NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = N.M.Stewart Found 33 matches. 1996RA44 Z.Phys. A356, 145 (1996) An IBM Description of 76Se and Neighbouring Se-Isotopes NUCLEAR STRUCTURE 72,74,76,78,80Se; calculated levels, B(λ). Interacting boson models.
doi: 10.1007/s002180050161
1996ST16 Z.Phys. A354, 261 (1996) Negative-Parity States of 75As and the Interacting Boson-Fermion Model NUCLEAR STRUCTURE 75As; calculated levels, δ, B(λ), electric quadrupole, magnetic dipole moments, transition Iγ. Single proton coupled to 74Ge core, interacting boson-fermion model. 74Ge; calculated levels, B(λ). Interacting boson model. RADIOACTIVITY 75Se(EC) [from Se(n, X)]; measured Eγ, Iγ, γγ-coin. 75As deduced transitions B(E2), B(M1), δ.
doi: 10.1007/s002180050043
1994ST05 Z.Phys. A348, 9 (1994) N.M.Stewart, N.I.Fawwaz, F.S.Radhi Interacting Boson-Fermion Model Analysis for 159Tb NUCLEAR STRUCTURE 159Tb; calculated levels, B(λ), δ, ICC, μ, quadrupole moment. Interacting boson-fermion model. RADIOACTIVITY 159Gd(β-) [from 158Gd thermal neutron irradiation]; measured Eγ, Iγ, γγ-coin. 159Tb levels deduced B(λ), δ, ICC. Interacting boson-fermion model comparison.
doi: 10.1007/BF01291646
1993FA02 J.Phys.(London) G19, 113 (1993) Interacting Boson-Fermion Model Description of the Odd-Mass 125Te Nucleus NUCLEAR STRUCTURE 125Te; calculated levels, B(λ), μ, quadrupole moments, δ. Interacting boson model. RADIOACTIVITY 125Sb(β-); measured Iγ. 125Te deduced levels, J, π, quadrupole moment, μ, δ, ICC, B(λ). Interacting boson model.
doi: 10.1088/0954-3899/19/1/008
1990JA02 J.Phys.(London) G16, 271 (1990) An Improved Description of 182W RADIOACTIVITY 182Ta(β-); measured Eγ, Iγ, γγ-coin. 182W deduced levels, B(λ), J, π. Interacting boson model calculations. NUCLEAR STRUCTURE 182W; calculated levels, B(λ). Interacting boson model.
doi: 10.1088/0954-3899/16/2/016
1990ST02 Z.Phys. A335, 13 (1990) N.M.Stewart, E.Eid, M.S.S.El-Daghmah, J.K.Jabber Levels in 152Gd and 152Sm Populated by the Decay of 152Eu RADIOACTIVITY 152Eu(β-), (β+), (EC) [from 151Eu neutron irradiation]; measured Eγ, Iγ, γγ-coin; deduced log ft. 152Gd, 152Sm deduced levels, J, π, B(λ). Interacting boson model.
1988SH06 Phys.Rev.Lett. 60, 901 (1988) R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis Evidence against Broad Dibaryons NUCLEAR REACTIONS 1H(polarized p, π+n), E=492-796 MeV; measured spin correlation parameters; deduced no broad dibaryons. Isobar analysis.
doi: 10.1103/PhysRevLett.60.901
1988SH09 Nucl.Phys. A477, 541 (1988) R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis A(SL), A(LL) and A(N0) for NN → πD at 492, 729 and 796 MeV NUCLEAR REACTIONS 1H(polarized p, π+), E=492-796 MeV; measured spin correlation parameters A(LL), A(SL), A(N0). Longitudinally polarized propanediol target.
doi: 10.1016/0375-9474(88)90404-6
1985EI01 Z.Phys. A320, 495 (1985) Studies of the Low-Lying Levels in 192Pt and 192Os RADIOACTIVITY 192Ir(β-), (EC) [from Ir thermal neutron irradiation]; measured Eγ, Iγ, γγ-coin; deduced log ft, EC-, β-branching ratios. 192Os, 192Pt deduced levels, ICC, γ-multipolarity, J, π, γ-branching, B(E2).
