Nuclear Science References (NSR)

Oscillating-Correlated Nonstatistical Structures, Slow Spin Decoherence, and Hyperdeformed Coherent Rotational States in ²⁴Mg + ²⁴Mg and ²⁸Si + ²⁸Si Scattering

NUCLEAR REACTIONS ²⁴Mg(²⁴Mg, ²⁴Mg), (²⁴Mg, ²⁴Mg'), E(cm)=42-56 MeV; ²⁸Si(²⁸Si, ²⁸Si), (²⁸Si, ²⁸Si'), E(cm)=52.5-60.5 MeV; analyzed energy autocorrelation functions; deduced dinucleus hyperdeformed coherent rotational states.

doi: 10.1103/PhysRevLett.83.504
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1999ZH34 Phys.Rev. C60, 054618 (1999)

Y.-S.Zhang, B.A.Robson, Y.Zhou, Y.-G.Li

Spin Effect of Antiproton-Nucleus Inelastic Scattering

NUCLEAR REACTIONS ¹²C(p-bar, p-bar'), E=46.8, 179.7 MeV; calculated σ(E, θ), induced polarization; deduced spin-orbit contribution. Comparison with data.

doi: 10.1103/PhysRevC.60.054618
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1997KU25 Z.Phys. A359, 145 (1997)

S.Yu.Kun, U.Abbondanno, M.Bruno, N.Cindro, M.D'Agostino, P.M.Milazzo, R.A.Ricci, T.Ritz, B.A.Robson, W.Scheid, A.V.Vagov, G.Vannini, L.Vannucci

Damped Oscillations in the Energy Autocorrelation Functions of the ⁵⁸Ni + ⁴⁶Ti Elastic and ⁵⁸Ni + ⁶²Ni Elastic and Inelastic Scattering Cross Sections

NUCLEAR REACTIONS ⁴⁶Ti(⁵⁸Ni, ⁵⁸Ni), E(cm)=95-106 MeV; ⁶²Ni(⁵⁸Ni, ⁵⁸Ni), (⁵⁸Ni, X), E(cm)=113-119 MeV; analyzed σ(E); deduced energy autocorrelation functions, possible decoherence, rotational damping effects.

doi: 10.1007/s002180050381
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1997KU31 Z.Phys. A359, 263 (1997)

S.Yu.Kun, D.J.Hinde, M.Dasgupta, J.R.Leigh, J.C.Mein, C.R.Morton, J.O.Newton, B.A.Robson, H.Timmers, A.V.Vagov

Correlated Oscillations in the Excitation Functions of Deep-Inelastic Collisions: Evidence for nuclear pulsars ( Question )

NUCLEAR REACTIONS ⁸⁹Y(¹⁹F, X), E=135-140 MeV; measured projectile-like fragment yields; deduced energy autocorrelation functions oscillations. Dissipative reactions, quantum chaos.

doi: 10.1007/s002180050401
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1996LI39 Phys.Rev. C54, 2509 (1996)

J.-F.Liu, Y.-S.Zhang, C.-Y.Yang, J.-F.Shen, B.A.Robson

Elastic and Inelastic Scattering of 1.37 GeV α Particles from ¹²C and ^40,42,44,48Ca

NUCLEAR REACTIONS ¹²C, ^40,42,44,48Ca(α, α), (α, α'), E=1.37 GeV; analyzed σ(θ). Glauber theory framework, Tassie model collective excitations.

doi: 10.1103/PhysRevC.54.2509
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1996ZH10 Phys.Rev. C54, 332 (1996)

Y.-S.Zhang, J.-F.Liu, B.A.Robson, Y.-G.Li

Antiproton-Nucleus Elastic and Inelastic Scattering at Intermediate Energies

NUCLEAR REACTIONS ¹²C(p-bar, p-bar), (p-bar, p-bar'), E=179.7-1833 MeV; ⁴⁰Ca, ¹⁶O, ²⁰⁸Pb(p-bar, p-bar), E ≈ 179-1833 MeV; analyzed σ(θ). Eikonal approximation.

