Coulomb excitation cross sections of gadolinium isotopes from inelastic scattering measurements

1958 ◽  
Vol 6 ◽  
pp. 451-459 ◽  
Author(s):  
V. Ramšak ◽  
M.C. Olesen ◽  
B. Elbek
2020 ◽  
Vol 102 (6) ◽  
Author(s):  
J. Casal ◽  
M. Rodríguez-Gallardo ◽  
J. M. Arias ◽  
E. Garrido ◽  
R. de Diego

2018 ◽  
Vol 27 (05) ◽  
pp. 1850042
Author(s):  
N. Burtebayev ◽  
A. Duisebayev ◽  
B. A. Duisebayev ◽  
T. Zholdybayev ◽  
Marzhan Nassurlla ◽  
...  

Differential cross-sections for the elastic and inelastic scattering of [Formula: see text]-particles had been measured at the energy of 48.8[Formula: see text]MeV with excitation of low-lying states of the [Formula: see text] nucleus. The data for transitions to the ground [Formula: see text] and excited [Formula: see text], [Formula: see text] states relating to the ground state band were analyzed in the framework of the optical model and the coupled-channel method based on the rotational model. It is shown that the analysis is sensitive not only to the magnitude, but also to the sign of the quadrupole and hexadecapole deformations. The extracted values of the parameters [Formula: see text] and [Formula: see text] are in good agreement with the results of other experiments on the scattering of protons, [Formula: see text] and [Formula: see text]-particles and correspond to the data known from the electron scattering and Coulomb excitation.


1974 ◽  
Vol 52 (23) ◽  
pp. 2422-2435 ◽  
Author(s):  
R. De Swiniarski ◽  
A. Genoux-Lubain ◽  
G. Bagieu ◽  
J. F. Cavaignac

Cross sections were measured for inelastic scattering of 30 MeV protons from 19F, 20Ne, 21Ne, and22Ne. The cross sections of the ground state rotational band in these nuclei were analyzed in the coupled channels formalism and yield further evidence for a large hexadecapole deformation in 19F (β4 = 0.14 ± 0.04) and in 20Ne (β4 = 0.28 ± 0.05) in good agreement with several recent proton inelastic scattering experiments. These calculations show also that the Y4 moment is small or close to zero in 21Ne and 22Ne (β4 ≤ 0.05). The analysis of the available 19F cross section in the DWBA formalism shows evidence for a large and significant octupole transition strength for the 1.35 MeV (5/2−) (3.6 W.u.), the 5.43 MeV (7/2−) state (6.70 W.u.), and the 5.63 MeV (5/2−) state (3.60 W.u.). The measured transition strengths are generally in disagreement with recent low energy (α, α′) or (d, d′) results but also with the earlier Coulomb excitation measurements. Thus, we confirm that a major discrepancy still exists between inelastic scattering and Coulomb excitation of the octupole transition strength to several states in 19F but mainly to the 1.35 MeV (5/2−) state as was already pointed out some time ago from a low energy inelastic proton scattering experiment. On a mesuré les sections efficaces pour la diffusion inélastique de protons de 30 MeV excitant les noyaux 19F, 20Ne, 21Ne et 22Ne.


2018 ◽  
Vol 98 (3) ◽  
Author(s):  
Yu. L. Parfenova ◽  
L. V. Grigorenko ◽  
I. A. Egorova ◽  
N. B. Shulgina ◽  
J. S. Vaagen ◽  
...  

2021 ◽  
pp. 2150170
Author(s):  
Monika Goyal ◽  
Rajiv Kumar ◽  
Pardeep Singh ◽  
Raj Kumar Seth ◽  
Rajesh Kharab

We have investigated the role of central depression parameter on the estimation of survival probability, the Coulomb excitation cross-sections and absorption effects of [Formula: see text] system. The variation in central depression is found to be affecting all the above-mentioned quantities significantly. The survival probability and the Coulomb excitation cross-section are found to be decreasing with increase in [Formula: see text] while the absorption effects are found to be increasing.


1962 ◽  
Vol 39 ◽  
pp. 124-129 ◽  
Author(s):  
R. Graetzer ◽  
R. Hooverman ◽  
E.M. Bernstein

Author(s):  
S. Golladay

The theory of multiple scattering has been worked out by Groves and comparisons have been made between predicted and observed signals for thick specimens observed in a STEM under conditions where phase contrast effects are unimportant. Independent measurements of the collection efficiencies of the two STEM detectors, calculations of the ratio σe/σi = R, where σe, σi are the total cross sections for elastic and inelastic scattering respectively, and a model of the unknown mass distribution are needed for these comparisons. In this paper an extension of this work will be described which allows the determination of the required efficiencies, R, and the unknown mass distribution from the data without additional measurements or models. Essential to the analysis is the fact that in a STEM two or more signal measurements can be made simultaneously at each image point.


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