Yilun Gu, Rufei Zhang, Haojie Zhang, Licheng Fu, Guoxiang Zhi, Jinou Dong, Xueqin Zhao, Lingfeng Xie, Fanlong Ning
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{"title":"122型铁基超导体的A型磁性半导体(Sr, Na)(Zn, Mn)2Sb2等构","authors":"Yilun Gu, Rufei Zhang, Haojie Zhang, Licheng Fu, Guoxiang Zhi, Jinou Dong, Xueqin Zhao, Lingfeng Xie, Fanlong Ning","doi":"10.1155/2022/4291923","DOIUrl":null,"url":null,"abstract":"A new diluted magnetic semiconductor (Sr, Na)(Zn, Mn)<sub>2</sub>Sb<sub>2</sub> has been successfully synthesized by doping Na and Mn into the parent compound <span><svg height=\"12.4894pt\" style=\"vertical-align:-3.181499pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.3079 48.943 12.4894\" width=\"48.943pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g190-84\"></use></g><g transform=\"matrix(.013,0,0,-0.013,6.084,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,10.907,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,18.928,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,26.137,3.132)\"><use xlink:href=\"#g50-51\"></use></g><g transform=\"matrix(.013,0,0,-0.013,31.083,0)\"><use xlink:href=\"#g190-84\"></use></g><g transform=\"matrix(.013,0,0,-0.013,37.245,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,43.897,3.132)\"><use xlink:href=\"#g50-51\"></use></g></svg>,</span> which has a <span><svg height=\"12.4894pt\" style=\"vertical-align:-3.181499pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.3079 46.4768 12.4894\" width=\"46.4768pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g190-68\"></use></g><g transform=\"matrix(.013,0,0,-0.013,8.762,0)\"><use xlink:href=\"#g190-98\"></use></g><g transform=\"matrix(.013,0,0,-0.013,14.47,0)\"><use xlink:href=\"#g190-66\"></use></g><g transform=\"matrix(.013,0,0,-0.013,23.492,0)\"><use xlink:href=\"#g190-109\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,26.88,3.132)\"><use xlink:href=\"#g50-51\"></use></g><g transform=\"matrix(.013,0,0,-0.013,31.827,0)\"><use xlink:href=\"#g190-84\"></use></g><g transform=\"matrix(.013,0,0,-0.013,37.911,0)\"><use xlink:href=\"#g190-106\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,41.431,3.132)\"><use xlink:href=\"#g50-51\"></use></g></svg>-</span>type crystal structure (space group <span><svg height=\"11.8174pt\" style=\"vertical-align:-0.2063999pt\" version=\"1.1\" viewbox=\"-0.0498162 -11.611 30.973 11.8174\" width=\"30.973pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g><rect height=\"0.65243\" width=\"6.26339\" x=\"8.02612\" y=\"-10.9087\"></rect><g transform=\"matrix(.013,0,0,-0.013,8.026,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,14.29,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,24.547,0)\"></path></g></svg>,</span> No. 164, <span><svg height=\"9.49473pt\" style=\"vertical-align:-0.2063999pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.28833 21.1472 9.49473\" width=\"21.1472pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,6.708,0)\"><use xlink:href=\"#g113-81\"></use></g><g transform=\"matrix(.013,0,0,-0.013,14.734,0)\"></path></g></svg>)</span> isostructural to the 122-type iron-based superconductor <span><svg height=\"11.9348pt\" style=\"vertical-align:-3.18146pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.75334 50.3131 11.9348\" width=\"50.3131pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g190-68\"></use></g><g transform=\"matrix(.013,0,0,-0.013,8.762,0)\"><use xlink:href=\"#g190-98\"></use></g><g transform=\"matrix(.013,0,0,-0.013,14.47,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,21.098,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,26.724,3.132)\"><use xlink:href=\"#g50-51\"></use></g><g transform=\"matrix(.013,0,0,-0.013,31.67,0)\"><use xlink:href=\"#g190-66\"></use></g><g transform=\"matrix(.013,0,0,-0.013,40.444,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,45.267,3.132)\"><use xlink:href=\"#g50-51\"></use></g></svg>.</span> No magnetic ordering has been observed when only spins are doped by (Zn, Mn) substitution. Only with carriers codoped by (Sr, Na) substitution, a ferromagnetic ordering occurs below the maximum Curie temperature <svg height=\"12.2532pt\" style=\"vertical-align:-3.29108pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.96212 13.9844 12.2532\" width=\"13.9844pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,7.176,3.132)\"></path></g></svg>∼9.5 K. Comparing with other <span><svg height=\"12.4894pt\" style=\"vertical-align:-3.181499pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.3079 46.4768 12.4894\" width=\"46.4768pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g190-68\"></use></g><g transform=\"matrix(.013,0,0,-0.013,8.762,0)\"><use xlink:href=\"#g190-98\"></use></g><g transform=\"matrix(.013,0,0,-0.013,14.47,0)\"><use xlink:href=\"#g190-66\"></use></g><g transform=\"matrix(.013,0,0,-0.013,23.492,0)\"><use xlink:href=\"#g190-109\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,26.88,3.132)\"><use xlink:href=\"#g50-51\"></use></g><g transform=\"matrix(.013,0,0,-0.013,31.827,0)\"><use xlink:href=\"#g190-84\"></use></g><g transform=\"matrix(.013,0,0,-0.013,37.911,0)\"><use xlink:href=\"#g190-106\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,41.431,3.132)\"><use xlink:href=\"#g50-51\"></use></g></svg>-</span>type diluted magnetic semiconductors, we will show that negative chemical pressure suppresses the Curie temperature.","PeriodicalId":7382,"journal":{"name":"Advances in Condensed Matter Physics","volume":"1189 ","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2022-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A -Type Magnetic Semiconductor (Sr, Na)(Zn, Mn)2Sb2 Isostructural to 122-Type Iron-Based Superconductors\",\"authors\":\"Yilun Gu, Rufei Zhang, Haojie Zhang, Licheng Fu, Guoxiang Zhi, Jinou Dong, Xueqin Zhao, Lingfeng Xie, Fanlong Ning\",\"doi\":\"10.1155/2022/4291923\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A