NSR Query Results

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NSR database version of April 26, 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
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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 g_9/2 strength in the stretched 8^- state and other negative parity states via the ⁵¹V(d, p)⁵²V reaction

doi: 10.1103/PhysRevC.109.024302
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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

g_9/2 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 2p_3/2, 2p_1/2, 1f_5/2, 1g_9/2 and 2d_5/2 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, s_3/2, s_1/2, and d_5/2 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.