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Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14)
The effect of high pressure (up to 8 GPa) on normal and superconducting state properties of PrFeAsO(0.6)F(0.12), an 1111-type iron based superconductor close to optimal doped region, has been investigated by measuring the temperature dependence of resistivity. Initially, the superconducting transiti...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Nature Publishing Group UK
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5601470/ https://www.ncbi.nlm.nih.gov/pubmed/28916795 http://dx.doi.org/10.1038/s41598-017-11927-1 |
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author | Arumugam, S. Ganguli, C. Thiyagarajan, R. Bhoi, D. Selvan, G. Kalai Manikandan, K. Pariari, A. Mandal, P. Uwatoko, Y. |
author_facet | Arumugam, S. Ganguli, C. Thiyagarajan, R. Bhoi, D. Selvan, G. Kalai Manikandan, K. Pariari, A. Mandal, P. Uwatoko, Y. |
author_sort | Arumugam, S. |
collection | PubMed |
description | The effect of high pressure (up to 8 GPa) on normal and superconducting state properties of PrFeAsO(0.6)F(0.12), an 1111-type iron based superconductor close to optimal doped region, has been investigated by measuring the temperature dependence of resistivity. Initially, the superconducting transition temperature (T (c)) is observed to increase slowly by about 1 K as pressure (P) increases from 0 to 1.3 GPa. With further increase in pressure above 1.3 GPa, T (c) decreases at the rate of ~1.5 K/GPa. The normal-state resistivity decreases monotonically up to 8 GPa. We have also measured the pressure dependence of magnetization (M) on the same piece of PrFeAsO(0.6)F(0.12) sample up to 1.1 GPa and observed T (c) as well as the size of the Meissner signal to increase with pressure in this low-pressure region. In contrast, for an over-doped PrFeAsO(0.6)F(0.14) sample, magnetization measurements up to 1.06 GPa show that both T (c) and the Meissner signal decrease with pressure. The present study clearly reveals two distinct regions in the dome-shaped (T (c)-P) phase diagram of PrFeAsO(0.6)F(0.12). |
format | Online Article Text |
id | pubmed-5601470 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-56014702017-09-20 Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14) Arumugam, S. Ganguli, C. Thiyagarajan, R. Bhoi, D. Selvan, G. Kalai Manikandan, K. Pariari, A. Mandal, P. Uwatoko, Y. Sci Rep Article The effect of high pressure (up to 8 GPa) on normal and superconducting state properties of PrFeAsO(0.6)F(0.12), an 1111-type iron based superconductor close to optimal doped region, has been investigated by measuring the temperature dependence of resistivity. Initially, the superconducting transition temperature (T (c)) is observed to increase slowly by about 1 K as pressure (P) increases from 0 to 1.3 GPa. With further increase in pressure above 1.3 GPa, T (c) decreases at the rate of ~1.5 K/GPa. The normal-state resistivity decreases monotonically up to 8 GPa. We have also measured the pressure dependence of magnetization (M) on the same piece of PrFeAsO(0.6)F(0.12) sample up to 1.1 GPa and observed T (c) as well as the size of the Meissner signal to increase with pressure in this low-pressure region. In contrast, for an over-doped PrFeAsO(0.6)F(0.14) sample, magnetization measurements up to 1.06 GPa show that both T (c) and the Meissner signal decrease with pressure. The present study clearly reveals two distinct regions in the dome-shaped (T (c)-P) phase diagram of PrFeAsO(0.6)F(0.12). Nature Publishing Group UK 2017-09-15 /pmc/articles/PMC5601470/ /pubmed/28916795 http://dx.doi.org/10.1038/s41598-017-11927-1 Text en © The Author(s) 2017 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/. |
spellingShingle | Article Arumugam, S. Ganguli, C. Thiyagarajan, R. Bhoi, D. Selvan, G. Kalai Manikandan, K. Pariari, A. Mandal, P. Uwatoko, Y. Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14) |
title | Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14) |
title_full | Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14) |
title_fullStr | Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14) |
title_full_unstemmed | Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14) |
title_short | Effect of pressure on normal and superconducting state properties of iron based superconductor PrFeAsO(0.6)F(y) (y = 0.12, 0.14) |
title_sort | effect of pressure on normal and superconducting state properties of iron based superconductor prfeaso(0.6)f(y) (y = 0.12, 0.14) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5601470/ https://www.ncbi.nlm.nih.gov/pubmed/28916795 http://dx.doi.org/10.1038/s41598-017-11927-1 |
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