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By John, editor Ross

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In terms of the coordinate system in Figure 3a, this experimental potential, obtained from appropriate scattering experiments in the same manner as atom-atom potentials, is then assumed to be ELASTIC SCATTERING OF HIGH-ENERGY BEAMS 49 where r is the distance between the center of mass of the molecule and the interacting atom, R is the distance between a constituent atom of the molecule and the interacting atom, and 0 is the angle between r and a, the half length o f the molecular bond, so that do = 2n sin 0 do.

D. R. Bates and A. Damgaard, Phil. Trans. Roy. Soc. (London), A242, 101 (1959). 23. M. Mizushima, Nutl. Bur. Std. , 6009,Boulder, Colorado, 1958. 24. M. Sundbom, Arkiv Fysik, 13, 539 (1958). 25. D. Parkinson, Proc. Phys. Soc. (London), A75, 169 (1960). Advance in Chemical Physics, VolunzeX Edited by John Ross Copyright © 1966 by John Wiley & Sons. Inc. 2 ELASTIC SCATTERING OF HIGH-ENERGY BEAMS : REPULSIVE FORCES . 1. AMDUR and J . E JORDAN Department of Chemistry. Massachusetts Institute of Technology.

Buckingham, Proc. Roy. (London), A160,94 (1937). 13. R. M. Sternheimer, Phys. , 127, 1220 (1962). 14. Kusch and V. W. Hughes, Encyclopediaof Physics, Vol. 37,Part I, Springer Verlag, Berlin. 1959. 15. N. FI Ramsey, Molecular Beams, Oxford University Press, Londoii, 1956, p. 397ff. ATOMIC POLARIZABILITIES 27 16. J. C . Zorn, G. E. Chamberlain, and V. W. Hughes, Phys. , 129, 2566 (1963). 17. R. S. b o x , Phys. , 110, 375 (1958). 18. D. R. Hartree and W. Hartree, Proc. Cumbridge Phil. , 34, 550 (1938).

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