1984
DOI: 10.1016/0003-4916(84)90141-6
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Nuclear photoabsorption and Compton scattering at intermediate energy

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1985
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Cited by 182 publications
(120 citation statements)
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“…This observation is important in view of the various parameterizations of the resonance spectral function used in transport models which substantially differ at high Δ masses as discussed in [38]. Our fit supports a parametrization of the total width based on the Moniz model [39] which strongly suppresses the high-mass tail of the resonance (see [38] for details).…”
Section: Acceptance Corrected Cross Sectionssupporting
confidence: 73%
“…This observation is important in view of the various parameterizations of the resonance spectral function used in transport models which substantially differ at high Δ masses as discussed in [38]. Our fit supports a parametrization of the total width based on the Moniz model [39] which strongly suppresses the high-mass tail of the resonance (see [38] for details).…”
Section: Acceptance Corrected Cross Sectionssupporting
confidence: 73%
“…(10,12,13,15,16 [14] with error bars. For the p-p case, the present parametrization of elastic and inelastic cross sections fits to the data for whole energy range up to 3 GeV except for the some deviation around 1 GeV, which is due to the elastic cross section and does not affect the result.…”
Section: Two-body Collision Termmentioning
confidence: 99%
“…The masses of the resonances are randomly distributed according to the Breit-Wigner distribution with the momentumdependent width [12], i.e.,…”
Section: Two-body Collision Termmentioning
confidence: 99%
“…For the modification of the real part of their energies, due to their interaction with the medium, we follow previous work on π-nucleus scattering [26,31], nuclear photo absorption [32], and nuclear response in the ∆ region [33,34], and take V ∆ − V N ≈ 25 MeV at normal nuclear density. Note that in our formalism the potentials only enter as the difference V ∆ − V N .…”
Section: Parameter Valuesmentioning
confidence: 99%