NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = P.E.Hodgson Found 118 matches. Showing 1 to 100. [Next]2007CO14 Phys.Rev. C 75, 054617 (2007) A.A.Cowley, J.Bezuidenhout, S.S.Dimitrova, P.E.Hodgson, S.V.Fortsch, G.C.Hillhouse, N.M.Jacobs, R.Neveling, F.D.Smit, J.A.Stander, G.F.Steyn, J.J.van Zyl Multistep direct mechanism in the (p(pol), 3He) inclusive reaction on 59Co and 93Nb at incident energies between 100 and 160 MeV NUCLEAR REACTIONS 59Co, 93Nb(polarized p, 3He), E=40-160 MeV; measured σ, angular distributions and analyzing powers. Compared results to model calculations.
doi: 10.1103/PhysRevC.75.054617
2004AN21 Int.J.Mod.Phys. E13, 759 (2004) A.N.Antonov, M.K.Gaidarov, D.N.Kadrev, P.E.Hodgson, E.Moya De Guerra Charge density distributions and related form factors in neutron-rich light exotic nuclei NUCLEAR STRUCTURE 4,6,8He, 6,11Li, 17,19B, 14Be; calculated charge density distributions, radii, form factors.
doi: 10.1142/S0218301304002430
2003HO01 Phys.Rep. 374, 1 (2003) Cluster emission, transfer and capture in nuclear reactions
doi: 10.1016/S0370-1573(02)00268-5
2002AN03 Phys.Rev. C65, 024306 (2002) A.N.Antonov, M.K.Gaidarov, M.V.Ivanov, D.N.Kadrev, G.Z.Krumova, P.E.Hodgson, H.V.von Geramb Nucleon Momentum Distribution in Deuteron and Other Nuclei within the Light-Front Dynamics Method NUCLEAR STRUCTURE 2H, 4He, 12C, 56Fe; calculated nucleon momentum distributions. Light-front dynamics model.
doi: 10.1103/PhysRevC.65.024306
2000CO29 Phys.Rev. C62, 064605 (2000) A.A.Cowley, G.F.Steyn, S.S.Dimitrova, P.E.Hodgson, G.J.Arendse, S.V.Fortsch, G.C.Hillhouse, J.J.Lawrie, R.Neveling, W.A.Richter, J.A.Stander, S.M.Wyngaardt Multistep Direct Mechanism in the (p(pol), 3He) Inclusive Reaction on 59Co and 93Nb at an Incident Energy of 100 MeV NUCLEAR REACTIONS 59Co, 93Nb(polarized p, 3He), E=100 MeV; measured σ(E, θ), Ay(θ); deduced one-step, multistep process contributions, other reaction mechanism features. Comparison with model predictions.
doi: 10.1103/PhysRevC.62.064605
2000SP09 J.Phys.(London) G26, 1489 (2000) K.Spasova, S.S.Dimitrova, P.E.Hodgson The Analysing Powers of (p, 3He) Reactions NUCLEAR REACTIONS 58Ni, 90Zr, 209Bi(p, 3He), E=72 MeV; analyzed σ(θ), Ay(θ); deduced one-, two-step contributions. Feshbach-Kerman-Koonin multistep theory.
doi: 10.1088/0954-3899/26/10/304
1998BE23 Rep.Prog.Phys. 61, 483 (1998) Particle-Hole State Densities in Pre-Equilibrium Nuclear Reaction Models
doi: 10.1088/0034-4885/61/5/002
1997CO05 Phys.Rev. C55, 1843 (1997) A.A.Cowley, G.J.Arendse, G.F.Steyn, J.A.Stander, W.A.Richter, S.S.Dimitrova, P.Demetriou, P.E.Hodgson Inclusive (p, 3He) Reactions on 59Co and 197Au at Incident Energies of 120, 160, and 200 MeV NUCLEAR REACTIONS 59Co, 197Au(p, 3He), E=120, 160, 200 MeV; measured σ(θ) vs E; deduced multi-step mechanisms role. Statistical multi-step direct reaction theory.
doi: 10.1103/PhysRevC.55.1843
1997DI07 J.Phys.(London) G23, 961 (1997) S.S.Dimitrova, G.Z.Krumova, P.E.Hodgson, V.Avrigeanu, A.N.Antonov (n, d)-Reactions on Medium Mass Nuclei NUCLEAR REACTIONS 58Ni, 63,65Cu(n, d), E=6-16 MeV; analyzed σ(E); deduced reaction mechanism. Hauser-Feshbach statistical model, pick-up, knockout mechanisms.
doi: 10.1088/0954-3899/23/8/010
1997DI14 J.Phys.(London) G23, 1685 (1997) S.S.Dimitrova, M.K.Gaidarov, A.N.Antonov, M.V.Stoitsov, P.E.Hodgson, V.K.Lukyanov, E.V.Zemlyanaya, G.Z.Krumova One-Nucleon Removal Reactions as a Test of Overlap Functions from the One-Body Density Matrix Calculations NUCLEAR REACTIONS 16O(p, d), E=45.34; 40Ca(p, d), E=27.5, 65 MeV; analyzed σ(θ); 40Ca(e, e'p), E not given; analyzed momentum distribution; deduced short-range correlations role. 15O, 39Ca deduced ground-state spectroscopic factors. One-body density matrix, overlap functions.
doi: 10.1088/0954-3899/23/11/016
1997HO27 Nuovo Cim. 110A, 967 (1997) P.E.Hodgson, P.Demetriou, S.S.Dimitrova Analysis of (p, α) and (p, 3He) Cross-Sections to Continuum States by the Feshbach-Kerman-Koonin Multistep Direct Theory NUCLEAR REACTIONS 93Nb, 118Sn(p, α), E=44.3 MeV; 59Co(p, α), E=120, 160 MeV; 59Co, 197Au(p, 3He), E=120, 160, 200 MeV; analyzed σ(E, θ); deduced clustering role in reaction mechanism.
doi: 10.1007/BF03035934
1996CO12 Phys.Rev. C54, 778 (1996) A.A.Cowley, G.J.Arendse, J.W.Koen, W.A.Richter, J.A.Stander, G.F.Steyn, P.Demetriou, P.E.Hodgson, Y.Watanabe Inclusive (p, α) Reactions on 27Al, 59Co, and 197Au at Incident Energies of 120, 160, and 200 MeV NUCLEAR REACTIONS 27Al, 59Co, 197Au(p, α), E=120, 160, 200 MeV; measured σ(Eα, θ); deduced higher-step contributions role. Multi-step DWBA analysis.
