C-12-12 ELASTIC-SCATTERING POTENTIALS OBTAINED BY UNIFYING PHASE-SHIFT ANALYSIS WITH THE MODIFIED NEWTON-SABATIER INVERSE METHOD(C)

Citation
B. Apagyi et al., C-12-12 ELASTIC-SCATTERING POTENTIALS OBTAINED BY UNIFYING PHASE-SHIFT ANALYSIS WITH THE MODIFIED NEWTON-SABATIER INVERSE METHOD(C), Physical review. C. Nuclear physics, 49(5), 1994, pp. 2608-2617
Citations number
26
Categorie Soggetti
Physics, Nuclear
ISSN journal
05562813
Volume
49
Issue
5
Year of publication
1994
Pages
2608 - 2617
Database
ISI
SICI code
0556-2813(1994)49:5<2608:CEPOBU>2.0.ZU;2-A
Abstract
A procedure to connect a model-independent phase-shift analysis with t he solution of the inverse quantum scattering problem has been develop ed and applied to experimental differential cross sections of C-12 + C -12 elastic scattering in the energy range E(c.m.) = 8-12 MeV. The min imization of the error square function chi2 is performed with respect to the spectral coefficients involved in the inverse procedure. Input quantities are measured differential cross sections; output results ar e complex potentials. The real part of the potentials, so obtained, is characterized by a pronounced minimum value of -(7-14) MeV at relativ e distances in the range 2.4-3 fm and by a Coulomb barrier of height 6 -7 MeV in the outer region around r almost-equal-to 8-9 fm. In additio n a second minimum, very shallow or vanishing at some incident energie s, is found to exist in the region 5-6 fm. The imaginary part of the p otential exhibits positive maxima in those regions of radial distances where the real part has minimum values indicating a possible feedback effect of flux to the elastic channel. The overall energy dependence of the potentials shows a shape transition resulting in diminishing th e outer potential minimum between E(c.m.) of 9 and 12 MeV. The inverte d (real) potentials yield phase shifts of pi/2 in those partial waves where resonances are known to exist. The procedure is tested by recalc ulating differential cross sections from the inverted energy-dependent potentials with the result that consistent agreement with the experim ental input data is found.