{"title":"Ni价带的实验自能修正","authors":"H. Starnberg, P. Nilsson","doi":"10.1088/0305-4608/18/11/001","DOIUrl":null,"url":null,"abstract":"The self-energy responsible for the narrowing of the Ni 3d band as observed in photoemission data is obtained from a comparison of a calculated band structure with a band structure determined from photoemission data. The self-energy is found to depend on both wavevector k and band index n, but the authors are able to demonstrate that this dependence is almost exclusively introduced through the hybridisation with sp bands. The self-energy of pure d states is found to be linear, Sigma ( epsilon )=-0.44 epsilon , down to about 3 eV below the Fermi energy.","PeriodicalId":16828,"journal":{"name":"Journal of Physics F: Metal Physics","volume":"17 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"1988-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Experimental self-energy corrections to the Ni valence band\",\"authors\":\"H. Starnberg, P. Nilsson\",\"doi\":\"10.1088/0305-4608/18/11/001\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The self-energy responsible for the narrowing of the Ni 3d band as observed in photoemission data is obtained from a comparison of a calculated band structure with a band structure determined from photoemission data. The self-energy is found to depend on both wavevector k and band index n, but the authors are able to demonstrate that this dependence is almost exclusively introduced through the hybridisation with sp bands. The self-energy of pure d states is found to be linear, Sigma ( epsilon )=-0.44 epsilon , down to about 3 eV below the Fermi energy.\",\"PeriodicalId\":16828,\"journal\":{\"name\":\"Journal of Physics F: Metal Physics\",\"volume\":\"17 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1988-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics F: Metal Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/0305-4608/18/11/001\",\"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/10.1088/0305-4608/18/11/001","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Experimental self-energy corrections to the Ni valence band
The self-energy responsible for the narrowing of the Ni 3d band as observed in photoemission data is obtained from a comparison of a calculated band structure with a band structure determined from photoemission data. The self-energy is found to depend on both wavevector k and band index n, but the authors are able to demonstrate that this dependence is almost exclusively introduced through the hybridisation with sp bands. The self-energy of pure d states is found to be linear, Sigma ( epsilon )=-0.44 epsilon , down to about 3 eV below the Fermi energy.