'The field has expanded in so many directions, in connection with the increase in accessible
energy, angular momentum, and nuclear species, and the new phenomena, which have …

Overlaps, used in calculation of nuclear one-and two-particle transfer are reviewed in
chapters 2 and 3 respectively. Their role in the reaction amplitudes is discussed in the …

Angular distributions for the (d, p) reaction leading to bound states in the 1 p shell have been
obtained at E d= 12 MeV for all stable targets. Spectroscopic factors obtained in distorted …

The reaction Ca 40 (d, p) Ca 41 has been studied at deuteron energies of 7.0, 8.0, 9.0, 10.0,
11.0, and 12.0 MeV. Absolute differential cross sections for the four most prominent proton …

The reactions Si 28 (d, p) Si 29, S 32 (d, p) S 33, and Ar 36 (d, p) Ar 37 were studied at an
incident deuteron energy of 18.00 MeV. Some Si 28 (d, p) Si 29 data were also obtained at …

The isotopes of nickel are described by a shell model within the identical-nucleon
configurations (2 p 3 2, 1 f 5 2, 2 p 1 2) n. A least-squares fit to observed level energies …

The energy levels of the Nb, Mo and Tc isotopes with a neutron number N between 50 and
56 are first calculated under the assumptions that their protons and neutrons outside Z= 40 …

States of spin 7 2− in Ti 47, Ti 49, Cr 51, Fe 53, Fe 55, Fe 57, Ni 57, Ni 59, and Ni 61 were
observed by means of the (p, d) reaction with 28-MeV incident protons. In each case the …

Angular distributions for O 16 (d, He 3) N 15 and Ca 40 (d, He 3) K 39 reactions were
measured at an energy of 34.4 MeV. The applicability of the distorted-wave theory to these …

Angular distributions from the (d, p) reactions on Zn 6 4, 6 6, 6 8, 7 0 have been measured
with 10.0-MeV deuterons from the Argonne Tandem van de Graaff accelerator. The …