Testing microscopically derived descriptions of nuclear collectivity: Coulomb excitation of 22Mg

Many-body nuclear theory utilizing microscopic or chiral potentials has developed to the point that collectivity might be dealt with in an {\it ab initio} framework without the use of effective charges; for example with the proper evolution of operators, or alternatively, through the use of an appro...

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Veröffentlicht in:arXiv.org 2017-09
Hauptverfasser: Henderson, J, Hackman, G, Ruotsalainen, P, Stroberg, S R, Launey, K D, Ali, F A, Bernier, N, Bentley, M A, Bowry, M, Cabellero-Folch, R, Evitts, L J, Frederick, R, Garnsworthy, A B, Garrett, P E, Holt, J D, Jigmeddorj, B, Kilic, A I, Measures, J, Muecher, D, Olaizola, B, O'Sullivan, E, Paetkau, O, Park, J, Smallcombe, J, Svensson, C E, Wu, C Y, Wadsworth, R
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Sprache:eng
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Zusammenfassung:Many-body nuclear theory utilizing microscopic or chiral potentials has developed to the point that collectivity might be dealt with in an {\it ab initio} framework without the use of effective charges; for example with the proper evolution of operators, or alternatively, through the use of an appropriate and manageable subset of particle-hole excitations. We present a precise determination of \(E2\) strength in \(^{22}\)Mg and its mirror \(^{22}\)Ne by Coulomb excitation, allowing for rigorous comparisons with theory. No-core symplectic shell-model calculations were performed and agree with the new \(B(E2)\) values while in-medium similarity-renormalization-group calculations consistently underpredict the absolute strength, with the missing strength found to have both isoscalar and isovector components.
ISSN:2331-8422
DOI:10.48550/arxiv.1709.03948