new diluted magnetic semiconductor (Sr, Na)(Zn, Mn)<sub>2</sub>Sb<sub>2</sub> has been successfully synthesized by doping Na and Mn into the parent compound <span><svg height=\\\"12.4894pt\\\" style=\\\"vertical-align:-3.181499pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -9.3079 48.943 12.4894\\\" width=\\\"48.943pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g190-84\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,6.084,0)\\\"></path></g><g transform=\\\"matrix(.013,0,0,-0.013,10.907,0)\\\"></path></g><g transform=\\\"matrix(.013,0,0,-0.013,18.928,0)\\\"></path></g><g transform=\\\"matrix(.0091,0,0,-0.0091,26.137,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,31.083,0)\\\"><use xlink:href=\\\"#g190-84\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,37.245,0)\\\"></path></g><g transform=\\\"matrix(.0091,0,0,-0.0091,43.897,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g></svg>,</span> which has a <span><svg height=\\\"12.4894pt\\\" style=\\\"vertical-align:-3.181499pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -9.3079 46.4768 12.4894\\\" width=\\\"46.4768pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g190-68\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,8.762,0)\\\"><use xlink:href=\\\"#g190-98\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,14.47,0)\\\"><use xlink:href=\\\"#g190-66\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,23.492,0)\\\"><use xlink:href=\\\"#g190-109\\\"></use></g><g transform=\\\"matrix(.0091,0,0,-0.0091,26.88,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,31.827,0)\\\"><use xlink:href=\\\"#g190-84\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,37.911,0)\\\"><use xlink:href=\\\"#g190-106\\\"></use></g><g transform=\\\"matrix(.0091,0,0,-0.0091,41.431,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g></svg>-</span>type crystal structure (space group <span><svg height=\\\"11.8174pt\\\" style=\\\"vertical-align:-0.2063999pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -11.611 30.973 11.8174\\\" width=\\\"30.973pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"></path></g><rect height=\\\"0.65243\\\" width=\\\"6.26339\\\" x=\\\"8.02612\\\" y=\\\"-10.9087\\\"></rect><g transform=\\\"matrix(.013,0,0,-0.013,8.026,0)\\\"></path></g><g transform=\\\"matrix(.013,0,0,-0.013,14.29,0)\\\"></path></g><g transform=\\\"matrix(.013,0,0,-0.013,24.547,0)\\\"></path></g></svg>,</span> No. 164, <span><svg height=\\\"9.49473pt\\\" style=\\\"vertical-align:-0.2063999pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -9.28833 21.1472 9.49473\\\" width=\\\"21.1472pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"></path></g><g transform=\\\"matrix(.013,0,0,-0.013,6.708,0)\\\"><use xlink:href=\\\"#g113-81\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,14.734,0)\\\"></path></g></svg>)</span> isostructural to the 122-type iron-based superconductor <span><svg height=\\\"11.9348pt\\\" style=\\\"vertical-align:-3.18146pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.75334 50.3131 11.9348\\\" width=\\\"50.3131pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g190-68\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,8.762,0)\\\"><use xlink:href=\\\"#g190-98\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,14.47,0)\\\"></path></g><g transform=\\\"matrix(.013,0,0,-0.013,21.098,0)\\\"></path></g><g transform=\\\"matrix(.0091,0,0,-0.0091,26.724,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,31.67,0)\\\"><use xlink:href=\\\"#g190-66\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,40.444,0)\\\"></path></g><g transform=\\\"matrix(.0091,0,0,-0.0091,45.267,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g></svg>.</span> No magnetic ordering has been observed when only spins are doped by (Zn, Mn) substitution. Only with carriers codoped by (Sr, Na) substitution, a ferromagnetic ordering occurs below the maximum Curie temperature <svg height=\\\"12.2532pt\\\" style=\\\"vertical-align:-3.29108pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.96212 13.9844 12.2532\\\" width=\\\"13.9844pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"></path></g><g transform=\\\"matrix(.0091,0,0,-0.0091,7.176,3.132)\\\"></path></g></svg>∼9.5 K. Comparing with other <span><svg height=\\\"12.4894pt\\\" style=\\\"vertical-align:-3.181499pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -9.3079 46.4768 12.4894\\\" width=\\\"46.4768pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g190-68\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,8.762,0)\\\"><use xlink:href=\\\"#g190-98\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,14.47,0)\\\"><use xlink:href=\\\"#g190-66\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,23.492,0)\\\"><use xlink:href=\\\"#g190-109\\\"></use></g><g transform=\\\"matrix(.0091,0,0,-0.0091,26.88,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,31.827,0)\\\"><use xlink:href=\\\"#g190-84\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,37.911,0)\\\"><use xlink:href=\\\"#g190-106\\\"></use></g><g transform=\\\"matrix(.0091,0,0,-0.0091,41.431,3.132)\\\"><use xlink:href=\\\"#g50-51\\\"></use></g></svg>-</span>type diluted magnetic semiconductors, we will show that negative chemical pressure suppresses the Curie temperature.\",\"PeriodicalId\":7382,\"journal\":{\"name\":\"Advances in Condensed Matter Physics\",\"volume\":\"1189 \",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2022-01-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in Condensed Matter Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1155/2022/4291923\",\"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}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in Condensed Matter Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2022/4291923","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}
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