{"title":"二阶矩紧约束模型的有效性","authors":"G. Ackland, M. Finnis, V. Vítek","doi":"10.1088/0305-4608/18/8/002","DOIUrl":null,"url":null,"abstract":"The second moment approximation of tight-binding theory gives an electronic band energy per atom which has the form of the square root of a pairwise sum of squared hopping integrals. This functional form for the dependence of the energy on local coordination has been the basis of empirical non-pairwise force models for transition and noble metals. Hitherto, it appeared to be valid only for a half-filled band. By introducing the assumption that the atoms keep the same charge in all environments, the authors show that the square root function is appropriate for all band fillings.","PeriodicalId":16828,"journal":{"name":"Journal of Physics F: Metal Physics","volume":"98 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"1988-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"87","resultStr":"{\"title\":\"Validity of the second moment tight-binding model\",\"authors\":\"G. Ackland, M. Finnis, V. Vítek\",\"doi\":\"10.1088/0305-4608/18/8/002\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The second moment approximation of tight-binding theory gives an electronic band energy per atom which has the form of the square root of a pairwise sum of squared hopping integrals. This functional form for the dependence of the energy on local coordination has been the basis of empirical non-pairwise force models for transition and noble metals. Hitherto, it appeared to be valid only for a half-filled band. By introducing the assumption that the atoms keep the same charge in all environments, the authors show that the square root function is appropriate for all band fillings.\",\"PeriodicalId\":16828,\"journal\":{\"name\":\"Journal of Physics F: Metal Physics\",\"volume\":\"98 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1988-08-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"87\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics F: Metal Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/0305-4608/18/8/002\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics F: Metal Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0305-4608/18/8/002","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The second moment approximation of tight-binding theory gives an electronic band energy per atom which has the form of the square root of a pairwise sum of squared hopping integrals. This functional form for the dependence of the energy on local coordination has been the basis of empirical non-pairwise force models for transition and noble metals. Hitherto, it appeared to be valid only for a half-filled band. By introducing the assumption that the atoms keep the same charge in all environments, the authors show that the square root function is appropriate for all band fillings.