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dc.contributor.authorKoyama, Chihiro
dc.contributor.authorTahara, Shuta
dc.contributor.authorKohara, Shinji
dc.contributor.authorOnodera, Yohei
dc.contributor.authorSmåbråten, Didrik Rene
dc.contributor.authorSelbach, Sverre Magnus
dc.contributor.authorAkola, Jaakko
dc.contributor.authorIshikawa, Takehiko
dc.contributor.authorMasuno, Atsunobu
dc.contributor.authorMizuno, Akitoshi
dc.contributor.authorOkada, Junpei T.
dc.contributor.authorWatanabe, Yuki
dc.contributor.authorNakata, Yui
dc.contributor.authorOhara, Koji
dc.contributor.authorTamaru, Haruka
dc.contributor.authorOda, Hirohisa
dc.contributor.authorObayashi, Ippei
dc.contributor.authorHiraoka, Yasuyuki
dc.contributor.authorSakata, Osami
dc.date.accessioned2020-09-08T07:04:09Z
dc.date.available2020-09-08T07:04:09Z
dc.date.created2020-08-12T09:28:28Z
dc.date.issued2020
dc.identifier.citationNPG Asia Materials. 2020, 12 .en_US
dc.identifier.issn1884-4049
dc.identifier.urihttps://hdl.handle.net/11250/2676772
dc.description.abstractUnderstanding the liquid structure provides information that is crucial to uncovering the nature of the glass-liquid transition. We apply an aerodynamic levitation technique and high-energy X-rays to liquid (l)-Er2O3 to discover its structure. The sample densities are measured by electrostatic levitation at the International Space Station. Liquid Er2O3 displays a very sharp diffraction peak (principal peak). Applying a combined reverse Monte Carlo – molecular dynamics approach, the simulations produce an Er–O coordination number of 6.1, which is comparable to that of another nonglass-forming liquid, l-ZrO2. The atomic structure of l-Er2O3 comprises distorted OEr4 tetraclusters in nearly linear arrangements, as manifested by a prominent peak observed at ~180° in the Er–O–Er bond angle distribution. This structural feature gives rise to long periodicity corresponding to the sharp principal peak in the X-ray diffraction data. A persistent homology analysis suggests that l-Er2O3 is homologically similar to the crystalline phase. Moreover, electronic structure calculations show that l-Er2O3 has a modest band gap of 0.6 eV that is significantly reduced from the crystalline phase due to the tetracluster distortions. The estimated viscosity is very low above the melting point for l-ZrO2, and the material can be described as an extremely fragile liquid.en_US
dc.language.isoengen_US
dc.publisherNature Researchen_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleVery sharp diffraction peak in nonglass-forming liquid with the formation of distorted tetraclustersen_US
dc.typePeer revieweden_US
dc.typeJournal articleen_US
dc.description.versionpublishedVersionen_US
dc.source.pagenumber11en_US
dc.source.volume12en_US
dc.source.journalNPG Asia Materialsen_US
dc.identifier.doi10.1038/s41427-020-0220-0
dc.identifier.cristin1822896
dc.relation.projectNotur/NorStore: NN9264Ken_US
dc.relation.projectNorges forskningsråd: 275139en_US
dc.description.localcode© The Author(s) 2020 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/.en_US
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