By D.R. Bates (ed.), Benjamin Bederson (ed.)
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Extra info for Advances in Atomic and Molecular Physics, Vol. 14
Morgan, M. R. C . McDowell, and J. Callaway (unpublished data, 1977). The total excitation cross-section calculation has used the DWPO method of Callaway et al. (1975) to obtain the contribution from the partial waves L 2 4, and the calculated cross sections do not include any allowance for the finite energy resolution of the experiment. The general agreement is good, but the calculated structure becomes more pronounced relative to the experimental structure as the y1 = 3 threshold is approached.
A very recent experiment by Bullis (1977),using a modified Ramsauer apparatus with improved technique, has obtained very good agreement with the results of Golden and Bandel (1965a) for the e--He total elastic scattering cross section at small electron 36 D. E. Golden energies. However, a further measurement by R. E. Kennerly (private communication, 1977) in a tof apparatus gives values that are about 15% higher than those of Golden and Bandel (1965a)at the lower electron energies (although the error analysis is not yet known).
The energy scale on the figure was obtained using the procedure described in Section II1,D. A summary of the positions of the structures observed by D . E. 22. 2 eV (from Golden et a/.. 1974b). (Copyright by The Institute of Physics. ) Golden et al. (1974b) is shown in Table I1 together with the positions of the structures observed previously by Kuyatt et al. (1965), Ehrhardt et al. (1968), Pichanick and Simpson (1968), Gibson and Dolder (1969), and Golden and Zecca (1970). The features labeled 1'-1"' are associated with the 22S of He-.
Advances in Atomic and Molecular Physics, Vol. 14 by D.R. Bates (ed.), Benjamin Bederson (ed.)