Electron momentum density and Compton profile by a semi-empirical approach
Here we propose a semi-empirical approach to describe with good accuracy the electron momentum densities and Compton profiles for a wide range of pure crystalline metals. In the present approach, we use an experimental Compton profile to fit an analytical expression for the momentum densities of the...
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Formato: | Capítulo de libro |
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Elsevier Ltd
2015
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001 | PAPER-13342 | ||
003 | AR-BaUEN | ||
005 | 20250225084750.0 | ||
008 | 190411s2015 xx ||||fo|||| 00| 0 eng|d | ||
024 | 7 | |2 scopus |a 2-s2.0-84926680604 | |
030 | |a JPCSA | ||
040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
100 | 1 | |a Aguiar, J.C. | |
245 | 1 | 0 | |a Electron momentum density and Compton profile by a semi-empirical approach |
260 | |b Elsevier Ltd |c 2015 | ||
270 | 1 | 0 | |m Aguiar, J.C.; Autoridad Regulatoria Nuclear, Av. Del Libertador 8250, Argentina |
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506 | |2 openaire |e Política editorial | ||
520 | 3 | |a Here we propose a semi-empirical approach to describe with good accuracy the electron momentum densities and Compton profiles for a wide range of pure crystalline metals. In the present approach, we use an experimental Compton profile to fit an analytical expression for the momentum densities of the valence electrons. This expression is similar to a Fermi-Dirac distribution function with two parameters, one of which coincides with the ground state kinetic energy of the free-electron gas and the other resembles the electron-electron interaction energy. In the proposed scheme conduction electrons are neither completely free nor completely bound to the atomic nucleus. This procedure allows us to include correlation effects. We tested the approach for all metals with Z=3-50 and showed the results for three representative elements: Li, Be and Al from high-resolution experiments. © 2015 Elsevier Ltd. All rights reserved. |l eng | |
536 | |a Detalles de la financiación: Universidad Nacional del Centro de la Provincia de Buenos Aires | ||
536 | |a Detalles de la financiación: We thank the support from Universidad Nacional del Centro de la Provincia de Buenos Aires (UNCPBA, Argentina). We also thank G. Stutz, S. Huotari and Y. Sakurai for kindly providing us with the high resolution Compton profiles of lithium, beryllium and aluminium, respectively. D.M. acknowledges support by UBACyT 239 from Universidad de Buenos Aires , and PIP 200901/552 from CONICET Argentina . | ||
593 | |a Autoridad Regulatoria Nuclear, Av. Del Libertador 8250, Buenos Aires, C1429BNP, Argentina | ||
593 | |a Instituto de Astronomía y Física Del Espacio, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, C.C. 67, Suc. 28, Buenos Aires, C1428EGA, Argentina | ||
593 | |a Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET), Argentina | ||
593 | |a Instituto de Física Arroyo Seco, CIFICEN (CONICET-UNCPBA), Pinto 399, Tandil, 7000, Argentina | ||
690 | 1 | 0 | |a APPROXIMATION |
690 | 1 | 0 | |a COMPTON PROFILE |
690 | 1 | 0 | |a ELECTRON MOMENTUM DENSITY |
690 | 1 | 0 | |a LAM-PLATZMAN CORRECTION |
690 | 1 | 0 | |a LOCAL DENSITY |
690 | 1 | 0 | |a BERYLLIUM |
690 | 1 | 0 | |a COMPTON SCATTERING |
690 | 1 | 0 | |a DISTRIBUTION FUNCTIONS |
690 | 1 | 0 | |a ELECTRON GAS |
690 | 1 | 0 | |a ELECTRON-ELECTRON INTERACTIONS |
690 | 1 | 0 | |a GROUND STATE |
690 | 1 | 0 | |a KINETIC ENERGY |
690 | 1 | 0 | |a KINETICS |
690 | 1 | 0 | |a MOMENTUM |
690 | 1 | 0 | |a ANALYTICAL EXPRESSIONS |
690 | 1 | 0 | |a APPROXIMATION |
690 | 1 | 0 | |a COMPTON PROFILES |
690 | 1 | 0 | |a CONDUCTION ELECTRONS |
690 | 1 | 0 | |a ELECTRON MOMENTUM DENSITIES |
690 | 1 | 0 | |a FERMI-DIRAC DISTRIBUTION FUNCTION |
690 | 1 | 0 | |a LOCAL DENSITY |
690 | 1 | 0 | |a SEMI-EMPIRICAL APPROACH |
690 | 1 | 0 | |a ELECTRONS |
700 | 1 | |a Mitnik, D. | |
700 | 1 | |a Di Rocco, Héctor Oscar | |
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