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NSR database version of April 27, 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, 64}Ni 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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