L. Xiang, E. Gati, S. Bud’ko, S. Saunders, P. Canfield
{"title":"Avoided ferromagnetic quantum critical point in pressurized \nLa5Co2Ge3","authors":"L. Xiang, E. Gati, S. Bud’ko, S. Saunders, P. Canfield","doi":"10.1103/PHYSREVB.103.054419","DOIUrl":null,"url":null,"abstract":"We present the pressure-temperature phase diagram ${\\mathrm{La}}_{5}{\\mathrm{Co}}_{2}{\\mathrm{Ge}}_{3}$ up to $\\ensuremath{\\sim}5$ GPa, which was constructed from magnetization, resistivity, and specific heat measurements. At ambient pressure, ${\\mathrm{La}}_{5}{\\mathrm{Co}}_{2}{\\mathrm{Ge}}_{3}$ is an itinerant ferromagnet with a Curie temperature ${T}_{\\text{C}}\\ensuremath{\\sim}$ 4 K. Upon increasing pressure up to $\\ensuremath{\\sim}1.7$ GPa, ${T}_{\\text{C}}$ is suppressed down to $\\ensuremath{\\sim}3$ K. Upon further increasing pressure, our results suggest that ${\\mathrm{La}}_{5}{\\mathrm{Co}}_{2}{\\mathrm{Ge}}_{3}$ enters a different low-temperature ground state. The corresponding transition temperature ${T}^{*}$ has a nonmonotonic pressure dependence up to $\\ensuremath{\\sim}5$ GPa. Our results demonstrate that the ferromagnetic quantum critical point in ${\\mathrm{La}}_{5}{\\mathrm{Co}}_{2}{\\mathrm{Ge}}_{3}$ is avoided by the appearance of a different, likely magnetically ordered, state that has an antiferromagnetic component.","PeriodicalId":9375,"journal":{"name":"Bulletin of the American Physical Society","volume":"6 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2020-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Bulletin of the American Physical Society","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1103/PHYSREVB.103.054419","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
We present the pressure-temperature phase diagram ${\mathrm{La}}_{5}{\mathrm{Co}}_{2}{\mathrm{Ge}}_{3}$ up to $\ensuremath{\sim}5$ GPa, which was constructed from magnetization, resistivity, and specific heat measurements. At ambient pressure, ${\mathrm{La}}_{5}{\mathrm{Co}}_{2}{\mathrm{Ge}}_{3}$ is an itinerant ferromagnet with a Curie temperature ${T}_{\text{C}}\ensuremath{\sim}$ 4 K. Upon increasing pressure up to $\ensuremath{\sim}1.7$ GPa, ${T}_{\text{C}}$ is suppressed down to $\ensuremath{\sim}3$ K. Upon further increasing pressure, our results suggest that ${\mathrm{La}}_{5}{\mathrm{Co}}_{2}{\mathrm{Ge}}_{3}$ enters a different low-temperature ground state. The corresponding transition temperature ${T}^{*}$ has a nonmonotonic pressure dependence up to $\ensuremath{\sim}5$ GPa. Our results demonstrate that the ferromagnetic quantum critical point in ${\mathrm{La}}_{5}{\mathrm{Co}}_{2}{\mathrm{Ge}}_{3}$ is avoided by the appearance of a different, likely magnetically ordered, state that has an antiferromagnetic component.