1985
DOI: 10.1016/0375-9474(85)90364-1
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Inclusive projectile fragmentation in the spectator model

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Cited by 147 publications
(159 citation statements)
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“…There is a consistent preference for potentials with very weak imaginary parts, with values of W around 5-7 MeV. We systematically find r V < r W and large diffuseness parameters a V ≃ 0.9 fm in agreement with theoretical expectations for loosely bound nuclei [19,20]. A grid search procedure on the real depth of the potential allowed us to identify discrete ambiguities.…”
Section: A Woods-saxon Form Factorssupporting
confidence: 81%
“…There is a consistent preference for potentials with very weak imaginary parts, with values of W around 5-7 MeV. We systematically find r V < r W and large diffuseness parameters a V ≃ 0.9 fm in agreement with theoretical expectations for loosely bound nuclei [19,20]. A grid search procedure on the real depth of the potential allowed us to identify discrete ambiguities.…”
Section: A Woods-saxon Form Factorssupporting
confidence: 81%
“…We first assume that the residue-target S matrix is diagonal with respect to different final states f of the residue, and that this diagonal interaction is the same as that for the residue ground state ͑denoted= S c ͒ for all final states f. This has been termed the spectator-core approximation when used in single-nucleon knockout [23]. It assumes that the amplitudes for dynamical excitation of the core during the collision are small.…”
Section: B Eikonal Model Of Two-nucleon Strippingmentioning
confidence: 99%
“…Generalizing Refs. [3,4] to the deformed core case, the integrated cross section σ strip for single-neutron stripping is now the following:…”
Section: A Eikonal Model Cross Sectionsmentioning
confidence: 99%
“…To date, essentially all calculations have made the spectatorcore approximation [3,4] in which it is assumed that the internal degrees of freedom of these reaction residues are inert and are not dynamically excited or deexcited during the reaction. This allows a direct structural connection to be made between the measured partial cross sections and the wave function overlaps between the projectile initial state and the measured residue final states.…”
Section: Introductionmentioning
confidence: 99%