Average angular momentum in compound nucleus reactions deduced from isomer ratio measurements

1997 ◽  
Vol 55 (2) ◽  
pp. 766-774 ◽  
Author(s):  
O. A. Capurro ◽  
D. E. DiGregorio ◽  
S. Gil ◽  
D. Abriola ◽  
M. di Tada ◽  
...  
1972 ◽  
Vol 50 (12) ◽  
pp. 1877-1881 ◽  
Author(s):  
C. L. Rao ◽  
L. Yaffe

An analysis has been made of the isomer ratio, σm/((σm + σg) for 134Cs isomers formed in the fission of 237Np by protons of energies 20–85 MeV. Compound nucleus formation was assumed up to a bombarding energy of 50 MeV, with direct interaction as the mechanism at higher energies. Values of the root-mean-square angular momentum of [Formula: see text] at 20 MeV and [Formula: see text] at 60–85 MeV bombarding energy agree with the experimental results. The results are consistent with the hypothesis that angular momentum is generated in the fission process.


1996 ◽  
Vol 45 (5) ◽  
pp. 754
Author(s):  
QIAN XING ◽  
JIANG DONG-XING ◽  
LIN JUN-SONG ◽  
LIU DA-MING ◽  
LI ZE

2020 ◽  
Vol 492 (4) ◽  
pp. 5366-5376 ◽  
Author(s):  
D N Razdoburdin

ABSTRACT We investigate the dynamics of linear perturbations in Keplerian flow under external stochastic force. To abstract from the details of flow structure and boundary conditions, we consider the problem in the shearing box approximation. An external force is assumed to have zero mean, even so, induced perturbations form a steady state, which provides angular momentum transfer to the periphery of the flow. The most effective scenario is based on the transient amplification of induced vortices with the following emission of a shearing sound wave, wherein the maximum of the flux linearly depends on Reynolds number. Thus such a mechanism is significant for astrophysical flows, for which enormous Reynolds numbers are typical. At the same time, addressing the problem analytically, we find that for incompressible fluid in the shearing box approximation stochastic forcing does not lead to average angular momentum transfer. Thus the compressibility of the fluid plays an important role here, and one cannot neglect it.


1987 ◽  
Vol 199 (2) ◽  
pp. 166-170 ◽  
Author(s):  
J. Czakanski ◽  
W. Zipper ◽  
W. Dünnweber ◽  
W. Hering ◽  
D. Konnerth ◽  
...  

1980 ◽  
Vol 22 (2) ◽  
pp. 546-552 ◽  
Author(s):  
H. Oeschler ◽  
H. Freiesleben ◽  
K. D. Hildenbrand ◽  
P. Engelstein ◽  
J. P. Coffin ◽  
...  

2010 ◽  
Vol 19 (05n06) ◽  
pp. 997-1008 ◽  
Author(s):  
AVAZBEK NASIROV ◽  
GIORGIO GIARDINA ◽  
GIUSEPPE MANDAGLIO ◽  
MARINA MANGANARO ◽  
AKHTAM MUMINOV

The mixing of the quasifission component to the fissionlike cross section causes ambiguity in the quantitative estimation of the complete fusion cross section from the observed angular and mass distributions of the binary products. We show that the partial cross section of quasifission component of binary fragments covers the whole range of the angular momentum values leading to capture. The calculated angular momentum distributions for the compound nucleus and dinuclear system going to quasifission may overlap: competition between complete fusion and quasifission takes place at all values of initial orbital angular momentum. Quasifission components formed at large angular momentum of the dinuclear system can show isotropic angular distribution and their mass distribution can be in mass symmetric region similar to the characteristics of fusion-fission components. As result the unintentional inclusion of the quasifission contribution into the fusion-fission fragment yields can lead to overestimation of the probability of the compound nucleus formation.


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