Shape coexistence and the N = 20 shell closure far from stability by inelastic scattering

2003 ◽  
pp. 273-276
Author(s):  
W. Mittig ◽  
H. Savajols ◽  
D. Baiborodin ◽  
J. M. Casandjian ◽  
C. E. Demonchy ◽  
...  
2002 ◽  
Vol 15 (1-2) ◽  
pp. 157-160 ◽  
Author(s):  
W. Mittig ◽  
H. Savajols ◽  
D. Baiborodin ◽  
J.M. Casandjian ◽  
C.E. Demonchy ◽  
...  

2018 ◽  
Vol 178 ◽  
pp. 02013 ◽  
Author(s):  
V. Werner ◽  
M. Lettmann ◽  
C. Lizarazo ◽  
W. Witt ◽  
D. Cline ◽  
...  

The region of neutron-rich nuclei above the N = 50 magic neutron shell closure encompasses a rich variety of nuclear structure, especially shapeevolutionary phenomena. This can be attributed to the complexity of sub-shell closures, their appearance and disappearance in the region, such as the N = 56 sub shell or Z = 40 for protons. Structural effects reach from a shape phase transition in the Zr isotopes, over shape coexistence between spherical, prolate, and oblate shapes, to possibly rigid triaxial deformation. Recent experiments in this region and their main physics viewpoints are summarized.


Exotic Nuclei ◽  
2002 ◽  
Author(s):  
W. MITTIG ◽  
H. SAVAJOLS ◽  
P. ROUSSEL-CHOMAZ ◽  
J. M. CASANDJIAN ◽  
C. E. DEMONCHY ◽  
...  

Author(s):  
K. Wimmer ◽  
T. Arici ◽  
W. Korten ◽  
P. Doornenbal ◽  
J.-P. Delaroche ◽  
...  

Author(s):  
F. Sarazin ◽  
H. Savajols ◽  
W. Mittig ◽  
F. Nowacki ◽  
N. A. Orr ◽  
...  

2002 ◽  
Vol 146 ◽  
pp. 16-22 ◽  
Author(s):  
W. Mittig ◽  
H. Savajols ◽  
D. Baiborodin ◽  
J. M. Casandjian ◽  
C. E. Demonchy ◽  
...  

2019 ◽  
Vol 26 ◽  
pp. 44
Author(s):  
A. Khaliel ◽  
D. Papaioannou ◽  
G. Zagoraios ◽  
T. J. Mertzimekis

Nuclear gfactors are highly sensitive to the single–particle aspects of the wave function, revealing important information for the nuclear structure along the isotopic chart. The sdshell has been thoroughly studied, resulting in “universal” shell model Hamiltonians [1] and the development of an M1 operator [2]. However, there is still shortage of precise experimental gfactor data of excited states to consolidate the nuclear structure in this regime.      Recently, the Time Differential Recoil in Vacuum (TDRIV) experimental technique was revamped to be applicable for radioactive beams. TDRIV has been tested successfully and produced high-precision results for the stable 24Mg nucleus [3]. However, the successful application of the technique relies heavily on calibrations of the de–orientation phenomenon.      A recent experiment using the MINIBALL array at REX/ISOLDE (IS628) has focused on the application of the method with a radioactive 28Mg beam. The gfactor of the 28Mg first 2+excited state can act as an excellent probe of the N=16 shell gap and the νd3/2singleparticle energy, as well as the possible presence of spdfadmixtures. The particular measurement will be a next step towards a gfactor measurement on 32Mg in the center of the “island of inversion”, where the N=20 shell closure breaks down enhancing 1p–1h excitations and shape–coexistence.           In this work, the analysis of the spectroscopic data recorded for a 22Ne beam, which was used for calibrating the experimental method before the actual run on 28Mg is reported. Preliminary data on the angular distributions for the 22Ne 21+→ 0+transition will be presented, an important prerequisite before a remeasurement of g(22Ne;21+).


2018 ◽  
Vol 98 (4) ◽  
Author(s):  
W. Witt ◽  
V. Werner ◽  
N. Pietralla ◽  
M. Albers ◽  
A. D. Ayangeakaa ◽  
...  

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.


Author(s):  
Kenneth H. Downing ◽  
Robert M. Glaeser

The structural damage of molecules irradiated by electrons is generally considered to occur in two steps. The direct result of inelastic scattering events is the disruption of covalent bonds. Following changes in bond structure, movement of the constituent atoms produces permanent distortions of the molecules. Since at least the second step should show a strong temperature dependence, it was to be expected that cooling a specimen should extend its lifetime in the electron beam. This result has been found in a large number of experiments, but the degree to which cooling the specimen enhances its resistance to radiation damage has been found to vary widely with specimen types.


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