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NSR database version of April 11, 2024.

Search: Author = P.V.Drumm

Found 27 matches.

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2002BE52      Nucl.Phys. A701, 327c (2002)

J.R.J.Bennett, U.C.Bergmann, P.V.Drumm, J.Lettry, T.Nilsson, R.Catherall, O.C.Jonsson, H.L.Ravn, H.Simon, and the ISOLDE Collaboration

Release Studies of a Thin Foil Tantalum Target for the Production of Short-Lived Radioactive Nuclei

doi: 10.1016/S0375-9474(01)01606-2
Citations: PlumX Metrics

2002BE53      Nucl.Phys. A701, 363c (2002)

U.C.Bergmann, L.Axelsson, J.R.J.Bennett, M.J.G.Borge, R.Catherall, P.V.Drumm, V.N.Fedoseyev, C.Forssen, L.M.Fraile, H.O.U.Fynbo, U.Georg, T.Giles, S.Grevy, P.Hornshoj, B.Jonson, O.C.Jonsson, U.Koster, J.Lettry, K.Markenroth, F.M.Marques, V.I.Mishin, I.Mukha, T.Nilsson, G.Nyman, A.Oberstedt, H.L.Ravn, K.Riisager, G.Schrieder, V.Sebastian, H.Simon, O.Tengblad, F.Wenander, K.Wilhelmsen Rolander

Light Exotic Isotopes: Recent beam developments and physics applications at ISOLDE

RADIOACTIVITY 12Be(β-), (β-n); measured Eβ, β-delayed neutron spectra, T1/2. 14Be(β-); measured β-delayed neutrons, charged particles; deduced decay branching ratios. 9C(β+); measured Ep, Eα following daughter nucleus decay.

doi: 10.1016/S0375-9474(01)01611-6
Citations: PlumX Metrics

1999BE52      Nucl.Instrum.Methods Phys.Res. B155, 515 (1999)

J.R.J.Bennett, P.V.Drumm, R.Catherall, O.C.Jonsson, J.Lettry, T.Nilsson, H.Ravn, H.Simon, and the ISOLDE Collaboration

Measurements of Intense Beams of 11Li from a Tantalum Foil Target

doi: 10.1016/S0168-583X(99)00555-8
Citations: PlumX Metrics

1995ZH10      Nucl.Phys. A586, 483 (1995)

K.Zhao, J.S.Lilley, P.V.Drumm, D.D.Warner, R.A.Cunningham, J.N.Mo

The Exotic Transfer Reaction (18O, 17F) on 198Pt: Existence and mass of 199Ir

NUCLEAR REACTIONS 198Pt(18O, 17F), E=140 MeV; measured σ(θ), Q-value. 199Ir deduced mass excess, n-p interaction strengths.

doi: 10.1016/0375-9474(94)00805-W
Citations: PlumX Metrics

1994KE08      Nucl.Phys. A571, 326 (1994)

N.Keeley, S.J.Bennett, N.M.Clarke, B.R.Fulton, G.Tungate, P.V.Drumm, M.A.Nagarajan, J.S.Lilley

Optical Model Analyses of 6,7Li + 208Pb Elastic Scattering Near the Coulomb Barrier

NUCLEAR REACTIONS 208Pb(6Li, 6Li), E=25-39 MeV; 208Pb(7Li, 7Li), E=25-60 MeV; measured σ(θ); deduced optical model parameters. Double folding model.

doi: 10.1016/0375-9474(94)90064-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1878.

