NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Nurzynski Found 49 matches. 1988HE06 Nucl.Phys. A481, 161 (1988) D.F.Hebbard, J.Nurzynski, T.R.Ophel, P.V.Drumm, Y.Kondo, B.A.Robson, R.Smith The 20Ne(16O, 16O)20Ne Excitation Function at θ(cm) = 90° and Parity-Dependent Interactions NUCLEAR REACTIONS 20Ne(16O, 16O), (16O, 16O'), E(cm)=21.5-31.2 MeV; measured σ(E); deduced optical model parameters. 36Ar resonances deduced parity. Extended optical model analysis.
doi: 10.1016/0375-9474(88)90478-2
1987NU01 Nucl.Phys. A465, 365 (1987) J.Nurzynski, T.Kihm, K.T.Knopfle, G.Mairle, H.Clement Reorientation Effects for 52 MeV Vector Polarized Deuterons NUCLEAR REACTIONS 20,22Ne, 26Mg, 28Si, 32,34S, 36,40Ar(polarized d, d), (polarized d, d'), E=52 MeV; measured σ(θ), iT11(θ); deduced optical model parameters. 20,22Ne, 26Mg, 28Si, 32,34S, 36,40Ar levels deduced β2. Natural 28Si, 32S, 40Ar targets, 20,22Ne, 26Mg, 34S, 36Ar enriched targets.
doi: 10.1016/0375-9474(87)90353-8
1987NU03 Nucl.Phys. A474, 285 (1987) J.Nurzynski, W.Gruebler, V.Konig, P.A.Schmelzbach Effects of Collective Excitations in the Elastic Scattering of Vector Polarized Deuterons NUCLEAR REACTIONS, MECPD 40Ar, 46,48,50Ti, 52,54Cr, 54,56Fe, 58,60Ni, 76,78,80,82Se, 90Zr(polarized d, d), E=12 MeV; analyzed σ(θ), iT11(θ) data; deduced optical model parameters. Coupled-channel analysis.
doi: 10.1016/0375-9474(87)90618-X
1986DR11 Aust.J.Phys. 39, 369 (1986) P.V.Drumm, D.F.Hebbard, T.R.Ophel, J.Nurzynski, Y.Kondo, B.A.Robson, R.Smith Excitation Function for 16O + 24Mg Elastic Scattering at θ(c.m.) = 90° NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), E=53-75.5 MeV; measured σ(E(16O)), σ(θ) vs E. Enge split-pole magnetic spectrometer. Optical model analysis.
doi: 10.1071/PH860369
1986NU01 J.Phys.(London) G12, 383 (1986) J.Nurzynski, D.F.Hebbard, T.R.Ophel, Y.Kondo, B.A.Robson, R.Smith Excitation Functions for 24Mg(16O, 16O')24Mg(*) (0 ≤ E(x) ≤ 8.4 MeV) Scattering at Forward Angles NUCLEAR REACTIONS 24Mg(16O, 16O'), E(cm)=33.6-49.2 MeV; measured σ(E(16O)), σ(θ) vs E. 16O, 24Mg levels deduced possible excitation. Enriched target, magnetic spectrometer. Coupled channels calculations.
doi: 10.1088/0305-4616/12/5/005
1983NU01 Nucl.Phys. A399, 259 (1983) J.Nurzynski, C.H.Atwood, T.R.Ophel, D.F.Hebbard, B.A.Robson, R.Smith The 24Mg(16O, 16O') Reaction and Triaxial Structures in 24Mg NUCLEAR REACTIONS 24Mg(16O, 16O'), E=43.5 MeV; measured σ(θ); deduced optical model parameters. 24Mg levels deduced B(E2), quadrupole moment, β4/β2, shape parameters. Asymmetric rotor model, coupled-channels analysis.
