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Search: Author = J.R.Leigh

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2002MU17      Phys.Rev. C66, 034607 (2002)

A.Mukherjee, M.Dasgupta, D.J.Hinde, K.Hagino, J.R.Leigh, J.C.Mein, C.R.Morton, J.O.Newton, H.Timmers

Dominance of Collective Over Proton Transfer Couplings in the Fusion of 32S and 34S with 89Y

NUCLEAR REACTIONS 89Y(32S, X), (34S, X), E=99-126 MeV; measured fusion σ; deduced barrier distributions. Coupled-channels analysis.

doi: 10.1103/PhysRevC.66.034607
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0588.

2001NE14      Phys.Rev. C64, 064608 (2001)

J.O.Newton, C.R.Morton, M.Dasgupta, J.R.Leigh, J.C.Mein, D.J.Hinde, H.Timmers, K.Hagino

Experimental Barrier Distributions for the Fusion of 12C, 16O, 28Si, and 35Cl with 92Zr and Coupled-Channel Analyses

NUCLEAR REACTIONS 92Zr(12C, X), E=31-50 MeV; 92Zr(16O, X), E=44-80 MeV; 92Zr(28Si, X), E=86-115 MeV; 92Zr(35Cl, X), E=107-135 MeV; measured fusion σ; deduced barrier distributions. Comparisons with coupled channels calculations.

doi: 10.1103/PhysRevC.64.064608
Citations: PlumX Metrics

1999HI07      Phys.Rev. C60, 054602 (1999)

D.J.Hinde, A.C.Berriman, M.Dasgupta, J.R.Leigh, J.C.Mein, C.R.Morton, J.O.Newton

Limiting Angular Momentum for Statistical Model Description of Fission

NUCLEAR REACTIONS 208Pb(19F, X), E=82-135 MeV; measured fission, evaporation residue σ, fission fragment angular distributions, anisotropies; deduced fusion barrier distribution. Comparison with statistical model calculations.

doi: 10.1103/PhysRevC.60.054602
Citations: PlumX Metrics

1998DA06      Nucl.Phys. A630, 78c (1998)

M.Dasgupta, D.J.Hinde, J.R.Leigh, K.Hagino

Barrier Distributions as a Tool to Investigate Fusion and Fission

doi: 10.1016/S0375-9474(97)00745-8
Citations: PlumX Metrics

1998HI20      Phys.Rev.Lett. 81, 4777 (1998)

D.J.Hinde, M.Dasgupta, J.R.Leigh, D.G.Marinaro, J.O.Newton

Comment on ' Anomalous Peaklike Structure in the Fission Fragment Anisotropies at Sub-Barrier Energies in 11B, 12C, 16O, 19F + 232Th Reactions '

NUCLEAR REACTIONS 232Th(19F, X), E not given; measured fission fragment anisotropies; deduced transfer fission, compound nucleus fission components.

doi: 10.1103/PhysRevLett.81.4777
Citations: PlumX Metrics

1998KE01      Nucl.Phys. A628, 1 (1998)

N.Keeley, J.S.Lilley, J.X.Wei, M.Dasgupta, D.J.Hinde, J.R.Leigh, J.C.Mein, C.R.Morton, H.Timmers, N.Rowley

Fusion Excitation Function Measurements for the 16O + 58Ni and 16O + 62Ni Systems

NUCLEAR REACTIONS 58,62Ni(16O, 16O), (16O, 16O'), (16O, X), E=35-60 MeV; measured elastic, inelastic, transfer reaction differential σ; deduced σ, barrier distributions. Coupled-reaction-channels calculations.

doi: 10.1016/S0375-9474(97)00597-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1532.

1997DA22      J.Phys.(London) G23, 1491 (1997)

M.Dasgupta, K.Hagino, C.R.Morton, D.J.Hinde, J.R.Leigh, N.Takigawa, H.Timmers, J.O.Newton

Evidence of Double Phonon Excitations in the Fusion of 16O + 208Pb

NUCLEAR REACTIONS, ICPND 208Pb(16O, X), E(cm)=68-83 MeV; measured fusion σ, barrier distribution; deduced coupling to double-phonon surface vibrations role in fusion dynamics.

doi: 10.1088/0954-3899/23/10/041
Citations: PlumX Metrics

1997HA02      Phys.Rev. C55, 276 (1997)

K.Hagino, N.Takigawa, M.Dasgupta, D.J.Hinde, J.R.Leigh

Validity of the Linear Coupling Approximation in Heavy-Ion Fusion Reactions at Sub-Barrier Energies

NUCLEAR REACTIONS, ICPND 92,96Zr(64Ni, X), E(cm)=120-150 MeV; 112Cd(16O, F), E(cm)=40-65 MeV; 144Sm(16O, F), E=55-75 MeV; calculated fusion σ(E).

doi: 10.1103/PhysRevC.55.276
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1997HA46      Phys.Rev.Lett. 79, 2014 (1997)

K.Hagino, N.Takigawa, M.Dasgupta, D.J.Hinde, J.R.Leigh

Adiabatic Quantum Tunneling in Heavy-Ion Sub-Barrier Fusion

NUCLEAR REACTIONS, ICPND 144Sm(16O, X), E(cm)=50-80 MeV; 194Pt(40Ca, X), E(cm)=160-200 MeV; 192Os(40Ca, X), E(cm)=150-190 MeV; calculated fusion σ with, without projectile excitation; deduced reaction mechanism, fusion barrier features. Comparison with data. Coupled-channels calculations.

doi: 10.1103/PhysRevLett.79.2014
Citations: PlumX Metrics

1997HA50      J.Phys.(London) G23, 1413 (1997)

K.Hagino, N.Takigawa, M.Dasgupta, D.J.Hinde, J.R.Leigh

Importance of Nonlinear Couplings in Fusion-Barrier Distributions and Mean Angular Momenta

NUCLEAR REACTIONS, ICPND 96Zr(64Ni, X), E(cm)=120-150 MeV; analyzed fusion σ, compound nucleus average angular momentum; 144Sm(16O, X), E(cm)=55-75 MeV; analyzed fusion σ, barrier distribution; deduced surface vibration coupling, projectile excitation effects. Coupled-channels calculations.

doi: 10.1088/0954-3899/23/10/031
Citations: PlumX Metrics

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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1997ME03      Phys.Rev. C55, R995 (1997)

