NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.J.Mills Found 26 matches. 1998CA11 Nucl.Phys. A630, 631 (1998) J.Carter, A.A.Cowley, H.Diesener, R.W.Fearick, S.V.Fortsch, M.N.Harakeh, J.J.Lawrie, S.J.Mills, P.von Neumann-Cosel, R.T.Newman, J.V.Pilcher, A.Richter, K.Schweda, F.D.Smit, G.F.Steyn, S.Strauch, D.M.Whittal Isoscalar Quadrupole Strength in 40Ca from the (p, p'α0) Reaction at E(p) = 100 MeV NUCLEAR REACTIONS 40Ca(p, p'α), E=99.5 MeV; measured σ(θ(p), θ(α), E(x)); deduced α0 channel multipole distribution, isoscalar E2 strength distribution.
doi: 10.1016/S0375-9474(98)00656-3
1997GA09 Phys.Lett. 394B, 29 (1997) E.Gadioli, C.Birattari, M.Cavinato, E.Fabrici, E.Gadioli Erba, V.Allori, C.Bovati, F.Cerutti, A.Di Filippo, E.Galbiati, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, S.J.Mills, F.M.Nortier, G.F.Steyn, C.Marchetta Comprehensive Study of the Reactions Induced by 12C on 103Rh up to 33 MeV/nucleon NUCLEAR REACTIONS 103Rh(12C, X)113Sb/110In/108In/107In/111In/105Ag/104Ag/103Ag/102Ag/101Pd/100Pd/99Rh/98Rh/97Ru/96Tc/95Ru/94Tc/93Mo/93mMo/90Nb, E=45-400 MeV; measured residuals production σ(E). Activation technique.
doi: 10.1016/S0370-2693(97)00003-8
1996BI19 Phys.Rev. C54, 3051 (1996) C.Birattari, M.Bonardi, M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, F.Groppi, M.Bello, C.Bovati, A.Di Filippo, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, S.J.Mills, F.M.Nortier, G.F.Steyn, C.Marchetta Preequilibrium Processes in the Fusion of 12C with 103Rh up to 20 MeV/nucleon NUCLEAR REACTIONS, ICPND 103Rh(12C, xnyp)113Sb/111Sn/110Sn/109Sn/108Sn/113Sn/111In/110In/110mIn, E=40-210 MeV; measured residuals production σ(E); deduced fusion σ, multiplicity of pre-equilibrium particles, mean-field interaction. Boltzmann master equation calculation.
doi: 10.1103/PhysRevC.54.3051
1995NO08 Appl.Radiat.Isot. 46, 1377 (1995) F.M.Nortier, S.J.Mills, G.F.Steyn Excitation Functions for the Production of Some Radioisotopes of Cs, Xe and I in Proton Bombardment of (nat)Xe up to 100 MeV NUCLEAR REACTIONS, ICPND Xe(p, X)125Cs/127Cs/129Cs/130Cs/132Cs/136Cs/136mCs/122Xe/123Xe/125Xe/125mXe/127Xe/127mXe/129Xe/129mXe/124I/126I/130I/130mI/131I, E=threshold-100 MeV; measured residuals production σ(E). Geometry-dependent hybrid model.
doi: 10.1016/0969-8043(95)00216-Z
1994NO10 Appl.Radiat.Isot. 45, 1051 (1994) F.M.Nortier, S.J.Mills, G.F.Steyn Excitation Function of the 111Cd(p, n)111m,111gIn Reaction NUCLEAR REACTIONS, ICPND 111Cd(p, n), E ≤ 30 MeV; compiled, reviewed σ(E) data.
