Haozhe Wang, Shuyuan Huyan, Eoghan Downey, Yang Wang, Shane Smolenski, Du Li, Li Yang, Aaron Bostwick, Chris Jozwiak, Eli Rotenberg, Sergey L. Bud'ko, Paul C. Canfield, R. J. Cava, Na Hyun Jo, Weiwei Xie
{"title":"Insulator to Metal Transition under High Pressure in FeNb$_3$Se$_{10}$","authors":"Haozhe Wang, Shuyuan Huyan, Eoghan Downey, Yang Wang, Shane Smolenski, Du Li, Li Yang, Aaron Bostwick, Chris Jozwiak, Eli Rotenberg, Sergey L. Bud'ko, Paul C. Canfield, R. J. Cava, Na Hyun Jo, Weiwei Xie","doi":"arxiv-2409.06460","DOIUrl":null,"url":null,"abstract":"Non-magnetic FeNb$_3$Se$_{10}$ has been demonstrated to be an insulator at\nambient pressure through both theoretical calculations and experimental\nmeasurements and it does not host topological surface states. Here we show that\non the application of pressure, FeNb$_3$Se$_{10}$ transitions to a metallic\nstate at around 3.0 GPa. With a further increase in pressure, its resistivity\nbecomes independent of both temperature and pressure. Its crystal structure is\nmaintained to at least 4.4 GPa.","PeriodicalId":501171,"journal":{"name":"arXiv - PHYS - Strongly Correlated Electrons","volume":"34 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Strongly Correlated Electrons","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.06460","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Non-magnetic FeNb$_3$Se$_{10}$ has been demonstrated to be an insulator at
ambient pressure through both theoretical calculations and experimental
measurements and it does not host topological surface states. Here we show that
on the application of pressure, FeNb$_3$Se$_{10}$ transitions to a metallic
state at around 3.0 GPa. With a further increase in pressure, its resistivity
becomes independent of both temperature and pressure. Its crystal structure is
maintained to at least 4.4 GPa.