By Daphne F. Jackson (auth.), Michel Baranger, Erich Vogt (eds.)
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Extra resources for Advances in Nuclear Physics: Volume 4
At 30 MeV the momentum transfer in the (P,pd) reaction is in the range 175-215 MeV/c. The matrix elements for the knockout and absorption processes are formally rather similar and it is illuminating to classify the methods used 1. The Investigation of Hole States in Nuclei 39 in their analysis according to philosophy rather than type of reaction. 3. 2. The Quasi-free or Peripheral Model The essential feature of this model is the assumption that the internal wave function of the group of nucleons to be ejected resembles very closely that of the corresponding free particle.
2, the outgoing protons in a symmetric experiment are in a relative singlet state, any j-dependence is most likely to be observed in a nonsymmetric experiment or in the (a, ap) reaction. 4. Proton States A considerable amount of information on proton separation energies is now available from measurements on the (P,2p), (e, ep), and (d,3He) reactions, and analyses of the data for these reactions and for elastic electron scattering in terms of a single-particle model yields information about the proton single-particle wave functions.
The function a(q), normalized to unity at q = 0, for various Is wave functions for the relative motion of a pair of nucleons in the nucleus. 23 MeV. l 18 Daphne F. Jackson Fig. 5. The function I PlZk(q)/Pd(q) ,0, normal- ized to unity at q = 0, for the deuteron cluster in BLi. 66 fm-I. The arrow (a) indicates the range of q for the (p, pd) reaction at 30 MeV and the arrow (b) indicates the range at 155 MeV. ] used. This point can best be examined if we write the overlap integral in the form (27) The equation for this overlap integral is (JG 69) where E = EA ;' - EBf, W(r1 , r 2) is the residual interaction between the two neutrons, and V(r1) is the potential which binds each neutron to the core.
Advances in Nuclear Physics: Volume 4 by Daphne F. Jackson (auth.), Michel Baranger, Erich Vogt (eds.)