doi: 10.1016/0375-9474(83)90607-3
1982EC01 Phys.Rev. C25, 2391 (1982) J.S.Eck, T.R.Ophel, P.D.Clark, J.Nurzynski, D.C.Weisser Optical Model and Coupled-Channels Analysis of 7Li + 28Si and 7Li + 40Ca Scattering NUCLEAR REACTIONS 28Si, 40Ca(7Li, 7Li), (7Li, 7Li'), E=45 MeV; measured σ(θ); deduced optical model parameters. 40Ca deduced deformation length. Double folding model, coupled-channels calculations.
doi: 10.1103/PhysRevC.25.2391
1981CL01 Nucl.Phys. A352, 267 (1981) P.D.Clark, T.R.Ophel, J.Nurzynski, C.H.Atwood, D.F.Hebbard Spin Assignments from the 142Nd(7Li, 6He)143Pm and 144Sm(7Li, 6He)145Eu Reactions at 52 MeV NUCLEAR REACTIONS 142Nd, 144Sm(7Li, 7Li), (7Li, 6He), E=52 MeV; 142Nd(6Li, 6Li), E=46 MeV; 144Sm(6Li, 6Li), E=45 MeV; measured σ(θ); deduced optical-model parameters. 143Pm, 145Eu levels deduced S, J, π. Enriched targets, finite-range DWBA analysis.
doi: 10.1016/0375-9474(81)90380-8
1981EC02 Phys.Rev. C23, 2068 (1981) J.S.Eck, J.Nurzynski, T.R.Ophel, P.D.Clark, D.F.Hebbard, D.C.Weisser Possible Triaxial Structures in 24Mg from 16O + 24Mg Elastic and Inelastic Scattering NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), E=67 MeV; measured σ(θ). Triaxial rotor model, coupled-channels analysis.
doi: 10.1103/PhysRevC.23.2068
1981NU01 Nucl.Phys. A359, 61 (1981) J.Nurzynski, W.Gruebler, H.R.Burgi, V.Konig, R.Risler, B.Jenny A Study of the Second-Order Processes in the Elastic Scattering of Polarized Deuterons NUCLEAR REACTIONS 76,78,80,82Se(polarized d, d), E=12 MeV; analyzed σ(θ), iT11(θ). CCBA, two-step processes.
doi: 10.1016/0375-9474(81)90211-6
1981NU02 Nucl.Phys. A363, 253 (1981) J.Nurzynski, T.R.Ophel, P.D.Clark, J.S.Eck, D.F.Hebbard, D.C.Weisser, B.A.Robson, R.Smith Energy Dependence of the 24Mg(16O, 12C)28Si Reaction NUCLEAR REACTIONS 24Mg(16O, 12C), E=32.4-48.6 MeV; measured σ(E, θ); 24Mg(16O, 16O), E=37.5, 40.2 MeV; measured σ(θ); deduced optical model parameters. 40Ca resonances deduced J. DWBA analysis, band crossing model.
doi: 10.1016/0375-9474(81)90465-6
1980BU02 Nucl.Phys. A334, 413 (1980) H.R.Burgi, W.Gruebler, J.Nurzynski, V.Konig, P.A.Schmelzbach, R.Risler, B.Jenny, R.A.Hardekopf Global Optical-Model Analysis of the Elastic Deuteron Scattering from Medium Heavy Target Nuclei NUCLEAR REACTIONS 46,48,50Ti, 52,54Cr, 54,56Fe, 58Ni, 76,78,80,82Se(polarized d, d), E=12 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced optical-model parameters. Enriched targets.
doi: 10.1016/0375-9474(80)90608-9
1980CL08 Nucl.Phys. A349, 258 (1980) P.D.Clark, T.R.Ophel, J.S.Eck, A.F.Zeller, J.Nurzynski, D.C.Weisser, D.F.Hebbard Spin Assignments from the 138Ba(7Li, 6He)139La and 140Ce(7Li, 6He)141Pr Reactions at 52 MeV NUCLEAR REACTIONS 138Ba, 140Ce(7Li, 7Li), (7Li, 6He), E=52 MeV; 139La(6Li, 6Li), E=48 MeV; 141Pr(6Li, 6Li), E=47 MeV; measured σ(θ); deduced optical model parameters. 139La, 141Pr levels deduced S, J, π. Enriched targets. Finite-range DWBA analysis.