J.C.Mein, D.J.Hinde, M.Dasgupta, J.R.Leigh, J.O.Newton, H.Timmers

Precise Fission Fragment Anisotropies for the 12C + 232Th Reaction: Supporting the nuclear orientation dependence of quasifission

NUCLEAR REACTIONS 232Th(12C, F), E=57-75 MeV; measured σ(fragment θ), fission fragment anisotropies; deduced deformed actinide nucleus orientation role in quasifission.

doi: 10.1103/PhysRevC.55.R995
Citations: PlumX Metrics

1997TI06      J.Phys.(London) G23, 1175 (1997)

H.Timmers, J.R.Leigh, N.Rowley, A.M.Stefanini, D.Ackermann, S.Beghini, L.Corradi, M.Dasgupta, J.H.He, D.J.Hinde, J.C.Mein, G.Montagnoli, C.R.Morton, J.O.Newton, F.Scarlassara, G.F.Segato

Barrier Distributions and Scattering

NUCLEAR REACTIONS 144,154Sm(16O, X), 96,90Zr(40Ca, X), 208Pb(16O, X), (32S, X), E not given; analyzed fusion barrier distribution data; deduced residual reaction channel role.

doi: 10.1088/0954-3899/23/10/004
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1996HI02      Phys.Rev. C53, 1290 (1996)

D.J.Hinde, M.Dasgupta, J.R.Leigh, J.C.Mein, C.R.Morton, J.O.Newton, H.Timmers

Conclusive Evidence for the Influence of Nuclear Orientation on Quasifission

NUCLEAR REACTIONS 238U(16O, F), E=76-112 MeV; measured fission fragment anisotropies, mass distributions; deduced nuclear orientation role in quasifission.

doi: 10.1103/PhysRevC.53.1290
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1996RO05      Phys.Lett. 373B, 23 (1996)

N.Rowley, H.Timmers, J.R.Leigh, M.Dasgupta, D.J.Hinde, J.C.Mein, C.R.Morton, J.O.Newton

Barrier Distributions from Elastic Scattering

NUCLEAR REACTIONS 144Sm(16O, 16O), E=55-75 MeV; 154Sm(16O, 16O), E=53-75 MeV; 186W(16O, 16O), E=61-85 MeV; 208Pb(16O, 16O), E=69-93 MeV; measured large angle potential barrier distribution functions; deduced weaker direct-reaction channels coupling evidence.

doi: 10.1016/0370-2693(96)00118-9
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1996WU07      Nucl.Phys. A607, 178 (1996)

C.Y.Wu, D.Cline, T.Czosnyka, A.Backlin, C.Baktash, R.M.Diamond, G.D.Dracoulis, L.Hasselgren, H.Kluge, B.Kotlinski, J.R.Leigh, J.O.Newton, W.R.Phillips, S.H.Sie, J.Srebrny, F.S.Stephens

Quadrupole Collectivity and Shapes of Os-Pt Nuclei

NUCLEAR REACTIONS 186,188,190,192Os, 194Pt(40Ca, 40Ca'), (58Ni, 58Ni'), (136Xe, 136Xe'), (208Pb, 208Pb'), E=3.3-4.8 MeV/nucleon; measured Eγ, Iγ following Coulomb excitation. 186,188,190,192Os, 194Pt deduced levels, J, π, E2, M1 matrix elements.

doi: 10.1016/0375-9474(96)00181-9
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1995HI05      Nucl.Phys. A583, 135c (1995); Erratum Nucl.Phys. A587, 853 (1995)

D.J.Hinde, C.R.Morton, M.Dasgupta, J.R.Leigh, J.P.Lestone, R.C.Lemmon, J.C.Mein, J.O.Newton, H.Timmers, N.Rowley, A.T.Kruppa

Fusion Barrier Distributions and Fission Anisotropies

NUCLEAR REACTIONS, ICPND 144Sm(16O, X), (17O, X), E(cm) ≈ 55-70 MeV; analyzed fusion σ(E). 208Pb(16O, F), (16O, X), E(cm) ≈ 70-85 MeV; measured fission anisotropies, fusion barrier distribution.

doi: 10.1016/0375-9474(94)00647-6
Citations: PlumX Metrics

1995HI07      Phys.Rev.Lett. 74, 1295 (1995)

D.J.Hinde, M.Dasgupta, J.R.Leigh, J.P.Lestone, J.C.Mein, C.R.Morton, J.O.Newton, H.Timmers

Fusion-Fission Versus Quasifission: Effect of nuclear orientation

NUCLEAR REACTIONS 238U(16O, F), E=76-104 MeV; measured fission fragment σ(θ) vs E; deduced quasifission evidence. 238U deduced deformation features role.

doi: 10.1103/PhysRevLett.74.1295
Citations: PlumX Metrics

1995HI17      Nucl.Phys. A592, 271 (1995)

D.J.Hinde, C.R.Morton, M.Dasgupta, J.R.Leigh, J.C.Mein, H.Timmers

Competition between Fusion-Fission and Quasi-Fission in the Reaction 28Si + 208Pb

NUCLEAR REACTIONS 208Pb(28Si, F), E=135-178 MeV; measured fission fragment anisotropy, σ(E); deduced fusion barrier distribution. 28Si deduced oblate deformation. 208Pb deduced double octupole phonon roles, fusion-fission, quasi-fission competition. Coupled-channels calculation.

doi: 10.1016/0375-9474(95)00306-L
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1995LE34      Phys.Rev. C52, 3151 (1995)

J.R.Leigh, M.Dasgupta, D.J.Hinde, J.C.Mein, C.R.Morton, R.C.Lemmon, J.P.Lestone, J.O.Newton, H.Timmers, J.X.Wei, N.Rowley

Barrier Distributions from the Fusion of Oxygen Ions with 144,148,154Sm and 186W

NUCLEAR REACTIONS, ICPND 186W, 144,148,154Sm(16O, X), 144Sm(17O, X), E=50-110 MeV; measured fusion σ(E), σ(evaporation residue, θ) vs E; deduced fusion barrier distributions. Enriched targets. Coupled-channels analysis.

doi: 10.1103/PhysRevC.52.3151
Citations: PlumX Metrics

1995MO22      Phys.Rev. C52, 243 (1995)

