1977
DOI: 10.1103/physrevlett.39.1632
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Resonant Photoemission in Nickel Metal

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Cited by 483 publications
(130 citation statements)
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“…As discussed above, LSDA calculations for fcc Ni cannot reproduce various features of the electronic structure of Ni which had been observed experimentally. Besides the fact that valence band photoemission spectra of Ni [21][22][23] show a reduced 3d-band width compared to LSDA calculations 88 the spectra show a dispersionless feature at a BE of about 6 eV, the so-called 6-eV satellite, 77,78,[89][90][91][92] which is not reproducible within the LSDA approach. On the other hand, an improved description of correlation effects for the 3d electrons using many-body techniques 19,85,86 or in a more modern view applying the LSDA + DMFT scheme 24,60,93 results more or less in the experimental width of the 3d-band complex and furthermore is able to reproduce the 6-eV satellite structure in the valence band region.…”
Section: Satellite Features: Nimentioning
confidence: 89%
See 1 more Smart Citation
“…As discussed above, LSDA calculations for fcc Ni cannot reproduce various features of the electronic structure of Ni which had been observed experimentally. Besides the fact that valence band photoemission spectra of Ni [21][22][23] show a reduced 3d-band width compared to LSDA calculations 88 the spectra show a dispersionless feature at a BE of about 6 eV, the so-called 6-eV satellite, 77,78,[89][90][91][92] which is not reproducible within the LSDA approach. On the other hand, an improved description of correlation effects for the 3d electrons using many-body techniques 19,85,86 or in a more modern view applying the LSDA + DMFT scheme 24,60,93 results more or less in the experimental width of the 3d-band complex and furthermore is able to reproduce the 6-eV satellite structure in the valence band region.…”
Section: Satellite Features: Nimentioning
confidence: 89%
“…The electronic structure of fcc Ni has been the subject of numerous experimental [77][78][79][80][81][82][83][84] and theoretical studies [85][86][87] as a prototype of an itinerant electron ferromagnet, since shortcomings of simple one-electron theory are obvious. As discussed above, LSDA calculations for fcc Ni cannot reproduce various features of the electronic structure of Ni which had been observed experimentally.…”
Section: Satellite Features: Nimentioning
confidence: 99%
“…Various low temperature properties of nickel can be understood by employing standard band-structure approaches. 26,38 Nevertheless, these techniques generally fail to reproduce many characteristic features of nickel, such as an existence of satellite structure 39 at −6 eV, 3d electron bandwidth, 40 and the value of exchange splitting. 40 Applications of LDA + DMFT to study the electronic and magnetic properties of nickel have given a good quantitative description of many of these phenomena.…”
Section: Nickelmentioning
confidence: 99%
“…The same physical process has been previously referred to as autoionisation, resonant photoemission or resonant Auger spectroscopy. Many of the previous studies of this deexcitation process have dealt with the phenomenon in terms of interference effects giving rise to Fano profiles in the absorption cross section (Guillot et al 1977;Schmidt et al 1983), which are more pronounced for lower energy excitations where the valence cross section is still appreciable compared with the core to bound absorption cross section. The experiments described in the present paper utilise the Is core level where, in general, the photon energy required for a core to bound excitation is sufficiently large that the direct valence photoemission is very weak and interference effects are minimal.…”
mentioning
confidence: 99%