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NSR database version of May 24, 2024.

Search: Author = M.P.Kelly

Found 17 matches.

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2005SE03      Nucl.Phys. A750, 245 (2005)

J.P.Seitz, B.B.Back, M.P.Carpenter, I.Dioszegi, K.Eisenman, P.Heckman, D.J.Hofman, M.P.Kelly, T.L.Khoo, S.Mitsuoka, V.Nanal, T.Pennington, R.H.Siemssen, M.Thoennessen, R.L.Varner

Observation of the hot GDR in neutron-deficient thorium evaporation residues

NUCLEAR REACTIONS 176Yb(48Ca, X), E=206, 219, 256, 259 MeV; measured Eγ, Iγ, (evaporation residue)γ-coin, γ-ray multiplicity and sum energy, fusion and evaporation residue σ. 224Th deduced GDR parameters. Comparison with model predictions.

doi: 10.1016/j.nuclphysa.2005.01.015
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2004NA03      Nucl.Phys. A731, 153 (2004)

V.Nanal, T.L.Khoo, D.J.Hofman, B.B.Back, M.P.Carpenter, I.Dioszegi, K.Eisenman, M.L.Halbert, P.Heckman, A.M.Heinz, D.Henderson, D.Jenkins, M.P.Kelly, F.G.Kondev, T.Lauritsen, C.J.Lister, B.McClintock, S.Mitsuoka, T.Pennington, J.Seitz, R.H.Siemssen, M.Thoennessen, R.J.van Swol, R.L.Varner, P.Wilt, Y.Alhassid

Highly Selective Studies of GDR in 164Er

NUCLEAR REACTIONS 124Sn(40Ar, xn), E=163, 187 MeV; measured Eγ, Iγ, (recoil)γ-coin. 164Er deduced GDR parameters, angular momentum dependence of strength function.

doi: 10.1016/j.nuclphysa.2003.11.028
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2001KI07      Acta Phys.Pol. B32, 825 (2001)

M.Kicinska-Habior, Z.Trznadel, M.P.Kelly, J.P.S.van Schagen, K.A.Snover

Giant Dipole Resonance Studied in Heavy-Ion Reactions at Projectile Energies 6-11 MeV/u


2001TR09      Nucl.Phys. A687, 198c (2001)

Z.Trznadel, M.Kicinska-Habior, M.P.Kelly, J.P.S.van Schagen, K.A.Snover

Giant Dipole Resonance in Hot Se Nuclei and Bremsstrahlung Emission in 12C + 58, 64Ni Experiments at 6-11 MeV/u

NUCLEAR REACTIONS 58,64Ni(12C, X), E=5.5-11 MeV/nucleon; measured Eγ, Iγ(θ), γγ-coin. 70Se, 76Se deduced GDR parameters. Statistical model calculations including precompound effects.

doi: 10.1016/S0375-9474(01)00621-2
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1999KE02      Phys.Rev.Lett. 82, 3404 (1999)

M.P.Kelly, K.A.Snover, J.P.S.van Schagen, M.Kicinska-Habior, Z.Trznadel

Giant Dipole Resonance in Highly Excited Nuclei: Does the width saturate ?

NUCLEAR REACTIONS 100Mo(18O, X), E=122-214 MeV; measured Eγ, Iγ(θ), proton-, α-spectra; deduced pre-equilibrium emission features. 118Sn deduced GDR parameters, no saturation of width.

doi: 10.1103/PhysRevLett.82.3404
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1999KE06      Nucl.Phys. A649, 123c (1999)

M.P.Kelly, K.A.Snover, J.P.S.van Schagen, M.Kicinska-Habior, Z.Trznadel

The GDR Width in Hot Sn Nuclei

NUCLEAR REACTIONS 100Mo(18O, xnypzα), E=125, 150, 169, 200, 217 MeV; measured Eγ, Iγ(θ), γ multiplicity, (charged particle)γ-coin; deduced GDR width vs temperature.

doi: 10.1016/S0375-9474(99)00049-4
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1998LE36      Phys.Rev.Lett. 81, 4776 (1998)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

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

NUCLEAR REACTIONS 232Th(11B, X), E(cm)=46-66 MeV; measured fission fragments angular distributions; deduced reaction mechanism features, no peaklike structure in anisotropies.

doi: 10.1103/PhysRevLett.81.4776
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1998SO01      Phys.Rev. C57, 722 (1998)

A.A.Sonzogni, J.D.Bierman, M.P.Kelly, J.P.Lestone, J.F.Liang, R.Vandenbosch

Transfer and Surface Vibration Couplings in the Fusion of 40Ca + 46,48,50Ti at Near-Barrier Energies

NUCLEAR REACTIONS 46,48,50Ti(40Ca, X), E=97-150 MeV; measured fusion, quasielastic σ(E, θ); deduced fusion, quasielastic σ(E), barrier distributions, surface vibration coupling parameters. Coupled-channel calculations.

doi: 10.1103/PhysRevC.57.722
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1997KE12      Phys.Rev. C56, 3201 (1997)

