Abstract
We present a collection of simple derivations for the neutron-induced resonance cross-sections. These formulae are commonly used to experimentally describe the fundamental properties of resonances for neutron-rich nuclei far from stability and to describe unbound nuclei. The main goal of this article is to illustrate their dependencies with basic observables in order to discuss the pertinence of experimental approaches in the derivation of their properties, especially for “N-body” resonances.
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Notes
Riccati-Bessel functions, solutions of the differential equation \( x^2 \frac{d^2 y}{dx^2} + \left[ x^2 - n (n+1)\right] y = 0\). To get back to the present problem simply put \(n=\ell , x=kr\) and \(y=u_\ell \left( kr\right) \).
Except for \(\ell =0\) states, see Sect. 3.2.
Mathematically the moment of order 3 of the reduced centered variable \(\gamma _{1}={\text {E}} \left[ \left( \frac{X-\mu }{\sigma } \right) ^{3}\right] =\frac{\mu _3}{\sigma ^3}\) with \(\mu _{k}={\text {E}} \left[ (X-\mu )^k\right] =\int _{-\infty }^{+\infty }(x-\mu )^k P(x)\textrm{d} x\) and \(^{2} = \mu _{2}\)
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Gibelin, J. On the Experimental Description of Neutron Resonances. Few-Body Syst 64, 14 (2023). https://doi.org/10.1007/s00601-023-01798-w
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DOI: https://doi.org/10.1007/s00601-023-01798-w