NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.W.Arrison Found 11 matches. 1996RE18 Phys.Rev. C54, 1084 (1996) P.H.Regan, J.W.Arrison, U.J.Huttmeier, D.P.Balamuth Yrast γ-Ray Spectroscopy of the Neutron Rich Isotopes 61,63Co NUCLEAR REACTIONS 16,18O(48Ca, 2np), E=110 MeV; measured Eγ, Iγ, (particle)γ-, (particle)γγ-coin, DSA, γ(θ). 61,63Co deduced high-spin levels, J, π, T1/2, B(λ). Other nuclei considered.
doi: 10.1103/PhysRevC.54.1084
1995PO01 Phys.Rev. C51, 519 (1995) K.R.Pohl, D.F.Winchell, J.W.Arrison, D.P.Balamuth Isomeric Transitions in 69Se and the Spin of the Ground State NUCLEAR REACTIONS 40Ca(32S, n2p), E=96 MeV; measured (particle)γ(t), γγ(t), γ(θ), Eγ, Iγ. 69Se deduced high-spin levels, isomer T1/2, decay features, ICC, γ-multipolarity.
doi: 10.1103/PhysRevC.51.519
1994PO03 Phys.Rev. C49, 1372 (1994) K.R.Pohl, P.H.Regan, J.W.Arrison, D.P.Balamuth Origin of Correlations between Evaporation Protons and Discrete γ Rays in Heavy-Ion Fusion-Evaporation Reactions NUCLEAR REACTIONS 58Ni(27Al, 3p), E=92, 100 MeV; 58Ni(28Si, 4p), E=115 MeV; measured pγ-coin; deduced correlations features between p-, γ-emission.
doi: 10.1103/PhysRevC.49.1372
1993BA62 Phys.Rev. C48, 2648 (1993) D.P.Balamuth, U.J.Huttmeier, J.W.Arrison In-Beam γ-Ray Spectroscopy of 40Cl NUCLEAR REACTIONS 9Be(36S, pα), E=105 MeV; measured γγ(particles)-coin, Iγ; deduced residual production σ. 40Cl deduced levels, possible J, π. Model comparison.
doi: 10.1103/PhysRevC.48.2648
1991BA20 Phys.Rev. C43, 2082 (1991) D.P.Balamuth, U.J.Huttmeier, T.Chapuran, D.G.Popescu, J.W.Arrison In-Beam γ-Ray Spectroscopy of the N = Z + 1 Nucleus 63Ga NUCLEAR REACTIONS 40Ca(28Si, pα); 40Ca(32S, p2α); 40Ca(29Si, npα), E=80-100 MeV; measured αpγ-coin, nγ(θ), nγγ(θ). 63Ga deduced levels, Jπ, δ, branching ratios.
doi: 10.1103/PhysRevC.43.2082
1990AR23 Phys.Lett. 248B, 39 (1990) J.W.Arrison, T.Chapuran, U.J.Huttmeier, D.P.Balamuth Electromagnetic Transitions in the N = Z + 1 Nucleus 71Br NUCLEAR REACTIONS 40Ca(34S, 2np), (35Cl, 2n2p), E not given; 58Ni(16O, 2np), E=70 MeV; measured γγ-, γp-, γn-coin, Eγ, Iγ, γγ(θ), nγγ-coin. 71Br deduced levels, J, π.
doi: 10.1016/0370-2693(90)90011-T
1989AR13 Phys.Rev. C40, 2010 (1989) J.W.Arrison, D.P.Balamuth, T.Chapuran, D.G.Popescu, J.Gorres, U.J.Huttmeier Structure of the N = Z + 1 Nucleus 69Se NUCLEAR REACTIONS 40Ca(32S, n2p), E=101 MeV; measured pγ-, γγ-, nγγ-, pnγ-coin, γ(θ). 69Se deduced levels, T1/2, possible J, π, δ.
doi: 10.1103/PhysRevC.40.2010
1989BA13 Nucl.Instrum.Methods Phys.Res. A275, 315 (1989) D.P.Balamuth, T.Chapuran, J.W.Arrison Applications of Complete Reconstruction of Multi-Particle Final States in Fusion-Evaporation Reactions Using a 4π Detector NUCLEAR REACTIONS 60Ni(27Al, xp), E=80 MeV; 58Ni(28Si, xp), E=108 MeV; measured pγ-coin. 4π detector, single, multiple protons.
doi: 10.1016/0168-9002(89)90703-1
1988CH41 Nucl.Instrum.Methods Phys.Res. A272, 767 (1988) T.Chapuran, D.P.Balamuth, J.W.Arrison, J.Gorres Channel Selection for In-Beam γ-Ray Spectroscopy Using a 4π Phoswich Array NUCLEAR REACTIONS 60Ni(27Al, Xγ), E=80 MeV; measured Eγ, Iγ, γ(fragment)-coin. 4π array for in-beam γ-spectroscopy.
doi: 10.1016/0168-9002(88)90759-0
1988MA20 Phys.Rev. C37, 1926 (1988) R.Ma, E.S.Paul, S.Shi, C.W.Beausang, W.F.Piel, Jr., N.Xu, D.B.Fossan, T.Chapuran, D.P.Balamuth, J.W.Arrison Band Structure in Doubly Odd 130Pr NUCLEAR REACTIONS 110Cd(28Si, 3npα), E=160 MeV; 106Pd(31P, 3nα), E=155 MeV; measured Eγ, Iγ, γγ(θ), γα-, γp-coin. 130Pr deduced levels, J, π, B(M1)/B(E2) ratios, configuration. Cranked shell model analysis.
doi: 10.1103/PhysRevC.37.1926
1987GO02 Phys.Rev.Lett. 58, 662 (1987) J.Gorres, T.Chapuran, D.P.Balamuth, J.W.Arrison Structure of the Very Neutron-Deficient Ge Region: 64Ge and 65Ge NUCLEAR REACTIONS 40Ca(28Si, n2p), E=60-100 MeV; measured (particle)γ-, (particle)γγ-coin, γ(θ). 65Ge deduced levels. 27Al(40Ca, 2np), E=102 MeV; measured γn-, (particle)γ-coin. 64Ge deduced levels, transition energies, Iγ. Ge, 4π multi-segment detectors.
doi: 10.1103/PhysRevLett.58.662
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