doi: 10.1007/BF01415728
1984MA13 Z.Phys. A315, 213 (1984) Low Energy Nuclear States in 124Te RADIOACTIVITY 124Sb(β-) [from 123Sb(n, γ), E=thermal]; measured Eγ, Iγ, γγ-coin; deduced log ft. 124Te deduced levels, J, π, ICC, γ-multipolarity, relative Iγ, B(E2) ratios. Interacting boson model calculations.
doi: 10.1007/BF01419382
1983EL02 Z.Phys. A309, 219 (1983) Levels and Transitions in 182W following the Decay of 182Ta RADIOACTIVITY 182Ta(β-) [from 181Ta(n, γ), E=reactor]; measured γγ-coin, Eγ, Iγ, γγ(t); deduced log ft. 182W deduced levels, Iγ, subshell ICC, γ-multipolarity, J, π, B(λ), T1/2. Dual parameter energy time spectrometer, high resolution Ge(Li) detectors.
doi: 10.1007/BF01413753
1983IB01 J.Phys.(London) G9, L195 (1983) Retarded Dissipation of the Z = 64 Shell Gap in 16066Dy94 NUCLEAR STRUCTURE 160Dy; calculated levels, B(E2) branching ratios; deduced proton subshell closure effects. Interacting boson model.
doi: 10.1088/0305-4616/9/9/003
1983ST08 Nucl.Phys. A403, 525 (1983) J.P.Stanley, N.M.Stewart, D.V.Bugg, J.A.Edgington, N.R.Stevenson, A.S.Clough, D.A.Axen, R.Shypit, M.Comyn, D.Healey, G.A.Ludgate Measurements of Δσ(L) and Δσ(T) in pp Scattering between 200 and 520 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=200, 520 MeV; measured spin-dependent σ differences. Longitudinal, transverse beam polarization, polarized target.
doi: 10.1016/0375-9474(83)90621-8
1982DU03 Nucl.Phys. A377, 554 (1982) R.Dubois, D.Axen, R.Keeler, M.Comyn, G.A.Ludgate, J.R.Richardson, N.M.Stewart, A.S.Clough, D.V.Bugg, J.A.Edgington Nucleon-Nucleon Phase Shifts from 142 to 800 MeV NUCLEAR REACTIONS 1H(n, n), E=120-550 MeV; 1H(p, p), E=120-831 MeV; analyzed σ(total), σ(θ); deduced unique set of phase shifts.
doi: 10.1016/0375-9474(82)90055-0
1982KE02 Nucl.Phys. A377, 529 (1982) R.K.Keeler, R.Dubois, E.G.Auld, D.A.Axen, M.Comyn, G.Ludgate, L.P.Robertson, J.R.Richardson, D.V.Bugg, J.A.Edgington, W.R.Gibson, A.S.Clough, N.M.Stewart, B.Dieterle Neutron-Proton Scattering Cross Sections between 200 and 500 MeV NUCLEAR REACTIONS 1H(n, n), E=212, 268, 319, 369, 417, 495 MeV; measured σ(total), σ(θ). Liquid hydrogen target, transmission method.
doi: 10.1016/0375-9474(82)90054-9
1981AX01 J.Phys.(London) G7, L225 (1981) D.Axen, R.Shypit, M.Comyn, D.Healey, J.Stanley, N.M.Stewart, D.V.Bugg, J.A.Edgington, N.Stevenson Δσ(L) and Δσ(T) between 200 amd 520 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=200-520 MeV; measured σ(total), σ(transverse), σ(longitudinal) differences. Transmission method, polarized beam, polarized target.
doi: 10.1088/0305-4616/7/10/003
1980AX01 Phys.Rev. C21, 998 (1980) D.Axen, R.Dubois, R.Keeler, G.A.Ludgate, C.J.Oram, L.P.Robertson, N.M.Stewart, C.Amsler, D.V.Bugg, J.A.Edgington, W.R.Gibson, N.Wright, A.S.Clough Neutron-Proton Elastic Scattering between 200 and 500 MeV. II. Measurement of R(t) and A(t) NUCLEAR REACTIONS 1H(polarized n, p), E=220, 325, 425, 495 MeV; measured P(θp); deduced parameters Rt(θ), At(θ).
