1932
DOI: 10.1007/bf01342150
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�ber die Anwendbarkeit der statistischen Methode auf Ionengitter

Abstract: Erstens n~mlich ~virkt es sehr entmutigenc[ auf die Inangriffnahme des notwendig nieht kugelsymmetrisehen ~olekifl-(Kristall-) Problems, dad wegen der zugrunde liegenden niehtlinearen Differentialgleichung schon die Berechnung der Elektronenverteflung kugelsym~etriseher Atome nach der statistisehen ~ethode eine umst~ndliche numerisehe Integration erfordert. Diesem l~angel ~ird bei dem im folgenden vorgesehlagenen Verfahren begegnet dutch Obergang zu dem der Differentialgleiehung entspreehenden Variationsproble… Show more

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Cited by 183 publications
(42 citation statements)
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“…the i = j term of Eq. (12). From the figure we can differentiate two different regions of the interatomic potentials.…”
Section: Resultsmentioning
confidence: 99%
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“…the i = j term of Eq. (12). From the figure we can differentiate two different regions of the interatomic potentials.…”
Section: Resultsmentioning
confidence: 99%
“…As observed from Eq. (12), when the projectile moves along the channel far from the surface plane, the factors of the polarization potential coming from F − and Li + have opposite signs and they compensate their contributions to order r −4 when F − and Li + ions are placed in front of each other, as it happens in the <100> direction. Furthermore, within a row model, the <100> rows -formed by alternate cations an anions -display a neutral charge, which reduces the polarization of the incident atom.…”
Section: Resultsmentioning
confidence: 99%
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“…However, as in classical mechanics, an explicit treatment beyond one-electron systems is elusive. This spurred the development of effective models of large Coulomb systems starting with Thomas [79], Fermi [29,30], and Lenz [46], who formulated the Thomas-Fermi model in the appropriate language of energy functionals. It asserts that in terms of the nuclear charge Z , the ground state energy of an atom is of leading order Z 7/3 .…”
Section: Introductionmentioning
confidence: 99%
“…Let us suppose that the system is built up from N electrons with k static nuclei of charges Zj>O and locations R j corresponding to the Hamiltonian U({Zj,R)) = L ZiZ) Ri-Rjl-l. i<j The kinetic energy of the nuclei is not considered. Now, in the Thomas-Fermi theory a functional is defined (LENZ, 1932) (3.2) -…”
Section: B Phonons In Insulatorsmentioning
confidence: 99%