doi: 10.1016/0969-8043(94)90177-5
1994VO05 Nucl.Phys. A569, 373c (1994) P.von Neumann-Cosel, H.Diesener, U.Helm, G.Herbert, V.Huck, A.Richter, G.Schrieder, A.Stascheck, A.Stiller, J.Ryckebusch, J.Carter, A.A.Cowley, R.W.Fearick, J.J.Lawrie, S.J.Mills, R.T.Newman, J.V.Pilcher, F.D.Smit, Z.Z.Vilakazi, D.M.Whittal Excitation and Decay of Electric Giant Resonances in the 40Ca(e, e'X) and 40Ca(p, p'X) Reactions NUCLEAR REACTIONS 40Ca(e, e'p), E=57, 78, 183.5 MeV; measured σ(θ(e), Ep). 40Ca(p, p'α), E=99.1 MeV; 40Ca(e, e'α), E=183.5 MeV; measured proton, α-channel decay. 40Ca deduced electric giant resonance decay features.
doi: 10.1016/0375-9474(94)90128-7
1992MI14 Appl.Radiat.Isot. 43, 1019 (1992) S.J.Mills, G.F.Steyn, F.M.Nortier Experimental and Theoretical Excitation Functions of Radionuclides Produced in Proton Bombardment of Copper up to 200 MeV NUCLEAR REACTIONS, ICPND Cu(p, X)60Co/52Fe/59Fe/52Mn/54Mn/56Mn/48Cr/49Cr/51Cr/48V/44Sc/44mSc/46Sc, E=200 MeV; measured residuals production effective σ. Model comparison.
doi: 10.1016/0883-2889(92)90221-Y
1992ST15 Appl.Radiat.Isot. 43, 1323 (1992) G.F.Steyn, B.R.S.Simpson, S.J.Mills, F.M.Nortier The Production of 55Fe with Medium-Energy Protons NUCLEAR REACTIONS 55Mn, 59Co, Ni(p, X)55Fe, E=threshold-100 MeV; measured residual production rates. Thick target. Model comparison.
doi: 10.1016/0883-2889(92)90003-W
1991NO02 Appl.Radiat.Isot. 42, 353 (1991) F.M.Nortier, S.J.Mills, G.F.Steyn Excitation Functions and Yields of Relevance to the Production of 67Ga by Proton Bombardment of (nat)Zn and (nat)Ge up to 100 MeV NUCLEAR REACTIONS, ICPND Zn(p, X)65Ga/66Ga/67Ga/68Ga, E=8.4-99.6 MeV; Ge(p, X)65Ga/66Ga/67Ga/68Ga/72Ga, E=4.9-97.9 MeV; measured residuals production σ, thick target yields.
doi: 10.1016/0883-2889(91)90138-Q
1991NO06 Appl.Radiat.Isot. 42, 1105 (1991) F.M.Nortier, S.J.Mills, G.F.Steyn Excitation Functions for the Production of 109Cd, 109In and 109Sn in Proton Bombardment of Indium up to 200 MeV NUCLEAR REACTIONS, ICPND In(p, X)109Cd/109In/109Sn, E ≤ 200 MeV; measured residuals production σ(E). Model calculations.
doi: 10.1016/0883-2889(91)90021-R
1991ST02 Appl.Radiat.Isot. 42, 361 (1991) G.F.Steyn, S.J.Mills, F.M.Nortier, F.J.Haasbroek Integral Excitation Functions for (nat)Kr + p up to 116 MeV and Optimization of the Production of 81Rb for 81mKr Generators NUCLEAR REACTIONS, ICPND Kr(p, X)79Rb/81Rb/81mRb/82Rb/82mRb/83Rb/84Rb/84mRb/86Rb/77Kr/79Kr/85Kr/85mKr/77Br/82Br, E=threshold-116 MeV; measured thick target production rates, σ(E). Geometry dependent hybrid model.
doi: 10.1016/0883-2889(91)90139-R
1990NO11 Appl.Radiat.Isot. 41, 1201 (1990) F.M.Nortier, S.J.Mills, G.F.Steyn Excitation Functions and Production Rates of Relevance to the Production of 111In by Proton Bombardment of (nat)Cd and (nat)In up to 100 MeV NUCLEAR REACTIONS, ICPND Cd(p, xn)111In, In(p, xn)111Sn, E=threshold-100 MeV; measured residual production σ(E); deduced thick target production rates.