doi: 10.1016/0375-9474(80)90453-4
1980GR03 Nucl.Phys. A334, 365 (1980) W.Gruebler, V.Konig, P.Schmelzbach, B.Jenny, H.R.Burgi, R.A.Hardekopf, J.Nurzynski, R.Risler, G.Heidenreich, F.Seiler, H.Roser A Study of the Highly Excited Six Nucleon System by Elastic d-α Scattering with Polarized Deuterons between 17 and 43 MeV NUCLEAR REACTIONS 4He(polarized d, d), E=17.0, 20.2, 24.0, 28.0, 33.0, 38.2, 42.8 MeV; measured vector, tensor A(θ, E).
doi: 10.1016/0375-9474(80)90604-1
1980NU01 J.Phys.(London) G6, L81 (1980) J.Nurzynski, W.Gruebler, H.R.Burgi, V.Konig, R.Risler, B.Jenny Two-Step Mechanism in Deuteron Polarisation NUCLEAR REACTIONS 76,78,80,82Se(polarized d, d), E(lab)=12 MeV; measured σ(θ), T11(θ); deduced optical-model parameters.
doi: 10.1088/0305-4616/6/1/015
1979BA61 Nucl.Phys. A331, 502 (1979) L.O.Barbopoulos, D.W.Gebbie, J.Nurzynski, M.Borsaru, C.L.Hollas Single-Neutron Transfer Reactions 76,78,80,82Se(p, d)75,77,79,81Se at E = 33 MeV NUCLEAR REACTIONS 76,78,80,82Se(p, d), E=33 MeV; measured σ(Ed, θ), Q. 75,77,79,81Se deduced levels, L, S. Enriched targets.
doi: 10.1016/0375-9474(79)90356-7
1979BU07 Nucl.Phys. A321, 445 (1979) H.R.Burgi, W.Gruebler, J.Nurzynski, V.Konig, P.A.Schmelzbach, R.Risler, B.Jenny, R.A.Hardekopf A Study of the Elastic Scattering of Polarized Deuterons from 60Ni and 90Zr Nuclei NUCLEAR REACTIONS 60Ni(polarized d, d), E=9, 12 MeV; 90Zr(polarized d, d), E=10, 11, 12 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ), σ(E, θ=175°), T20(175°); deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(79)90137-4
1979BU18 Helv.Phys.Acta 52, 421 (1979) H.R.Burgi, W.Gruebler, J.Nurzynski, V.Konig, P.A.Schmelzbach, R.Risler, B.Jenny, R.A.Hardekopf Optisches Modell fur die elastische Deuteronstreuung NUCLEAR STRUCTURE A=40-90; analyzed σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ) of (pold, d) reaction. Optical, coupled-channel model.
1979RI03 Nucl.Phys. A315, 310 (1979) R.Risler, W.Gruebler, P.A.Schmelzbach, B.Jenny, V.Konig, J.Nurzynski, H.R.Burgi Search for Ay = 1 and Ayy = 1 Points in the 6Li(d, α)4He Reaction NUCLEAR REACTIONS 6Li(polarized d, α), E=5.0-6.5, 8.0-10.0 MeV; measured Ay(θ, E), Ayy(θ, E).
doi: 10.1016/0375-9474(79)90613-4
1978AN10 Nucl.Phys. A303, 154 (1978) K.A.Aniol, D.W.Gebbie, C.L.Hollas, J.Nurzynski The 50, 52, 54Cr(α, p)53, 55, 57Mn Reactions at E = 18 and 26 MeV NUCLEAR REACTIONS 50,52,54Cr(α, p), E=18, 26 MeV; measured σ(Ep, θ); deduced Q. 53,55,57Mn deduced levels, J, π, L, relative strengths. Enriched targets.
