{"title":"多铁金属单层Cu(CrSe2)2†","authors":"Ke Yang, Yuxuan Zhou, Yaozhenghang Ma and Hua Wu","doi":"10.1039/D4TC03941F","DOIUrl":null,"url":null,"abstract":"<p >The two-dimensional (2D) Cu(CrSe<small><sub>2</sub></small>)<small><sub>2</sub></small> monolayer stands out for its combined ferromagnetic (FM), ferroelectric (FE), and metallic properties, marking itself as a prominent 2D multiferroic metal. This work studies those properties and the relevant physics, using density functional calculations, Monte Carlo simulations, and <em>ab initio</em> molecular dynamics. Our results show that Cu(CrSe<small><sub>2</sub></small>)<small><sub>2</sub></small> monolayer is in the Cr<small><sup>3+</sup></small> t<small><sup>3</sup></small><small><sub>2g</sub></small> state with <em>S</em> = 3/2 and Cu<small><sup>1+</sup></small> 3d<small><sup>10</sup></small> with <em>S</em> = 0. A ligand hole in the Se 4p orbitals gives rise to metallic behavior and enhances the FM coupling between the local Cr<small><sup>3+</sup></small><em>S</em> = 3/2 spins. The observed in-plane magnetic anisotropy primarily arises from exchange anisotropy, which is associated with the Cr–Se–Cr itinerant ferromagnetism. In contrast, both single-ion anisotropy and shape magnetic anisotropy contribute negligibly. The Dzyaloshinskii–Moriya interaction is also quite weak, only about 3% of the intralayer exchange parameters. Our Monte Carlo simulations show a FM Curie temperature (<em>T</em><small><sub>C</sub></small>) of 190 K. Moreover, the monolayer exhibits a vertical FE polarization of 1.79 pC m<small><sup>−1</sup></small> and a FE polarization switching barrier of 182 meV f.u.<small><sup>−1</sup></small>, and the FE state remains stable above room temperature as shown by <em>ab initio</em> molecular dynamics simulations. Furthermore, a magnetoelectric coupling is partially manifested by a magnetization rotation from in-plane to out-of-plane associated with a FE-to-paraelectric transition. The magnetization rotation can also be induced by either hole or electron doping, and the hole doping increases the <em>T</em><small><sub>C</sub></small> up to 238 K. In addition, tensile strain reduces the FE polarization but enhances <em>T</em><small><sub>C</sub></small> to 290 K, while a compressive strain gives an opposite effect. Therefore, the multiferroic metallic Cu(CrSe<small><sub>2</sub></small>)<small><sub>2</sub></small> monolayer may be explored for advanced multifunctional electronic devices.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" 9","pages":" 4549-4556"},"PeriodicalIF":5.1000,"publicationDate":"2025-01-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Multiferroic metallic monolayer Cu(CrSe2)2†\",\"authors\":\"Ke Yang, Yuxuan Zhou, Yaozhenghang Ma and Hua Wu\",\"doi\":\"10.1039/D4TC03941F\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >The two-dimensional (2D) Cu(CrSe<small><sub>2</sub></small>)<small><sub>2</sub></small> monolayer stands out for its combined ferromagnetic (FM), ferroelectric (FE), and metallic properties, marking itself as a prominent 2D multiferroic metal. This work studies those properties and the relevant physics, using density functional calculations, Monte Carlo simulations, and <em>ab initio</em> molecular dynamics. Our results show that Cu(CrSe<small><sub>2</sub></small>)<small><sub>2</sub></small> monolayer is in the Cr<small><sup>3+</sup></small> t<small><sup>3</sup></small><small><sub>2g</sub></small> state with <em>S</em> = 3/2 and Cu<small><sup>1+</sup></small> 3d<small><sup>10</sup></small> with <em>S</em> = 0. A ligand hole in the Se 4p orbitals gives rise to metallic behavior and enhances the FM coupling between the local Cr<small><sup>3+</sup></small><em>S</em> = 3/2 spins. The observed in-plane magnetic anisotropy primarily arises from exchange anisotropy, which is associated with the Cr–Se–Cr itinerant ferromagnetism. In contrast, both single-ion anisotropy and shape magnetic anisotropy contribute negligibly. The Dzyaloshinskii–Moriya interaction is also quite weak, only about 3% of the intralayer exchange parameters. Our Monte Carlo simulations show a FM Curie temperature (<em>T</em><small><sub>C</sub></small>) of 190 K. Moreover, the monolayer exhibits a vertical FE polarization of 1.79 pC m<small><sup>−1</sup></small> and a FE polarization switching barrier of 182 meV f.u.