doi: 10.1103/PhysRevC.54.332
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1993KU23 Z.Phys. A347, 123 (1993)

S.Yu.Kun, M.Papa, B.A.Robson

Time Evolution of Collision Process and Applicability of Angular Momentum Correlation Description for Heavy-Ion Reactions

NUCLEAR REACTIONS ⁶⁴Ni(²⁸Si, X), E=123 MeV; analyzed σ(fragment θ, E); deduced pole spin correlation meaningfulness.

doi: 10.1007/BF01284679
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1993RO05 Nucl.Phys. A554, 322 (1993)

B.A.Robson, R.H.Spear, W.J.Vermeer, M.Zielinska-Pfabe

Low-Energy Behaviour of the Heavy-Ion Optical Model Potentials for ¹²C and ¹⁶O Scattering from ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹²C, ¹²C), (¹²C, ¹²C'), E=42-61 MeV; measured σ(θ); deduced model parameters. Coupled-channels analysis, other data analyzed.

doi: 10.1016/0375-9474(93)90344-W
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1991GA14 Nucl.Phys. A529, 234 (1991)

C.Gao, Y.Kondo, B.A.Robson

Analysis of Resonant Structures in the ¹⁶O + ²⁰Ne System using a Deep Optical Potential and the LCNO Model

NUCLEAR REACTIONS ²⁰Ne(¹⁶O, ¹⁶O), E(cm)=20-40 MeV; calculated σ(θ) vs E; deduced model parameters. Optical, nuclear orbital linear combination models.

doi: 10.1016/0375-9474(91)90793-6
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1989KO23 Phys.Lett. 227B, 310 (1989)

Y.Kondo, B.A.Robson, R.Smith

A Deep Potential Description of the ¹⁶O + ¹⁶O System

NUCLEAR REACTIONS ¹⁶O(¹⁶O, ¹⁶O), E(cm)=15-35 MeV; calculated σ(θ) vs E, absorption σ(E); deduced model parameters. ³²S deduced possible quasimolecular states.

doi: 10.1016/0370-2693(89)90935-0
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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
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1988LI01 Phys.Lett. 200B, 263 (1988)

C.S.Lim, M.D.Rebgetz, R.H.Spear, W.J.Vermeer, M.P.Fewell, B.A.Robson, R.Smith

Energy Dependence of the ¹⁶O-²⁰⁸Pb Effective Interaction

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, ¹⁶O), (¹⁶O, ¹⁶O'), E=57-79 MeV; measured σ(ratio). ²⁰⁸Pb level deduced excitation probability. Effective interaction description, Coulomb-nuclear interference effects.

doi: 10.1016/0370-2693(88)90768-X
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1987KO03 Phys.Rev. C35, 828 (1987)

Y.Kondo, B.A.Robson, J.J.M.Bokhorst, D.J.Hinde, J.R.Leigh

Angular Momentum Distribution in Heavy Ion Fusion Reactions

NUCLEAR REACTIONS ¹²⁴Sn(⁵⁸Ni, F), E=225-250 MeV; measured fission σ(E); analyzed fusion σ(E) data; deduced model parameters. Enriched target, ΔE-E telescope.

doi: 10.1103/PhysRevC.35.828
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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
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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
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1985KO38 Phys.Lett. 162B, 39 (1985)

Y.Kondo, B.A.Robson, R.Smith, H.H.Wolter

Transfer Contribution to Elastic ¹⁶O + ²⁰Ne Scattering and Parity-Dependent Interactions

NUCLEAR REACTIONS ²⁰Ne(¹⁶O, ¹⁶O), E(cm)=22-40 MeV; calculated σ(θ); deduced potential parameters, reaction mechanism.

doi: 10.1016/0370-2693(85)91057-3
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1985KO43 Nucl.Phys. A437, 117 (1985)

