Lowitzer, Stephan ; Koedderitzsch, Diemo ; Ebert, Hubert ; Tulip, P. R. ; Marmodoro, A. ; Staunton, J. B.
Alternative Links zum Volltext:DOI
Dokumentenart: | Artikel |
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Titel eines Journals oder einer Zeitschrift: | Europhysics Letters |
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Verlag: | EDP Sciences |
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Band: | 92 |
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Nummer des Zeitschriftenheftes oder des Kapitels: | 3 |
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Seitenbereich: | S. 37009 |
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Datum: | 29 November 2010 |
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Institutionen: | Nicht ausgewählt |
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Identifikationsnummer: | Wert | Typ |
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10.1209/0295-5075/92/37009 | DOI |
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Klassifikation: | Notation | Art |
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72.15.Eb | PACS | 72.10.-d | PACS | 71.20.Be | PACS |
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Dewey-Dezimal-Klassifikation: | 500 Naturwissenschaften und Mathematik > 530 Physik |
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Status: | Veröffentlicht |
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Begutachtet: | Ja, diese Version wurde begutachtet |
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An der Universität Regensburg entstanden: | Nein |
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Dokumenten-ID: | 19681 |
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Zusammenfassung
For a class of transition metal materials residual resistivity is observed to decrease when the materials are deformed and short-range order is removed. We investigate this counter-intuitive behavior with an ab initio theoretical study of the residual resistivity of several late transition metal-rich disordered alloys. The calculations are performed using the Korringa-Kohn-Rostoker (KKR) method ...
Zusammenfassung
For a class of transition metal materials residual resistivity is observed to decrease when the materials are deformed and short-range order is removed. We investigate this counter-intuitive behavior with an ab initio theoretical study of the residual resistivity of several late transition metal-rich disordered alloys. The calculations are performed using the Korringa-Kohn-Rostoker (KKR) method applied to the Kubo-Greenwood formalism. The electronic effects arising from short-range ordering and clustering within the disorder are described using the non-local coherent-potential approximation (NL-CPA). We find a simple, general explanation of this K-state–like effect in terms of changes to the amplitude for d-electron hopping between majority late transition metal nearest-neighbor atoms at the Fermi energy.