Energy and range focusing of in-flight separated exotic nuclei – A study for the energy-buncher stage of the low-energy branch of the Super-FRS

2003 ◽  
Vol 204 ◽  
pp. 119-123 ◽  
Author(s):  
C. Scheidenberger ◽  
H. Geissel ◽  
M. Maier ◽  
G. Münzenberg ◽  
M. Portillo ◽  
...  
Keyword(s):  
Exotic Nuclei ◽  
Low Energy

scholarly journals Formation of light exotic nuclei in low-energy multinucleon transfer reactions

2014 ◽  
Vol 89 (5) ◽  
Author(s):  
V. I. Zagrebaev ◽  
B. Fornal ◽  
S. Leoni ◽  
Walter Greiner
Keyword(s):  
Exotic Nuclei ◽  
Low Energy ◽  
Transfer Reactions ◽  
Multinucleon Transfer Reactions

scholarly journals SPECTROSCOPIC FEATURES OF LOW-ENERGY EXCITATIONS IN SKIN NUCLEI

2010 ◽  
Vol 25 (21n23) ◽  
pp. 1779-1782 ◽  
Author(s):  
NADIA TSONEVA ◽  
HORST LENSKE
Keyword(s):  
Fine Structure ◽  
Dynamic Properties ◽  
Exotic Nuclei ◽  
Low Energy ◽  
Close Connection ◽  
Dipole Strength ◽  
Spin Flip

Systematic studies of dipole and other multipole excitations in stable and exotic nuclei are discussed theoretically. Exploring the relation of the strengths of low-energy dipole and quadrupole pygmy resonances to the thickness of the neutron (proton) skin a close connection between static and dynamic properties of the nucleus is observed. The fine structure of low-energy dipole strength in 138 Ba nucleus is revealed from E1 and spin-flip M1 strengths distributions.

scholarly journals Pairing and (9/2)n configuration in nuclei in the 208Pb region

2018 ◽  
Vol 177 ◽  
pp. 03004
Author(s):  
M. Stepanov ◽  
L. Imasheva ◽  
B. Ishkhanov ◽  
T. Tretyakova
Keyword(s):  
Experimental Data ◽  
Excited States ◽  
Ground State ◽  
Exotic Nuclei ◽  
Low Energy ◽  
Energy Spectra ◽  
Pairing Energy ◽  
Multiplet Splitting ◽  
Wide Range ◽  
Nuclear Masses

Excited states in low-energy spectra in nuclei near 208Pb are considered. The pure (j = 9/2)n configuration approximation with delta-force is used for ground state multiplet calculations. The multiplet splitting is determined by the pairing energy, which can be defined from the even-odd straggering of the nuclear masses. For the configurations with more than two valence nucleons, the seniority scheme is used. The results of the calculations agree with the experimental data for both stable and exotic nuclei within 0.06-6.16%. Due to simplicity and absence of the fitted parameters, the model can be easily applied for studies of nature of the excited states in a wide range of nuclei.

MITA: A Multilayer Ionization-chamber Telescope Array for low-energy reactions with exotic nuclei

2019 ◽  
Vol 55 (6) ◽  
Author(s):  
N. R. Ma ◽  
L. Yang ◽  
C. J. Lin ◽  
H. Yamaguchi ◽  
D. X. Wang ◽  
...  
Keyword(s):  
Ionization Chamber ◽  
Exotic Nuclei ◽  
Low Energy ◽  
Telescope Array

Low-energy excitations in nuclear systems: From exotic nuclei to the crust of neutron stars

2008 ◽  
Vol 807 (1-2) ◽  
pp. 1-10 ◽  
Author(s):  
M. Grasso ◽  
E. Khan ◽  
J. Margueron ◽  
N. Van Giai
Keyword(s):  
Neutron Stars ◽  
Exotic Nuclei ◽  
Low Energy ◽  
Nuclear Systems

Dissociated Σ=27 boundaries in silicon

1988 ◽  
Vol 46 ◽  
pp. 624-625
Author(s):  
A. Garg ◽  
W.A.T. Clark ◽  
J.P. Hirth
Keyword(s):  
Electron Diffraction ◽  
Local Minimum ◽  
Boundary Energy ◽  
Coincidence Site Lattice ◽  
Boundary Plane ◽  
Low Energy ◽  
Theoretical Understanding ◽  
Site Lattice ◽  
Kikuchi Pattern ◽  
Analysis Techniques

In the last twenty years, a significant amount of work has been done in the theoretical understanding of grain boundaries. The various proposed grain boundary models suggest the existence of coincidence site lattice (CSL) boundaries at specific misorientations where a periodic structure representing a local minimum of energy exists between the two crystals. In general, the boundary energy depends not only upon the density of CSL sites but also upon the boundary plane, so that different facets of the same boundary have different energy. Here we describe TEM observations of the dissociation of a Σ=27 boundary in silicon in order to reduce its surface energy and attain a low energy configuration.The boundary was identified as near CSL Σ=27 {255} having a misorientation of (38.7±0.2)°/[011] by standard Kikuchi pattern, electron diffraction and trace analysis techniques. Although the boundary appeared planar, in the TEM it was found to be dissociated in some regions into a Σ=3 {111} and a Σ=9 {122} boundary, as shown in Fig. 1.

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