Y.Kondo, B.A.Robson, R.Smith

Coupled-Channel Description of Resonant Structures in the ¹⁶O + ²⁰Ne System

NUCLEAR REACTIONS, ICPND ²⁰Ne(¹⁶O, ¹⁶O), (¹⁶O, ¹⁶O'), E(cm)=24.5-35.5 MeV; analyzed σ(θ), σ(E), reaction σ(E). ³⁶S deduced resonances, J, π. Coupled-channels model.

doi: 10.1016/0375-9474(85)90229-5
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1983KO31 Nucl.Phys. A410, 289 (1983)

Y.Kondo, B.A.Robson, R.Smith

Resonant Structures in the ¹⁶O + ²⁰Ne System

NUCLEAR REACTIONS ²⁰Ne(¹⁶O, ¹⁶O), E(cm)=24.5-35.5 MeV; ²⁰Ne(¹⁶O, ¹²C), E(cm)=22.8-38.6 MeV; analyzed σ(θ) vs E. ²⁴Mg(¹²C, ¹²C), E(cm)=26.67 MeV; analyzed σ(θ); deduced optical model parameters. Exact finite-range DWBA calculations.

doi: 10.1016/0375-9474(83)90203-8
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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
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1983RO05 Phys.Lett. 123B, 160 (1983)

B.A.Robson, R.Smith

Resonant Structures in the ²⁴Mg(¹⁶O, ¹²C)²⁸Si Reaction

NUCLEAR REACTIONS ²⁴Mg(¹⁶O, ¹²C), E(cm)=28-50 MeV; analyzed σ(θ) vs E. ⁴⁰Ca deduced resonances, J, π. Exact, finite-range DWBA, spin-, parity-dependent term in entrance channel potentials.

doi: 10.1016/0370-2693(83)90413-6
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1982BA29 Nucl.Phys. A381, 138 (1982)

R.F.Barrett, R.A.Baldock, B.A.Robson

Antisymmetrisation Effects in Composite Particle Scattering

NUCLEAR REACTIONS ⁴He(α, α), E=0-30 MeV; calculated phase shifts. Antisymmetrization effects, equivalent local potential.

doi: 10.1016/0375-9474(82)90502-4
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1981BA02 Nucl.Phys. A351, 157 (1981)

R.A.Baldock, B.A.Robson, R.F.Barrett

Nucleon Exchange Effects in ¹⁶O-¹⁶O Elastic Scattering

NUCLEAR REACTIONS ¹⁶O(¹⁶O, ¹⁶O), E(cm)=10-36 MeV; calculated phase shifts; deduced nucleon exchange effects. Microscopic method, natural boundary condition, antisymmetrized wave function.

doi: 10.1016/0375-9474(81)90551-0
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1981BA32 Nucl.Phys. A366, 270 (1981)

R.A.Baldock, B.A.Robson, R.F.Barrett

Application of an Inverse-Scattering Method to Determine the Effective Interaction between Composite Particles

NUCLEAR REACTIONS ⁴He(α, α), E=5-30 MeV; calculated effective potential. Inverse scattering method.

doi: 10.1016/0375-9474(81)90288-8
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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
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1979BA18 Nucl.Phys. A321, 171 (1979)

R.A.Baldock, R.F.Barrett, B.A.Robson

Natural Boundary Condition Methods for the Microscopic Treatment of Composite-Particle Scattering

NUCLEAR REACTIONS ⁴He(α, α), E(cm)= < 40 MeV; calculated phase shifts. Natural boundary condition, generator coordinate methods.

doi: 10.1016/0375-9474(79)90690-0
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1978ZE02 Nucl.Phys. A301, 130 (1978)

A.F.Zeller, G.T.Hickey, D.C.Weisser, D.F.Hebbard, B.A.Robson

The ²⁶Mg(¹⁴N, ¹⁰B)³⁰Si and ²⁶Mg(¹⁴N, ¹¹B)²⁹Si Reactions

NUCLEAR REACTIONS ²⁶Mg(¹⁴N, ¹⁴N), (¹⁴N, ¹⁰B), (¹⁴N, ¹¹B), E=60-95 MeV; measured σ(E, θ); deduced optical model parameters, reaction mechanism. ³⁰Si levels deduced S. DWBA, Hauser-Feshbach analysis. Enriched targets.

