The width of the giant dipole resonance built on excited states of Cu compound nuclei

1991 ◽  
Vol 340 (1) ◽  
pp. 59-62 ◽  
Author(s):  
B. Fornal ◽  
F. Gramegna ◽  
G. Prete ◽  
R. Burch ◽  
G. D'Erasmo ◽  
...  
1982 ◽  
Vol 35 (3) ◽  
pp. 301 ◽  
Author(s):  
FC Barker

The contribution to the Coulomb excitation of the first excited state of 170 due to virtual excitation of the giant dipole resonance (GDR) is calculated, using shell model wavefunctions for the ground and first excited states. A large value is obtained.


1987 ◽  
Vol 36 (2) ◽  
pp. 612-627 ◽  
Author(s):  
M. Kicińska-Habior ◽  
K. A. Snover ◽  
C. A. Gossett ◽  
J. A. Behr ◽  
G. Feldman ◽  
...  

1988 ◽  
Vol 200 (1-2) ◽  
pp. 13-16 ◽  
Author(s):  
A. Stolk ◽  
W.H.A. Hesselink ◽  
H. Rijneveld ◽  
A. Balanda ◽  
J. Penninga ◽  
...  

1996 ◽  
pp. 231-236
Author(s):  
T. Suomijärvi ◽  
J. H. Le Faou ◽  
Y. Blumenfeld ◽  
P. Piattelli ◽  
C. Agodi ◽  
...  

1982 ◽  
Vol 35 (4) ◽  
pp. 377 ◽  
Author(s):  
FC Barker

The discrepancy between the values of B(E2) for the transition between the ground and first excited states in 180 as obtained from Coulomb excitation measurements and from other measurements is here attributed to the giant dipole resonance (GDR) contribution to Coulomb excitation; an estimate based on shell model calculations predicts this contribution to be much larger than previously assumed.


1975 ◽  
Vol 53 (8) ◽  
pp. 795-801 ◽  
Author(s):  
J. G. Woodworth ◽  
J. W. Jury ◽  
K. H. Lokan ◽  
N. K. Sherman

Photoneutron energy distributions from a target of liquid neon have been measured at 90° by time of flight for bremsstrahlung endpoint energies increasing in 1 MeV steps from 19 to 32 MeV. The differential ground state cross section for the major (91%) isotope 20Ne has been obtained, together with an estimate of the strength of transitions to excited states of 19Ne. Six photoneutron groups are observed, reflecting photon absorption which correlates excellently with existing photoproton data, although the absolute cross section is about 10% smaller.It is noted that the giant dipole resonance, estimated by combining the photoneutron and photoproton data, is centered at approximately 20 MeV, which is anomalously low, and that the integrated cross section up to 28 MeV exhausts only half of the dipole sum.


1989 ◽  
Vol 505 (2) ◽  
pp. 241-256 ◽  
Author(s):  
A. Stolk ◽  
A. Balanda ◽  
M.N. Harakeh ◽  
W.H.A. Hesselink ◽  
J. Penninga ◽  
...  

1994 ◽  
Vol 569 (1-2) ◽  
pp. 225-236 ◽  
Author(s):  
T. Suomijärvi ◽  
J.H. Le Faou ◽  
Y. Blumenfeld ◽  
P. Piattelli ◽  
C. Agodi ◽  
...  

1986 ◽  
Vol 176 (3-4) ◽  
pp. 297-301 ◽  
Author(s):  
M.N. Harakeh ◽  
D.H. Dowell ◽  
G. Feldman ◽  
E.F. Garman ◽  
R. Loveman ◽  
...  

1982 ◽  
Vol 35 (3) ◽  
pp. 291 ◽  
Author(s):  
FC Barker

The contributions to the Coulomb excitation of the first excited states of 6Li, 7Li, lOB and 12C due to virtual excitation of the giant dipole resonance (GDR) are calculated, using shell model wavefunctions for the ground and first excited states. When the radial integrals are renormalized in order to fit the experimental B(E2) values for the transitions between these states, the calculated GDR contributions agree reasonably with the measured values in 6Li, 7Li and lOB.


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