doi: 10.1016/0375-9474(78)90049-0
1977BO18 Nucl.Phys. A284, 379 (1977) M.Borsaru, D.W.Gebbie, J.Nurzynski, C.L.Hollas, L.O.Barbopoulos, A.R.Quinton A Study of the 78,76Se(p, t)76,74Se Reactions at E = 33 MeV NUCLEAR REACTIONS 78,76Se(p, t), E=33 MeV; measured σ(Et, θ). 76,74Se deduced levels, J, π, L, enhancement coefficients. Enriched targets.
doi: 10.1016/0375-9474(77)90391-8
1977HA34 Nucl.Phys. A287, 237 (1977) R.A.Hardekopf, W.Gruebler, B.Jenny, V.Konig, R.Risler, H.R.Burgi, J.Nurzynski Investigation of the 1+ Resonance in 6Li by d-α Scattering between 6 and 7 MeV NUCLEAR REACTIONS 4He(polarized d, d), E=6.04-7.05 MeV; measured σ(θ), A(θ); deduced phase shifts. 6Li deduced resonance parameters.
doi: 10.1016/0375-9474(77)90494-8
1977HO02 Nucl.Phys. A276, 1 (1977) C.L.Hollas, K.A.Aniol, D.W.Gebbie, M.Borsaru, J.Nurzynski, L.O.Barbopoulos States in 97,101Ru Observed in the Reactions 96,100Ru(d, p) NUCLEAR REACTIONS 96,100Ru(d, p), E=11.5 MeV; measured σ(Ep, θ); deduced Q. 97,101Ru deduced levels, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(77)90155-5
1977NU02 Phys.Lett. 67B, 23 (1977) J.Nurzynski, W.Gruebler, V.Konig, R.Risler, R.A.Hardekopf, H.R.Burgi, B.Jenny Shell Closure Effects in the Elastic Scattering of Polarized Deuterons NUCLEAR REACTIONS 76,78,80,82Se(polarized d, d), E=12 MeV; measured A(θ); deduced shell closure effects.
doi: 10.1016/0370-2693(77)90794-8
1976GR08 Phys.Lett. 63B, 273 (1976) W.Gruebler, P.A.Schmelzbach, V.Konig, B.Jenny, R.Risler, H.R.Burgi, J.Nurzynski Maximum Tensor Analysing Power A(yy) = 1 in Nuclear Reactions NUCLEAR REACTIONS 3He(polarized d, p), E=8.5-10.5 MeV; measured A(E, θ); deduced maximum.
doi: 10.1016/0370-2693(76)90261-6
1976GR10 Nucl.Phys. A271, 29 (1976) W.Gruebler, P.A.Schmelzbach, V.Konig, B.Jenny, R.Risler, H.R.Burgi, J.Nurzynski Maximum Tensor Analysing Power A(yy) = 1 in the 3He(d, p)4He Reaction NUCLEAR REACTIONS 3He(polarized d, p), E=8.5-10.5 MeV; measured A(θ, E).
doi: 10.1016/0375-9474(76)90265-7
1975BO01 Nucl.Phys. A237, 93 (1975) M.Bonsaru, J.Nurzynski, D.W.Gebbie, C.L.Hollas, S.Whineray, N.H.Merrill, L.O.Barbopoulos, A.R.Quinton (d, t) Reactions on 54Cr, 67,68Zn Nuclei NUCLEAR REACTIONS 54Cr, 67,68Zn(d, t), E=12 MeV; measured σ(Et, θ). 53Cr, 66,67Zn deduced levels, J, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(75)90465-0
1975NU02 Nucl.Phys. A246, 333 (1975) The Surface Absorption Optical Model Potential for 20 MeV Tritons NUCLEAR REACTIONS 40Ca, 52Cr, 54Fe, 62,64Ni, 90,92,94,96Zr, 116,118,120,122,124Sn, 182W, 207,208Pb(t, t'), E=20 MeV; calculated potential.