doi: 10.1103/PhysRevC.54.778
1996DE01 Nucl.Phys. A596, 67 (1996) P.Demetriou, A.Marcinkowski, P.E.Hodgson A New Multistep Direct Reaction Mechanism: Collective excitations in the continuum NUCLEAR REACTIONS 56Fe, 58Ni, 90Zr, 93Nb, 208Pb, 209Bi(n, n'), E=14.1 MeV; analyzed σ(θ, En); deduced collective components role. Multi-step compound, direct mechanisms, collective excitations.
doi: 10.1016/0375-9474(95)00378-9
1996DE23 J.Phys.(London) G22, 629 (1996) P.Demetriou, P.E.Hodgson, A.Marcinkowski, Y.Watanabe A Consistent Analysis of (n, n'), (p, p'), (n, p) and (p, n) Multistep Reactions using the Feshbach-Kerman-Koonin Theory NUCLEAR REACTIONS 63,65Cu(n, p), E=14.8 MeV; 93Nb(n, p), E=14.1 MeV; 93Nb(n, n'), (p, p'), 98Mo(p, p'), E=18, 25.6 MeV; analyzed σ(θ, E). Feshbach-Kerman-Koonin multi-step reaction theory.
doi: 10.1088/0954-3899/22/5/010
1996DE58 J.Phys.(London) G22, 1813 (1996) The Energy Dependence of the Proton-Alpha Reaction to Continuum States NUCLEAR REACTIONS 165Ho, 93Nb(p, α), E=19.9-44.3 MeV; 169Tm(p, α), E=29.7-44.3 MeV; 118Sn(p, α), E=25.1-44.3 MeV; analyzed σ(θ, Eα). Feshbach-Kerman-Koonin multi-step theory, knockout model. Hauser-Feshbach theory.
doi: 10.1088/0954-3899/22/12/012
1996GU03 Z.Phys. A354, 53 (1996) P.Guazzoni, L.Zetta, P.Demetriou, P.E.Hodgson Multistep Direct Analysis of (p, α) Reactions to the Continuum NUCLEAR REACTIONS 90,91Zr(p, α), E=24.02 MeV; 142,143Nd(p, α), E=23.1 MeV; measured σ(θ, Eα); deduced angle integrated σ, unpaired neutron spectators, pairing effects roles. Hauser-Feshbach, Feshbach-Kerman-Koonin theories, multi-step direct analysis.
doi: 10.1007/s002180050012
1996MA46 J.Phys.(London) G22, 1219 (1996) A.Marcinkowski, P.Demetriou, P.E.Hodgson Pre-Equilibrium and Collective Reactions in Neutron Inelastic Scattering by the Rotational Nuclei 184,186W NUCLEAR REACTIONS 184W(n, n'), E=26 MeV; 186W(n, n'), E=14.1 MeV; analyzed angle integrated σ vs E(n), σ(θ).
doi: 10.1088/0954-3899/22/8/010
1996RI11 Phys.Rev. C54, 1756 (1996) W.A.Richter, S.W.Steyn, A.A.Cowley, J.A.Stander, J.W.Koen, R.Lindsay, G.C.Hillhouse, R.E.Julies, J.J.Lawrie, J.V.Pilcher, P.E.Hodgson Inclusive (p, p') Reactions on Nuclei in the Mass Range 115 to 181 at Incident Energies from 120 to 200 MeV NUCLEAR REACTIONS 115In, 167Er, 173Yb, 181Ta(p, p'X), E=120, 150, 175, 200 MeV; 141Pr(p, p'X), E=120, 200 MeV; measured inclusive σ(E, θ); deduced reaction mechanism. Statistical multistep direct theory analysis.
doi: 10.1103/PhysRevC.54.1756
1995AN22 J.Phys.(London) G21, 1333 (1995) A.N.Antonov, M.V.Stoitsov, M.K.Gaidarov, S.S.Dimitrova, P.E.Hodgson The Hole Spectral Function and the Relationship between Overlap Functions, Natural Orbitals and the One-Body Density Matrix in Nuclei
doi: 10.1088/0954-3899/21/10/007
1995AV03 J.Phys.(London) G21, 837 (1995) M.Avrigeanu, V.Avrigeanu, A.N.Antonov, M.B.Chadwick, P.E.Hodgson, M.V.Stoitsov Pauli-Blocking Effects in Neutron-Alpha Reactions NUCLEAR REACTIONS 54Fe, 51V, 55Mn, 59Co, 48Ti, 52Cr(n, α), E ≈ 4-20 MeV; analyzed σ(E); deduced model parameters variations range limitations, Pauli-blocking effects.
doi: 10.1088/0954-3899/21/6/011
1995GA33 Phys.Rev. C52, 3026 (1995) M.K.Gaidarov, A.N.Antonov, G.S.Anagnostatos, S.E.Massen, M.V.Stoitsov, P.E.Hodgson Proton Momentum Distribution in Nuclei Beyond 4He NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Fe, 208Pb; calculated proton momentum distribution. Natural orbital representation model, empirical 4He nucleon momentum distribution input.
doi: 10.1103/PhysRevC.52.3026
1995MA47 J.Phys.(London) G21, 1089 (1995) A.Marcinkowski, P.Demetriou, P.E.Hodgson Are Pre-Equilibrium Reactions Mainly Direct ( Question ) NUCLEAR REACTIONS 49Ti, 58Fe(p, n), E=9.6, 14 MeV; 63Cu(p, n), E=14.8 MeV; 169Tm, 159Tb(p, xn), E=18 MeV; 98Mo(p, xn), (p, n), 100Mo(p, n), E=25.6 MeV; 65Cu(p, xn), E=26.7 MeV; calculated σ(θ, En); deduced preequilibrium process dominance over direct process conditions, model parameters. Multi-step, statistical direct reaction approaches.
doi: 10.1088/0954-3899/21/8/007
1995MA67 Phys.Rev. C52, 2021 (1995) A.Marcinkowski, B.Marianski, P.Demetriou, P.E.Hodgson Collective Reactions to the Continuum in Neutron Scattering by Niobium NUCLEAR REACTIONS 93Nb(n, xn), E=14-26 MeV; analyzed σ(θ, En), angle integrated σ. Combined multi-step direct, compound plus preequilibrium components.
