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| DC Field | Value | Language |
|---|---|---|
| dc.contributor.author | Lagaris, I. E. | en |
| dc.contributor.author | Pandharipande, V. R. | en |
| dc.date.accessioned | 2015-11-24T17:02:59Z | - |
| dc.date.available | 2015-11-24T17:02:59Z | - |
| dc.identifier.issn | 0375-9474 | - |
| dc.identifier.uri | https://olympias.lib.uoi.gr/jspui/handle/123456789/11118 | - |
| dc.rights | Default Licence | - |
| dc.title | Phenomenological two-nucleon interaction operator | en |
| heal.type | journalArticle | - |
| heal.type.en | Journal article | en |
| heal.type.el | Άρθρο Περιοδικού | el |
| heal.identifier.primary | 10.1016/0375-9474(81)90240-2 | - |
| heal.language | en | - |
| heal.access | campus | - |
| heal.recordProvider | Πανεπιστήμιο Ιωαννίνων. Σχολή Θετικών Επιστημών. Τμήμα Μηχανικών Ηλεκτρονικών Υπολογιστών και Πληροφορικής | el |
| heal.publicationDate | 1981 | - |
| heal.abstract | We report a phenomenological two-nucleon interaction operator obtained by fitting the nucleon-nucleon phase shifts up to 425 MeV in S, P, D and F waves, and the deuteron properties. The operator has the standard eight potentials associated with the two-body operators 1, σ1 · σ2, τ1 · τ2, σ1 · σ2τ1 · τ2, S12, S12τ2, S12τ1 · τ2, L · S and L · Sτ1 · τ2; and six phenomenological potentials associated with operators L2, L2σ1 · σ2, L2τ1 · τ2, L2σ1 · σ2τ1· τ2, (L · S)2 and (L · S)2τ1 · τ2. The six quadratic L terms are relatively weak, and are chosen in order to make many-body calculations with this operator simpler. | en |
| heal.journalName | Nuclear Physics A | en |
| heal.journalType | peer reviewed | - |
| heal.fullTextAvailability | TRUE | - |
| Appears in Collections: | Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά) | |
Files in This Item:
| File | Description | Size | Format | |
|---|---|---|---|---|
| Lagaris-1981-Phenomenologicaltwo-nucleoninteractionoperator.pdf | 823.69 kB | Adobe PDF | View/Open Request a copy |
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