C.R.Morton, D.J.Hinde, J.R.Leigh, J.P.Lestone, M.Dasgupta, J.C.Mein, J.O.Newton, H.Timmers

Resolution of the Anomalous Fission Fragment Anisotropies for the 16O + 208Pb Reaction

NUCLEAR REACTIONS, ICPND 208Pb(16O, X), (16O, F), E(cm)=71-85 MeV; measured evaporation residue, fission σ, fission fragment anisotropies, Eα, Iα; deduced fusion barrier distribution, σ(E). Transition state model.

doi: 10.1103/PhysRevC.52.243
Citations: PlumX Metrics

1995TI02      Nucl.Phys. A584, 190 (1995)

H.Timmers, J.R.Leigh, M.Dasgupta, D.J.Hinde, R.C.Lemmon, J.C.Mein, C.R.Morton, J.O.Newton, N.Rowley

Probing Fusion Barrier Distributions with Quasi-Elastic Scattering

NUCLEAR REACTIONS 92Zr(16O, X), E=35-70 MeV; 144Sm(16O, X), E=55-75 MeV; 154Sm(16O, X), E=53-75 MeV; 186W(16O, X), E=61-85 MeV; measured quasielastic, elastic, inelastic, transfer σ(θ)/σ(Rutherford), sub-barrier fusion; deduced fusion barrier distribution. Coupled-channels calculations, ECIS.

doi: 10.1016/0375-9474(94)00521-N
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1994MO24      Phys.Rev.Lett. 72, 4074 (1994)

C.R.Morton, M.Dasgupta, D.J.Hinde, J.R.Leigh, R.C.Lemmon, J.P.Lestone, J.C.Mein, J.O.Newton, H.Timmers, N.Rowley, A.T.Kruppa

Clear Signatures of Specific Inelastic and Transfer Channels in the Distribution of Fusion Barriers

NUCLEAR REACTIONS, ICPND 144Sm(16O, X), (17O, X), E=61-100 MeV; measured fusion σ(E); deduced fusion barrier distribution structure, specific transfer channels signature.

doi: 10.1103/PhysRevLett.72.4074
Citations: PlumX Metrics

1993LE01      Phys.Rev. C47, R437 (1993)

J.R.Leigh, N.Rowley, R.C.Lemmon, D.J.Hinde, J.O.Newton, J.X.Wei, J.C.Mein, C.R.Morton, S.Kuyucak, A.T.Kruppa

Reconciling Deformation Parameters from Fusion with Those from Coulomb Excitation

NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 55-68 MeV; analyzed fusion data. 154Sm deduced deformation parameters consistency with Coulomb excitation fits.

doi: 10.1103/PhysRevC.47.R437
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1993LE11      Nucl.Phys. A559, 277 (1993)

J.P.Lestone, J.R.Leigh, J.O.Newton, D.J.Hinde, J.X.Wei, J.X.Chen, S.Elfstrom, M.Zielinska-Pfabe

Pre-Scission Charged-Particle Multiplicities following the Reactions 164,167,170Er + 28Si

NUCLEAR REACTIONS 164,167,170Er(28Si, F), E=140-185 MeV; measured fission (fragment)p-, (fragement)α-coin, σ(fragment, θ, E(α, p)); deduced pre-, post-fission proton and alpha multiplicities. 192,195,198Pb deduced statistical model level-density parameters, dynamical effects.

doi: 10.1016/0375-9474(93)90192-Z
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1993LE17      Phys.Lett. 316B, 32 (1993)

R.C.Lemmon, J.R.Leigh, J.X.Wei, C.R.Morton, D.J.Hinde, J.O.Newton, J.C.Mein, M.Dasgupta, N.Rowley

Strong Dependence of Sub-Barrier Fusion on the Nuclear Hexadecapole Deformation

NUCLEAR REACTIONS, ICPND 186W(16O, X), E=68-90 MeV; measured fusion σ(E). 154Sm(16O, X), E not given; analyzed data; deduced hexadecapole deformation role. 186W deduced deformation parameters.

doi: 10.1016/0370-2693(93)90653-Y
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1992RO03      Phys.Rev. C45, 719 (1992)

H.Rossner, D.J.Hinde, J.R.Leigh, J.P.Lestone, J.O.Newton, J.X.Wei, S.Elfstrom

Influence of Pre-Fission Particle Emission on Fragment Angular Distributions Studied for 208Pb(16O, f)

NUCLEAR REACTIONS 208Pb(16O, F), E=80-130 MeV; measured σ(fragment θ, En); deduced pre-, post-scission multiplicities. 224Th deduced fission yield vs decay time, temperature.

doi: 10.1103/PhysRevC.45.719
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1991HI08      Phys.Lett. 258B, 35 (1991)

D.J.Hinde, J.R.Leigh, J.P.Lestone, J.O.Newton, S.Elfstrom, J.X.Wei, M.Zielinska-Pfabe

The Effect of the Angular Momentum Dependence of the Fission Probability on the Determination of Fission Time Scales from Fission Excitation Functions

NUCLEAR REACTIONS 197Au(16O, F), 181Ta(19F, F), E not given; calculated fission probability vs excitation energy; deduced angular momentum role in fission time scales determination.

doi: 10.1016/0370-2693(91)91204-9
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1991LE21      Phys.Rev.Lett. 67, 1078 (1991)

J.P.Lestone, J.R.Leigh, J.O.Newton, D.J.Hinde, J.X.Wei, J.X.Chen, S.Elfstrom, D.G.Popescu

Fission Time Scales from Prescisson Charged-Particle Multiplicities

NUCLEAR REACTIONS 164,167,170Er(28Si, X), E=140-185 MeV; measured proton, α-spectra, multiplicities; deduced reaction mechanism. 192,195,198Pb deduced fission characteristics.

doi: 10.1103/PhysRevLett.67.1078
Citations: PlumX Metrics

1991WE18      Phys.Rev.Lett. 67, 3368 (1991)

J.X.Wei, J.R.Leigh, D.J.Hinde, J.O.Newton, R.C.Lemmon, S.Elfstrom, J.X.Chen, N.Rowley

Experimental Determination of the Fusion-Barrier Distribution for the 154Sm + 16O Reaction

NUCLEAR REACTIONS 154Sm(16O, X), E=54-110 MeV; measured σ(evaporation residue θ); deduced fusion σ(E), barrier distributions.

