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NSR database version of April 11, 2024.

Search: Author = P.E.Hodgson

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0443.


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
Citations: PlumX Metrics


2003HO01      Phys.Rep. 374, 1 (2003)

P.E.Hodgson, E.Betak

Cluster emission, transfer and capture in nuclear reactions

doi: 10.1016/S0370-1573(02)00268-5
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0443.


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
Citations: PlumX Metrics


1998BE23      Rep.Prog.Phys. 61, 483 (1998)

E.Betak, P.E.Hodgson

Particle-Hole State Densities in Pre-Equilibrium Nuclear Reaction Models

doi: 10.1088/0034-4885/61/5/002
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0507.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0508.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1996DE58      J.Phys.(London) G22, 1813 (1996)

P.Demetriou, P.E.Hodgson

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0936.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0513.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1845.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1994HO20      Z.Phys. A349, 197 (1994)

P.E.Hodgson

A Survey of Alpha-Clustering

NUCLEAR STRUCTURE A=24-215; compiled, reviewed α-clustering features.

doi: 10.1007/BF01288959
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0179.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1993OL07      Roum.J.Phys. 38, 371 (1993)

H.B.Olaniyi, P.E.Hodgson

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1992HO15      Hyperfine Interactions 74, 75 (1992)

P.E.Hodgson

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0535.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0180.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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)

N.Koumdjieva, P.E.Hodgson

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
Citations: PlumX Metrics


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
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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
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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
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1988SU17      J.Phys.(London) G14, 1485 (1988)

Su Zongdi, P.E.Hodgson

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
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1988WI04      J.Phys.(London) G14, 485 (1988)

D.Wilmore, P.E.Hodgson

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
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1987AI03      J.Phys.(London) G13, 945 (1987)

S.Ait-Tahar, P.E.Hodgson

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
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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
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1987HO22      Rep.Prog.Phys. 50, 1171 (1987)

P.E.Hodgson

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
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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
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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
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1986ST01      Nucl.Sci.Eng. 92, 459 (1986)

A.M.Street, P.E.Hodgson

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
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1985HO03      Nucl.Sci.Eng. 89, 111 (1985)

P.E.Hodgson, A.M.Kobos

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
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1985WI11      J.Phys.(London) G11, 1007 (1985)

D.Wilmore, P.E.Hodgson

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
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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
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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
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1984SW01      J.Phys.(London) G10, 75 (1984)

R.J.M.Sweet, P.E.Hodgson

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
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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
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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
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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
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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
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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
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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
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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
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1981KU03      Phys.Lett. 100B, 453 (1981)

K.-I.Kubo, P.E.Hodgson

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
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1981KU09      Nucl.Phys. A366, 320 (1981)

K.-I.Kubo, P.E.Hodgson

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
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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
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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
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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
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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
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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
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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
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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)

L.Ray, P.E.Hodgson

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
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1978BE56      J.Phys.(London) G4, L287 (1978)

K.Bear, P.E.Hodgson

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
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1978LE06      Nucl.Phys. A295, 301 (1978)

A.Lejeune, P.E.Hodgson

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
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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
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1976MA04      Nucl.Phys. A257, 37 (1976)

F.Malaguti, P.E.Hodgson

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
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1975GE05      Nucl.Phys. A246, 173 (1975)

H.V.Geramb, P.E.Hodgson

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
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1973MA48      Nucl.Phys. A215, 243 (1973)

F.Malaguti, P.E.Hodgson

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
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1973MI06      Nucl.Phys. A209, 59 (1973)

D.J.Millener, P.E.Hodgson

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0274.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1102.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0576.


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