Particle-unstable light nuclei with a Sturmian approach that preserves the Pauli principle.pdf
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Particle-unstable light nuclei with a Sturmian approach that preserves the Pauli principle
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Particle-unstable light nuclei with a Sturmian approach that
preserves the Pauli principle.
L. Cantona, K. Amosb, S. Karataglidisc, G. Pisenta, J. P. Svenned, D. van der Knijffe
a Istituto Nazionale di Fisica Nucleare, e Dipartimento di Fisica dell’Universita?,
via Marzolo 8, Padova I-35131, Italia,
b School of Physics, The University of Melbourne, Victoria 3010, Australia
c Department of Physics and Electronics, Rhodes University, Grahamstown 6140, South Africa
d Department of Physics and Astronomy, University of Manitoba, and WITP,
Winnipeg, MB, Canada R3T 2N2
e Advanced Research Computing, Information Div., The University of Melbourne, Australia
Sturmian theory for nucleon-nucleus scattering is discussed in the presence of all the
phenomenological ingredients necessary for the description of weakly-bound (or particle-
unstable) light nuclear systems. Currently, we use a macroscopic potential model of
collective nature. The analysis shows that the couplings to low-energy collective-core
excitations are fundamental but they are physically meaningful only if the constraints
introduced by the Pauli principle are taken into account. The formalism leads one to
discuss a new concept, Pauli hindrance, which appears to be important to understand the
structure of weakly-bound and unbound systems.
1. Sturmians
Sturmians provide the solution of the scattering problems by matrix manipulation and
represent an efficient formalism for determination of S-matrix, and scattering wave func-
tions, bound states and resonances [ 1]. They work well with non-local interactions (such
as those non localities arising from the effects due to Pauli exchanges). They allow a
consistent treatment of Coulomb plus nuclear interactions, as well as the inclusion in the
scattering process of coupled-channel (CC) dynamics. This occurs, for instance, when
strong coupling to low-lying excitations of the target nucleus have to be taken
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