{ "id": "0912.2509", "version": "v2", "published": "2009-12-14T15:38:55.000Z", "updated": "2010-11-16T21:41:01.000Z", "title": "Relationships between nonmesonic-weak-decays in different hypernuclei", "authors": [ "Franjo Krmpotić" ], "comment": "7 pages, 1 figure", "journal": "Phys.Rev.C82:055204,2010", "doi": "10.1103/PhysRevC.82.055204", "categories": [ "nucl-th" ], "abstract": "Using as a tool the s-wave approximation (sWA), this work demonstrates that the nonmesonic weak decay transition rates $\\Gamma_{n}$ and $\\Gamma_{p}$ can be expressed in all hypernuclei up to $^{29}_\\Lambda $Si (and very likely in heavier ones too) in the same way as in the s-shell hypernuclei, i.e. as a linear combination of only three elementary transition rates. This finding leads to the analytic prediction that, independently of the transition mechanism, all hypernuclei that are on the stability line (N = Z), i.e. $^5_\\Lambda $He, $^7_\\Lambda $Li, $^9_\\Lambda $Be, $^{11}_\\Lambda$B, $^{13}_\\Lambda $C, $^{17}_\\Lambda $O, $^{29}_\\Lambda $Si, etc should roughly have the same ratio $\\Gamma_{n}/\\Gamma_{p}$, the magnitude of which rapidly increases when one approaches the neutron drip-line (N >> Z), and opposite happens when one goes toward the proton drip-line (N << Z).", "revisions": [ { "version": "v2", "updated": "2010-11-16T21:41:01.000Z" } ], "analyses": { "subjects": [ "21.80.+a", "21.60.Cs", "13.75.Ev" ], "keywords": [ "hypernuclei", "nonmesonic weak decay transition rates", "relationships", "nonmesonic-weak-decays", "elementary transition rates" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review C", "year": 2010, "month": "Nov", "volume": 82, "number": 5, "pages": "055204" }, "note": { "typesetting": "TeX", "pages": 7, "language": "en", "license": "arXiv", "status": "editable", "inspire": 839982, "adsabs": "2010PhRvC..82e5204K" } } }