Rotational-energy contributions to the kinetic energies of deep-inelastic reaction products

1979 ◽  
Vol 19 (5) ◽  
pp. 2070-2072 ◽  
Author(s):  
R. R. Betts ◽  
S. B. DiCenzo
Keyword(s):  
Rotational Energy ◽  
Reaction Products ◽  
Inelastic Reaction ◽  
Deep Inelastic Reaction

scholarly journals Short-range Lifetime Measurements for Deep-inelastic Reaction Products: the \(^{19}\)O Test Case

2020 ◽  
Vol 51 (3) ◽  
pp. 699
Author(s):  
M. Ciemała ◽  
S. Ziliani ◽  
F. Crespi ◽  
S. Leoni ◽  
B. Fornal ◽  
...  
Keyword(s):  
Short Range ◽  
Test Case ◽  
Reaction Products ◽  
Lifetime Measurements ◽  
Inelastic Reaction ◽  
Deep Inelastic Reaction

scholarly journals Angular momentum transfer and partition in the deep-inelastic reaction 664 MeV 84Kr + natAg

1981 ◽  
Vol 371 (3) ◽  
pp. 510-532 ◽  
Author(s):  
L.G. Sobotka ◽  
C.C. Hsu ◽  
G.J. Wozniak ◽  
D.J. Morrissey ◽  
L.G. Moretto
Keyword(s):  
Angular Momentum ◽  
Momentum Transfer ◽  
Angular Momentum Transfer ◽  
Inelastic Reaction ◽  
Deep Inelastic Reaction

scholarly journals A SEMI-CLASSICAL ANALYSIS OF THE PROTON SEQUENTIAL EMISSION IN 16O+58Ni DEEP INELASTIC COLLISIONS

2005 ◽  
Vol 14 (02) ◽  
pp. 239-254
Author(s):  
L. AUDITORE ◽  
R. BARNÁ ◽  
D. DE PASQUALE ◽  
A. ITALIANO ◽  
A. TRIFIRÓ ◽  
...  
Keyword(s):  
Charged Particles ◽  
Inelastic Collisions ◽  
Classical Analysis ◽  
Fan Effect ◽  
Decay Times ◽  
Inelastic Reaction ◽  
Polarization Phenomena ◽  
Deep Inelastic Reaction ◽  
Light Charged Particles ◽  
Α Particles

We study the 16 O +58 Ni deep inelastic reaction by using coincident charged techniques. Inclusive as well as exclusive data of the C , N , and O fully-damped fragments and their associated light charged particles ( p , d , t , and α-particles) have been collected at the IReS Strasbourg VIVITRON Tandem facility. The velocity distributions of the emitted protons and the associated multiplicity polar plots are analyzed by means of a model which describes simultaneously the nonequilibrium and the evaporative (equilibrated) components of a deep inelastic reaction mechanism. Estimates on polarization phenomena as well as the associated "decay times" of the reaction have been obtained. The hypothesis of a new "fan effect" is proposed for the proton sequential emission in the deep inelastic scattering of 16 O +58 Ni at 8.25 MeV/nucleon.

Projectile-like fragments excitation and gamma-rays emission after the deep inelastic reaction of32S on58Ni

1987 ◽  
Vol 328 (2) ◽  
pp. 227-232
Author(s):  
B. Fornal ◽  
F. Gramegna ◽  
W. Meczynski ◽  
G. Prete ◽  
R. A. Ricci ◽  
...  
Keyword(s):  
Gamma Rays ◽  
Inelastic Reaction ◽  
Deep Inelastic Reaction

Proton and α Sequential Emission in the 16 O + 58 Ni Deep Inelastic Reaction: A Semi-Classical Approach

2002 ◽  
Vol 16 (1-4) ◽  
pp. 281-289 ◽  
Author(s):  
R.C. Barnŕ ◽  
D. De Pasquale ◽  
A. Italiano ◽  
al et
Keyword(s):  
Classical Approach ◽  
Inelastic Reaction ◽  
Deep Inelastic Reaction

Fast-Particle Emission in the Deep-Inelastic Reaction Cu+Ne20at 12.6 MeV/nucleon

1981 ◽  
Vol 46 (8) ◽  
pp. 522-525 ◽  
Author(s):  
R. P. Schmitt ◽  
G. J. Wozniak ◽  
G. U. Rattazzi ◽  
G. J. Mathews ◽  
R. Regimbart ◽  
...  
Keyword(s):  
Particle Emission ◽  
Fast Particle ◽  
Inelastic Reaction ◽  
Deep Inelastic Reaction

Restrictions on shape-coexistence descriptions of A ~ 150 nuclei from the 156Dy(p, t) 154Dy reaction

1992 ◽  
Vol 70 (12) ◽  
pp. 1236-1240 ◽  
Author(s):  
Tao Qu ◽  
D. G. Burke
Keyword(s):  
Rotational Energy ◽  
Spherical Nucleus ◽  
Shape Coexistence ◽  
Reaction Products ◽  
Ground State Band ◽  
The Third ◽  
Population Pattern ◽  
State Band ◽  
Spherical Nuclei ◽  
Mev Protons

The 156Dy(p, t),154Dy reaction was studied, using 20 MeV protons and a magnetic spectrograph to analyze the reaction products. This reaction on the "deformed" target 156Dy has three strong L = 0 transitions populating levels in the "spherical" nucleus 154Dy at 0, 661, and 1058 keV with relative strengths of 100:74:16, respectively. This population pattern is similar to those observed in the isotones 152Gd and,150Sm, in which the third 0+ bands have been interpreted as deformed bands coexisting in spherical nuclei. However, the third 0+ band in 154Dy has a rotational energy spacing as large as that for the ground-state band, which suggests that it does not have a large deformation, and its (p, t) strength is significantly less than those for the corresponding states in the samarium and gadolinium isotones. This restricts the shape-coexistence interpretation of excited 0+ states in 154Dy. The systematics suggest that,152Gd is probably also not as good an example of shape coexistence as 150Sm.

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