1993FR01      Nucl.Phys. A552, 10 (1993)

S.J.Freeman, R.Chapman, J.L.Durell, M.A.C.Hotchkis, F.Khazaie, J.C.Lisle, J.N.Mo, A.M.Bruce, R.A.Cunningham, P.V.Drumm, D.D.Warner

Two-Quasiproton Structures in Ytterbium-174

NUCLEAR REACTIONS 175Lu(t, α), E=35.5 MeV; measured absolute σ(θ). 174Yb deduced levels, L, J, π, K, M1 transition strengths distributions. Natural targets.

doi: 10.1016/0375-9474(93)90328-U
Citations: PlumX Metrics

1993FR04      Nucl.Phys. A554, 333 (1993)

S.J.Freeman, R.Chapman, J.L.Durell, M.A.C.Hotchkis, F.Khazaie, J.C.Lisle, J.N.Mo, A.M.Bruce, R.A.Cunningham, P.V.Drumm, D.D.Warner, J.D.Garrett

Two-Quasiproton Configurations in Dysprosium-164

NUCLEAR REACTIONS 165Ho(t, α), E=37.3 MeV; measured σ(θ). 164Dy deduced levels, transferred proton L, Nilsson assignments, J, π, K, configuration strengths. Natural targets.

doi: 10.1016/0375-9474(93)90225-M
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Data from this article have been entered in the XUNDL database. For more information, click here.

1993ZH31      Chin.Phys.Lett. 10, 265 (1993)

K.Zhao, J.S.Lilley, P.V.Drumm, D.D.Warner, R.A.Cunningham, J.N.Mo

Production of 199Ir via Exotic Nucleon Transfer Reaction

NUCLEAR REACTIONS 198Pt(18O, 17F), E=140 MeV; measured Q. 199Ir deduced mass excess.

doi: 10.1088/0256-307X/10/5/003
Citations: PlumX Metrics

1990SM03      Nucl.Phys. A517, 193 (1990)

M.J.Smithson, J.S.Lilley, M.A.Nagarajan, P.V.Drumm, R.A.Cunningham, B.R.Fulton, I.J.Thompson

The Threshold Anomaly in Inelastic Scattering

NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, 16O'), E=70-94 MeV; measured σ(θ); deduced model parameters. 208Pb deduced deformation lengths, quadrupole moment. DWBA analysis.

doi: 10.1016/0375-9474(90)90268-Q
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1989DR03      Nucl.Phys. A496, 530 (1989)

P.V.Drumm, L.K.Fifield, R.A.Bark, M.A.C.Hotchkis, C.L.Woods

The 40Ar(13C, 14O)39S Reaction and the Ground-State Mass of 39S

NUCLEAR REACTIONS 40Ar(13C, 14O), (13C, 15O), (13C, 12C), E=96 MeV; measured σ(E(14O)), σ(E(15O)), σ(E(12C)); deduced reaction mechanism, Q. 39S deduced mass excess, excited state. DWBA calculations. Gas target.

doi: 10.1016/0375-9474(89)90075-4
Citations: PlumX Metrics

1989FR06      Phys.Lett. 222B, 347 (1989)

S.J.Freeman, R.Chapman, J.L.Durell, M.A.C.Hotchkis, F.Khazaie, J.C.Lisle, J.N.Mo, A.M.Bruce, R.A.Cunningham, P.V.Drumm, D.D.Warner, J.D.Garrett

The Microscopic Structure of the M1 Mode in 164Dy

NUCLEAR REACTIONS 165Ho(t, α), E=37.3 MeV; measured σ(Eα), yield vs θ. 164Dy deduced levels, J, π, K, M1 transition features.

doi: 10.1016/0370-2693(89)90321-3
Citations: PlumX Metrics

1988FI04      Nucl.Phys. A484, 117 (1988)

L.K.Fifield, R.Chapman, J.L.Durell, J.N.Mo, R.J.Smith, P.J.Woods, B.R.Fulton, R.A.Cunningham, P.V.Drumm

The Mass of 37P

NUCLEAR REACTIONS 48Ca(36S, 37P), E=198 MeV; measured σ(E(37P)); deduced σ(θ), Q. 37P deduced mass excess.

doi: 10.1016/0375-9474(88)90144-3
Citations: PlumX Metrics

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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1986DR03      Nucl.Phys. A448, 93 (1986)

P.V.Drumm, O.Karban, A.K.Basak, P.M.Lewis, S.Roman, G.C.Morrison

Study of 14N by One-Nucleon Transfer Reactions Induced with Polarised 3He

NUCLEAR REACTIONS 13C, 15N(polarized 3He, 3He), 13C(polarized 3He, d), 15N(polarized 3He, α), E=33 MeV; measured σ(θ), A(θ); deduced optical-model parameters. 14N levels deduced j-transfer values, S(lj).

doi: 10.1016/0375-9474(86)90182-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0086.

