P. Genoud, Ashutosh Kumar Singh, A. Manuel, T. Jarlborg, E. Walker, M. Peter, M. Weller
{"title":"用自旋极化正电子湮灭研究铁磁性铁的电子动量分布和自旋密度","authors":"P. Genoud, Ashutosh Kumar Singh, A. Manuel, T. Jarlborg, E. Walker, M. Peter, M. Weller","doi":"10.1088/0305-4608/18/9/014","DOIUrl":null,"url":null,"abstract":"The authors report the first study of the Fermi surface topology, electron momentum density and spin momentum density in ferromagnetic iron using two-dimensional angular correlation of polarised positron annihilation radiation. A calculation made in the independent-particle model was obtained from the self-consistent linear muffin-tin orbital method. Comparison between experiment and calculation reveals marked discrepancies which are due to both electron-electron and electron-positron correlation effects. Analysis of experimental distributions shows that the large N-centred hole pocket of minority third band does not exist in contrast with the self-consistent calculation results. A parametrised band-structure calculation has been performed to account for the electron-electron correlation effects. Distributions resulting from this procedure were in better agreement with experiment than the self-consistent ones. Once again the nature of electron-positron correlation effects is found to resemble those observed by Sing et al. for nickel. This confirms the systematic trends of electron-positron correlation effects for localised d electrons. The correct description of the relative spin momentum density distribution requires different enhancement factors for majority and minority electron bands.","PeriodicalId":16828,"journal":{"name":"Journal of Physics F: Metal Physics","volume":"1 1","pages":"1933-1947"},"PeriodicalIF":0.0000,"publicationDate":"1988-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"27","resultStr":"{\"title\":\"Electron momentum distribution and spin density of ferromagnetic iron studied by spin-polarised positron annihilation\",\"authors\":\"P. Genoud, Ashutosh Kumar Singh, A. Manuel, T. Jarlborg, E. Walker, M. Peter, M. Weller\",\"doi\":\"10.1088/0305-4608/18/9/014\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The authors report the first study of the Fermi surface topology, electron momentum density and spin momentum density in ferromagnetic iron using two-dimensional angular correlation of polarised positron annihilation radiation. A calculation made in the independent-particle model was obtained from the self-consistent linear muffin-tin orbital method. Comparison between experiment and calculation reveals marked discrepancies which are due to both electron-electron and electron-positron correlation effects. Analysis of experimental distributions shows that the large N-centred hole pocket of minority third band does not exist in contrast with the self-consistent calculation results. A parametrised band-structure calculation has been performed to account for the electron-electron correlation effects. Distributions resulting from this procedure were in better agreement with experiment than the self-consistent ones. Once again the nature of electron-positron correlation effects is found to resemble those observed by Sing et al. for nickel. This confirms the systematic trends of electron-positron correlation effects for localised d electrons. The correct description of the relative spin momentum density distribution requires different enhancement factors for majority and minority electron bands.\",\"PeriodicalId\":16828,\"journal\":{\"name\":\"Journal of Physics F: Metal Physics\",\"volume\":\"1 1\",\"pages\":\"1933-1947\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1988-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"27\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics F: Metal Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/0305-4608/18/9/014\",\"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/10.1088/0305-4608/18/9/014","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Electron momentum distribution and spin density of ferromagnetic iron studied by spin-polarised positron annihilation
The authors report the first study of the Fermi surface topology, electron momentum density and spin momentum density in ferromagnetic iron using two-dimensional angular correlation of polarised positron annihilation radiation. A calculation made in the independent-particle model was obtained from the self-consistent linear muffin-tin orbital method. Comparison between experiment and calculation reveals marked discrepancies which are due to both electron-electron and electron-positron correlation effects. Analysis of experimental distributions shows that the large N-centred hole pocket of minority third band does not exist in contrast with the self-consistent calculation results. A parametrised band-structure calculation has been performed to account for the electron-electron correlation effects. Distributions resulting from this procedure were in better agreement with experiment than the self-consistent ones. Once again the nature of electron-positron correlation effects is found to resemble those observed by Sing et al. for nickel. This confirms the systematic trends of electron-positron correlation effects for localised d electrons. The correct description of the relative spin momentum density distribution requires different enhancement factors for majority and minority electron bands.