{"title":"Prediction of the Pressure-Resistant Hardest AlFeO3","authors":"Runqing Zhang, Lingling Bai, JingYi Zhang, Junzhao Li, Minru Wen, Fugen Wu, Huafeng Dong, Lei Shen","doi":"10.1021/acs.jpcc.4c07134","DOIUrl":null,"url":null,"abstract":"Perovskite iron-oxide AlFeO<sub>3</sub> is an environmentally friendly (lead-free) multiferroic material that simultaneously exhibits ferromagnetism and the potential magnetoelectric coupling, making it ideal for next-generation spintronic devices. Recently, high pressure has emerged as an effective approach in achieving superior physical properties of perovskite structures. Here, we systematically study the phase diagram and physical properties of AlFeO<sub>3</sub> under pressure. Using an <i>ab initio</i> evolutionary algorithm, we explore all of the potential stable phases of bulk AlFeO<sub>3</sub> between 0 and 50 GPa, and we successfully discover two new stable phases (<i>P</i>2<sub>1</sub>/<i>c</i> and <i>R</i>32). We identify three pressure-induced phase transition sequences <i></i><span style=\"color: inherit;\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>P</mi><mi>n</mi><mi>a</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mi mathvariant=\"normal\">&#x2010;A&#x2010;AFM</mi><mover><mrow><mo stretchy=\"true\">&#x2192;</mo></mrow><mrow><mn>3</mn><mi>GPa</mi></mrow></mover><mi>P</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mo>/</mo><mi>c</mi><mi mathvariant=\"normal\">&#x2010;G&#x2010;AFM</mi><mover><mrow><mo stretchy=\"true\">&#x2192;</mo></mrow><mrow><mn>15</mn><mi>GPa</mi></mrow></mover><mi>P</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mo>/</mo><mi>c</mi><mi mathvariant=\"normal\">&#x2010;FM</mi></math>' role=\"presentation\" style=\"position: relative;\" tabindex=\"0\"><nobr aria-hidden=\"true\"><span style=\"width: 23.128em; display: inline-block;\"><span style=\"display: inline-block; position: relative; width: 21.026em; height: 0px; font-size: 110%;\"><span style=\"position: absolute; clip: rect(1.139em, 1021.03em, 2.901em, -999.997em); top: -2.554em; left: 0em;\"><span><span style=\"font-family: STIXMathJax_Normal-italic;\">𝑃<span style=\"display: inline-block; overflow: hidden; height: 1px; width: 0.116em;\"></span></span><span style=\"font-family: STIXMathJax_Normal-italic;\">𝑛</span><span style=\"font-family: STIXMathJax_Normal-italic;\">𝑎</span><span><span style=\"display: inline-block; position: relative; width: 0.912em; height: 0px;\"><span style=\"position: absolute; clip: rect(3.128em, 1000.46em, 4.151em, -999.997em); top: -3.974em; left: 0em;\"><span><span style=\"font-family: STIXMathJax_Main;\">2</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; top: -3.804em; left: 0.514em;\"><span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">1</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span><span style=\"font-family: STIXMathJax_Marks;\">‐<span style=\"font-family: STIXMathJax_Main;\">A</span>‐<span style=\"font-family: STIXMathJax_Main;\">AFM</span></span><span style=\"padding-left: 0.344em;\"><span style=\"display: inline-block; position: relative; width: 1.594em; height: 0px;\"><span style=\"position: absolute; clip: rect(3.355em, 1001.54em, 4.094em, -999.997em); top: -3.974em; left: 0.003em;\"><span><span style=\"\"><span style=\"display: inline-block; position: relative; width: 1.537em; height: 0px;\"><span style=\"position: absolute; font-family: STIXMathJax_Main; top: -3.974em; left: -0.054em;\">−<span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; font-family: STIXMathJax_Main; top: -3.974em; left: 0.685em;\">→<span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"font-family: STIXMathJax_Main; position: absolute; top: -3.974em; left: 0.344em;\">−<span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; clip: rect(3.241em, 1001.59em, 4.151em, -999.997em); top: -4.656em; left: 