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
Citations: PlumX Metrics

1986FI06      Nucl.Phys. A453, 497 (1986)

L.K.Fifield, C.L.Woods, W.N.Catford, R.A.Bark, P.V.Drumm, K.T.Keoghan

The Mass of 35Si

NUCLEAR REACTIONS 34,36S(13C, 14O), E=91 MeV; measured σ(E(14O)). 35Si deduced mass excess. 33Si deduced energy levels. Enriched targets.

doi: 10.1016/0375-9474(86)90449-5
Citations: PlumX Metrics

1986WO07      Phys.Lett. 182B, 297 (1986)

P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, R.J.Smith, B.R.Fulton, R.A.Cunningham, P.V.Drumm, L.K.Fifield

The Mass of 33Al

NUCLEAR REACTIONS 48Ca(36S, 33Al), E=198 MeV; measured σ(E(33Al)). 33Al deduced mass excess. Enriched target, magnetic spectrometer. Mass, large basis shell models.

doi: 10.1016/0370-2693(86)90094-8
Citations: PlumX Metrics

1985DR06      Nucl.Phys. A441, 95 (1985)

P.V.Drumm, L.K.Fifield, R.A.Bark, M.A.C.Hotchkis, C.L.Woods, P.Maier-Komor

Ground-State Mass Excesses and Low-Lying Levels of the Neutron-Rich Nuclei 36P, 35P and 34P

NUCLEAR REACTIONS 36,34S(7Li, 7Be), 36S(6Li, 7Be), E=52 MeV; 36,34S(11B, 11C), E=83 MeV; measured σ(E(7Be)), σ(E(11C)). 36,35,34P deduced mass excess, levels. Enriched targets.

doi: 10.1016/0375-9474(85)90169-1
Citations: PlumX Metrics

1985FI03      Nucl.Phys. A440, 531 (1985)

L.K.Fifield, C.L.Woods, R.A.Bark, P.V.Drumm, M.A.C.Hotchkis

Masses and Level Schemes of 33Si and 34Si

NUCLEAR REACTIONS 36S(11B, 13N), (11B, 14N), E=83 MeV; measured σ(E(13N)), σ(E(14N)). 33,34Si deduced ground-state mass excesses, levels. Enriched targets.

doi: 10.1016/0375-9474(85)90244-1
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1985FI08      Nucl.Phys. A437, 141 (1985)

L.K.Fifield, P.V.Drumm, M.A.C.Hotchkis, T.R.Ophel, C.L.Woods

The 26Mg(18O, 17F)27Na and 26Mg(18O, 15O)29Mg Reactions and the Level Schemes of 27Na and 29Mg

NUCLEAR REACTIONS 26Mg(18O, 17F), (18O, 15O), E=100-117 MeV; measured σ(E(17F)), σ(E(15O)). 27Na, 29Mg deduced levels, ground state mass excesses. Enriched targets.

doi: 10.1016/0375-9474(85)90230-1
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1985WO04      Nucl.Phys. A437, 454 (1985)

C.L.Woods, L.K.Fifield, R.A.Bark, P.V.Drumm, M.A.C.Hotchkis

A Study of 25Ne via the 26Mg(13C, 14O)25Ne Reactions

NUCLEAR REACTIONS 24,26Mg(13C, 14O), E=96 MeV; measured σ(E(14O)). 25Ne deduced mass excess, levels. Enriched target.