doi: 10.1103/PhysRevLett.67.3368
Citations: PlumX Metrics

1991WE19      Nucl.Instrum.Methods Phys.Res. A306, 557 (1991)

J.X.Wei, J.R.Leigh, D.C.Weisser, J.O.Newton, S.Elfstrom, J.P.Lestone, J.X.Chen, D.G.Popescu, D.J.Hinde

A Compact Velocity Filter for Evaporation Residue Measurements

NUCLEAR REACTIONS 130Te(28Si, X), E=100-160 MeV; 170Er(16O, X), E=110 MeV; 176Yb(16O, X), E=100 MeV; 186W(16O, X), E=70 MeV; 154Sm(16O, X), E=60 MeV; measured σ(evaporation residue θ). Velocity filter.

doi: 10.1016/0168-9002(91)90052-R
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1990LE07      Nucl.Phys. A509, 178 (1990)

J.P.Lestone, J.R.Leigh, J.O.Newton, J.X.Wei

Fission Fragment Angular Distributions following Transfer Reactions for 232Th + 16O

NUCLEAR REACTIONS 232Th(16O, F), E=80-92 MeV; measured fission fragment σ(E, θ), (fragment)(particle)-coin, σ(fragment φ, θ) following transfer, X=C, N.

doi: 10.1016/0375-9474(90)90380-5
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1990NE09      Phys.Rev. C42, 1772 (1990)

J.O.Newton, D.G.Popescu, J.R.Leigh

Inclusion of Temperature Dependence of Fission Barriers in Statistical Model Calculations

NUCLEAR REACTIONS, ICPND 181Ta, 159Tb(19F, F), E ≈ 80-120 MeV; calculated fission σ(E). Statistical model, fission barrier temperature dependence from data.

NUCLEAR STRUCTURE A=109-240; calculated zero temperature fission barriers.

doi: 10.1103/PhysRevC.42.1772
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1988LE04      J.Phys.(London) G14, L55 (1988)

J.R.Leigh, J.J.M.Bokhorst, D.J.Hinde, J.O.Newton

Observation of Sub-Barrier Fusion Enhancement Due to Negative Hexadecapole Deformations ( Question )

NUCLEAR REACTIONS, ICPND 176,180Hf, 182,184,186W(16O, X), E=70-90 MeV; measured fusion σ(E). 150,152,154Sm(16O, X), 181Ta, 159Tb, 139La, 169Tm(19F, X), E not given; calculated fusion σ(E). 176,180Hf, 182,184,186W deduced hexadecapole deformation nature.

doi: 10.1088/0305-4616/14/4/002
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1988NE03      Nucl.Phys. A483, 126 (1988)

J.O.Newton, D.J.Hinde, R.J.Charity, J.R.Leigh, J.J.M.Bokhorst, A.Chatterjee, G.S.Foote, S.Ogaza

Measurement and Statistical Model Analysis of Pre-Fission Neutron Multiplicities

NUCLEAR REACTIONS 150Sm(18O, F), E=108-122 MeV; 159Tb(19F, F), E=110-124 MeV; 169Tm(19F, F), E=105-135 MeV; 164Er(28Si, F), E=170 MeV; 170Er(28Si, F), E=135-165 MeV; 181Ta(19F, F), E=95-135 MeV; 170Er(30Si, F), E=160 MeV; 192Os(18O, F), 197Au(16O, F), E=95-124 MeV; 232Th(19F, F), E=105-138 MeV; measured fission (fragment)n-coin, σ(fragment θ, E(n)); deduced pre-, post-fission neutron multiplicities. 168Yb, 178W, 188Pt, 192,198,200Pb, 210Po, 213Fr, 251Es deduced statistical model parameters, dynamical, temperature effects.

doi: 10.1016/0375-9474(88)90068-1
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1987HI11      Nucl.Phys. A472, 318 (1987)

D.J.Hinde, J.R.Leigh, J.J.M.Bokhorst, J.O.Newton, R.L.Walsh, J.W.Boldeman

Mass-Split Dependence of the Pre- and Post-Scission Neutron Multiplicities for Fission of 251Es

NUCLEAR REACTIONS 232Th(19F, F), E=105, 120 MeV; measured fission (fragment)n-coin, σ(fragment θ, mass, E(n)); deduced transfer-induced fission, pre-, post-fission neutron multiplicities. 251Es deduced fission characteristics. Random neck rupture model, quasifission.

doi: 10.1016/0375-9474(87)90213-2
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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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1986CH30      Nucl.Phys. A457, 441 (1986)

R.J.Charity, J.R.Leigh, J.J.M.Bokhorst, A.Chatterjee, G.S.Foote, D.J.Hinde, J.O.Newton, S.Ogaza, D.Ward

Heavy-Ion Induced Fusion-Fission Systematics and the Effect of the Compound-Nucleus Spin Distribution on Fission-Barrier Determination

NUCLEAR REACTIONS, ICPND 139La, 159Tb, 169Tm(19F, X), (19F, F), E=70-129 MeV; 150Sm, 192Os(18O, X), (18O, F), E=65-124 MeV; measured fission, evaporation σ(fragment θ), σ(E). Statistical model.

doi: 10.1016/0375-9474(86)90388-X
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1986HI01      Nucl.Phys. A452, 550 (1986)

D.J.Hinde, R.J.Charity, G.S.Foote, J.R.Leigh, J.O.Newton, S.Ogaza, A.Chatterjee

Neutron Multiplicities in Heavy-Ion-Induced Fission: Timescale of fusion-fission

NUCLEAR REACTIONS 150Sm(18O, F), E=108-122 MeV; 164Er(28Si, F), E=170 MeV; 170Er(28Si, F), E=135-165 MeV; 170Er(30Si, F), E=160 MeV; 181Ta(19F, F), E=95-135 MeV; 192Os(18O, F), 197Au(16O, F), E=95-124 MeV; 232Th(19F, F), E=105-138 MeV; measured (fragment)n-coin, σ(fragment θ, En); deduced pre-, post-fission neutron multiplicities. 168Yb, 192,198,200Pb, 210Po, 213Fr, 251Es deduced fission dynamics. Statistical model.

doi: 10.1016/0375-9474(86)90214-9
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1985LE18      Phys.Lett. 159B, 9 (1985)

