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The intermolecular arrangement in the plastic crystal (phase Ia) of carbon tetrachloride studied by x‐ray diffraction
1.T. Oda, X‐rays 4, 2 (1945).
2.J. Timmermanns, J. Chim. Phys. 35, 331 (1938).
3.I. Nitta, Z. Krist. 112, 234 (1959).
4.I. Nitta and T. Watanabe, Nature 140, 365 (1937);
4.I. Nitta and T. Watanabe, Sci. Papers Inst. Phys. Chem. Res. 34, 1669 (1938);
4.I. Nitta and T. Watanabe, Bull. Chem. Soc. Jpn. 13, 28 (1938).
5.T. Oda, T. Iida, and I. Nitta, J. Chem. Soc. Jpn. 64, 616 (1943).
6.T. Oda and T. Watanabe, J. Chem. Soc. Jpn. 65, 154 (1944).
7.T. Oda and I. Nitta, J. Chem. Soc. Jpn. 65, 621 (1944).
8.T. Oda, X‐rays 5, 95 (1949);
8.T. Matsubara, X‐rays 5, 102 (1949).
9.T. Matsubara, X‐rays 6, 15 (1950).
10.T. Oda and T. Matsubara, Bull. Chem. Soc. Jpn. 27, 273 (1954).
11.K. Nishikawa and Y. Murata, Bull. Chem. Soc. Jpn. 52, 293 (1979).
12.K. Nishikawa, K. Tohji, M. Shima, and Y. Murata, Chem. Phys. Lett. 64, 154 (1979).
13.A. H. Narten, M. D. Danford, and H. A. Levy, J. Chem. Phys. 46, 4875 (1967).
14.G. Reichelt, J. U. Weidner, and W. Zimmermann, Ber. Bunsenges. Phys. Chem. 78, 1050 (1974).
15.A. H. Narten, J. Chem. Phys. 65, 573 (1976).
16.R. Rudman and B. Post, Science 154, 1009 (1966).
17.Y. Murata and K. Nishikawa, Bull. Chem. Soc. Jpn. 51, 411 (1978).
18.K. Tohji, K. Nishikawa, and Y. Murata, Jpn. J. Appl. Phys. 19, L365 (1980).
19.J. A. Morrison and L. Richards, J. Chem. Thermodyn. 8, 1033 (1976).
20.Since their papers1,8 were published in a journal which is not readily available, their formulations are reproduced in the present paper as an application to the plastic crystal.
21.Accordlng to Eq. (1), the weighted structure function is defined as where the summation is made for all the component atoms in a unit. This definition applies to a general discussion of the scattering intensity for the liquid. In the case of a plastic crystal, however, the total coherent intensity does not contain self‐scattering of the atom at the center of the unit cell, as shown in Eqs. (9) and (12). Since the weighted structure function is the intensity representing the interference between atoms, the weighted structure function for a plastic crystal is defined as where the central atom is excluded from the summation. However, the observed si(s) listed in Table I is calculated by using Eq. (1).
22.Y. Morino, Y. Nakamura, and T. Iijlma, J. Chem. Phys. 32, 643 (1960).
23.In the present study the value is used in the calculation of the intensities for all the packing models of the plastic crystal.
24.B. Post, Acta Crystallogr. 12, 349 (1959).
25.T. Kihara, Intermolecular Force (Wiley, New York, 1977).
26.L. J. Lowden and D. Chandler, J. Chem. Phys. 61, 5228 (1974).
27.The peak at 3.8 Å appears in the radial distribution curve for the liquid reported in most of the previous papers. It seems to be accepted generally that this peak corresponds to the interference between the two chlorine atoms belonging to adjacent molecules.
28.M. Postel and J. G. Riess, J. Phys. Chem. 81, 2634 (1977).
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