<small><sup>−1</sup></small>, and the FE state remains stable above room temperature as shown by <em>ab initio</em> molecular dynamics simulations. Furthermore, a magnetoelectric coupling is partially manifested by a magnetization rotation from in-plane to out-of-plane associated with a FE-to-paraelectric transition. The magnetization rotation can also be induced by either hole or electron doping, and the hole doping increases the <em>T</em><small><sub>C</sub></small> up to 238 K. In addition, tensile strain reduces the FE polarization but enhances <em>T</em><small><sub>C</sub></small> to 290 K, while a compressive strain gives an opposite effect. Therefore, the multiferroic metallic Cu(CrSe<small><sub>2</sub></small>)<small><sub>2</sub></small> monolayer may be explored for advanced multifunctional electronic devices.</p>\",\"PeriodicalId\":84,\"journal\":{\"name\":\"Journal of Materials Chemistry C\",\"volume\":\" 9\",\"pages\":\" 4549-4556\"},\"PeriodicalIF\":5.1000,\"publicationDate\":\"2025-01-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Materials Chemistry C\",\"FirstCategoryId\":\"1\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2025/tc/d4tc03941f\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Materials Chemistry C","FirstCategoryId":"1","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/tc/d4tc03941f","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
The two-dimensional (2D) Cu(CrSe2)2 monolayer stands out for its combined ferromagnetic (FM), ferroelectric (FE), and metallic properties, marking itself as a prominent 2D multiferroic metal. This work studies those properties and the relevant physics, using density functional calculations, Monte Carlo simulations, and ab initio molecular dynamics. Our results show that Cu(CrSe2)2 monolayer is in the Cr3+ t32g state with S = 3/2 and Cu1+ 3d10 with S = 0. A ligand hole in the Se 4p orbitals gives rise to metallic behavior and enhances the FM coupling between the local Cr3+S = 3/2 spins. The observed in-plane magnetic anisotropy primarily arises from exchange anisotropy, which is associated with the Cr–Se–Cr itinerant ferromagnetism. In contrast, both single-ion anisotropy and shape magnetic anisotropy contribute negligibly. The Dzyaloshinskii–Moriya interaction is also quite weak, only about 3% of the intralayer exchange parameters. Our Monte Carlo simulations show a FM Curie temperature (TC) of 190 K. Moreover, the monolayer exhibits a vertical FE polarization of 1.79 pC m−1 and a FE polarization switching barrier of 182 meV f.u.−1, and the FE state remains stable above room temperature as shown by ab initio molecular dynamics simulations. Furthermore, a magnetoelectric coupling is partially manifested by a magnetization rotation from in-plane to out-of-plane associated with a FE-to-paraelectric transition. The magnetization rotation can also be induced by either hole or electron doping, and the hole doping increases the TC up to 238 K. In addition, tensile strain reduces the FE polarization but enhances TC to 290 K, while a compressive strain gives an opposite effect. Therefore, the multiferroic metallic Cu(CrSe2)2 monolayer may be explored for advanced multifunctional electronic devices.
期刊介绍:
The Journal of Materials Chemistry is divided into three distinct sections, A, B, and C, each catering to specific applications of the materials under study:
Journal of Materials Chemistry A focuses primarily on materials intended for applications in energy and sustainability.
Journal of Materials Chemistry B specializes in materials designed for applications in biology and medicine.
Journal of Materials Chemistry C is dedicated to materials suitable for applications in optical, magnetic, and electronic devices.
Example topic areas within the scope of Journal of Materials Chemistry C are listed below. This list is neither exhaustive nor exclusive.
Bioelectronics
Conductors
Detectors
Dielectrics
Displays
Ferroelectrics
Lasers
LEDs
Lighting
Liquid crystals
Memory
Metamaterials
Multiferroics
Photonics
Photovoltaics
Semiconductors
Sensors
Single molecule conductors
Spintronics
Superconductors
Thermoelectrics
Topological insulators
Transistors