J.R.Leigh, W.R.Phillips, J.O.Newton, G.S.Foote, D.J.Hinde, G.D.Dracoulis

Angular Momentum Partition in Heavy Ion Induced Fission and the Effects of Shells on Gamma-Ray Multiplicities

NUCLEAR REACTIONS 181Ta(32S, F), E=150 MeV; 197Au, 181Ta, 170Er, 232Th(19F, F), E=115 MeV; 197Au(19F, F), E=100 MeV; measured γ multiplicity vs fission fragment mass asymmetry. 213Ac, 189Ir, 200Pb, 216Ra, 251Es deduced average fission (L).

doi: 10.1016/0370-2693(85)90109-1
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1984HI04      Phys.Rev.Lett. 52, 986 (1984)

D.J.Hinde, R.J.Charity, G.S.Foote, J.R.Leigh, J.O.Newton, S.Ogaza, A.Chatterjee

Neutron Emission from Fission Fragments during Acceleration

NUCLEAR REACTIONS 232Th(19F, F), E=124 MeV; measured fission fragment(n)-coin vs neutron velocity, neutron multiplicity vs excitation, fragment(n)(θ); deduced neutron emission mechanism.

doi: 10.1103/PhysRevLett.52.986
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1984OM02      Phys.Rev. C30, 896 (1984)

A.R.Omar, J.S.Eck, J.R.Leigh, T.R.Ophel

Elastic and Inelastic Scattering of 9Be + 9Be at E(9Be) = 35-50 MeV

NUCLEAR REACTIONS 9Be(9Be, 9Be), (9Be, 9Be'), E=35, 40, 45, 50 MeV; measured σ(E(9Be)), σ(θ); deduced potential parameters, β. Optical, coupled-channels model analysis.

doi: 10.1103/PhysRevC.30.896
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1527.

1984OM03      Phys.Rev. C30, 1516 (1984)

A.R.Omar, J.S.Eck, T.R.Ophel, J.R.Leigh

Total Fusion of 9Be + 9Be at E(9Be) = 35-55 MeV

NUCLEAR REACTIONS, ICPND 9Be(9Be, X), E=35, 40, 45, 50, 55 MeV; measured evaporation residue σ(θ), σ vs Z, fusion σ(E). 12C(13C, X), E(cm)=10-45 MeV; calculated total reaction σ. Optical model.

doi: 10.1103/PhysRevC.30.1516
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1983EC01      Phys.Rev. C27, 1807 (1983)

J.S.Eck, A.R.Omar, J.R.Leigh, T.R.Ophel

Fusion Cross Sections for 9Be + 40Ca

NUCLEAR REACTIONS, ICPND 40Ca(9Be, X), E=35, 40, 45, 50, 55, 60 MeV; measured σ(evaporation residue θ); deduced fusion σ. 40Ca(9Be, 9Be), E=35-60 MeV; calculated σ(θ); deduced reaction σ. Optical model.

doi: 10.1103/PhysRevC.27.1807
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1983HI02      Nucl.Phys. A398, 308 (1983)

D.J.Hinde, J.O.Newton, J.R.Leigh, R.J.Charity

Fission Barriers of Pb Nuclei at High Angular Momentum

NUCLEAR REACTIONS 170Er(28Si, X), (30Si, X), (28Si, F), (30Si, F), E=125-180 MeV; 164,167Er(28Si, X), (28Si, F), E=130-180 MeV; measured fission σ(fragment θ), σ(evaporation residue θ); deduced total fission probabilities. Statistical model.

doi: 10.1016/0375-9474(83)90489-X
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1983HO08      Nucl.Phys. A398, 130 (1983)

M.A.C.Hotchkis, L.K.Fifield, J.R.Leigh, T.R.Ophel, G.D.Putt, D.C.Weisser

New Measurements of the Masses of 15B and 19N

NUCLEAR REACTIONS 48Ca(18O, 15B), (18O, 19N), E=108-119 MeV; measured σ(E(15B)), σ(E(19N)). 15B, 19N deduced mass excess. Enriched target.

doi: 10.1016/0375-9474(83)90652-8
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1983WA15      Nucl.Phys. A403, 189 (1983)

D.Ward, R.J.Charity, D.J.Hinde, J.R.Leigh, J.O.Newton

Measurement of Pre-Fission Neutrons from 200Pb; Further limits to the statistical fission parameters

NUCLEAR REACTIONS 181Ta(19F, X)(19F, F), E=105, 115, 125 MeV; measured fission (fragment)n(θ), pre-fission, post-fission neutron multiplicity; deduced saddle point equilibrium deformation level density parameters.

doi: 10.1016/0375-9474(83)90196-3
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1983WA20      Nucl.Phys. A406, 591 (1983)

D.Ward, G.D.Dracoulis, J.R.Leigh, R.J.Charity, D.J.Hinde, J.O.Newton

High-Spin States in 222Th

NUCLEAR REACTIONS, ICPND 208Pb(18O, 4n), E=85-102 MeV; measured Eγ, Iγ, γ(residue)-, γγ(residue)-coin, γ-multiplicity, relative σ(E). 222Th deduced levels, J, π, rotational band B(λ) ratios, average γ-multiplicity per cascade. Ge(Li), NaI(Tl) detectors.

doi: 10.1016/0375-9474(83)90379-2
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1982FI10      Nucl.Phys. A385, 505 (1982)

L.K.Fifield, J.L.Durell, M.A.C.Hotchkis, J.R.Leigh, T.R.Ophel, D.C.Weisser

The Mass of 18C from a Heavy Ion Double-Charge-Exchange Reaction

NUCLEAR REACTIONS 48Ca(18O, 18C), 48Ca(18O, 17C), E=112 MeV; measured σ(E(18C)), σ(E(17C)). 18C, 17C deduced mass excesses, levels. Enriched target.

doi: 10.1016/0375-9474(82)90100-2
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1982HI09      Nucl.Phys. A385, 109 (1982)

D.J.Hinde, J.R.Leigh, J.O.Newton, W.Galster, S.Sie

Fission and Evaporation Competition in 200Pb

NUCLEAR REACTIONS 181Ta(19F, X), (19F, F), E=80-125 MeV; 170Er(30Si, X), (30Si, F), E=125-170 MeV; measured σ(fragment E, θ). 200Pb deduced fission probability versus angular momentum. Statistical model fits.

