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NSR database version of April 27, 2024.

Search: Author = C.Sword

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2022XU03      Phys.Rev. C 105, 024902 (2022)

Z.Xu, X.Wu, C.Sword, G.Wang, S.A.Voloshin, H.Z.Huang

Flow-plane decorrelations in heavy-ion collisions with multiple-plane cumulants

doi: 10.1103/PhysRevC.105.024902
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2020VO08      Phys.Rev. C 102, 014325 (2020)

D.Votaw, P.A.DeYoung, T.Baumann, A.Blake, J.Boone, J.Brown, D.Chrisman, J.E.Finck, N.Frank, J.Gombas, P.Gueye, J.Hinnefeld, H.Karrick, A.N.Kuchera, H.Liu, B.Luther, F.Ndayisabye, M.Neal, J.Owens-Fryar, J.Pereira, C.Persch, T.Phan, T.Redpath, W.F.Rogers, S.Stephenson, K.Stiefel, C.Sword, A.Wantz, M.Thoennessen

Low-lying level structure of the neutron-unbound N=7 isotones

NUCLEAR REACTIONS ⁹Be(¹¹Be, ⁸He), (¹¹Be, ⁹Li), E=44 MeV/nucleon; ⁹Be(¹²B, ⁸He), (¹²B, ⁹Li), E=45 MeV/nucleon, [secondary ¹¹Be and ¹²B beams from ⁹Be(¹⁶O, X), E=120 MeV/nucleon, followed by separation of ions of interest using A1900 Fragment Separator at the Coupled Cyclotron Facility of NSCL-MSU]; measured E(n), I(n), charged-particles, (particle)n-coin using the MoNA-LISA detector array for neutron detection and cathode readout drift chambers (CRDCs) for charged particles; deduced decay energy spectra of ⁹He and ¹⁰Li and neutron-unbound states. ⁹He, ¹⁰Li; deduced levels, resonances, widths, J, π, l-values of neutrons from the resonances in ⁹He and ¹⁰Li. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.102.014325
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Data from this article have been entered in the XUNDL database. For more information, click here.

2019SW04      Phys.Rev. C 100, 034323 (2019)

C.Sword, J.Brett, T.Baumann, B.A.Brown, N.Frank, J.Herman, M.D.Jones, H.Karrick, A.N.Kuchera, M.Thoennessen, J.A.Tostevin, M.Tuttle-Timm, P.A.DeYoung

Observation of three-neutron sequential emission from ²⁵O^*

NUCLEAR REACTIONS ²H(²⁷Ne, 2p)²⁵O^*, E=101.3 MeV/nucleon, [secondary ²⁷Ne beam mixed with other light nuclei from fragmentation of 140 MeV/nucleon ⁴⁸Ca primary beam from the Coupled Cyclotron Facility, and separated by A1900 Fragment Separator at NSCL-MSU]; measured E(n), ²²O fragments, (²²O)n-coin, four-body (²²O+3n), three-body (²²O+2n), and two-body (²²O+1n) ungated and gated decay-energy and hit-multiplicity spectra using the Modular Neutron Array (MoNA) and Large multi-Institutional Scintillator Array (LISA); deduced mass of ²⁵O from the invariant of the sum of the energy-momentum four-vectors of an ²²O fragment and the three associated neutrons emitted from the excited states of ²⁵O. ²⁵O; deduced neutron-unbound levels, resonances, decay via three-neutron sequential emission to levels in ²⁴O, ²³O and ²²O. Comparison with shell-model and eikonal calculations for two-proton removal reaction from ²⁷Ne.

NUCLEAR STRUCTURE ^23,24,25O; calculated levels using Gamow shell model with the density-matrix renormalization-group (GSM-DMRG) method, and a continuum shell model (CSM). Comparison with experimental data.

doi: 10.1103/PhysRevC.100.034323
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Data from this article have been entered in the XUNDL database. For more information, click here.