scholarly journals Dependence of the Giant Dipole Strength Function on Excitation Energy

1982 ◽  
Vol 49 (7) ◽  
pp. 434-437 ◽  
Author(s):  
J. E. Draper ◽  
J. O. Newton ◽  
L. G. Sobotka ◽  
H. Lindenberger ◽  
G. J. Wozniak ◽  
...  
1991 ◽  
Vol 43 (5) ◽  
pp. R2049-R2051 ◽  
Author(s):  
N. Teruya ◽  
C. A. Bertulani ◽  
S. Krewald ◽  
H. Dias ◽  
M. S. Hussein

1999 ◽  
Vol 649 (1-4) ◽  
pp. 173-180 ◽  
Author(s):  
G. Gervais ◽  
M. Thoennessen ◽  
W.E. Ormand

2018 ◽  
Vol 194 ◽  
pp. 04002
Author(s):  
N.N. Arsenyev ◽  
A.P. Severyukhin ◽  
V.V. Voronov ◽  
N.V. Giai

We study the effects of the phonon-phonon coupling on the low-energy electric dipole response within a microscopic model based on an effective Skyrme interaction. The finite rank separable approach for the quasiparticle random phase approximation is used. Choosing as an example the isotopic chain of Calcium, we show the ability of the method to describe the low-energy E1 strength distribution. With one and the same set of parameters we describe available experimental data for 48Ca and predict the electric dipole strength function for 50Ca.


2018 ◽  
Vol 178 ◽  
pp. 04001
Author(s):  
Stephane Goriely ◽  
Stephane Hilaire ◽  
Sophie Péru

Valuable theoretical predictions of nuclear dipole excitations in the whole chart are of great interest for different nuclear applications, including in particular nuclear astrophysics. Here we extend our large-scale calculations of the E1 and M1 absorption γ-ray strength function obtained in the framework of the axially-symmetric deformed quasiparticle random phase approximation (QRPA) based on the finite-range D1M Gogny force to the determination of the de-excitation strength function. To do so, shell-model calculations of the de-excitation dipole strength function as well as experimental data are considered to provide insight in the low-energy limit and to complement the QRPA estimate phenomenologically. We compare our final prediction of the E1 and M1 strengths with available experimental data at low energies and show that a relatively good agreement can be obtained. Its impact on the average radiative width as well as radiative neutron capture cross section is discussed.


1970 ◽  
Vol 48 (6) ◽  
pp. 687-708 ◽  
Author(s):  
G. A. Bartholomew ◽  
I. Bergqvist ◽  
E. D. Earle ◽  
A. J. Ferguson

The spectra of gamma rays detected in coincidence with protons from the (d,pγ) reaction in elements [Formula: see text] and [Formula: see text] have been measured in gross structure with a NaI detector. The region of excitation energies covered in the product nuclei was from 0.8 MeV to about the neutron separation energy, typically 7 MeV. The gamma-ray anomalous bump at about 5.5 MeV was found from regions near the separation energy with an intensity comparable to that previously observed in (n,γ) reactions. By gating techniques the decay of many contiguous intervals of excitation energy, populated in the reaction, was studied. From the results, a strength function for gamma rays between 0.8 and 7 MeV approximately was extracted for Au, where the bump is prominent, and for Ta where the bump is essentially absent. In the particular case of 206Pb(d,pγ)207Pb, the gamma-ray spectra are interpreted in terms of the decay of known single particle states. An interpretation of the intensity anomaly in terms of doorway states is discussed.


2001 ◽  
Vol 687 (1-2) ◽  
pp. 231-236 ◽  
Author(s):  
E. Tryggestad ◽  
T. Aumann ◽  
D. Bazin ◽  
J.R. Beene ◽  
Y. Blumenfeld ◽  
...  

1990 ◽  
Vol 41 (3) ◽  
pp. 1300-1302 ◽  
Author(s):  
G. Bertsch ◽  
J. Foxwell

2021 ◽  
Vol 103 (2) ◽  
Author(s):  
F. Heim ◽  
J. Mayer ◽  
M. Müller ◽  
P. Scholz ◽  
A. Zilges

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