doi: 10.1016/0375-9474(75)90650-8
1972DJ01 Nucl.Phys. A181, 280 (1972) Tensor Polarization and Differential Cross Sections for the Elastic Scattering of Deuterons by Si at Low Energies NUCLEAR REACTIONS Si(d, d), E=7-11 MeV; measured T20(θ), T21(θ), T22(θ), σ(Ed, θ). Natural target.
doi: 10.1016/0375-9474(72)90920-7
1971DJ01 Nucl.Phys. A163, 113 (1971) Tensor Polarization of Deuterons from the Mg(d, d)Mg Elastic Scattering at 7.0 MeV NUCLEAR REACTIONS Mg(d, d), Ed=7.0 MeV; measured tensor polarization(θ). Natural target.
doi: 10.1016/0375-9474(71)90524-0
1971DJ02 Nucl.Phys. A163, 131 (1971) A.Djaloeis, H.Cords, J.Nurzynski Tensor Polarization and Differential Cross Section for the 9Be(d, d)9Be Elastic Scattering at Low Energies NUCLEAR REACTIONS 9Be(d, d), E=5-7 MeV; measured tensor polarization(θ), σ(Ed, θ). Natural target.
doi: 10.1016/0375-9474(71)90525-2
1970NU01 Nucl.Phys. A141, 257 (1970) The Dependence of the Spectroscopic Factors on Parameters of Distorting Potentials for the Reaction 26Mg(t, α)25Mg NUCLEAR REACTIONS 26Mg(3He, α), E=10.2 MeV; measured σ(θ). 25Mg levels deduced S(L, J), normalization coefficient D. Enriched target.
doi: 10.1016/0375-9474(70)90846-8
1970RO04 Nucl.Phys. A142, 469 (1970) D.M.Rosalky, D.J.Baugh, J.Nurzynski, B.A.Robson j-Dependence of l = 1 Transitions in the 54Cr(d, p)55Cr Reaction NUCLEAR REACTIONS 54Cr(d, p), E=8 MeV; measured σ(Ep, θ). 55Cr levels deduced J, S. Enriched target.
doi: 10.1016/0375-9474(70)90805-5
1969BA62 Australian J.Phys. 22, 555 (1969) D.J.Baugh, J.Nurzynski, D.M.Rosalky, C.H.Osman The Spin of the 2.78 MeV State of 19Ne NUCLEAR REACTIONS 20Ne(3He, 3He), (3He, α), E=10, 15 MeV; measured σ(θ); deduced optical model parameters. 19Ne level deduced L(n), J.
doi: 10.1071/PH690555
1969BR07 Nucl.Phys. A127, 622 (1969) Energy Dependence of the 16O(3He, 3He)16O and the 16O(3He, α0)15O Angular Distributions in the Range 9.8-11.7 MeV NUCLEAR REACTIONS 16O(3He, 3He), (3He, α0), E=9.802-11.738 MeV; measured σ(E;θ). Natural target.
doi: 10.1016/0375-9474(69)91033-1
1969BR08 Nucl.Phys. A130, 41 (1969) The Reaction 28Si(3He, α)27Si at E = 12 MeV NUCLEAR REACTIONS 28Si(3He, α), (3He, 3He), E=12 MeV, measured σ(θ). 28Si deduced neutron occupation numbers.
doi: 10.1016/0375-9474(69)90957-9
1969NU02 Nucl.Phys. A133, 23(1969) The Optical Model for Low-Energy Helions Scattered from 16O Nuclei NUCLEAR REACTIONS 16O(3He, 3He), E=9.8-10.7 MeV;measured σ(E;θ); deduced optical model parameters.