doi: 10.1016/0375-9474(82)90492-4
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1982LE05      Phys.Rev.Lett. 48, 527 (1982)

J.R.Leigh, D.J.Hinde, J.O.Newton, W.Galster, S.H.Sie

Fission-Imposed Limits to the Angular Momentum Carried by Evaporation Residues from the Compound Nucleus 200Pb

NUCLEAR REACTIONS, Fission 181Ta(19F, X), (19F, F), E=80-126 MeV; 170Er(30Si, X), (30Si, F), E=125-168 MeV; measured σ(fission), σ(evaporation residue) vs E, θ; deduced σ(fusion, E). 200Pb deduced total fission probability vs (L). Bohr independence hypothesis, complete fusion.

doi: 10.1103/PhysRevLett.48.527
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1981LE13      Nucl.Instrum.Methods 186, 541 (1981)

J.R.Leigh, D.J.Hinde, W.Galster

Application of a Simple MWPC to Measurement of Heavy (A ≈ 200) Evaporation Residues

NUCLEAR REACTIONS 181Ta(19F, X), E=95 MeV; measured σ(evaporation residue θ). Tof, multiwire proportional chamber.

doi: 10.1016/0029-554X(81)90233-0
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1981SI01      Phys.Rev.Lett. 46, 405 (1981)

S.H.Sie, J.O.Newton, J.R.Leigh, R.M.Diamond

Multiplicity of the Statistical γ Rays following (16O, xn) Reactions

NUCLEAR REACTIONS 110Pd, 122Sn(16O, 4n), E=65, 83 MeV; 149Sm(16O, 3n), 150,154Sm(16O, 4n), E=73, 85 MeV; 166Er(α, 2n), E=27 MeV; measured statistical, total γ-multiplicity; deduced γ-multiplicity correlation. 166,162Yb, 134Ce, 122Xe deduced mean excitation energy, angular momentum input effects.

doi: 10.1103/PhysRevLett.46.405
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1981SI02      Nucl.Phys. A352, 279 (1981)

S.H.Sie, R.M.Diamond, J.O.Newton, J.R.Leigh

The Dipole Component in the Yrast Cascade and the Multiplicity of Statistical γ-Rays

NUCLEAR REACTIONS 149Sm(16O, 3n), 150Sm, 154Sm(16O, 4n), E=73, 85 MeV; 122Sn, 110Pd(16O, 4n), E=65, 83 MeV; measured σ(E, Eγ, θγ), γ-multiplicities, γγ-coin. 162,166Yb, 134Ce, 122Xe deduced γ-multipolarity, dipole component in yrast cascade. Enriched targets, model analysis.

doi: 10.1016/0375-9474(81)90381-X
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1980EC03      Phys.Rev. C21, 2352 (1980)

J.S.Eck, J.R.Leigh, T.R.Ophel, P.D.Clark

Total Fusion Cross Section for the 9Be + 28Si System

NUCLEAR REACTIONS 28Si(9Be, X), E=30-60 MeV; measured evaporation residue σ(θ), total fusion σ.

doi: 10.1103/PhysRevC.21.2352
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1980PA21      Nucl.Phys. A350, 139 (1980)

V.Paar, G.Vanden Berghe, C.Garrett, J.R.Leigh, G.D.Dracoulis

Expermental and Theoretical Investigation of a Quasi-f7/2 Multiplet Pattern in 147Sm

NUCLEAR REACTIONS 147Sm(α, α'), E=8, 10, 13 MeV; measured σ(Eα). 147Sm levels deduced B(E2), configuration. Enriched target.

doi: 10.1016/0375-9474(80)90392-9
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1979LE01      Phys.Rev.Lett. 42, 153 (1979)

J.R.Leigh, R.M.Diamond, A.Johnston, J.O.Newton, S.H.Sie

Fission Following Transfer to 232Th at Energies below the Coulomb Barrier

NUCLEAR REACTIONS 232Th(16O, X), E=75-95 MeV; 232Th(19F, X), E=85-95 MeV; measured σ(θ) for transfer-induced fission at sub-Coulomb energies.

doi: 10.1103/PhysRevLett.42.153
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1979PO16      Nucl.Phys. A330, 173 (1979)

E.C.Pollacco, D.M.Parkinson, J.R.Leigh, D.C.Weisser, N.Shikazono, G.S.Foote, D.Branford

12C and 13C Induced Reactions on N = 28 Nuclei at Energies Near the Coulomb Barrier

NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr, 54Fe(13C, 13C); 48Ca, 50Ti, 52Cr, 53Cr, 54Fe(12C, 12C); 52Cr, 54Fe(12C, 12C'); 52Cr, 54Fe(13C, 13C'); 48Ca, 50Ti, 52Cr, 54Fe(13C, 12C); 53Cr(12C, 13C); measured σ(E). 52Cr, 54Fe deduced B(E2), β of ion-ion potential. 49Ca, 51Ti, 53Cr, 55Fe levels deduced S. Enriched targets. DWBA analysis.

doi: 10.1016/0375-9474(79)90543-8
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1978WA16      J.Phys.(London) G4, 1655 (1978)

P.M.Walker, G.D.Dracoulis, A.Johnston, J.R.Leigh, M.G.Slocombe, I.F.Wright

High-Spin States and Single-Particle Structure in 173W and 175W

NUCLEAR REACTIONS 161,163Dy(16O, 4nγ), E=83-89 MeV; measured Eγ, Iγ, γγ-coin, nγ-coin, γ(θ). 173,175W deduced levels, J, π, T1/2. Ge(Li), Ge, NE213 detectors. Enriched targets. Single-quasiparticle Coriolis mixing calculation.

doi: 10.1088/0305-4616/4/10/014
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1977DR04      J.Phys.(London) G3, 533 (1977)

G.D.Dracoulis, J.R.Leigh, A.Johnson, C.Garrett

Coulomb Excitation of 151Eu

RADIOACTIVITY 151Gd [from 151Eu(p, n)]; measured Eγ, Iγ, γγ-coin. 151Eu deduced levels.

