A direct Fourier transform method is employed for the first time to reconstruct the electron momentum density projected onto the (110) plane from seven high-resolution Compton profiles. The topological features of the projected Fermi surface obtained by the LCW-folding is compared with the most rece
Fermi-surface and electron correlation in Al studied by Compton scattering
✍ Scribed by P. Suortti; T. Buslaps; V. Honkimäki; C. Metz; A. Shukla; Th. Tschentscher; J. Kwiatkowska; F. Maniawski; A. Bansil; S. Kaprzyk; A.S. Kheifets; D.R. Lun; T. Sattler; J.R. Schneider; F. Bell
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 88 KB
- Volume
- 61
- Category
- Article
- ISSN
- 0022-3697
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✦ Synopsis
We have studied the electron-momentum density distribution in Al using the coincidence as well as the conventional highresolution Compton scattering technique. In order to interpret the results, corresponding band theory based computations of the electron momentum density (EMD) and the Compton profiles (CPs) have been carried out. Our focus here is on determining the size of the break Z F in the EMD at the Fermi momentum. For this purpose, differences between measurements and theoretical predictions are analyzed in terms of a simple model for describing electron correlation effects which are missing from the independent particle band theory framework; the model involves Z F as the only adjustable parameter. A good fit with the coincidence measurements is obtained for Z F of about 0.7, while the CP data yields Z F 0:7 to 0.8. This study suggests that, in sharp contrast to the case of Li where recent high-resolution Compton work indicates Z F Ϸ 0; the standard picture of the interacting electron gas is substantially correct in Al.
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