NSR Query Results


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NSR database version of May 24, 2024.

Search: Author = G.W.McCann

Found 8 matches.

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2024CO04      Nucl.Instrum.Methods Phys.Res. A1058, 168827 (2024)

A.L.Conley, B.Kelly, M.Spieker, R.Aggarwal, S.Ajayi, L.T.Baby, S.Baker, C.Benetti, I.Conroy, P.D.Cottle, I.B.D'Amato, P.DeRosa, J.Esparza, S.Genty, K.Hanselman, I.Hay, M.Heinze, D.Houlihan, M.I.Khawaja, P.S.Kielb, A.N.Kuchera, G.W.McCann, A.B.Morelock, E.Lopez-Saavedra, R.Renom, L.A.Riley, G.Ryan, A.Sandrik, V.Sitaraman, E.Temanson, M.Wheeler, C.Wibisono, I.Wiedenhover

The CeBrA demonstrator for particle-γ coincidence experiments at the FSU Super-Enge Split-Pole Spectrograph

NUCLEAR REACTIONS 49Ti, 61Ni, 52Cr, 34S(d, p), E=16 MeV; measured reaction products, Eγ, Iγ, particle-γ-coin.; deduced γ-ray energies and relative intensities, excited states lifetimes. Comparison with available data. The CeBrA demonstrator for particle-γ coincidence experiments at the Super-Enge Split-Pole Spectrograph of the John D. Fox Superconducting Linear Accelerator Laboratory at Florida State University.

doi: 10.1016/j.nima.2023.168827
Citations: PlumX Metrics


2024HA06      Phys.Rev. C 109, 024302 (2024)

I.C.S.Hay, P.D.Cottle, L.A.Riley, L.T.Baby, S.Baker, A.L.Conley, J.Esparza, K.Hanselman, M.Heinze, D.Houlihan, B.Kelly, K.W.Kemper, G.W.McCann, R.Renom, A.Sandrik, D.Simms, M.Spieker, I.Wiedenhover

Measurement of g9/2 strength in the stretched 8- state and other negative parity states via the 51V(d, p)52V reaction

doi: 10.1103/PhysRevC.109.024302
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2023AY06      Eur.Phys.J. A 59, 294 (2023)

Y.Ayyad, A.K.Anthony, D.Bazin, J.Chen, G.W.McCann, W.Mittig, B.P.Kay, D.K.Sharp, J.C.Zamora

Kinematics reconstruction in solenoidal spectrometers operated in active target mode

NUCLEAR REACTIONS 2H(10Be, 10Be'), E=9 MeV/nucleon; 1H(14C, p), (14C, p'), (14C, d), E=12 MeV/nucleon; measured reaction products; deduced yields. The Active Target Time Projection Chamber (AT-TPC) of the Facility for Rare Isotope (FRIB) of the Michigan State University (MSU).

doi: 10.1140/epja/s10050-023-01205-2
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2023RI03      Phys.Rev. C 108, 044306 (2023)

L.A.Riley, D.T.Simms, L.T.Baby, A.L.Conley, P.D.Cottle, J.Esparza, K.Hanselman, I.C.S.Hay, M.Heinze, B.Kelly, K.W.Kemper, G.W.McCann, R.Renom, M.Spieker, I.Wiedenhover

g9/2 neutron strength in the N=29 isotones and the 52Cr(d, p)53Cr reaction

doi: 10.1103/PhysRevC.108.044306
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2023TE05      Phys.Rev. C 108, 065804 (2023)

E.Temanson, J.Baker, L.T.Baby, K.Hanselman, P.Hoflich, S.A.Kuvin, G.W.McCann, A.Volya, I.Wiedenhover

Measurement of the 25Al(d, n)26Si reaction and impact on the 25Al(p, γ)26Si reaction rate

doi: 10.1103/PhysRevC.108.065804
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022PE02      Phys.Rev. C 105, 035805 (2022)

J.F.Perello, S.Almaraz-Calderon, B.W.Asher, L.T.Baby, C.Benetti, K.W.Kemper, E.Lopez-Saavedra, G.W.McCann, A.B.Morelock, V.Tripathi, I.Wiedenhover, B.Sudarsan

Low-lying resonances in 26Si relevant for the determination of the astrophysical 25Al(p, γ)26Si reaction rate

NUCLEAR REACTIONS 24Mg(3He, n), E=10 MeV; measured ToF, En, In, Eγ, Iγ, nγ-coin. 26Si; deduced levels, J, π, partial decay widths. 25Al(p, γ), T=0.01-1 GK; deduced proton capture rate using newly observed states in 26Si, contribution of individual resonances to the total reaction rate. Comparison to reaction rate values from JINA REACLIB database. CATRiNA neutron detector array (16 deuterated liquid scintillators) combined with 3 HPGe clover detectors.

doi: 10.1103/PhysRevC.105.035805
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022RI07      Phys.Rev. C 106, 064308 (2022)

L.A.Riley, I.C.S.Hay, L.T.Baby, A.L.Conley, P.D.Cottle, J.Esparza, K.Hanselman, B.Kelly, K.W.Kemper, K.T.Macon, G.W.McCann, M.W.Quirin, R.Renom, R.L.Saunders, M.Spieker, I.Wiedenhover

54Fe(d, p)55Fe and the evolution of single neutron energies in the N=29 isotones

NUCLEAR REACTIONS 54Fe(d, p), E=16 MeV; measured Ep, Ip, angular distribution. 55Fe; deduced levels, J, π, spectroscopic factors, single-neutron energies for the 2p3/2, 2p1/2, 1f5/2, 1g9/2 and 2d5/2 orbits, spin-orbit splitting. Comparison with calculations made in the framework of covariant density functional theory using the covariant energy density functional FSUGarnet. Systematics of single-neutron energy for N=28 isotones (49Ca, 51Ti, 53Cr, 55Fe, 57Ni). Super-Enge Split-Pole Spectrograph at 9MV Super FN Tandem Van de Graaff Accelerator at the John D. Fox Laboratory (FSU).

doi: 10.1103/PhysRevC.106.064308
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021RI08      Phys.Rev. C 103, 064309 (2021)

L.A.Riley, J.M.Nebel-Crosson, K.T.Macon, G.W.McCann, L.T.Baby, D.Caussyn, P.D.Cottle, J.Esparza, K.Hanselman, K.W.Kemper, E.Temanson, I.Wiedenhover

50Ti(d, p)51Ti: Single-neutron energies in the N=29 isotones, and the N=32 subshell closure

NUCLEAR REACTIONS 50Ti(d, p)51Ti, E=16 MeV; measured E(p), I(p), σ(θ) using the Super Enge Split-Pole Spectrograph (SPS) spectrometer at the J. D. Fox Laboratory at Florida State University. 51Ti; deduced levels, J, L-transfers, spectroscopic factors, s3/2, s1/2, and d5/2 single-neutron energy centroids and compared with covariant density functional theory calculations. Adiabatic distorted wave approximation (ADW) and DWBA calculations using global optical potentials.

doi: 10.1103/PhysRevC.103.064309
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2638. Data from this article have been entered in the XUNDL database. For more information, click here.


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