By Duane W.
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M . Zahurak. References 1. Kroto, H . ; Heath, J. ; O'Brien, S. ; Curl, R. ; Smalley, R. E. Nature (London) 1985, 318, 162. 2. ; Lamb, L. ; Huffman, D. R. Nature (London) 1990, 347, 354. 3. ; Haddon, R. ; Glarum, S. ; Douglas, D. ; Mujsce, A. M . J. Phys. Chem. 1991, 95, 518. 4. Yannoni, C. ; Johnson, R. ; Bethune, D. ; Salem, J. R. J. Phys. Chem. 1991, 95, 9. 5. Yannoni, C. ; Bernier, P. ; Bethune, D. ; Salem, J. R. J. Am. Chem. Soc. 1991, 113, 3190. 6. ; Hare, J. ; Abdul-Sada, A. ; Kroto, H .
Practically speaking, little difference is seen in the magnitude of the errors using the ordered model and the smooth-sphere model. For calculations such as band structures, the choice of model largely depends on one's taste and the ease of application. An interesting feature of the diffraction in pure C ^ is the conspicuous absence of the (200) reflection, caused by the hollow nature of the molecule. ; ACS Symposium Series; American Chemical Society: Washington, DC, 1992. ch002 / = f 4ΤΓΓ 2 sin Ε]* Qr\ Assuming a shell of charge where p(r) = 6{r — R), then the molecular form fac tor is given by / ~ sin (QR/QR) where Q is the X-ray momentum transfer 4π (sin Θ)/Χ.
Murphy, D. ; Haddon, R. ; Mujsce, A . M . ; Kaplan, M . ; Zahurak S. M . Mater. Res. Soc. Symp. Proc. 1991, 206, 691. 18. Luzzi, D. ; Fischer, J. ; Wang, X . ; Ricketts-Foot, D. ; McGhie, A. ; Romanow, W. J. J. Mater. , submitted. 19. See, for example, The Physics of Quasicrystals; Steinhardt, P. ; World Scientific: Singapore, 1987. 20. ; Reidel: Dordrecht, Netherlands, 1983; Vol. A, p 781. 21. ; Robinson, K. Acta Cryst. 1966, 20, 614. 22. See, for example, Cold Spring Harbor Symposia on Quantitative Biology, Vol.