doi: 10.1103/PhysRevC.52.2021
1995OL01 J.Phys.(London) G21, 361 (1995) H.B.Olaniyi, P.Demetriou, P.E.Hodgson Analysis of the (p, α) Reaction using the Pre-Equilibrium Multi-Step Direct Feshbach-Kerman-Koonin Theory NUCLEAR REACTIONS 93Nb, 118Sn, 107Ag, 169Tm(p, α), E ≈ 8-40 MeV; analyzed σ(θ, Eα); deduced no multi-step compound emission evidence. Feshbach-Kerman-Koonin theory.
doi: 10.1088/0954-3899/21/3/011
1995WA07 Phys.Rev. C51, 1891 (1995) Y.Watanabe, A.Aoto, H.Kashimoto, S.Chiba, T.Fukahori, K.Hasegawa, M.Mizumoto, S.Meigo, M.Sugimoto, Y.Yamanouti, N.Koori, M.B.Chadwick, P.E.Hodgson Feshbach-Kerman-Koonin Model Analysis of Preequilibrium (p, p') and (p, n) Reactions at 12 to 26 MeV NUCLEAR REACTIONS 98Mo(p, xp), E=25.6 MeV; 106Pd(p, xp), E=26 MeV; measured σ(θ, Ep); 98Mo(p, xn), E=25.6 MeV; 106Pd(p, xn), E=26 MeV; 93Nb(n, n'), E=14.1-25.7 MeV; 106Pd, 98Mo(p, p'), E=12-26 MeV; 98Mo, 106Pd(p, n), E=26 MeV; 93Nb(p, p'), E=18 MeV; analyzed σ(θ, E) data; deduced effective N-N interaction strength. Feshbach-Kerman-Koonin model analysis.
doi: 10.1103/PhysRevC.51.1891
1994AN11 Phys.Rev. C50, 164 (1994) A.N.Antonov, D.N.Kadrev, P.E.Hodgson Effect of Nucleon Correlations on Natural Orbitals NUCLEAR STRUCTURE 40Ca, 16O; calculated single hole, particle state wave functions. Nucleon correlation effects, generator coordinate method.
doi: 10.1103/PhysRevC.50.164
1994AV01 Phys.Rev. C49, 2136 (1994) V.Avrigeanu, P.E.Hodgson, M.Avrigeanu Global Optical Potentials for Emitted Alpha Particles NUCLEAR REACTIONS 54Fe, 52Cr, 59Co, 48,50Ti, 51V(n, α), E < 10 MeV; calculated σ(E). 40Ca, 55Mn, 59Co(α, X), E < 13 MeV; calculated reaction σ(E). Global optical potentials.
doi: 10.1103/PhysRevC.49.2136
1994DE41 J.Phys.(London) G20, 1779 (1994) P.Demetriou, P.Kanjanarat, P.E.Hodgson FKK Analysis of 14 MeV Neutron-Induced Reactions NUCLEAR REACTIONS 51V, 93Nb, 56Fe, Zr, 93Nb, Sb, Mo(n, n'), E=14.1 MeV; analyzed σ(θ). Feshbach-Kerman-Koonin model.
doi: 10.1088/0954-3899/20/11/007
1994HO20 Z.Phys. A349, 197 (1994) A Survey of Alpha-Clustering NUCLEAR STRUCTURE A=24-215; compiled, reviewed α-clustering features.
doi: 10.1007/BF01288959
1994RI01 Phys.Rev. C49, 1001 (1994) W.A.Richter, A.A.Cowley, G.C.Hillhouse, J.A.Stander, J.W.Koen, S.W.Steyn, R.Lindsay, R.E.Julies, J.J.Lawrie, J.V.Pilcher, P.E.Hodgson Preequilibrium (p, p') Measurements and Calculations for 90Zr and Neighboring Nuclei for Incident Energies up to 200 MeV NUCLEAR REACTIONS 89Y, 90Zr, 92,94,96,98Mo(p, p'), E=120, 160, 200 MeV; measured inclusive σ(E, θ); deduced reaction mechanism. Statistical multi-step, direct theory analysis.
doi: 10.1103/PhysRevC.49.1001
1993AV02 J.Phys.(London) G19, 745 (1993) M.Avrigeanu, P.E.Hodgson, A.J.Koning Semiclassical and Quantum Mechanical Pre-Equilibrium Neutron Emission NUCLEAR REACTIONS 56Fe, 58Ni, 51V, 55Mn, 52Cr, 59Co(n, xn), E=14 MeV; analyzed angle-integrated σ data. 58Fe(p, n), E=14 MeV; 59Co(p, n), E=14.7 MeV; analyzed σ(θn, En) data. Semi-classical, quantum approach, preequilibrium neutron emission.
doi: 10.1088/0954-3899/19/5/008
1993DE39 J.Phys.(London) G19, L193 (1993) P.Demetriou, P.Kanjanarat, P.E.Hodgson Analysis of the Multistep Direct Component of 14 MeV Neutron Inelastic Scattering NUCLEAR REACTIONS 93Nb(n, n'), (n, 2n), E=14.1 MeV; calculated σ(θn, En), angle integrated σ(E); deduced effective finite-range Yukawa interaction mean value. Feshbach-Kerman-Koonin multi-step direct theory.
doi: 10.1088/0954-3899/19/12/003
1993OL04 J.Phys.(London) G19, 1029 (1993) H.B.Olaniyi, P.Kanjanarat, P.E.Hodgson Multistep Compound Reaction Calculations Using the Feshbach-Kerman-Koonin Theory NUCLEAR REACTIONS 48Ti, 51V, 52Cr, 55Mn, 56Fe, 59Co, 63Cu, 93Nb(n, n'), E=14.1 MeV; 48Ti, 59Co, 55Mn, 63Cu(p, n), E=14.8 MeV; calculated σ(θ, En); deduced multi-step compound, direct processes contributions. Feshbach-Kerman-Koonin theory.
doi: 10.1088/0954-3899/19/7/013
1993OL07 Roum.J.Phys. 38, 371 (1993) Multistep Processes in Nuclear Reactions. The Feshbach-Kerman-Koonin Theory NUCLEAR REACTIONS 63Cu(n, n'), (n, 2n), E=14.1 MeV; 93Nb(n, n'), E=14, 25.7 MeV; compiled, reviewed angle-integrated neutron spectra, analyses. Multi-step reactions.
