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NSR database version of April 27, 2024.

Search: Author = J.Wylie

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2023CH46      Phys.Rev.Lett. 131, 172501 (2023)

R.J.Charity, J.Wylie, S.M.Wang, T.B.Webb, K.W.Brown, G.Cerizza, Z.Chajecki, J.M.Elson, J.Estee, D.E.M.Hoff, S.A.Kuvin, W.G.Lynch, J.Manfredi, N.Michel, D.G.McNeel, P.Morfouace, W.Nazarewicz, C.D.Pruitt, C.Santamaria, S.Sweany, J.Smith, L.G.Sobotka, M.B.Tsang, A.H.Wuosmaa

Strong Evidence for ⁹N and the Limits of Existence of Atomic Nuclei

RADIOACTIVITY ⁹N(p), ⁸C, ⁶Be(2p) [from ⁹Be(¹³O, X)⁹N, E=69.5 MeV/nucleon]; measured decay products, Ep, Ip. ⁹N, ⁸C; deduced invariant-mass spectra, level diagrams, possible single resonancelike peak in the spectrum. R-matrix fits, comparison with the theoretical predictions of an open-quantum-system approach. The National Superconducting Cyclotron Laboratory at Michigan State University.

doi: 10.1103/PhysRevLett.131.172501
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2021WY01      Phys.Rev. C 104, L061301 (2021)

J.Wylie, J.Okolowicz, W.Nazarewicz, M.Ploszajczak, S.M.Wang, X.Mao, N.Michel

Spectroscopic factors in dripline nuclei

NUCLEAR STRUCTURE ⁹C, ⁹Li; calculated spectroscopic factors for the knockout of a p_3/2 nucleon from the 3/2- g.s. of ⁹C and ⁹Li to ground states of ⁸C, ⁸He, ⁸B, and ⁸Li. ⁸C, ⁸He, ⁸B, ⁸Li, ⁹C, ⁹Li; calculated squared harmonic-oscillator basis shell model HO-SM and Gamow shell model (GCM) amplitudes of shell-model configurations, with details of GSM spectra and dominant configurations in ps-space and psd-space given in the Supplemental Material ¹³O, ¹³F; calculated ratio of spectroscopic in shell model embedded in the continuum (SMEC) and HO-SM for neutron and proton removal from the g.s. of ¹³O to ¹²O and ¹²N ground states, and ¹³F proton resonance to the second 2+ state of ¹²O.

doi: 10.1103/PhysRevC.104.L061301
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