doi: 10.1016/0375-9474(85)90101-0
Citations: PlumX Metrics

1984CO20      Phys.Rev. C30, 1538 (1984)

J.Cook, K.W.Kemper, P.V.Drumm, L.K.Fifield, M.A.C.Hotchkis, T.R.Ophel, C.L.Woods

16O(7Li, 7Be)16N Reaction at 50 MeV

NUCLEAR REACTIONS 16O(7Li, 7Li), (7Li, 7Be), E=50 MeV; measured σ(θ), σ(E(16N)); deduced optical model parameters. 16N levels deduced spectroscopic amplitudes. Microscopic DWBA analysis.

doi: 10.1103/PhysRevC.30.1538
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1521.

1984FI02      Nucl.Phys. A417, 534 (1984)

L.K.Fifield, M.A.C.Hotchkis, P.V.Drumm, T.R.Ophel, G.D.Putt, D.C.Weisser

The Mass and Low-Lying Levels of 40Cl

NUCLEAR REACTIONS 40Ar(7Li, 7Be), E=52, 54 MeV; 40Ar(11B, 11C), (11B, 13N), E=81 MeV; measured σ(E(7Be)), σ(E(11C)), σ(E(13N)). 40Cl deduced mass excess, levels. 38S deduced levels.

doi: 10.1016/0375-9474(84)90411-1
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1983DR06      Phys.Lett. 126B, 155 (1983)

P.V.Drumm, J.B.A.England, O.Karban, J.M.Nelson, J.M.Barnwell, N.E.Sanderson

Break-Up of Polarized 3He at 33 MeV

NUCLEAR REACTIONS 12C, 27Al, 58Ni(polarized 3He, pd), E=33 MeV; measured σ(θd, θp, Ed), analyzing power vs θd, σ(θd, θp); deduced breakup yield on 3He spin orientation. Kinematically complete experiment.

doi: 10.1016/0370-2693(83)90581-6
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1983LE03      Nucl.Phys. A395, 204 (1983)

P.M.Lewis, A.K.Basak, J.D.Brown, P.V.Drumm, O.Karban, E.C.Pollacco, S.Roman

The Elastic and Inelastic Scattering of 33 MeV Polarized 3He from Oxygen and Iron Isotopes

NUCLEAR REACTIONS 17,18O, 54,56Fe(polarized 3He, 3He), (polarized 3He, 3He'), E=33 MeV; measured σ(θ), A(θ); deduced optical model parameters, deformation parameters. Enriched targets.

doi: 10.1016/0375-9474(83)90096-9
Citations: PlumX Metrics

1983LE17      Nucl.Phys. A404, 205 (1983)

P.M.Lewis, O.Karban, J.M.Barnwell, J.D.Brown, P.V.Drumm, J.M.Nelson, S.Roman

The (3He, p) Reaction Induced by Polarized 3He on 7Li, 9Be and 12C

NUCLEAR REACTIONS 12C, 9Be, 7Li(polarized 3He, p), E=33 MeV; 9Be, 7Li(polarized 3He, p), E=14 MeV; measured σ(θ), A(θ). Natural targets. Microscopic model, cluster transfer DWBA, coupled-channels analyses.

doi: 10.1016/0375-9474(83)90547-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0048.

1983RO22      Phys.Rev. C28, 2515 (1983)

S.Roman, O.Karban, M.Barnwell, J.D.Brown, P.V.Drumm, P.M.Lewis, J.M.Nelson

Polarization Effects in Two-Nucleon Transfer Reactions and Time-Reversal Invariance

NUCLEAR REACTIONS 7Li, 9Be(polarized 3He, p), E=14 MeV; 12C(polarized 3He, p), E=33 MeV; measured analyzing power vs θ; deduced reaction mechanism, time reversal invariance validity.

doi: 10.1103/PhysRevC.28.2515
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