1993PA15 Nucl.Phys. A559, 266 (1993) G.Pantis, S.A.Sofianos, H.Fiedeldey, R.Lipperheide, P.E.Hodgson Dispersive Correction to the p + 16O Optical Model and the Effective Nucleon-Nucleon Potential NUCLEAR REACTIONS, ICPND 16O(p, p), E=23.4-52.5 MeV; analyzed σ(θ); deduced potential parameters, reaction σ(E). Optical model, dispersive corrections.
doi: 10.1016/0375-9474(93)90191-Y
1993SO16 J.Phys.(London) G19, 1929 (1993) S.A.Sofianos, K.C.Panda, P.E.Hodgson The Microscopic Alpha-Alpha Potential NUCLEAR REACTIONS 4He(α, α), E(cm)=1, 10, 17 MeV; calculated microscopic potential. Skyrme effective interaction, folding, energy-density models.
doi: 10.1088/0954-3899/19/11/019
1992HO15 Hyperfine Interactions 74, 75 (1992) Nuclear Matter Distributions NUCLEAR STRUCTURE 40,48Ca, 39K, 90,92,94Zr, 206,208Pb, 205Tl; compiled, reviewed charge density distribution fits. 40,48Ca, 64Ni, 116,124Sn, 208Pb; compiled, reviewed neutron density distribution fits. 198,200,202,204,206,208,210,212,214Pb; N ≤ 160; compiled, reviewed rms charge radii fits. A=169-230; compiled, reviewed α-decay Geiger-Nuttall plots.
doi: 10.1007/BF02398619
1992ME06 Nucl.Sci.Eng. 111, 132 (1992) A.C.Merchant, P.E.Hodgson, H.R.Schelin The Interaction of 1- to 20-MeV Neutrons with 238U NUCLEAR REACTIONS 238U(n, n), (n, n'), E=1-20 MeV; 238U(n, 2n), (n, 3n), E=threshold-20 MeV; analyzed σ(E), other data. Optical potential, dispersion relation approach.
doi: 10.13182/NSE92-A23929
1992RI06 Phys.Rev. C46, 1030 (1992) W.A.Richter, A.A.Cowley, R.Lindsay, J.J.Lawrie, S.V.Fortsch, J.V.Pilcher, R.Bonetti, P.E.Hodgson Statistical Multistep Direct Calculations for (p, p') Continuum Spectra up to 200 MeV NUCLEAR REACTIONS 100Mo(p, p'), E=100-200 MeV; measured σ(θ, Ep'). 58Ni, 197Au(p, p'), E=100-200 MeV; analyzed σ(θ, Ep'). Statistical multi-step direct theory.
doi: 10.1103/PhysRevC.46.1030
1992SO03 Nucl.Phys. A540, 199 (1992) S.A.Sofianos, H.Fiedeldey, R.Lipperheide, G.Pantis, P.E.Hodgson Dispersive Corrections to the Resonating Group αα Potential NUCLEAR REACTIONS 4He(α, α), E(cm) ≈ 20-70 MeV; calculated phase shifts vs E. Resonating group method, phenomenological potentials, dispersive corrections.
doi: 10.1016/0375-9474(92)90200-4
1991CH23 Phys.Rev. C44, 814 (1991) M.B.Chadwick, P.Oblozinsky, P.E.Hodgson, G.Reffo Pauli-Blocking in the Quasideuteron Model of Photoabsorption NUCLEAR REACTIONS Pb, Ta, Ce, Sn(γ, X), E=20-140 MeV; calculated photoabsorption σ(E). Pauli blocking, quasideuteron model.
doi: 10.1103/PhysRevC.44.814
1991CO03 Phys.Rev. C43, 678 (1991) A.A.Cowley, A.van Kent, J.J.Lawrie, S.V.Fortsch, D.M.Whittal, J.V.Pilcher, F.D.Smit, W.A.Richter, R.Lindsay, I.J.van Heerden, R.Bonetti, P.E.Hodgson Preequilibrium Proton Emission Induced by 80 and 120 MeV Protons Incident on 90Zr NUCLEAR REACTIONS 90Zr(p, p'), E=80, 120 MeV; measured σ(Ep', θp'); deduced reaction mechanism, effective interaction strength. Phenomenological parametrization.
doi: 10.1103/PhysRevC.43.678
1991KU14 Nucl.Phys. A534, 393 (1991) K.-I.Kubo, P.Manyum, P.E.Hodgson The Spin Distribution in Heavy-Ion Fusion NUCLEAR REACTIONS 64Ni(32S, X), E=88 MeV; 40Ca(16O, X), E=55.6, 60 MeV; 40,42,44,48Ca(16O, X), E=56 MeV; calculated elastic, inelastic dynamical polarization, optical imaginary potentials; deduced heavy-ion fusion spin-distribution.
doi: 10.1016/0375-9474(91)90508-4
1989AN16 Nuovo Cim. 102A, 1701 (1989) A.N.Antonov, E.N.Nikolov, I.Zh.Petkov, Chr.V.Christov, P.E.Hodgson Natural Orbitals and Occupation Numbers in the Coherent Density Fluctuation Model NUCLEAR STRUCTURE 16O, 40Ca, 58Ni, 208Pb; calculated natural single particle orbital occupation numbers. Coherent density fluctuation model.
doi: 10.1007/BF02825160
1989CH03 J.Phys.(London) G15, 250 (1989) M.B.Chadwick, R.Bonetti, P.E.Hodgson Multistep Compound Processes in Nuclear Reactions from 9 to 18 MeV NUCLEAR REACTIONS 58Fe(p, xn), Ag, 93Nb(n, xp), 93Nb, 58Ni, 59Co(n, xn), E=14 MeV; 181Ta(p, xn), E=18 MeV; 63Cu, 89Y, 59Co(p, xn), E=15 MeV; 93Nb(n, xn), E=9 MeV; calculated σ(θ(n), E(n)), σ(θ(p), E(p)). Multi-step compound process.