NUCLEAR REACTIONS 151Eu(16O, 16O'γ), E=25-42 MeV; measured σ(E, Eγ, θ), γγ-coin, DSA, Coulomb excitation. 151Eu(p, p'γ), E=4 MeV; measured Eγ, Iγ. 151Eu(α, α'), E=10 MeV; measured σ(Eα'). 151Eu deduced levels, J, π, T1/2, B(λ), δ, γ-branching. Enriched targets, Ge(Li) detectors.

doi: 10.1088/0305-4616/3/4/014
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1977LE07      J.Phys.(London) G3, 519 (1977)

J.R.Leigh, G.D.Dracoulis, M.G.Slocombe, J.O.Newton

Band Structure in the N = 88 Nucleus 151Eu

NUCLEAR REACTIONS 150,152Sm(d, 3nγ), E=18-25 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 149,151Eu deduced levels, J, π. Coriolis coupling calculations.

doi: 10.1088/0305-4616/3/4/013
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1977WA16      Nucl.Phys. A293, 481 (1977)

P.M.Walker, G.D.Dracoulis, A.Johnston, J.R.Leigh

High-Spin States and Two-Quasiparticle Structure in 172Hf

NUCLEAR REACTIONS 160Gd(16O, 4n), E=75-84 MeV; measured Eγ, Iγ, γγ-coin, γγ(t), γ(θ). 172Hf deduced levels, K, J, π, T1/2. Ge, Ge(Li) detectors, enriched target.

doi: 10.1016/0375-9474(77)90109-9
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1976DR05      J.Phys.(London) G2, L87 (1976)

G.D.Dracoulis, J.R.Leigh

Deformed States in 151Eu

NUCLEAR STRUCTURE 151Eu; calculated wave functions, levels.

doi: 10.1088/0305-4616/2/6/003
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1976GA10      Nucl.Phys. A262, 137 (1976)

C.Garrett, J.R.Leigh, G.D.Dracoulis

Coulomb Excitation of 147Sm and 149Sm and an Intermediate Coupling Description for the Transitional Sm Isotopes

RADIOACTIVITY 149Eu; measured Eγ, Iγ, γγ-coin. 149Sm deduced levels, γ-branching. Ge(Li) detectors.

NUCLEAR REACTIONS 147,149Sm(16O, 16O'γ), E=38-48 MeV; 147,149Sm(α, α'γ), E=6-11 MeV; measured σ(E, Eγ, θ), 16O'γ(θ), γγ-coin. 147,149Sm deduced levels, J, π, δ, B(E2), γ-branching. Ge(Li) detectors, magnetic spectrometer.

doi: 10.1016/0375-9474(76)90445-0
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1976LE12      J.Phys.(London) G2, L39 (1976)

J.R.Leigh, E.C.Pollacco, N.Shikazono, D.C.Weisser, C.Garrett

Differences in the Coulomb-Nuclear Interference Patterns Produced with 12C and 13C Ions

NUCLEAR REACTIONS 52Cr, 54Fe(12C, 12C), (12C, 12C'), (13C, 13C), (13C, 13C'), E=18-26 MeV; measured σ(E); deduced differences in Coulomb-nuclear interference patterns.

doi: 10.1088/0305-4616/2/3/005
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1976LE15      J.Phys.(London) G2, L97 (1976)

J.R.Leigh, C.Garrett, G.D.Dracoulis

Spin Assignments in 149Sm

NUCLEAR REACTIONS 148Nd(α, 3n); analyzed γ(θ) data. 149Sm(16O, 16O'γ); analyzed Coulomb excitation data. 149Sm levels deduced J, π.

doi: 10.1088/0305-4616/2/7/002
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1976WA16      J.Phys.(London) G2, L197 (1976)

P.M.Walker, G.D.Dracoulis, A.Johnston, J.R.Leigh, M.G.Slocombe, I.F.Wright

High Spin States and Backbending in the Light Tungsten Isotopes

NUCLEAR REACTIONS 160,161,162,162,163,164Dy(16O, 4nγ), E=74-91 MeV; measured nγ(t), γγ(t), σ(E, Eγ, θ). 172,174,175,176W deduced levels, K, J, π.

doi: 10.1088/0305-4616/2/12/001
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1975DR07      J.Phys.(London) G1, 853 (1975)

G.D.Dracoulis, J.R.Leigh, M.G.Slocombe, J.O.Newton

Rotational Bands in 153Eu

NUCLEAR REACTIONS 154Sm(d, 3nγ), E=18-25 MeV; measured σ(E, Eγ, θ), γγ-coin, nγ-coin, γ(t). 153Eu deduced levels, J, π, K, δ. Coriolis calculations. Enriched targets.

doi: 10.1088/0305-4616/1/8/008
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1975NE01      Phys.Rev.Lett. 34, 99 (1975)

J.O.Newton, J.C.Lisle, G.D.Dracoulis, J.R.Leigh, D.C.Weisser

Observation of the Yrast and Statistical Cascades in (Heavy-Ion, xnγ) Reactions

NUCLEAR REACTIONS 147,149Sm(16O, 3nγ), E=75 MeV; 150Sm(16O, 4nγ), E=88 MeV; 148Sm(16O, 4nγ), E=94 MeV; measured nγ-coin, Eγ(θ). 160,162Yb deduced yrast, statistical cascades.

doi: 10.1103/PhysRevLett.34.99
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1973LE09      Nucl.Phys. A213, 1 (1973)

J.R.Leigh, K.Nakai, K.H.Maier, F.Puhlhofer, F.S.Stephens, R.M.Diamond

Energy-Level Systematics of Odd-Mass Lanthanum Isotopes; a New Coupling Scheme

NUCLEAR REACTIONS 130,128,126,124,122Te(11B, 4nγ), E=40, 45, 50, 52.6, 56.5 MeV; 124Sn(14N, 5nγ), 120,118,116Sn(14N, 3nγ), E=50.5, 53, 58, 62, 64.8, 67, 68.5, 72, 76 MeV; 112Sn(16O, 2npγ), E=72, 76, 82, 88, 94 MeV; measured σ(Eγ, θ), γγ-coin, γγ(t). 125,127,129,131,133,135,137La deduced levels, J, π, T1/2, γ-multipolarity. Enriched targets. Ge(Li) detector.

doi: 10.1016/0375-9474(73)90178-4
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1973NA08      Phys.Lett. 44B, 443 (1973)

K.Nakai, P.Kleinheinz, J.R.Leigh, K.H.Maier, F.S.Stephens, R.M.Diamond, G.Lovhoiden

Prolate Deformation in Neutron-Deficient Lanthanum Isotopes

NUCLEAR REACTIONS 116,118,120,122Sn(14N, xnγ), E=not given; measured Eγ, Iγ(θ), γγ-coin. 130Ba(α, t), E=27 MeV; 138Ba(3He, d), E=22 MeV; measured σ(Et), σ(Ed), L. 125,127,129,131,133,135,137,139La deduced levels, J, π.

doi: 10.1016/0370-2693(73)90329-8
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1973PR16      Phys.Rev.Lett. 31, 896 (1973)

D.Proetel, R.M.Diamond, P.Kienle, J.R.Leigh, K.H.Maier, F.S.Stephens

Evidence for Strongly Deformed Shapes in 186Hg

RADIOACTIVITY 186Tl, 186mHg; measured Eγ, Iγ. 186Hg deduced transitions.

