TY - JOUR
T1 - Energy-dependent target widths in a coupled-channel scattering study
AU - Canton, L.
AU - Fraser, P. R.
AU - Svenne, J. P.
AU - Amos, K.
AU - Karataglidis, S.
AU - Van Der Knijff, D.
PY - 2011/4/19
Y1 - 2011/4/19
N2 - The question of how the scattering cross section changes when the spectra of the colliding nuclei have low-excitation particle-emitting resonances is explored using a multichannel algebraic scattering method. As a test case, the particle-unstable nucleus Be8 has been considered as a target. Nucleon-nucleus scattering cross sections, as well as the spectra of the compound nuclei formed, have been determined from calculations that consider, as well as those that disregard, particle-emission widths of the target nuclear states. The resonant character of the unstable excited states introduces a problem because the low-energy tails of these resonances can intrude into the subthreshold, bound-state region. This unphysical behavior needs to be corrected by modifying, in an energy-dependent way, the shape of the target resonances from the usual Lorentzian form. The resonance function must smoothly reach zero at the elastic threshold. We explore herein a way of achieving this condition.
AB - The question of how the scattering cross section changes when the spectra of the colliding nuclei have low-excitation particle-emitting resonances is explored using a multichannel algebraic scattering method. As a test case, the particle-unstable nucleus Be8 has been considered as a target. Nucleon-nucleus scattering cross sections, as well as the spectra of the compound nuclei formed, have been determined from calculations that consider, as well as those that disregard, particle-emission widths of the target nuclear states. The resonant character of the unstable excited states introduces a problem because the low-energy tails of these resonances can intrude into the subthreshold, bound-state region. This unphysical behavior needs to be corrected by modifying, in an energy-dependent way, the shape of the target resonances from the usual Lorentzian form. The resonance function must smoothly reach zero at the elastic threshold. We explore herein a way of achieving this condition.
UR - http://www.scopus.com/inward/record.url?scp=79960927848&partnerID=8YFLogxK
U2 - 10.1103/PhysRevC.83.047603
DO - 10.1103/PhysRevC.83.047603
M3 - Article
AN - SCOPUS:79960927848
SN - 0556-2813
VL - 83
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 4
M1 - 047603
ER -