1989KO38 J.Phys.(London) G15, 1689 (1989) The Interactions of 14 MeV Neutrons with 59Co and 93Nb NUCLEAR REACTIONS 93Nb(n, xn), (n, xnyp), 59Co(n, xnyp), E ≈ 14 MeV; calculated σ vs En, σ(θ) vs Ep. Multi-step compound reactions.
doi: 10.1088/0954-3899/15/11/013
1989MA41 Nuovo Cim. 101A, 1045 (1989) A.Malecki, P.Picozza, P.E.Hodgson A Simple Description of Nucleon High-Momentum Components Due to Short-Range Correlations in Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated nucleon momentum distribution. Short range correlations.
doi: 10.1007/BF02800172
1989MA42 Nucl.Phys. A501, 1 (1989) A.Marcinkowski, R.W.Finlay, J.Rapaport, P.E.Hodgson, M.B.Chadwick Neutron Emission Cross Sections on 184W at 11.5 and 26 MeV and the Neutron-Nucleus Scattering Mechanism NUCLEAR REACTIONS 184W(n, xn), (n, n), E=11.5, 26 MeV; measured σ(En, θ). Statistical multistep theory analysis. Tof.
doi: 10.1016/0375-9474(89)90562-9
1989ME05 J.Phys.(London) G15, 601 (1989) A.C.Merchant, K.F.Pal, P.E.Hodgson The Alpha-Particle Structure of 44Ti NUCLEAR STRUCTURE 44Ti; calculated levels widths. α-cluster model.
doi: 10.1088/0954-3899/15/5/014
1988SU17 J.Phys.(London) G14, 1485 (1988) Dispersion Relation Analysis of the Total Neutron Cross Section Anomaly NUCLEAR REACTIONS 40Ca(n, n), E ≈ 0.5-10 MeV; calculated σ. Dispersion relations.
doi: 10.1088/0305-4616/14/12/010
1988WI04 J.Phys.(London) G14, 485 (1988) Neutron Scattering and Reactions on 93Nb from 1 to 20 MeV NUCLEAR REACTIONS 93Nb(n, γ), (n, n'), (n, nα), (n, np), (n, d), (n, 2n), (n, 3n), E=1-20 MeV; calculated absorption, total, elastic, reaction σ(E). Optical model, Hauser-Feshbach, Weisskopf-Ewing, Feshbach-Kerman-Koonin theories.
doi: 10.1088/0305-4616/14/4/010
1987AI03 J.Phys.(London) G13, 945 (1987) Weisskopf-Ewing Calculations: Neutron-induced reactions NUCLEAR REACTIONS 55Mn(n, n), 55Mn, 59Co, 63,65Cu(n, p), (n, np), (n, 2n), (n, γ), (n, α), (n, nα), (n, t), (n, nd), (n, 2p), (n, pα), 59Co, 63,65Cu(n, n'), E=1-20 MeV; calculated σ(E). Weisskopf-Ewing model.
doi: 10.1088/0305-4616/13/7/008
1987AN07 Nuovo Cim. 97A, 117 (1987) A.N.Antonov, I.Zh.Petkov, P.E.Hodgson Natural Orbital Calculations of Nucleon Momentum Distributions NUCLEAR STRUCTURE 40Ca; calculated nucleon momentum, nuclear charge distributions. 208Pb; calculated proton momentum distribution. Single particle potential method, natural orbital representation.
doi: 10.1007/BF02733842
1987HO22 Rep.Prog.Phys. 50, 1171 (1987) Compound Nucleus Reactions NUCLEAR REACTIONS, ICPND 26Mg, 56Fe(p, p), (p, p'), E=8-14 MeV; analyzed σ(E, θ). 28Si(d, α), E=9 MeV; 25Mg, 30Si(p, p), E=6, 9-10.7 MeV; 89Y(n, n), (n, n'), E=2.35 MeV; analyzed σ(θ). 181Ta(n, n'), 64Ni, 68Zn(p, n), E=0.4-5.5 MeV; 58Ni(α, p), 56Fe(n, p), E=4-30 MeV; analyzed σ(E). 181Ta(n, p), E ≤ 12 MeV; 40Ca(n, X), E=14.5 MeV; analyzed damping, escape widths. 25Mg(3He, α), E=8-20 MeV; analyzed five-excitation stage width. 27Al(3He, p), 93Nb, 181Ta, 59Co(n, X), E=2-20 MeV; analyzed σ(E), σ(En, θn). 40Ca(n, p), 59Co(p, n), E=14.5 MeV; analyzed σ(Ep, θp), σ(En, θn). 59Co(n, n'), (n, 2n), (n, pn), (n, p), (n, α), (n, αn), E=14 MeV; analyzed σ.
doi: 10.1088/0034-4885/50/9/002
1987MA61 Z.Phys. A328, 393 (1987) A.Malecki, A.N.Antonov, I.Zh.Petkov, P.E.Hodgson A Study of Short-Range Correlation Effects on Nuclear Spatial and Momentum Distribution NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated weighting functions; deduced nuclear spacial, momentum distributions short-range correlations dependences.
1986AN35 Bulg.J.Phys. 13, 110 (1986) A.N.Antonov, I.Zh.Petkov, P.E.Hodgson Nucleon Momentum Distributions in the Coherent Fluctuation Model NUCLEAR STRUCTURE 4He, 16O, 40Ca, 12C, 90Zr; calculated nucleon momentum distributions. Coherent fluctuation model.
1986FI01 J.Phys.(London) G12, 93 (1986) G.M.Field, R.Bonetti, P.E.Hodgson Pre-Equilibrium Processes in the Reactions of Neutrons on 59Co and 93Nb NUCLEAR REACTIONS 59Co, 93Nb(n, n'), (n, p), E=14 MeV; analyzed σ(E); deduced (n, 2n), (n, np) reactions. Statistical multi-step compound theory.
doi: 10.1088/0305-4616/12/2/008
1986HO28 Radiat.Eff. 95, 27 (1986) P.E.Hodgson, G.M.Field, H.Gruppelaar, P.Nagel Pre-Equilibrium Processes in Nuclear Reactions NUCLEAR REACTIONS 93Nb(n, xn), E=10, 14.6, 20, 25.7 MeV; calculated angle integrated σ(En). 59Co(n, xn), (n, xp), E=14 MeV; 65Cu(p, xn), E=26.7 MeV; calculated σ(θ), σ(θn, En), σ(θp, Ep). Semi-classical models, quantum mechanical theory.
doi: 10.1080/00337578608208667
1986ST01 Nucl.Sci.Eng. 92, 459 (1986) The Inelastic Scattering of Neutrons by 232Th NUCLEAR REACTIONS 232Th(n, n'), E ≈ 0.5-3 MeV; calculated σ(E); deduced fission, capture channel contributions. Incoherent compound plus direct components.
doi: 10.13182/NSE86-A17533
1985HO03 Nucl.Sci.Eng. 89, 111 (1985) The Inelastic Scattering of Neutrons by 238U NUCLEAR REACTIONS 238U(n, n'), E=0.2-5 MeV; analyzed σ(E); deduced direct, compound nuclear contributions. Distorted wave approach, approximate treatment of channel coupling.