doi: 10.1016/0375-9474(78)90133-1
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1976AH02 Nucl.Phys. A257, 378 (1976)

S.S.Ahmad, R.F.Barrett, B.A.Robson

Natural Boundary Condition Methods for Nuclear Reactions

NUCLEAR REACTIONS ¹²C(n, n), E(cm) < 4 MeV; calculated σ.

doi: 10.1016/0375-9474(76)90577-7
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1974DE40 Nucl.Phys. A232, 493 (1974)

G.Delic, B.A.Robson

The Deuteron D-State and Exact Finite-Range DWBA Calculations for ⁵²Cr(d, p)⁵³Cr

NUCLEAR REACTIONS ⁵²Cr(polarized d, p), E=10 MeV; calculated σ(Ep, θ), A(θ).

doi: 10.1016/0375-9474(74)90634-4
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1974IR01 Nucl.Phys. A218, 504 (1974)

M.Irshad, B.A.Robson

Elastic Scattering of 15 MeV Deuterons

NUCLEAR REACTIONS ⁵²Cr, ⁹⁰Zr, ¹²²Sn(polarized d, d); measured nothing, analyzed σ, analyzing power data.

doi: 10.1016/0375-9474(74)90038-4
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1972DE42 Nucl.Phys. A193, 510 (1972)

G.Delic, B.A.Robson

j-Dependence in l = 3 Transitions in (d, p) and (p, d) Reactions

NUCLEAR REACTIONS ⁵⁴Cr(p, d), E=17.5 MeV; calculated σ(θ), analyzing power(θ), P(θ); deduced deuteron D-state effects.

doi: 10.1016/0375-9474(72)90337-5
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1972RO07 Nucl.Phys. A184, 50 (1972)

B.A.Robson, W.J.Van Megen

Comparison of Feshbach and R-Matrix Reaction Theories for ¹²C(n, n)¹²C (I). Shell Model

NUCLEAR REACTIONS ¹²C(n, n), E < 5 MeV; calculated σ(E). ¹³C calculated levels. Feshbach, r-matrix theories; shell model.

doi: 10.1016/0375-9474(72)90443-5
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1972RO08 Nucl.Phys. A184, 67 (1972)

B.A.Robson, W.J.Van Megen

Comparison of Feshbach and R-Matrix Reaction Theories for ¹²C(n, n)¹²C (II). Particle-Rotator Model

NUCLEAR REACTIONS ¹²C(n, n), E < 5 MeV; calculated σ(E). ¹³C calculated levels. Feshbach, r-matrix theories; particle-rotator model.

doi: 10.1016/0375-9474(72)90444-7
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1970DE33 Nucl.Phys. A156, 97 (1970)

G.Delic, B.A.Robson

DWBA Calculations for (d, p) Reactions Including the d-State of the Deuteron

NUCLEAR REACTIONS ⁵²Cr(d, p), E=8 MeV; calculated σ(θ);analyzing power(θ).

doi: 10.1016/0375-9474(70)91118-8
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1970PO03 Nucl.Phys. A147, 65 (1970)

D.L.Powell, G.M.Crawley, B.V.N.Rao, B.A.Robson

Deuteron-Induced Reactions in ⁶Li, ⁹Be and ¹⁰B at Bombarding Energies of 4.5 to 6.0 MeV

NUCLEAR REACTIONS ⁶Li(d, d), (d, p), E=4.5-5.5 MeV; measured σ(E, θ), σ(E, Ep, θ). ⁹Be(d, d), (d, p), E=4.5-6.0 MeV; measured σ(E, θ), σ(E, Ep, θ). ¹⁰B(d, p), E=4.5-5.5 MeV; measured σ(E, Ep, θ). Enriched targets.

doi: 10.1016/0375-9474(70)90510-5
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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
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1969CO02 Nucl.Phys. A127, 95 (1969)

