2013
DOI: 10.1103/physrevc.88.054607
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Experimental differential cross sections, level densities, and spin cutoffs as a testing ground for nuclear reaction codes

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Cited by 4 publications
(3 citation statements)
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“…The nuclear reaction cross sections induced by different energy neutrons and photons remains a major problem in applications such as data evaluation [6], applied nuclear physics, nuclear models, and nuclear reaction codes [7]. Therefore, an experimental study on the input parameters for nuclear reaction codes is necessary [8].…”
Section: Introductionmentioning
confidence: 99%
“…The nuclear reaction cross sections induced by different energy neutrons and photons remains a major problem in applications such as data evaluation [6], applied nuclear physics, nuclear models, and nuclear reaction codes [7]. Therefore, an experimental study on the input parameters for nuclear reaction codes is necessary [8].…”
Section: Introductionmentioning
confidence: 99%
“…Up to date, the independent particle model of Fermi gas (FG) model after the Bethe's LD expression [3] and its various modifications [4,5,6] are frequently used in describing the corresponding experimental data including the LD of discrete energy levels and s-wave neutron resonance densities, as well as in the description of nuclear reaction product particle spectra [7][8][9][10][11][12][13]. The so-called composite Gilbert-Cameron (GC) model [4,2,13] unifies further FG model with the constant temperature (CT) approximation.…”
Section: Introductionmentioning
confidence: 99%
“…Up to date, the independent particle model of Fermi gas (FG) model after the Bethe's LD expression [3] and its various modifications [4,5,6] are frequently used in describing the corresponding experimental data including the LD of discrete energy levels and s-wave neutron resonance densities, as well as in the description of nuclear reaction product particle spectra [7][8][9][10][11][12][13]. The so-called composite Gilbert-Cameron (GC) model [4,2,13] unifies further FG model with the constant temperature (CT) approximation. These models however do not involve the collective excitation mechanism of the nucleus in the form of collective vibrations and rotation effects in an explicit manner, despite these effects may be described somehow by the LD parameter (a) and the concerning energy shift (∆).…”
Section: Introductionmentioning
confidence: 99%