doi: 10.13182/NSE85-A18185
1985WI11 J.Phys.(London) G11, 1007 (1985) Neutron Scattering and Reactions on 59Co from 1-20 MeV NUCLEAR REACTIONS 59Co(n, n), E ≈ 2-20 MeV; calculated σ(E), reaction σ(E). 59Co(n, n), E=1-8 MeV; calculated σ(θ). 59Co(n, n'), (n, 2n), (n, p), (n, α), (n, np), (n, d), (n, γ), (n, nd), (n, t), (n, 3He), (n, pα), (n, 3n), (n, nt), (n, nα), E=2-20 MeV; calculated σ(E). 59Co(n, n'), E=1-3 MeV; calculated σ(E). 59Co(n, α), (n, αX), E=5-20 MeV; calculated σ(E). 59Co(n, γ), E=2-16 MeV; calculated σ(E). Optical model, Weisskopf-Ewing, Hauser-Feshbach, Feshbach-Kerman-Koonin theories.
doi: 10.1088/0305-4616/11/9/010
1984BR25 J.Phys.(London) G10, 1683 (1984) B.A.Brown, C.R.Bronk, P.E.Hodgson Systematics of Nuclear RMS Charge Radii NUCLEAR STRUCTURE N=8-160; analyzed rms charge radii, B(E2) data; deduced deformation, zero-point vibrational motion role.
doi: 10.1088/0305-4616/10/12/008
1984GA25 Z.Phys. A318, 147 (1984) E.Gadioli, E.Gadioli-Erba, P.Guazzoni, P.E.Hodgson, L.Zetta The Mechanism of the (p, α) Reaction: Pick-up or knock-out ( Question ) NUCLEAR REACTIONS 90Zr(p, α), E=22.8 MeV; 92Zr(p, α), E=22.8, 35 MeV; 118Sn(p, α), E=20.4-22.8, 35 MeV; 92Zr(polarized p, α), E=35 MeV; 118Sn(polarized p, α), E=20.4, 22 MeV; calculated σ(θ), analyzing power vs θ; deduced pickup, knockout mechanism validity. DWBA analysis.
doi: 10.1007/BF01413463
1984SW01 J.Phys.(London) G10, 75 (1984) Nuclear Charge Distribution Differences NUCLEAR STRUCTURE 40Ca, 64,58,60,62Ni, 39K, 68,70,64Zn, 89Y, 88Sr, 207,204,206,208Pb, 203,205Tl, 209Bi, 56,54,58Fe, 92,94,96Mo; calculated isotone pair charge distribution differences. Single particle potential model, electron scattering data input.
doi: 10.1088/0305-4616/10/1/012
1983AN27 Blug.J.Phys. 10, 590 (1983) A.N.Antonov, V.A.Nikolaev, I.Zh.Petkov, P.E.Hodgson The Nucleon Momentum Distributions of 39K, 40Ca and 48Ca NUCLEAR REACTIONS 40Ca(e, e'), E=500 MeV; calculated σ(θ, E(e')). Flucton model. NUCLEAR STRUCTURE 39K, 40,48Ca; calculated proton momentum distribution. Model independent charge distributions.
1983BR05 J.Phys.(London) G9, 423 (1983) B.A.Brown, S.E.Massen, J.I.Escudero, P.E.Hodgson, G.Madurga, J.Vinas The Charge and Matter Distributions of 208Pb NUCLEAR STRUCTURE 208Pb; analyzed charge, matter distribution, single particle energies, valence orbital rms radii; deduced best potential.
doi: 10.1088/0305-4616/9/4/009
1982BA07 J.Phys.(London) G8, 525 (1982) M.Bauer, E.Hernandez-Saldana, P.E.Hodgson, J.Quintanilla A Unified Potential for Bound and Scattering States NUCLEAR REACTIONS 40,48Ca, 58Ni, 90Zr, 208Pb(p, p), 0-80 MeV; analyzed phenomenological potential fits; deduced unified bound, scattering state potential. Least-squares fit, linear, quadratic, exponential energy dependence.
doi: 10.1088/0305-4616/8/4/011
1982BO34 Phys.Rev. C26, 2417 (1982) R.Bonetti, L.Colli Milazzo, I.Doda, P.E.Hodgson Analyzing Powers in the 58Ni(p, p') Reaction Calculated with the Statistical Multistep Direct Emission Theory NUCLEAR REACTIONS 58Ni(polarized p, p'), E=65 MeV; calculated σ(θ), analyzing power vs θ. Statistical multi-step direct emission theory.
doi: 10.1103/PhysRevC.26.2417
1982KO19 Nucl.Phys. A384, 65 (1982) A.M.Kobos, B.A.Brown, P.E.Hodgson, G.R.Satchler, A.Budzanowski Folding Model Analysis of α-Particle Elastic Scattering with a Semirealistic Density-Dependent Effective Interaction NUCLEAR REACTIONS 40Ca, 46,48,50Ti, 58Ni, 90Zr, 208Pb(α, α), E=140 MeV; 58,60,62,64Ni(α, α), E=172 MeV: analyzed σ(θ). Folding model, density-dependent effective interaction.
doi: 10.1016/0375-9474(82)90305-0
1982ST07 J.Phys.(London) G8, 839 (1982) J.Streets, B.A.Brown, P.E.Hodgson Nuclear Matter Distributions NUCLEAR STRUCTURE 28Si, 32,34S, 40,42,44,48Ca, 46,48Ti, 58,60,62,64Ni, 90Zr, 116,124Sn, 208Pb; calculated nucleon density distribution, charge radii, proton-neutron radius difference. Single particle potential model.
doi: 10.1088/0305-4616/8/6/013
1981BO24 Phys.Rev. C24, 71 (1981) R.Bonetti, M.Camnasio, L.Colli Milazzo, P.E.Hodgson Analysis of Precompound Processes in (p, n) Reactions with the Statistical Multistep Direct Emission Theory NUCLEAR REACTIONS 48Ca, 90Zr, 120Sn, 208Pb(p, n), E=45 MeV; 120Sn(p, n), E=25, 35 MeV; analyzed σ(θ); deduced two-body interaction strength.
doi: 10.1103/PhysRevC.24.71
1981GY02 J.Phys.(London) G7, L209 (1981) B.Gyarmati, R.G.Lovas, T.Vertse, P.E.Hodgson Low-Energy Behaviour of the Real Depth of the Proton Optical Potential NUCLEAR REACTIONS 116Sn(p, p), (n, n), E=5-25 MeV; calculated σ(E); deduced collective effects on optical potential real term energy dependence. Model calculation, elastic to inelastic channel coupling.