doi: 10.1016/0375-9474(69)90446-1
1968NU01 Nucl.Phys. A107, 581 (1968) J.Nurzynski, K.H.Bray, B.A.Robson The 27Al(3He, α)26Al Reaction at 10 MeV Bombarding Energy NUCLEAR REACTIONS 27Al(3He, α), E = 10 MeV; measured σ(Eα, θ). 26Al levels deduced L.
doi: 10.1016/0375-9474(68)90785-9
1967BR19 Nature 215, 501 (1967) States in Neon-21 Near 3 MeV NUCLEAR STRUCTURE 21Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1038/215501b0
1966BR13 Phys.Letters 21, 536 (1966) K.H.Bray, J.Nurzynski, W.P.Bourke Some Anomalies in the Reaction 16O(3He, α0)15O NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91290-X
1966NI02 Phys.Rev. 146, 799 (1966) H.Niewodniczanski, J.Nurzynski, A.Strzalkowski, G.R.Satchler 40Ca(d, d), (d, d'), and (d, p) Reactions with 12.8-MeV Deuterons NUCLEAR STRUCTURE 40Ca, 41Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.146.799
1966NU02 Aust.J.Sci. 29, 93 (1966) Isotopic-Spin Effects in Elastic Scattering
1965BR15 Nucl.Phys. 67, 417 (1965) K.H.Bray, J.Nurzynski, G.R.Satchler The Elastic Scattering of 5.5-10.0 MeV 3He Particles by 27Al Nuclei NUCLEAR REACTIONS 27Al(3He, 3He), E(3He) = 5.5-10 MeV; measured σ(E;θ). Natural target.
doi: 10.1016/0029-5582(65)90821-7
1964NI06 Nucl.Phys. 55, 386 (1964) H.Niewodniczanski, J.Nurzynski, A.Strzalkowski, J.Wilczynski, J.R.Rook, P.E.Hodgson Elastic and inelastic scattering of 12.8 MeV deuterons by 27Al and 28Si nuclei NUCLEAR REACTIONS 27Al(d, d), 27Al(d, d'), 28Si(d, d), 28Si(d, d'), E=12.8 MeV; measured products, 27Al, 28Si; deduced σ(θ). Data were imported from EXFOR entry F1102.
doi: 10.1016/0029-5582(64)90161-0
1963NI08 J.Phys. 24, 944 (1963) H.Niewodniczanski, J.Nurzynski, A.Strzalkowski Diffusion Elastique et Inelastique de Deutons de 12, 8 MeV sur le Noyau 28Si et Excitation du Coeur dans le Noyau 27Al NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
1962FR15 PAN-203, Nuclear Sci.Abstr. 17, 1230, Abstr.9507 (1963) L.Freindl, H.Niewodniczanski, J.Nurzynski, M.Slapa, A.Strzalkowski NUCLEAR STRUCTURE C, Be, Mg, Ca; measured not abstracted; deduced nuclear properties.
1962NI08 PAN-204 (1962); Nuclear Sci.Abstr. 17, 1510, Abstr.11625 (1963) H.Niewodniczanski, J.Nurzynski, J.Wilczynski Elastic and Inelastic Scattering of 12.8 MeV Deuterons on Al27 Nuclei NUCLEAR STRUCTURE 27Al; measured not abstracted; deduced nuclear properties.
1961FR09 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.529 (1961) L.Freindl, H.Niewodniczanski, J.Nurzynski, M.Slapa, A.Strzalkowski Elastic Scattering of 13 MeV Deuterons of Some Light Nuclei NUCLEAR STRUCTURE Ca, C, Mg, Be; measured not abstracted; deduced nuclear properties.
1960BU15 J.Phys.Radium 21, 366 (1960) A.Budzanowski, K.Grotowski, H.Niewodniczanski, J.Nurzynski NUCLEAR STRUCTURE 13N; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphysrad:01960002105036601
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