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NSR database version of April 11, 2024.

Search: Author = N.Viscariello

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2015MA62      Phys.Rev. C 92, 054320 (2015)

B.R.Marks, P.A.DeYoung, J.K.Smith, T.Baumann, J.Brown, N.Frank, J.Hinnefeld, M.Hoffman, M.D.Jones, Z.Kohley, A.N.Kuchera, B.Luther, A.Spyrou, S.Stephenson, C.Sullivan, M.Thoennessen, N.Viscariello, S.J.Williams

Population of ¹³Be in a nucleon exchange reaction

NUCLEAR REACTIONS ⁹Be(¹³B, ¹³Be), E=71 MeV/nucleon, [secondary ¹³B beam from ⁹Be(¹⁸O, X), E=120 MeV/nucleon primary reaction]; measured E(n), I(n) from the decay of ¹³Be into ¹²B+n, decay energy spectrum reconstructed by invariant-mass method using A1900 fragment separator and MoNA-LISA array at NSCL-MSU. Nucleon (-1p, +1n) exchange reaction. ¹³Be; deduced levels, resonances, J, π, widths, relative populations. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.92.054320
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2204. Data from this article have been entered in the XUNDL database. For more information, click here.

2014SM03      Phys.Rev. C 90, 024309 (2014)

J.K.Smith, T.Baumann, D.Bazin, J.Brown, S.Casarotto, P.A.DeYoung, N.Frank, J.Hinnefeld, M.Hoffman, M.D.Jones, Z.Kohley, B.Luther, B.Marks, N.Smith, J.Snyder, A.Spyrou, S.L.Stephenson, M.Thoennessen, N.Viscariello, S.J.Williams

Low-lying neutron unbound states in ¹²Be

NUCLEAR REACTIONS ⁹Be(¹³B, ¹²Be), E=71 MeV/nucleon, [secondary ¹³B beam from ⁹Be(¹⁸O, X), E=120 MeV/nucleon primary reaction; measured particle and neutron spectra, (¹²Be)n-, (¹¹Be)2n-coin using A1900 fragment separator and MoNA-LISA array for neutron and fragment detection at NSCL-MSU facility. ¹²Be; deduced decay energy, level energy, resonance, L-value, J, π, width, one-neutron decay, no evidence for the 2n-decay channel to ¹⁰Be. Comparison with previous experimental results, and with continuum shell model calculation.

doi: 10.1103/PhysRevC.90.024309
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Data from this article have been entered in the XUNDL database. For more information, click here.