NUCLEAR REACTIONS 162Dy(28Si, xnγ), E=135 MeV; measured nγ-coin, Eγ. 186Hg level deduced T1/2, transitions, γ-multipolarty.

doi: 10.1103/PhysRevLett.31.896
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1972DI06      Nucl.Phys. A184, 481 (1972)

R.M.Diamond, G.D.Symons, J.L.Quebert, K.H.Maier, J.R.Leigh, F.S.Stephens

Lifetimes of Ground-Band States in 154Sm

NUCLEAR REACTIONS 154Sm(40Ar, 40Ar'), E=146 MeV; measured recoil distance. 154Sm levels deduced T1/2, B(E2).

doi: 10.1016/0375-9474(72)90423-X
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1972LE04      Nucl.Phys. A183, 177 (1972)

J.R.Leigh, J.O.Newton, L.A.Ellis, M.C.Evans, M.J.Emmott

A Study of the Odd-A Rhenium Isotopes: 179Re and 177Re

NUCLEAR REACTIONS 172Yb(11B, 4n)E=52-60 MeV; 169Tm(12C, 4n)E=62-76 MeV; measured σ(E:Eγ, θ(γ)), γγ-coin. 177Re, 179Re deduced levels, J, π.

doi: 10.1016/0375-9474(72)90938-4
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1972MA10      Nucl.Phys. A183, 289 (1972)

K.H.Maier, K.Nakai, J.R.Leigh, R.M.Diamond, F.S.Stephens

Effective Single-Particle Magnetic Moments Around 208Pb

NUCLEAR STRUCTURE 206,207,208Pb, 207,209,210,211Bi, 205Tl, 208,209,210Po; calculated effective single-particle μ.

doi: 10.1016/0375-9474(72)90660-4
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1972MA24      Nucl.Phys. A186, 97 (1972)

K.H.Maier, K.Nakai, J.R.Leigh, R.M.Diamond, F.S.Stephens

Stroboscopic Measurement of the g-Factors of the 7- Isomer in 206Pb and the 21/2+ Isomer in 207Bi

NUCLEAR REACTIONS 204Hg(α, 2nγ), E=26 MeV; 204Hg(7Li, 4nγ), E=41 MeV; measured αγ(θ, H, t). 206mPb, 207mBi deduced μ. Stroboscopic method.

doi: 10.1016/0375-9474(72)90127-3
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1972ST18      Phys.Rev.Lett. 29, 438 (1972)

F.S.Stephens, R.M.Diamond, J.R.Leigh, T.Kammuri, K.Nakai

Decoupled Yrast States in Odd-Mass Nuclei

doi: 10.1103/PhysRevLett.29.438
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1971EV02      Phys.Lett. 34B, 609 (1971)

M.Evans, A.E.Ellis, J.R.Leigh, J.O.Newton

The 9/2- [514] State in 185Re

NUCLEAR REACTIONS 186W(d, 3nγ), E=12, 16, 19.6 MeV; measured Eγ, Iγ, dγ-delay. 185Re deduced levels, J, π, T1/2.

doi: 10.1016/0370-2693(71)90151-1
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1971MA36      Phys.Lett. 35B, 401 (1971)

K.H.Maier, J.R.Leigh, F.Puhlhofer, R.M.Diamond

A High-Spin Isomer in 211At

NUCLEAR REACTIONS 204Hg, 208Pb, 209Bi(HI, X), E not given; measured σ(E; Eγ, θ(γ)), Eγ, Iγ, I(ce), (HI)(γ)-delay γγ-coin, (HI)(γ)(θ, t). 211mAt deduced levels, J, π, ICC, T1/2, γ-multipolarity.

doi: 10.1016/0370-2693(71)90405-9
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1971MA59      Nucl.Phys. A176, 497 (1971)

K.H.Maier, J.R.Leigh, R.M.Diamond

Measurement of the Magnetic Moment and Lifetime of the 13/2+ Level in 205Pb

NUCLEAR REACTIONS 204Hg(α, 3nγ), E=41 MeV; measured αγ-delay, Iγ, αγ(θ, H, t). 205mPb deduced g, T1/2, γ-branching.

doi: 10.1016/0375-9474(71)90931-6
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1971ST16      Nucl.Phys. A170, 321 (1971)

F.S.Stephens, J.R.Leigh, R.M.Diamond

Some Limitations on the Production of Very Neutron-Deficient Nuclei

NUCLEAR REACTIONS 112Sn(16O, X), E=76, 88, 94 MeV; 144Sm(28Si, X), E=155 MeV; measured σ(Eα, Eγ), σ(Ep, Eγ), in-beam/out-of-beam γ yield ratios; deduced effective Coulomb barrier for proton evaporation.

doi: 10.1016/0375-9474(71)90638-5
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1970LE22      Phys.Lett. 33B, 410 (1970)

J.R.Leigh, F.S.Stephens, R.M.Diamond

Rotational Bands in Odd-Odd Holmium Isotopes

NUCLEAR REACTIONS 154Sm(11B, 5nγ), 159Tb(α, 3nγ), 160Gd(7Li, 5nγ), E not given; measured σ(E;Eγ, θ(γ)), γγ-coin. 160,162Ho deduced levels, J, π, Nilsson assignments.

doi: 10.1016/0370-2693(70)90617-9
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1966EM02      Phys.Letters 20, 56 (1966)

M.J.Emmott, J.R.Leigh, D.Ward, J.O.Newton

An Isomer of Spin 25/2+ in 183Re

NUCLEAR STRUCTURE 183Re; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)91046-8
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