_fullStr | Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals |
title_full_unstemmed | Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals |
title_short | Transport and Point Contact Measurements on Pr(1−x)Ce(x)Pt(4)Ge(12) Superconducting Polycrystals |
title_sort | transport and point contact measurements on pr(1−x)ce(x)pt(4)ge(12) superconducting polycrystals |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7558182/ https://www.ncbi.nlm.nih.gov/pubmed/32927868 http://dx.doi.org/10.3390/nano10091810 |
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