Vaibhav Kumar Singh, Seong-Hoon Kim, Ki Wan Nam, Uma Jena, Boya Krishnamraju, Panchanan Khuntia, Edwin Kermarrec, Kee Hoon Kim, Sayantika Bhowal, Koteswararao Bommisetti
{"title":"Magnetic properties and electronic structure of<i>J</i><sub>eff</sub>= 1/2 square lattice quantum magnet Bi<sub>2</sub>ErO<sub>4</sub>Cl.","authors":"Vaibhav Kumar Singh, Seong-Hoon Kim, Ki Wan Nam, Uma Jena, Boya Krishnamraju, Panchanan Khuntia, Edwin Kermarrec, Kee Hoon Kim, Sayantika Bhowal, Koteswararao Bommisetti","doi":"10.1088/1361-648X/adc6e5","DOIUrl":null,"url":null,"abstract":"<p><p>Two-dimensional rare-earth-based square lattice quantum magnets provide a pathway to achieve distinctive ground states characterized by unusual excitations. We investigate the magnetic, heat capacity, structural, and electronic properties of a magnetic system Bi<sub>2</sub>ErO<sub>4</sub>Cl. This compound features a structurally ideal two-dimensional square lattice composed of Er<sup>3+</sup>rare-earth magnetic ions. The single-phase polycrystalline sample was synthesized using hydrothermal, followed by a vacuum-sealed tube technique. The analysis of heat capacity and magnetic data indicates that the Er<sup>3+</sup>ion adopts a<i>J</i><sub>eff</sub>= 1/2 state at low temperatures. Fitting the Curie-Weiss law to the low-temperature magnetic susceptibility data reveals a Curie-Weiss temperature of approximately -2.1 K, suggesting antiferromagnetic (AFM) interactions between the Er<sup>3+</sup>moments. Our first-principles calculations validate a two-dimensional spin model relevant to the titled Er compound. The presence of AFM interaction between the Er<sup>3+</sup>ions is further confirmed using total energy calculations (LDA+<i>U</i>), aligning with the experimental results. The heat capacity measurements reveal the presence of magnetic long-range order
below<i>T</i><sub>N</sub>= 0.47 K. The magnetic heat capacity data follows<i>T</i><sup>1.8</sup>power law
dependence below<i>T</i><sub>N</sub>.</p>","PeriodicalId":16776,"journal":{"name":"Journal of Physics: Condensed Matter","volume":" ","pages":""},"PeriodicalIF":2.3000,"publicationDate":"2025-03-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics: Condensed Matter","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-648X/adc6e5","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
引用次数: 0
Abstract
Two-dimensional rare-earth-based square lattice quantum magnets provide a pathway to achieve distinctive ground states characterized by unusual excitations. We investigate the magnetic, heat capacity, structural, and electronic properties of a magnetic system Bi2ErO4Cl. This compound features a structurally ideal two-dimensional square lattice composed of Er3+rare-earth magnetic ions. The single-phase polycrystalline sample was synthesized using hydrothermal, followed by a vacuum-sealed tube technique. The analysis of heat capacity and magnetic data indicates that the Er3+ion adopts aJeff= 1/2 state at low temperatures. Fitting the Curie-Weiss law to the low-temperature magnetic susceptibility data reveals a Curie-Weiss temperature of approximately -2.1 K, suggesting antiferromagnetic (AFM) interactions between the Er3+moments. Our first-principles calculations validate a two-dimensional spin model relevant to the titled Er compound. The presence of AFM interaction between the Er3+ions is further confirmed using total energy calculations (LDA+U), aligning with the experimental results. The heat capacity measurements reveal the presence of magnetic long-range order
belowTN= 0.47 K. The magnetic heat capacity data followsT1.8power law
dependence belowTN.
期刊介绍:
Journal of Physics: Condensed Matter covers the whole of condensed matter physics including soft condensed matter and nanostructures. Papers may report experimental, theoretical and simulation studies. Note that papers must contain fundamental condensed matter science: papers reporting methods of materials preparation or properties of materials without novel condensed matter content will not be accepted.