On the theory of rotation of non-axial nuclei

Semiphenomenological Model of the Nucleus and its Application to Description of the Rotational Spectra. I

“…The value of the isobaric-spin potential for heavy deformed nuclei waa determined in [13], using the connection between the difference of the proton and neutron occupations numbers and the difference of the proton and neutron well depths. Considering, in accordance with this paper, the depth of the isobaricspin potential to equal…”

“…But for heavy nuclei the depth of the neutron single-particle potential differs from the depth of the proton one by 14-17 MeV, as follows from the difference of the occupation numbers N and Z (see, for instance, [13]). Actually, the proton levels corresponding to the quantum numbers of the neutron excess appear to be blocked for the scattering of isospin pairs.…”

“…Folge * Band 29, Heft 3 * 1973 5) Formulae (37a-b) are as yet merely a prescription for calculating the moments of inertia. Folge * Band 29, Heft 3 * 1973 5) Formulae (37a-b) are as yet merely a prescription for calculating the moments of inertia.…”

“…I n this caee /I and y are derived in SPM from the values of the moments of inertia (gee formulae (40a-b)), Befrom the quadrupole moments, y e -from the ratios of the intensities of the transitions between the states I I, K = 2) and I 1', K' = 0) (the more precise definitions of the parameters are considered in [5,241 and in IT). The successful description (with these parameters) of a large amount of various experimentaldata [l-G, 241 is the essentialargument in favor of SPM, making the prospects of its further development encouraging.…”

“…I n the papers [5,61 this conception was applied to the description of the electromagnetic E2and M 1-transition probabilities and to the description of the gyromagnetic factors of the rotational states; in the paper [7] it is phown how the excited 0+-states are described in the framework of the approach suggested, i.e., without introduction of the long-range residual interactions of the quadrupole type. I n the papers [5,61 this conception was applied to the description of the electromagnetic E2and M 1-transition probabilities and to the description of the gyromagnetic factors of the rotational states; in the paper [7] it is phown how the excited 0+-states are described in the framework of the approach suggested, i.e., without introduction of the long-range residual interactions of the quadrupole type.…”