THE IMPULSE APPROXIMATION AND EXPERIMENT


    The results of the calculations are compared with the experimental data in Figs. 1- 14. A calculation in which the coefficients in the potential were evaluated in terms of the amplitudes for free xN scattering, taken at the energy determined by the initial particle, is shown by the dashed curves (in the impulse approximation). It is evident from Figs. 2, 7, 9, and 10 that in this case the results of the calculations for p A and pA scattering agree with the conclusions of other authors discussed above, i.e., for p +,- 12C scattering it is possible to obtain satisfactory agreement with experiment at pion energies above 100 MeV for the total cross sections s tot and the reaction cross sections the reaction cross sections s r (Figs. 7a and 7b), and above 70 MeV for the elastic-scattering differential distributions (Figs. 9 and 10).
    For p 12C and p4He interactions, the calculated results are close to the experimental data in the region of energies above 300 MeV (see Figs. 2a, 2b, and 4). It is found that for the total cross section s tot, of the pd interaction (Fig. 2d) over the entire interval of energies the theoretical cross sections are larger than the experimental ones. This excess becomes smaller with increasing energy. An analogous picture (Figs. 2a - 2c) is seen for p12C and p4He interactions in the interval 100-300 MeV. In the range of energies below 70- 100 MeV for p12C and p4He interactions, a different picture is observed (see Figs. la - 1c): the calculated total cross sections s tot are smaller than the experimental ones, and the reaction cross sections s r are close to experiment. An analysis has shown that this situation occurs because the calculation underestimates the elastic-scattering cross sections [mainly as a result of a substantial underestimation of small- angle scattering (see Figs. 3 and 5) ]. In contrast to pA and p A interactions, the calculated results for scattering of K+ on d and 12C in the impulse approximation are found to be very close to the experimental data (see Figs. 11-14 and Refs. 40 and 41). This may indicate that the mechanism of the K+ A interaction is simpler than that of the p-nucleus and p -nucleus interactions.

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