L. Xiang, E. Gati, S. Bud’ko, S. Saunders, P. Canfield
{"title":"避免了加压La5Co2Ge3中的铁磁量子临界点","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":"{\"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}","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}
Avoided ferromagnetic quantum critical point in pressurized
La5Co2Ge3
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.