doi: 10.1088/0305-4616/7/9/005
1981KU03 Phys.Lett. 100B, 453 (1981) Equivalent Bare Optical Potentials in Heavy-Ion Inelastic Scattering NUCLEAR REACTIONS 40Ca(16O, 16O'), E=60 MeV; 40Ca(13C, 13C'), E=68 MeV; calculated σ(θ). Equivalent bare optical potentials.
doi: 10.1016/0370-2693(81)90603-1
1981KU09 Nucl.Phys. A366, 320 (1981) Exit-Channel Distorting Potentials in Heavy-Ion Inelastic Scattering and the Equivalent Bare Optical Potential NUCLEAR REACTIONS 40Ca(16O, 16O'), E=60 MeV; 40Ca(13C, 13C'), E=68 MeV; 208Pb(11B, 11B'), E=72.2 MeV; 208Pb(16O, 16O'), E=80-180 MeV; calculated σ(θ). Equivalent local bare potential.
doi: 10.1016/0375-9474(81)90291-8
1981LO03 Nucl.Phys. A357, 205 (1981) R.G.Lovas, B.A.Brown, P.E.Hodgson Coulomb Mixing and Core Polarization in (p, n(bar)) Quasi-Elastic Scattering NUCLEAR REACTIONS 42,44,48Ca(p, n), E=25 MeV; 58Ni(p, n), E=22.8 MeV; calculated σ(θ). Generalized Lane model, Coulomb distortions, excess neutron polarizing effect.
doi: 10.1016/0375-9474(81)90634-5
1981OW01 J.Phys.(London) G7, 1057 (1981) A.S.Owen, B.A.Brown, P.E.Hodgson Nucleon Orbit Radii in Tin Isotopes NUCLEAR STRUCTURE 112,116,118,120,124Sn; calculated rms charge radius, proton separation, binding energies. 113,115,117,119Sn; calculated neutron radius, separation, binding energies.
doi: 10.1088/0305-4616/7/8/011
1979BR17 Phys.Lett. 85B, 167 (1979) B.A.Brown, S.E.Massen, P.E.Hodgson The Charge Distributions of the Oxygen and Calcium Isotopes NUCLEAR STRUCTURE 16,17,18O, 40,42,44,46,48Ca; calculated rms radii. Squares of single particle wave functions of occupied orbits summed, core-valence nucleon interaction, configuration mixing, iterative procedure.
doi: 10.1016/0370-2693(79)90569-0
1979BR30 J.Phys.(London) G5, 1655 (1979) B.A.Brown, S.E.Massen, P.E.Hodgson Proton and Neutron Density Distributions for A = 16-58 Nuclei NUCLEAR STRUCTURE A=16-58; calculated p, n density distributions. Squared sum of single particle functions, iterative procedure.
doi: 10.1088/0305-4616/5/12/008
1979LO05 Phys.Lett. 82B, 170 (1979) M.Lozano, G.Madurga, P.E.Hodgson Critical Radii for Alpha-Particle Elastic Scattering NUCLEAR STRUCTURE 110,112,114,116Cd, 112,114,116,118,120,122,124Sn, 122,124,126,128,130Te, 142,144,146,148,150Nd, 144,146,148,150,152Sm, 204,206,208Pb; calculated nuclear density distribution using Saxon-Woods single particle functions; deduced method to obtain α-optical potentials from target nucleus structure.
doi: 10.1016/0370-2693(79)90727-5
1979MA10 Nuovo Cim. 49A, 412 (1979) F.Malaguti, A.Uguzzoni, E.Verondini, P.E.Hodgson Charge Density and Single-Particle Structure: the Nuclei 39K, 40Ca and 48Ca NUCLEAR STRUCTURE 39K, 40,48Ca; calculated charge distributions. One-body nonlocal potential.
doi: 10.1007/BF02773455
1979MA33 Nuovo Cim. 53A, 1 (1979) F.Malaguti, A.Uguzzoni, E.Verondini, P.E.Hodgson The Charge Densities and Single-Particle Structure of the Even Zirconium Isotopes NUCLEAR STRUCTURE 90,92,94Zr; calculated densities, squared one-body potential single-particle functions, weighted by occupation numbers.
1979RA33 Phys.Rev. C20, 2403 (1979) Neutron Densities and the Single Particle Structure of Several Even-Even Nuclei from 40Ca to 208Pb NUCLEAR STRUCTURE 40,48Ca, 58,64Ni, 116,124Sn, 208Pb; calculated proton, neutron one-body densities. Summed squares of single particle functions, nonlocal potentials, nonorthogonal effects.
doi: 10.1103/PhysRevC.20.2403
1978BE56 J.Phys.(London) G4, L287 (1978) The Systematics of Nuclear Bound States NUCLEAR STRUCTURE 12C, 16O, 40Ca, 48Ca, 58Ni, 90Zr, 208Pb; calculated charge distributions using a realistic potential that reproduces bound single particle states.
doi: 10.1088/0305-4616/4/2/018
1978LE06 Nucl.Phys. A295, 301 (1978) Microscopic Optical Model Analyses of Proton and Neutron Elastic Scattering Cross Sections NUCLEAR REACTIONS 12C, 16O, 27Al, 40Ca, 56Fe, 58,60,62,64Ni, 63,65Cu, 68Zn, 90Zr, 116,120Sn, 208Pb, 209Bi(n, n), E=1-15 MeV; 12C, 16O, 27Al, 40Ca, 56Fe, 58,60,62,64Ni, 63,65Cu, 68Zn, 90Zr, 116,120Sn, 208Pb, 209Bi(p, p), E=10-70 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(78)90118-5
1978MA09 Nucl.Phys. A297, 287 (1978) F.Malaguti, A.Uguzzoni, E.Verondini, P.E.Hodgson Charge Density and Single-Particle Structure of 58Ni NUCLEAR STRUCTURE 58Ni; calculated charge distribution.
doi: 10.1016/0375-9474(78)90277-4
1976MA04 Nucl.Phys. A257, 37 (1976) The Systematics of Nuclear Single-Particle States (III). Widths and Rearrangement Energies NUCLEAR STRUCTURE A=6-65; calculated single-particle level widths, rearrangement energies.
doi: 10.1016/0375-9474(76)90473-5
1975GE05 Nucl.Phys. A246, 173 (1975) Microscopic Analyses of Proton Inelastic Scattering by 16O and 40Ca Using a Complex t-Matrix NUCLEAR REACTIONS 16O, 40Ca(p, p'), E=25-61 MeV; calculated σ(Ep', θ).