0em;\"><span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">3</span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">GPa</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span><span style=\"font-family: STIXMathJax_Normal-italic; padding-left: 0.344em;\">𝑃<span style=\"display: inline-block; overflow: hidden; height: 1px; width: 0.116em;\"></span></span><span><span style=\"display: inline-block; position: relative; width: 0.912em; height: 0px;\"><span style=\"position: absolute; clip: rect(3.128em, 1000.46em, 4.151em, -999.997em); top: -3.974em; left: 0em;\"><span><span style=\"font-family: STIXMathJax_Main;\">2</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; top: -3.804em; left: 0.514em;\"><span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">1</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span><span style=\"font-family: STIXMathJax_Main;\">/</span><span style=\"font-family: STIXMathJax_Normal-italic;\">𝑐</span><span style=\"font-family: STIXMathJax_Marks;\">‐<span style=\"font-family: STIXMathJax_Main;\">G</span>‐<span style=\"font-family: STIXMathJax_Main;\">AFM</span></span><span style=\"padding-left: 0.344em;\"><span style=\"display: inline-block; position: relative; width: 1.935em; height: 0px;\"><span style=\"position: absolute; clip: rect(3.355em, 1001.88em, 4.094em, -999.997em); top: -3.974em; left: 0.003em;\"><span><span style=\"\"><span style=\"display: inline-block; position: relative; width: 1.878em; height: 0px;\"><span style=\"position: absolute; font-family: STIXMathJax_Main; top: -3.974em; left: -0.054em;\">−<span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; font-family: STIXMathJax_Main; top: -3.974em; left: 1.026em;\">→<span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"font-family: STIXMathJax_Main; position: absolute; top: -3.974em; left: 0.287em;\">−<span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"font-family: STIXMathJax_Main; position: absolute; top: -3.974em; left: 0.685em;\">−<span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; clip: rect(3.241em, 1001.93em, 4.151em, -999.997em); top: -4.656em; left: 0em;\"><span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">15</span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">GPa</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span><span style=\"font-family: STIXMathJax_Normal-italic; padding-left: 0.344em;\">𝑃<span style=\"display: inline-block; overflow: hidden; height: 1px; width: 0.116em;\"></span></span><span><span style=\"display: inline-block; position: relative; width: 0.912em; height: 0px;\"><span style=\"position: absolute; clip: rect(3.128em, 1000.46em, 4.151em, -999.997em); top: -3.974em; left: 0em;\"><span><span style=\"font-family: STIXMathJax_Main;\">2</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; top: -3.804em; left: 0.514em;\"><span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">1</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span><span style=\"font-family: STIXMathJax_Main;\">/</span><span style=\"font-family: STIXMathJax_Normal-italic;\">𝑐</span><span style=\"font-family: STIXMathJax_Marks;\">‐<span style=\"font-family: STIXMathJax_Main;\">FM</span></span></span><span style=\"display: inline-block; width: 0px; height: 2.56em;\"></span></span></span><span style=\"display: inline-block; overflow: hidden; vertical-align: -0.247em; border-left: 0px solid; width: 0px; height: 1.691em;\"></span></span></nobr><span role=\"presentation\"><math display=\"inline\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi>P</mi><mi>n</mi><mi>a</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mi mathvariant=\"normal\">‐A‐AFM</mi><mover><mrow><mo stretchy=\"true\">→</mo></mrow><mrow><mn>3</mn><mi>GPa</mi></mrow></mover><mi>P</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mo>/</mo><mi>c</mi><mi mathvariant=\"normal\">‐G‐AFM</mi><mover><mrow><mo stretchy=\"true\">→</mo></mrow><mrow><mn>15</mn><mi>GPa</mi></mrow></mover><mi>P</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mo>/</mo><mi>c</mi><mi