doi: 10.1016/0883-2889(90)90207-W
1990ST03 Appl.Radiat.Isot. 41, 315 (1990) G.F.Steyn, S.J.Mills, F.M.Nortier, B.R.S.Simpson, B.R.Meyer Production of 52Fe via Proton-Induced Reactions on Manganese and Nickel NUCLEAR REACTIONS, ICPND 55Mn(p, 4n), E=40-200 MeV; 27Al(p, X)22Na, E=75-200 MeV; Ni(p, X)52Fe, E=45-200 MeV; measured residual production σ(E).
doi: 10.1016/0883-2889(90)90197-O
1986LA28 Z.Phys. A325, 175 (1986) J.J.Lawrie, A.A.Cowley, D.M.Whittal, S.J.Mills, W.R.McMurray Resonances in Low Energy Elastic Scattering of α-Particles from 28Si NUCLEAR REACTIONS 28Si(α, α), E=5-12 MeV; measured σ(Eα), σ(E), σ(θ). 32S deduced no quasimolecular resonance evidence. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0658. 1985WA13 Phys.Rev. C31, 1662 (1985) C.W.Wang, P.G.Roos, N.S.Chant, G.Ciangaru, F.Khazaie, D.J.Mack, A.Nadasen, S.J.Mills, R.E.Warner, E.Norbeck, F.D.Becchetti, J.W.Janecke, P.M.Lister 9Be(p, pα)5He Cluster Knockout Reaction with 150 MeV Polarized Protons NUCLEAR REACTIONS 9Be(polarized p, pα), E=150 MeV; measured quasifree σ(θ), analyzing power vs θ, σ(θp, Ep), energy sharing σ; deduced optical potentials parameters. 9Be deduced Sα for cluster breakup. DWIA, cluster knockout.
doi: 10.1103/PhysRevC.31.1662
1985WE12 Phys.Rev. C32, 1474 (1985) J.S.Wesick, P.G.Roos, N.S.Chant, C.C.Chang, A.Nadasen, L.Rees, N.R.Yoder, A.A.Cowley, S.J.Mills, W.W.Jacobs 2H, 3,4He(p(pol), p') and 3,4He(p(pol), d') Continuum Yields for 100 and 150 MeV Protons NUCLEAR REACTIONS 2H, 3,4He(polarized p, p'), 3,4He(polarized p, d), E=100, 150 MeV; measured inclusive σ(θ), analyzing power vs θ; deduced reaction mechanism. DWIA analysis.
doi: 10.1103/PhysRevC.32.1474
1978CO10 J.Phys.(London) G4, L149 (1978) A.A.Cowley, S.J.Mills, G.Heymann Correlation between the Forward-Angle Yield of the Reaction 16O(α, d)18F (Ex = 1.125 MeV) and Anomalous Large-Angle Elastic Scattering in 16O(α, α)16O NUCLEAR REACTIONS 16O(α, d), E=28.0-33.6 MeV; measured σ(E, θ) to lowest 5+ level in 18O. Natural solid target, DWBA analysis.
doi: 10.1088/0305-4616/4/6/009
1978CO11 Nucl.Phys. A301, 429 (1978) A.A.Cowley, J.C.van Staden, S.J.Mills, P.M.Cronje, G.Heymann, G.F.Burdzik Large-Angle Elastic Scattering of α-Particles from 20Ne and 22Ne NUCLEAR REACTIONS 20,22Ne(α, α), E=24.6-31.7 MeV; measured σ(E;θ), θ=13°-177°; deduced Regge-pole parameters. Enriched targets.