H.Cords, G.U.Din, B.A.Robson

Deuteron-Induced Reactions in ¹²C at Bombarding Energies of 5 to 10 MeV

NUCLEAR REACTIONS ¹²C(d, d), (d, p), (d, α), E=5 to 10 MeV; measured σ(E, θ), σ(E;Ep, θ), σ(E;Eα, θ). Natural target.

doi: 10.1016/0375-9474(69)90770-2
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1969CO12 Nucl.Phys. A134, 561 (1969)

H.Cords, G.U.Din, B.A.Robson

Tensor Polarization and Reactions of Deuterons on ¹⁶O at Bombarding Energies of 4.4 to 8.4 MeV

NUCLEAR REACTIONS ¹⁶O(d, d), (d, p), (d, α), E = 4.4 to 8.4 MeV; measured tensor polarization (θ), σ(E, θ). Natural target.

doi: 10.1016/0375-9474(69)90022-0
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1969DE17 Nucl.Phys. A134, 470 (1969)

G.Delic, B.A.Robson

J-Dependence in L= 1 Transitions in Cr(d, p) Reactions

NUCLEAR REACTIONS ^50,52Cr(d, p), E=7.5, 8 MeV; measured σ(θ), vector analyzing power; deduced J-dependence of L=1 transitions. ^51,53Cr levels deduced S. Reanalysis using DWBA.

doi: 10.1016/0375-9474(69)91069-0
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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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1968CO10 Nucl.Phys. A113, 608(1968)

H.Cords, G.U.Din, M.Ivanovich, B.A.Robson

Tensor Polarization of Deuterons from ¹²C-d Elastic Scattering

NUCLEAR REACTIONS ¹²C(d, d), E=3.5 to 7.1 MeV; measured tensor polarization (E, θ). Natural target.

doi: 10.1016/0375-9474(68)90170-X
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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
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1965PA10 Proc.Phys.Soc.(London) 86, 1297 (1965)

J.R.Patterson, J.M.Poate, E.W.Titterton, B.A.Robson

A Study of the Reaction ¹⁰B(³He, d)¹¹C Between 3.5 and 10 MeV

NUCLEAR STRUCTURE ¹⁰B, ¹³N; measured not abstracted; deduced nuclear properties.

doi: 10.1088/0370-1328/86/6/317
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1964BR25 Proc. Phys. Soc. (London) 84, 201 (1964)

T.A.Brinkley, B.A.Robson, E.W.Titterton

The Mechanism of the Reaction ¹²C(n, n')3α at 14.18 MeV Neutron Energy

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

doi: 10.1088/0370-1328/84/2/303
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1963HE04 Nucl.Phys. 42, 563 (1963)

D.F.Hebbard, B.A.Robson

Tables of Whittaker Functions and their Logarithmic Derivatives

doi: 10.1016/0029-5582(63)90757-0
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1963RO22 Nucl.Phys. 46, 321 (1963)

B.A.Robson, E.Weigold

Reactions Induced by Low Energy Deuteron Bombardment of B¹¹

NUCLEAR STRUCTURE ¹¹B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90603-5
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1963SH10 Bull.Am.Phys.Soc. 8, No.6, 477, N3 (1963)

R.E.Shamu, J.G.Jenkin, B.A.Robson

Neutron-Alpha Scattering in the 20-MeV Range

1962BR11 Nuclear Phys. 29, 442 (1962)

E.Bradford, B.A.Robson

Distorted Wave Analysis of the Inelastic Scattering of Protons and the 9.63 MeV State of C¹²

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90194-3
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1961BR08 Phys.Rev.Letters 6, 550 (1961); Erratum Phys.Rev.Letters 6, 711 (1961)

E.Bradford, B.A.Robson

Inelastic Scattering of 18.9-MeV Nucleons from the 9.6-MeV State of C¹²

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.6.550
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1960RO24 Proc.Phys.Soc.(London) 76, 611 (1960)

B.A.Robson, D.Robson

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