doi: 10.1016/0375-9474(75)90570-9
1973MA48 Nucl.Phys. A215, 243 (1973) The Systematics of Nuclear Single-Particle States (II). The Region A < 35 NUCLEAR STRUCTURE 4He, 6,7Li, 9,10Be, 10,11B, 12,13,14C, 14,15N, 16,17,18O, 19F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34S, 35Cl; levels calculated binding energies.
doi: 10.1016/0375-9474(73)90653-2
1973MI06 Nucl.Phys. A209, 59 (1973) The Systematics of Nuclear Single-Particle States (I). The Region 35 < A < 65 NUCLEAR STRUCTURE 36,38,40Ar, 40,42,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 51V, 48,50,52,54Cr, 55Mn, 52,54,56,58Fe, 57,59Co, 56,58,60,62,64Ni, 63,65Cu; calculated binding energies.
doi: 10.1016/0375-9474(73)90051-1
1969GO14 Nucl.Phys. A136, 385 (1969) V.Gomes Porto, N.Ueta, R.A.Douglas, O.Sala, D.Wilmore, B.A.Robson, P.E.Hodgson Deuteron Induced Reactions on 14N NUCLEAR REACTIONS 14N(d, d), (d, p), (d, α), E = 1-3.1 MeV; measured σ(E;θ), σ(E;Ep, θ), σ(E;Eα, θ).
doi: 10.1016/0375-9474(69)90060-8
1968BU10 Nucl.Phys. A117, 509(1968) A.Budzanowski, A.D.Hill, P.E.Hodgson The Elastic and Inelastic Scattering of 25 MeV Alpha Particles by 31P, 32S and 40Ca NUCLEAR REACTIONS 31P, 32S, 40Ca(α, α'), E=25 MeV; measured σ(Eα', θ). 31P, 32S, 40Ca levels deduced deformation parameters. Natural targets.
doi: 10.1016/0375-9474(68)90827-0
1968DI02 Nucl.Phys. A106, 527 (1968) O.Dietzsch, D.Wilmore, P.E.Hodgson Analysis of the 24Mg(d, n)25Al Reaction from 1.38 to 2.8 MeV NUCLEAR REACTIONS 24Mg(d, n), E = 1.3 to 2.8 MeV; measured σ(E; En, θ). Natural, enriched targets.
doi: 10.1016/0375-9474(68)90514-9
1968DI06 Nucl.Phys. A114, 330(1968) O.Dietzsch, R.A.Douglas, E.F.Pessoa, V.G.Porto, E.W.Hamburger, T.Polga, O.Sala, S.M.Perez, P.E.Hodgson Deuteron-Induced Reactions on 16O NUCLEAR REACTIONS 16O(d, d), (d, p), (d, n), (d, α), E=2 to 3.5 MeV; measured σ(E;θ).
doi: 10.1016/0375-9474(68)90358-8
1968TJ01 Nucl.Phys. A106, 85 (1968) H.R.E.Tjin a Djie, K.Mulder, F.Udo, A.Groeneveld, L.A.C.Koerts, A.D.Hill, P.E.Hodgson Inelastic Scattering of 26 MeV Deuterons NUCLEAR REACTIONS 24,26Mg, 40Ca, 56Fe, 58Ni, Zn, 140Ce(d, d'), E = . 24,26Mg, 40Ca, 56Fe, 58Ni, Zn, 140Ce deduced deformation parameters. Enriched 58Ni, natural targets.
doi: 10.1016/0375-9474(67)90829-9
1966GA09 Nucl.Phys. 82, 161(1966) A.Gallman, P.Fintz, P.E.Hodgson Reactions (d, p) sur 11B, 12C, 14N et 16O a E < 5.5 MeV NUCLEAR REACTIONS 12C, 16O(d, d), E = 4 MeV; measured σ(θ). 11B(d, p), E = 5.5 MeV; 12C(d, p), E = 1.2-4.5 MeV; 14N(d, p), E = 1.3-5.5 MeV; 16O(d, p), E = 1.3, 4 MeV; measured σ(Ep, θ). 12B, 13C, 15N, 17O deduced S.
doi: 10.1016/0029-5582(66)90529-3
1966GA17 Nucl.Phys. 88, 654(1966); Erratum Nucl.Phys. A99, 696(1967) A.Gallmann, P.Wagner, G.Franck, D.Wilmore, P.E.Hodgson Analyse des Reactions 25Mg(p, p)25Mg et 24Mg(d, p)25Mg a 5 et a 6 MeV NUCLEAR REACTIONS 25Mg(p, p'), E = 5, 6 MeV; 24Mg(d, p), E = 5, 6 MeV; measured σ(Ep', θ). Enriched target.
doi: 10.1016/0029-5582(66)90422-6
1966GA18 Nucl.Phys. 88, 675(1966) A.Gallmann, P.Wagner, P.E.Hodgson Fluctuations des Sections Efficaces des Reactions 25Mg(p, p)25Mg et 24Mg(d, p)25Mg NUCLEAR REACTIONS 25Mg(p, p), E = 4.5-6.1 MeV; 24Mg(d, p), E = 2.8-6.1 MeV; measured σ(E;Ep, θ). Fluctuation analysis. Enriched targets.
doi: 10.1016/0029-5582(66)90423-8
1965GA02 Phys.Rev. 138, B560 (1965) A.Gallman, F.Hibou, P.Fintz, P.E.Hodgson, E.K.Warburton B10(d, p)B12 Angular Distributions at E = 5.5 MeV for the B12 2.62- and 2.72-MeV Levels NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B560
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
1963BU24 Nucl.Phys. 49, 144 (1963) A.Budzanowski, L.Freindl, K.Grotowski, M.Rzeszutko, M.Slapa, J.Szmider, P.E.Hodgson Elastic scattering and total reaction cross-sections for the interaction of 12.8 MeV deuterons with 12C, 58Ni, 60Ni and 209Bi nuclei NUCLEAR REACTIONS 12C(d, n), 12C(d, X), 58Ni(d, d), 58Ni(d, n), 58Ni(d, X), 60Ni(d, 2n), 60Ni(d, d), 60Ni(d, n), 60Ni(d, X), 209Bi(d, 2n), 209Bi(d, d), 209Bi(d, n), 209Bi(d, X), E=12.8 MeV; measured products, 59Cu, Eν, Iν; deduced σ, σ(E), σ(θ). Data were imported from EXFOR entry D0576.
doi: 10.1016/0029-5582(63)90082-8
Back to query form [Next] |