1978
DOI: 10.1103/physrevlett.41.719
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Ionic Model for Cr, Mn, and Fe Impurities in Cu

Abstract: Commun. 23, 511 (1977). 1J An etched 8x8x3-mm 3 dislocation-free sample with N D~NA ™ 2X10 11 cm" 3 . 12 Both thermalization-and recombination-related phonons must be considered. See also J. M. Worlock and J. Doehler, Bull 0 Am. Phys. Soc. 23, 422 (1978).Our photographs indicate that a significant component of the phonon wind emanates from the excitation point. 13 L. V. Keldysh, Pis'ma Zh.

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Cited by 16 publications
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“…1. Interestingly, the same approach has been employed to model charge fluctuations for TM impurities in metal hosts 23,24 and bulk ferromagnetic metals, 25 where an Anderson-like mixing term transfers electrons between the 3d shell and the conduction band, but is treated as a second-order perturbation with respect to leading intraionic interactions. This similarity with metal systems rather than with, for example, oxides, underlines the hybrid character of TM complexes on metal surfaces, for which strong electron correlation and delocalization coexist and determine the overall magnetic behavior.…”
mentioning
confidence: 99%
“…1. Interestingly, the same approach has been employed to model charge fluctuations for TM impurities in metal hosts 23,24 and bulk ferromagnetic metals, 25 where an Anderson-like mixing term transfers electrons between the 3d shell and the conduction band, but is treated as a second-order perturbation with respect to leading intraionic interactions. This similarity with metal systems rather than with, for example, oxides, underlines the hybrid character of TM complexes on metal surfaces, for which strong electron correlation and delocalization coexist and determine the overall magnetic behavior.…”
mentioning
confidence: 99%