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Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution
The heavy fermion intermetallic compound URu(2)Si(2) exhibits a hidden-order phase below the temperature of 17.5 K, which supports both anomalous metallic behavior and unconventional superconductivity. While these individual phenomena have been investigated in detail, it remains unclear how they are...
Autores principales: | , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4762885/ https://www.ncbi.nlm.nih.gov/pubmed/26891903 http://dx.doi.org/10.1038/ncomms10712 |
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author | Gallagher, A. Chen, K.-W. Moir, C. M. Cary, S. K. Kametani, F. Kikugawa, N. Graf, D. Albrecht-Schmitt, T. E. Riggs, S. C. Shekhter, A. Baumbach, R. E. |
author_facet | Gallagher, A. Chen, K.-W. Moir, C. M. Cary, S. K. Kametani, F. Kikugawa, N. Graf, D. Albrecht-Schmitt, T. E. Riggs, S. C. Shekhter, A. Baumbach, R. E. |
author_sort | Gallagher, A. |
collection | PubMed |
description | The heavy fermion intermetallic compound URu(2)Si(2) exhibits a hidden-order phase below the temperature of 17.5 K, which supports both anomalous metallic behavior and unconventional superconductivity. While these individual phenomena have been investigated in detail, it remains unclear how they are related to each other and to what extent uranium f-electron valence fluctuations influence each one. Here we use ligand site substituted URu(2)Si(2-x)P(x) to establish their evolution under electronic tuning. We find that while hidden order is monotonically suppressed and destroyed for x≤0.035, the superconducting strength evolves non-monotonically with a maximum near x≈0.01 and that superconductivity is destroyed near x≈0.028. This behavior reveals that hidden order depends strongly on tuning outside of the U f-electron shells. It also suggests that while hidden order provides an environment for superconductivity and anomalous metallic behavior, it's fluctuations may not be solely responsible for their progression. |
format | Online Article Text |
id | pubmed-4762885 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-47628852016-03-04 Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution Gallagher, A. Chen, K.-W. Moir, C. M. Cary, S. K. Kametani, F. Kikugawa, N. Graf, D. Albrecht-Schmitt, T. E. Riggs, S. C. Shekhter, A. Baumbach, R. E. Nat Commun Article The heavy fermion intermetallic compound URu(2)Si(2) exhibits a hidden-order phase below the temperature of 17.5 K, which supports both anomalous metallic behavior and unconventional superconductivity. While these individual phenomena have been investigated in detail, it remains unclear how they are related to each other and to what extent uranium f-electron valence fluctuations influence each one. Here we use ligand site substituted URu(2)Si(2-x)P(x) to establish their evolution under electronic tuning. We find that while hidden order is monotonically suppressed and destroyed for x≤0.035, the superconducting strength evolves non-monotonically with a maximum near x≈0.01 and that superconductivity is destroyed near x≈0.028. This behavior reveals that hidden order depends strongly on tuning outside of the U f-electron shells. It also suggests that while hidden order provides an environment for superconductivity and anomalous metallic behavior, it's fluctuations may not be solely responsible for their progression. Nature Publishing Group 2016-02-19 /pmc/articles/PMC4762885/ /pubmed/26891903 http://dx.doi.org/10.1038/ncomms10712 Text en Copyright © 2016, Nature Publishing Group, a division of Macmillan Publishers Limited. All Rights Reserved. http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 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 to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Gallagher, A. Chen, K.-W. Moir, C. M. Cary, S. K. Kametani, F. Kikugawa, N. Graf, D. Albrecht-Schmitt, T. E. Riggs, S. C. Shekhter, A. Baumbach, R. E. Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution |
title | Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution |
title_full | Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution |
title_fullStr | Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution |
title_full_unstemmed | Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution |
title_short | Unfolding the physics of URu(2)Si(2) through silicon to phosphorus substitution |
title_sort | unfolding the physics of uru(2)si(2) through silicon to phosphorus substitution |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4762885/ https://www.ncbi.nlm.nih.gov/pubmed/26891903 http://dx.doi.org/10.1038/ncomms10712 |
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