By D. Weaire, F. Wooten (auth.), David Adler, Hellmut Fritzsche, Stanford R. Ovshinsky (eds.)
This quantity and its spouse volumes, entitled Tetrahedrally-Bonded Amorphous Semiconductors and Localization and Metal-Insulator Transitions, are our manner of paying unique tribute to Sir Nevill Mott and to precise our heartfelt needs to him at the celebration of his 80th birthday. Sir Nevill has set the top criteria as a physicist, instructor, and medical chief. Our emotions for him comprise not just the dignity and admiration due an excellent scientist, but additionally a deep affection for a very good man or woman, who possesses a unprecedented blend of remarkable own traits. We thank him for enriching our lives, and we will without end hold loved stories of this noble guy. Scientists most sensible convey their thank you through contributing their techniques and observations to a Festschrift. This one honoring Sir Nevill fills 3 volumes, with actually 1000s of authors assembly a strict time limit. the truth that contributions poured in from all components of the area attests to the foreign solidarity of our clinical neighborhood. it's a tribute to Sir Nevill's stand for peace and realizing, transcending nationwide borders. The editors desire to show their gratitude to Ghazaleh Koefod for her diligence and services in interpreting and typing a number of the papers, in addition to supporting in several alternative routes. The blame for the blunders that stay belongs to the editors.
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Extra info for Physics of Disordered Materials
V. (r>r core ) ~v(r>rcore)' The hope is that this pseudo V a om is then transferable to the crystal where en V = L V atom (8) en atoms en and one again solves (6) self-consistently using the same functional form for the screening. The all-electron atom potential is simply (9) 23 Let us now break up the single particle density in terms of core electrons and valence electrons so that V atom eff where V. ::c__ -______ v c v r Ir-r' I op (ll) op The potential in (10) looks like a potential describing only valence electrons except that Vion is very strong for r < r core This is shown in Fig.
1983); N. J. A. Sloane, private communication. H. S. M. Coxeter, Proc. Sympos. Pure Math 7, 53 (1963). N. F. Mott, Current Contents 51, 18 (Dec. 22, 1980). 17 PREDICTING THE STRUCTURE OF SOLIDS J. D. Joannopoulos Department of Physi~s Massachusetts Institute of Technology Cambridge, Massachusetts INTRODUCTION One of the oldest fundamental problems in condensed matter physics has been the prediction of the crystal structure of solids from first principles. Given only the atomic number of the constituent atoms as input, what are the possible geometric structures of a solid?
7eV for glassy As 2 Se 3 by Thio, Monroe, and 45 Kastner. More detailed theoretical investigations of defects in the compound chalcogenide glasses are currently on the way. Acknowledgement It is a pleasure to acknowledge the important participation and input of T. Starkloff, D. Vanderbilt, J. Ihm and A. Antonelli on all aspects of this work. This work was supported in part by NSF Grant DMR 76-80895 and by JSEP Grant No. DAAG-29-78-C-0020. 33 References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13.