scholarly journals Role of N/Z in giant dipole resonance γ rays as a probe of post-saddle nuclear dissipation

2009 ◽  
Vol 681 (5) ◽  
pp. 413-417 ◽  
Author(s):  
W. Ye
1981 ◽  
Vol 59 (6) ◽  
pp. 781-783 ◽  
Author(s):  
G. Kajrys ◽  
W. Del Bianco ◽  
J. Kim ◽  
S. Landsberger ◽  
R. Lecomte ◽  
...  

The 90° differential cross section of the 11B(d,γ0)13C reaction has been measured at deuteron energies from 1.95 to 12.0 MeV in steps varying from 100 to 200 keV. The γ-rays have been detected by a 23 cm long × 23 cm diameter NaI(Tl) crystal spectrometer enclosed in a plastic scintillator anticoincidence shield. The yield curve shows a resonant structure at the energies Eexe = 20.4 ± 0.1 and 22.0 ± 0.2 MeV.


1999 ◽  
Vol 649 (1-4) ◽  
pp. 130-134
Author(s):  
M. Kicińska-Habior ◽  
Z. Trznadel ◽  
A. Maj ◽  
M.P. Kelly ◽  
J.P.S. van Schagen ◽  
...  

1984 ◽  
Vol 62 (3) ◽  
pp. 288-296 ◽  
Author(s):  
W. Del Bianco ◽  
G. Kajrys ◽  
J. Kim ◽  
S. Kundu ◽  
S. Landsberger ◽  
...  

The angular distributions of the 11B(α,γ0)15N and 12C(3He, γ0)15O reactions have been measured at several energies over the giant dipole resonance (GDR) of the two residual nuclei. The 90° yield curve of the 11B(α,γ0)15N reaction has been remeasured with improved energy resolution over the energy ranges Eα = 6.89 – 8.0 and 12.8 – 15 MeV. The γ-rays were detected by a 23-cm long × 23-cm diameter NaI(Tl) crystal spectrometer enclosed in a plastic scintillator anticoincidence shield. Spins and parities of the resonances observed in the yield curves were obtained; the structure previously observed in the yield curve of the 11B(α, γ0)15N reaction between Eα = 7 and 8 MeV has been resolved into two peaks.


2010 ◽  
Vol 19 (08n09) ◽  
pp. 1616-1622
Author(s):  
WEI YE ◽  
FENG WU

We study the variation of the post-saddle giant dipole resonance (GDR) γ-ray multiplicity associated with the fission of the heavy nuclei 240 Cf , 246 Cf , 252 Cf and 240 U with the post-saddle friction strength (β) in the framework of a Langevin model. Calculations show the emitted post-saddle γ emission becomes less sensitive to β with increasing isospin of the the system, and the sensitivity almost disappears for the case of 240 U . We suggest that to accurately obtain information of the post-saddle friction strength by measuring pre-scission GDR γ-ray multiplicities, it is optimal to choose among the various compound systems those with low isospin.


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