doi: 10.1103/PhysRevC.21.998
1980BU03 Phys.Rev. C21, 1004 (1980) D.V.Bugg, J.A.Edgington, W.R.Gibson, N.Wright, N.M.Stewart, A.S.Clough, D.Axen, G.A.Ludgate, C.J.Oram, L.P.Robertson, J.R.Richardson, C.Amsler Neutron-Proton Elastic Scattering between 200 and 500 MeV. III. Phase Shift Analysis NUCLEAR REACTIONS 1H(n, n), E=210, 325, 425, 515 MeV; calculated σ(θ). Phase shift analysis.
doi: 10.1103/PhysRevC.21.1004
1980CL02 Phys.Rev. C21, 988 (1980) A.S.Clough, D.R.Gibson, D.Axen, R.Dubois, L.Felawka, R.Keeler, G.A.Ludgate, C.J.Oram, C.Amsler, D.V.Bugg, J.A.Edgington, L.P.Robertson, N.M.Stewart, J.Beveridge, J.R.Richardson Neutron-Proton Elastic Scattering between 200 and 500 MeV. I. Experimental Details and Measurements of the D(t) and P Parameters NUCLEAR REACTIONS 1H(polarized n, p), E=220, 325, 425, 495 MeV; measured analyzing power, polarization transfer vs θ.
doi: 10.1103/PhysRevC.21.988
1980ST20 Z.Phys. A296, 165 (1980) Low Lying Energy Levels of 56Fe from γ-γ Coincidences RADIOACTIVITY 56Co [from 56Fe(p, n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 56Fe deduced levels, ICC, J, π, γ-multipolarity.
doi: 10.1007/BF01412657
1979SH16 Nucl.Instrum.Methods 165, 109 (1979) A.M.Shaban, N.M.Stewart, T.D.Macmahon Relative Intensities of Gamma Transitions in the Decay of 56Co RADIOACTIVITY 56Co measured Eγ, Iγ. Ge(Li) detectors.
doi: 10.1016/0029-554X(79)90313-6
1978AM07 Nucl.Instrum.Methods 157, 203 (1978) C.Amsler, R.C.Brown, D.V.Bugg, J.A.Edgington, C.Oram, D.Axen, R.Dubois, L.Felawka, S.Jaccard, R.Keeler, J.Vavra, A.Clough, D.Gibson, G.A.Ludgate, N.M.Stewart, L.P.Robertson, J.R.Richardson A Monoenergetic Polarized Neutron Beam from 200 to 500 MeV NUCLEAR REACTIONS 2H(polarized p, n), E=237, 343, 445, 516 MeV; measured polarization of n, polarization transfer R.
doi: 10.1016/0029-554X(78)90608-0
1978ON02 Nucl.Phys. A304, 51 (1978) Y.Onel, R.C.Brown, J.A.Edgington, N.M.Stewart, I.M.Blair Further Study of the Reaction 2H(n, p2n) Near 120 MeV NUCLEAR REACTIONS 2H(n, 2np), E=120 MeV; measured σ(En1, En2); deduced n-n scattering length. Kinematically complete experiment, scintillating target.
doi: 10.1016/0375-9474(78)90095-7
1977AX01 Lett.Nuovo Cim. 20, 151 (1977) D.Axen, L.Felawka, S.Jaccard, J.Vavra, G.A.Ludgate, N.M.Stewart, C.Amsler, R.C.Brown, D.V.Bugg, J.A.Edgington, C.J.Oram, K.Shakarchi, A.S.Clough D, R, R' and P in pp Elastic Scattering from 209 to 515 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=209-515 MeV; measured scattering parameters.