doi: 10.1016/0375-9474(78)90059-3
1977HU10 Nucl.Phys. A292, 267 (1977) D.Husar, S.J.Mills, H.Graf, U.Neumann, D.Pelte, G.Seiler-Clark Lifetimes of the Yrast States of Even Ce Isotopes NUCLEAR REACTIONS 118,120,122Sn(16O, 4nγ), E=76 MeV; measured recoil distance Doppler shift. 130,132,134Ce yrast levels deduced T1/2, side-feeding times, intensities. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(77)90373-6
1976HU03 Phys.Rev.Lett. 36, 1291 (1976) D.Husar, S.J.Mills, H.Graf, U.Neumann, D.Pelte, J.C.Merdinger Observed Retardation of the E2 Transitions in the Backbending Region of 134Ce NUCLEAR REACTIONS 122Sn(16O, 4nγ), E=76 MeV; measured recoil distance DSA. 134Ce yrast levels deduced T1/2, feeding times.
doi: 10.1103/PhysRevLett.36.1291
1974CO28 Nucl.Phys. A229, 256 (1974) A.A.Cowley, P.M.Cronje, G.Heymann, S.J.Mills, J.C.van Staden Diffraction Scattering of α-Particles from Even Isotopes of Ni at Backward Angles NUCLEAR REACTIONS 58,60,62,64Ni(α, α), (α, α'), Eα=24.3-32.3 MeV; measured σ(E;θ), θ=15-179degrees; deduced optical model parameters. 58,60,62,64Ni levels deduced β(L).
doi: 10.1016/0375-9474(74)90787-8
1974DE12 Nucl.Phys. A225, 1 (1974) W.Dehnhardt, S.J.Mills, M.Muller-Veggian, U.Neumann, D.Pelte, G.Poggi, B.Povh, P.Taras Yrast Cascades in Even-Mass Ce Isotopes NUCLEAR REACTIONS 118,120,122,124Sn(16O, 4nγ), E=68-76 MeV; measured Eγ, Iγ(θ), γγ coin. 130,132,134,136Ce deduced levels, J, T1/2. Enriched targets.
doi: 10.1016/0375-9474(74)90361-3
1972TA25 Phys.Lett. 41B, 295 (1972) P.Taras, W.Dehnhardt, S.J.Mills, M.Veggian, J.C.Merdinger, U.Neumann, B.Povh High-Spin Yrast States in 132C NUCLEAR REACTIONS 120Sn(16O, 4nγ), E=68-76 MeV; measured σ(E;Eγ, θ(γ), θ(γγ)), γγ-coin. 132Ce deduced high-J yrast states, J.
doi: 10.1016/0370-2693(72)90582-5
1971DE26 Nucl.Phys. A172, 323 (1971) A.S.M.de Jesus, S.J.Mills, W.L.Rautenbach The Population of the Ground-State Rotational Band of 168Yb by Means of 4He-, 3He-, Deuteron- and Proton-Induced Reactions NUCLEAR REACTIONS 166Er(α, 2nγ), Eα=21.2-34.1 MeV; 167Er(α, 3nγ), Eα=26.6-33.7 MeV; 168Er(3He, 3nγ), E(3He)=19.8-27.3 MeV; 169Tm(d, 3nγ), Ed=13.5-17.3 MeV; 169Tm(p, 2nγ), Ep=9.8-14.7 MeV; measured σ(E;Eγ). Enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(71)90717-2
1969MI03 Nucl.Phys. A124, 597 (1969) Population of Ground-State Rotational Levels in (α, 2nγ) Reactions NUCLEAR REACTIONS 152Sm, 162Dy, 176,178,180Hf, 188Os(α, 2nγ), Eα=19.2-31.7 MeV; measured σ(E; Eγ). 154Gd, 164Er, 178,180,182W, 190Pt deduced levels, γ-branching. Enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90652-6
1969MI16 Phys.Letters 30B, 481 (1969) Anomalous Population of the Ground-State Rotational Band of 174Hf in the 172Yb(α, 2nγ)174Hf NUCLEAR REACTIONS 172Yb(α, 2nγ), E = 21-32 MeV; measured σ(E; Eγ). 174Hf deduced anomalous ground-state rotational band population.
doi: 10.1016/0370-2693(69)90178-6
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