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The R-matrix theory

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arxiv 1001.0678 v1 pith:AK2R32EK submitted 2010-01-05 nucl-th

The R-matrix theory

classification nucl-th
keywords matrixnuclearphysicsmethodscatteringatomicdevelopedsimple
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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abstract

The different facets of the $R$-matrix method are presented pedagogically in a general framework. Two variants have been developed over the years: $(i)$ The "calculable" $R$-matrix method is a calculational tool to derive scattering properties from the Schr\"odinger equation in a large variety of physical problems. It was developed rather independently in atomic and nuclear physics with too little mutual influence. $(ii)$ The "phenomenological" $R$-matrix method is a technique to parametrize various types of cross sections. It was mainly (or uniquely) used in nuclear physics. Both directions are explained by starting from the simple problem of scattering by a potential. They are illustrated by simple examples in nuclear and atomic physics. In addition to elastic scattering, the $R$-matrix formalism is applied to transfer and radiative-capture reactions. We also present more recent and more ambitious applications of the theory in nuclear physics.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Constructing Effective Interactions via Projection-Based Inversion

    nucl-th 2026-08 conditional novelty 6.0

    Discrete energy levels from truncated many-body calculations are inverted, via a Multiparameter Eigenvalue Problem emulator, into effective contact interactions that yield scattering phase shifts and resonance predictions.

  2. Light antiproton-nucleus systems at low energies with the ab initio NCSM/RGM method

    nucl-th 2026-02 conditional novelty 6.0

    Antiproton-deuteron, antiproton-triton, and antiproton-helium-3 scattering and antiprotonic-atom observables were computed with an adapted ab initio NCSM/RGM method, showing peripheral annihilation at about 2 fm.