{ "id": "1101.4046", "version": "v2", "published": "2011-01-20T22:48:36.000Z", "updated": "2011-07-18T19:52:32.000Z", "title": "Spin-aligned neutron-proton pair mode in atomic nuclei", "authors": [ "Chong Qi", "J. Blomqvist", "T. Bäck", "B. Cederwall", "A. Johnson", "R. J. Liotta", "R. Wyss" ], "comment": "11 pages, 5 figures, version to appear in Phys. Rev. C (Rapid communication)", "journal": "Phys.Rev.C84:021301,2011", "doi": "10.1103/PhysRevC.84.021301", "categories": [ "nucl-th", "nucl-ex" ], "abstract": "Shell model calculations using realistic interactions reveal that the ground and low-lying yrast states of the $N=Z$ nucleus $^{92}_{46}$Pd are mainly built upon isoscalar neutron-proton pairs each carrying the maximum angular momentum J=9 allowed by the shell $0g_{9/2}$ which is dominant in this nuclear region. This structure is different from the ones found in the ground and low-lying yrast states of all other even-even nuclei studied so far. The low-lying spectrum of excited states generated by such correlated neutron-proton pairs has two distinctive features: i) the levels are almost equidistant at low energies and ii) the transition probability $I\\rightarrow I-2$ is approximately constant and strongly selective. This unique mode is shown to replace normal isovector pairing as the dominating coupling scheme in $N=Z$ nuclei approaching the doubly-magic nucleus $^{100}$Sn.", "revisions": [ { "version": "v2", "updated": "2011-07-18T19:52:32.000Z" } ], "analyses": { "subjects": [ "21.60.Cs", "21.10.Re", "23.20.-g", "21.30.Fe" ], "keywords": [ "spin-aligned neutron-proton pair mode", "atomic nuclei", "low-lying yrast states", "realistic interactions reveal", "shell model calculations" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review C", "year": 2011, "month": "Aug", "volume": 84, "number": 2, "pages": "021301" }, "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable", "inspire": 885128, "adsabs": "2011PhRvC..84b1301Q" } } }