1990
DOI: 10.1007/bf02407589
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Theory of63Cu and17O quadrupole interactions in copper oxide high-T c systems

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Cited by 3 publications
(6 citation statements)
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“…In this paper, we attempt to fill this gap, and present the results of cluster electronic structure calculations at the UHF and the Møller-Plesset levels for YBa 2 Cu 3 O 7 ceramics with a self-consistent account taken of the infinite-crystal surroundings of the quantum cluster; these calculations, where the lattice is considered as a static lattice, correspond to overdoped ceramics. The Gaussian basis set employed is larger than those used in previous cluster calculations [15,19,21,28]. The results obtained in this study reveal the strong influence of the electron correlation effect on the charge distribution and the orbital population of Cu and O atoms.…”
Section: Introductionmentioning
confidence: 79%
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“…In this paper, we attempt to fill this gap, and present the results of cluster electronic structure calculations at the UHF and the Møller-Plesset levels for YBa 2 Cu 3 O 7 ceramics with a self-consistent account taken of the infinite-crystal surroundings of the quantum cluster; these calculations, where the lattice is considered as a static lattice, correspond to overdoped ceramics. The Gaussian basis set employed is larger than those used in previous cluster calculations [15,19,21,28]. The results obtained in this study reveal the strong influence of the electron correlation effect on the charge distribution and the orbital population of Cu and O atoms.…”
Section: Introductionmentioning
confidence: 79%
“…The charges of the outermost ions are adjusted in order to provide the correct value of the Madelung potential at each cluster site as well as the electrical neutrality of the set: cluster plus background charges. This is achieved by using a procedure originally proposed by Kelires and Das [44,21]. To a shell of n i equal exterior charges q i which creates at the site j a potential V i (j ) is associated a charge scaling factor f i such that the Madelung potential at the site j due to the infinite crystal, V M (j ), is equal to the potential of each shell of scaled charges plus that created by the whole set of charges minus those included in the shells, denoted as V q (j ).…”
Section: Methodsmentioning
confidence: 99%
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“…There is a multi-pronged attack from both the experimentalist and theorist which are not always cooperative. The theoretical methods, which investigate the electronic structure of these materials, range from band structure [1,2] and supercell approaches which account for dopants [3,4] to cluster calculations [5][6][7][8][9][10][11], but are largely complementary in their areas of success.…”
Section: Introductionmentioning
confidence: 99%