doi: 10.1007/BF02785134
1975MC05 Nucl.Phys. A239, 29 (1975) M.W.McNaughton, R.J.Griffiths, I.M.Blair, B.E.Bonner, J.A.Edgington, M.P.May, N.M.Stewart The 2H(n, np)n Reaction at 130 MeV. Differential Cross Sections from Kinematically Complete Data over a Wide Range of Phase Space NUCLEAR REACTIONS 2H(n, np), E=130 MeV; measured σ(En, Ep, θ(n), θ(p)); deduced n-n scattering length. Liquid 2H target.
doi: 10.1016/0375-9474(75)91131-8
1974HO01 Nucl.Phys. A218, 140 (1974) V.J.Howard, J.A.Edgington, S.S.Das Gupta, I.M.Blair, B.E.Bonner, F.P.Brady, M.W.McNaughton, N.M.Stewart Differential Cross Sections for np and nd Elastic Scattering Near 130 MeV NUCLEAR REACTIONS 1H(n, np), 2H(n, nd), E=130 MeV; measured σ(θ).
doi: 10.1016/0375-9474(74)90026-8
1972ST12 Nucl.Phys. A188, 205 (1972) Triple Scattering Measurements for the Proton-Deuteron System NUCLEAR REACTIONS 2H(polarized p, p), E=48.3 MeV; measured Wolfenstein parameter a(θ). Enriched target.
doi: 10.1016/0375-9474(72)90195-9
1971SQ01 Nucl.Phys. A160, 602 (1971) G.T.A.Squier, A.R.Johnston, E.W.Spiers, S.A.Harbison, N.M.Stewart Cross-Section Measurements for the Reaction 10B(p, 3He)8Be NUCLEAR REACTIONS 10B(p, 3He), E=49.5 MeV; measured σ(E(3He), θ). Enriched target.
doi: 10.1016/0375-9474(71)90100-X
1971ST17 Nucl.Phys. A171, 225 (1971) N.M.Stewart, W.R.Gibson, F.G.Kingston Depolarization Measurements in the Elastic Scattering of Protons by Deuterons NUCLEAR REACTIONS 2H(polarized p, p)2H, E=48.3 MeV; measured depolarization d(θ). Enriched target.
doi: 10.1016/0375-9474(71)90019-4
1971ST25 Nucl.Phys. A174, 338 (1971) N.M.Stewart, W.R.Gibson, J.H.P.C.Megaw A Measurement of the Rotation Parameter R in Proton-Deuteron Scattering NUCLEAR REACTIONS 2H(polarized p, p), E=48.3 MeV; measured rotation parameter.
doi: 10.1016/0375-9474(71)90666-X
1970HA25 Nucl.Phys. A150, 570 (1970) S.A.Harbison, R.J.Griffiths, N.M.Stewart, A.R.Johnston, G.T.A.Squier An Analysis of Polarization and Cross-Section Data for the p-3He System at 30 and 50 MeV NUCLEAR REACTIONS 3He(p, p), E=50 MeV; measured P(θ); E=30, 50 MeV; measured σ(θ); deduced phase shifts. Enriched gas target.
doi: 10.1016/0375-9474(70)90418-5
1970HA36 Nucl.Phys. A152, 503 (1970) S.A.Harbison, R.J.Griffiths, N.M.Stewart, A.R.Johnston, G.T.A.Squier An Analysis of the Angular Distributions of the Reactions 4He(p, d)3He, 4He(p, t)2p, 4He(p, 3He)pn and 3He(p, d)2p NUCLEAR REACTIONS 4He(p, d), E=49.5 MeV; measured σ(θ). 4He(p, t), (p, 3He), 3He(p, d), E=49.5 MeV; 3He(p, d), E=30.5 MeV; analysed σ(θ).
doi: 10.1016/0375-9474(70)90928-0
1970SQ01 Nucl.Phys. A141, 158 (1970) G.T.A.Squier, A.R.Johnston, E.W.Spiers, S.A.Harbison, N.M.Stewart Cross-Section Measurements for the Reactions 10B(p, d)9B and 10B(p, t)8B NUCLEAR REACTIONS 10B(p, d), (p, t), (p, p), E=49.5 MeV; measured σ(Ed, θ), σ(Et, θ). 8,9B deduced levels, J. Enriched target.
doi: 10.1016/0375-9474(70)90301-5
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