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85033041498
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note
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We can quantitatively predict the peak energy of the slow shoulder in all spectra using Eq. (1) by assuming that the incident atom undergoes two hard sphere collisions, each with a deflection angle of 145°. The sum of these two backward-scattering deflection angles is equal to the experimental deflection angle of 70°.
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-
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31
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36549100563
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liq (which is obtained when β is a constant). Since there is little intensity at low final energies in Fig. 1(b), our estimates of the TD fractions are likely to be upper limits. See, for example, C. T. Rettner, E. K. Schweizer, and C. B. Mullins, J. Chem. Phys. 90, 3800 (1989).
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M. E. King, G. M. Nathanson, M. A. Hanning-Lee, and T. K. Minton, Phys. Rev. Lett. 70, 1026 (1993).
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King, M.E.1
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Hanning-Lee, M.A.3
Minton, T.K.4
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