M.P.Kelly, J.F.Liang, A.A.Sonzogni, K.A.Snover, J.P.S.van Schagen, J.P.Lestone

Preequilibrium Particle Emission and the Giant-Dipole Resonance in Sn Nuclei

NUCLEAR REACTIONS 100Mo(18O, X), E=200 MeV; measured Eγ, Iγ, (particle)γ-coin, p-, α-spectra; deduced pre-equilibrium emission features. 115In, 118Sn deduced GDR pre-equilibrium emission effects.

doi: 10.1103/PhysRevC.56.3201
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1997KI13      Acta Phys.Pol. B28, 189 (1997)

M.Kicinska-Habior, Z.Trznadel, K.A.Snover, A.Maj, M.P.Kelly

New Results in High-Energy γ-Ray Studies from Heavy-Ion Reactions at Around 10 MeV/u

NUCLEAR REACTIONS 26Mg(12C, X), E=6, 8.5, 11 MeV/nucleon; 24Mg(12C, X), E=11 MeV/nucleon; measured Eγ, Iγ(θ); deduced GDR, bremsstrahlung parameters. Statistical models, BUU nuclear transport equation.


1997LE01      Phys.Rev. C55, R16 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, D.Prindle

Near- and Sub-Barrier 12C + 232Th Fission Fragment Anisotropies

NUCLEAR REACTIONS 232Th(12C, F), E=57.6-75.2 MeV; measured fission σ, fission fragment anisotropies.

doi: 10.1103/PhysRevC.55.R16
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1997LE30      J.Phys.(London) G23, 1349 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Near- and Sub-Barrier Fission Fragment Anisotropies and the Failure ofthe Statistical Theory of Fission Decay Rates

NUCLEAR REACTIONS 232Th(16O, F), (19F, F), E(cm)=70-110 MeV; 238U(16O, F), E(cm)=75-90 MeV; 236,238U, 237Np, 232Th(12C, F), E(cm)=55-80 MeV; 232Th, 238U(11B, F), E(cm)=40-50 MeV; 238U(7Li, F), E(cm)=24-40 MeV; measured fission fragment σ(θ); deduced anisotropy, entrance channel effects, compound nucleus features. Statistical model analysis.

doi: 10.1088/0954-3899/23/10/024
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1997LE31      Phys.Rev. C56, R2907 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Influence of the Ground State Spin of Target Nuclei on the Anomalous Behavior of Fission Fragment Anisotropies

NUCLEAR REACTIONS 235,236,238U(12C, F), E(cm)=57-82 MeV; measured fission σ, fragment σ(θ); deduced K-states equilibration time, anomalous behaviour target spin dependence.

doi: 10.1103/PhysRevC.56.R2907
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1997LI07      Phys.Rev.Lett. 78, 3074 (1997)

J.F.Liang, J.D.Bierman, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch, J.P.S.van Schagen

Entrance Channel Dependent Light Charged Particle Emission from the 156Er Compound Nucleus

NUCLEAR REACTIONS 144Sm(12C, X), E=142 MeV; 96Zr(60Ni, X), E=333 MeV; measured light charged particle energy spectra, (particle)(evaporation residue)-coin. 156Er deduced decay entrance channel dependent features.

doi: 10.1103/PhysRevLett.78.3074
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1997LI17      Phys.Rev. C56, 908 (1997)

J.F.Liang, J.D.Bierman, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch, J.P.S.van Schagen

Dissipative Effects in the Formation of the 156Er Compound Nucleus

NUCLEAR REACTIONS 144Sm(12C, X), E=142 MeV; 121Sb(35Cl, X), E=218 MeV; 96Zr(60Ni, X), E=333 MeV; measured E(p), I(p), E(alpha), I(alpha), (light charged particle)(residual nucleus)-coin, compound nucleus formation time scale. 156Er deduced entrance channel dependent features. Statistical model, preequilibrium decay.

doi: 10.1103/PhysRevC.56.908
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1455.


1996BI10      Phys.Rev.Lett. 76, 1587 (1996)

J.D.Bierman, P.Chan, J.F.Liang, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch

Experimental Fusion Barrier Distributions Reflecting Projectile Octupole State Coupling to Prolate and Oblate Target Nuclei

NUCLEAR REACTIONS, ICPND 194Pt(40Ca, X), E(cm) ≈ 160-200 MeV; 192Os(40Ca, X), E(cm) ≈ 150-190 MeV; measured fusion σ(E); deduced targets, projectile deformations role.

doi: 10.1103/PhysRevLett.76.1587
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1996BI20      Phys.Rev. C54, 3068 (1996)

J.D.Bierman, P.Chan, J.F.Liang, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch

Fusion Barrier Distributions for Heavy Ion Systems Involving Prolate and Oblate Target Nuclei

NUCLEAR REACTIONS, ICPND 192Os, 194Pt(40Ca, X), E(cm)=160-200 MeV; measured fusion σ(E). 197Au(40Ca, F), E=311, 233 MeV; measured fission fragment σ(θ); deduced fusion barriers.

doi: 10.1103/PhysRevC.54.3068
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