dorsal/arxiv
View SchemaNucleon-Nucleon interaction in a chiral constituent quark model
| Authors | D. Bartz, Fl. Stancu |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/9910075 |
| URL | https://arxiv.org/abs/nucl-th/9910075 |
| DOI | 10.1063/1.1303013 |
Abstract
We study the nucleon-nucleon (NN) problem as a six-quark system in a nonrelativistic chiral constituent quark model where the Hamiltonian contains a linear confinement and a pseudoscalar meson (Goldstone boson) exchange interaction between the quarks. This interaction has a long range Yukawa-type part, depending on the mass of the exchanged meson and a short range part, mainly responsible for the good description of the baryon spectra. We calculate the NN potential in the adiabatic approximation as a function of Z, the separation distance between the centres of the two three-quark clusters. The orbital part of the six-quark states is constructed either from the usual cluster model states or from molecular orbital single particle states. The latter are more realistic, having proper axially and reflectionally symmetries. In both cases the potential presents an important hard core at short distances, explained through the dominance of the [51]{FS} configuration. However in the molecular orbital basis the core is less repulsive, as a consequence of the fact that this basis gives a better upper bound for the energy of the six-quark system. We calculate the potential for the 3S1 and 3S0 channels with two different parametrizations. We find a small (few MeV) attractive pocket for one of these parametrizations. A middle range attraction is simulated by the addition of a sigma-meson exchange interaction between quarks, of a form similar to that of the pseudoscalar meson exchange. The present study is an intermediate, useful step towards dynamical calculations based on the resonating group method.
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"date_created": "2026-03-02T18:00:29.333000Z",
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"abstract": "We study the nucleon-nucleon (NN) problem as a six-quark system in a\nnonrelativistic chiral constituent quark model where the Hamiltonian contains a\nlinear confinement and a pseudoscalar meson (Goldstone boson) exchange\ninteraction between the quarks. This interaction has a long range Yukawa-type\npart, depending on the mass of the exchanged meson and a short range part,\nmainly responsible for the good description of the baryon spectra. We calculate\nthe NN potential in the adiabatic approximation as a function of Z, the\nseparation distance between the centres of the two three-quark clusters. The\norbital part of the six-quark states is constructed either from the usual\ncluster model states or from molecular orbital single particle states. The\nlatter are more realistic, having proper axially and reflectionally symmetries.\nIn both cases the potential presents an important hard core at short distances,\nexplained through the dominance of the [51]{FS} configuration. However in the\nmolecular orbital basis the core is less repulsive, as a consequence of the\nfact that this basis gives a better upper bound for the energy of the six-quark\nsystem. We calculate the potential for the 3S1 and 3S0 channels with two\ndifferent parametrizations. We find a small (few MeV) attractive pocket for one\nof these parametrizations. A middle range attraction is simulated by the\naddition of a sigma-meson exchange interaction between quarks, of a form\nsimilar to that of the pseudoscalar meson exchange. The present study is an\nintermediate, useful step towards dynamical calculations based on the\nresonating group method.",
"arxiv_id": "nucl-th/9910075",
"authors": [
"D. Bartz",
"Fl. Stancu"
],
"categories": [
"nucl-th"
],
"doi": "10.1063/1.1303013",
"title": "Nucleon-Nucleon interaction in a chiral constituent quark model",
"url": "https://arxiv.org/abs/nucl-th/9910075"
},
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