mathvariant=\"normal\">‐FM</mi></math></span></span><script type=\"math/mml\"><math display=\"inline\"><mi>P</mi><mi>n</mi><mi>a</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mi mathvariant=\"normal\">‐A‐AFM</mi><mover><mrow><mo stretchy=\"true\">→</mo></mrow><mrow><mn>3</mn><mi>GPa</mi></mrow></mover><mi>P</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mo>/</mo><mi>c</mi><mi mathvariant=\"normal\">‐G‐AFM</mi><mover><mrow><mo stretchy=\"true\">→</mo></mrow><mrow><mn>15</mn><mi>GPa</mi></mrow></mover><mi>P</mi><msub><mrow><mn>2</mn></mrow><mrow><mn>1</mn></mrow></msub><mo>/</mo><mi>c</mi><mi mathvariant=\"normal\">‐FM</mi></math></script> from 0 to 50 GPa, providing a comprehensive pressure-induced phase diagram. It is found that the coplanar Fe–O octahedron configuration and ferromagnetic configuration can effectively enhance the structural stability of AlFeO<sub>3</sub> under high pressure. Moreover, the stable new phase (<i>P</i>2<sub>1</sub>/<i>c</i>-AlFeO<sub>3</sub>) exhibits superior physical properties. It is the hardest AlFeO<sub>3</sub>, with the largest shear modulus, bulk modulus, and Young’s modulus among all phases. Additionally, AFM and FM configurations of this phase could maintain stable semiconductor performance in their respective pressure ranges. This study not only resolves the longstanding issue of the pressure-induced phase transition sequence in the AlFeO<sub>3</sub> system, but also discovers the hardest <i>P</i>2<sub>1</sub>/<i>c</i>-AlFeO<sub>3</sub> with a stable electronic structure. These findings offer critical scientific insights that may guide future applications of AlFeO<sub>3</sub> in high-performance materials and devices.","PeriodicalId":61,"journal":{"name":"The Journal of Physical Chemistry C","volume":"11 1","pages":""},"PeriodicalIF":3.3000,"publicationDate":"2025-01-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Journal of Physical Chemistry C","FirstCategoryId":"1","ListUrlMain":"https://doi.org/10.1021/acs.jpcc.4c07134","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
Perovskite iron-oxide AlFeO3 is an environmentally friendly (lead-free) multiferroic material that simultaneously exhibits ferromagnetism and the potential magnetoelectric coupling, making it ideal for next-generation spintronic devices. Recently, high pressure has emerged as an effective approach in achieving superior physical properties of perovskite structures. Here, we systematically study the phase diagram and physical properties of AlFeO3 under pressure. Using an ab initio evolutionary algorithm, we explore all of the potential stable phases of bulk AlFeO3 between 0 and 50 GPa, and we successfully discover two new stable phases (P21/c and R32). We identify three pressure-induced phase transition sequences 𝑃𝑛𝑎21‐A‐AFM−→−3GPa𝑃21/𝑐‐G‐AFM−→−−15GPa𝑃21/𝑐‐FM from 0 to 50 GPa, providing a comprehensive pressure-induced phase diagram. It is found that the coplanar Fe–O octahedron configuration and ferromagnetic configuration can effectively enhance the structural stability of AlFeO3 under high pressure. Moreover, the stable new phase (P21/c-AlFeO3) exhibits superior physical properties. It is the hardest AlFeO3, with the largest shear modulus, bulk modulus, and Young’s modulus among all phases. Additionally, AFM and FM configurations of this phase could maintain stable semiconductor performance in their respective pressure ranges. This study not only resolves the longstanding issue of the pressure-induced phase transition sequence in the AlFeO3 system, but also discovers the hardest P21/c-AlFeO3 with a stable electronic structure. These findings offer critical scientific insights that may guide future applications of AlFeO3 in high-performance materials and devices.
期刊介绍:
The Journal of Physical Chemistry A/B/C is devoted to reporting new and original experimental and theoretical basic research of interest to physical chemists, biophysical chemists, and chemical physicists.