NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = A.R.Poletti

Found 113 matches.

    Showing 1 to 100.

   [Next]

Back to query form


2005PO10      Nucl.Phys. A756, 83 (2005)

A.R.Poletti, A.P.Byrne, G.D.Dracoulis, T.Kibedi, P.M.Davidson

High spin states in 210Rn approaching the region of 3-particle-hole neutron excitations

NUCLEAR REACTIONS 198Pt(17O, 5n), E=96 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin, E(ce), I(ce). 210Rn deduced high-spin levels, J, π, ICC, configurations. Enriched target, pulsed beam, superconducting electron spectrometer.

NUCLEAR STRUCTURE 210Rn; calculated levels, J, π, configurations. Semi-empirical shell model, neutron core excitation.

doi: 10.1016/j.nuclphysa.2005.03.020
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

2000PO03      Nucl.Phys. A665, 318 (2000)

A.R.Poletti, G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery, B.Fabricius, T.Kibedi, P.M.Davidson

Core-Excitations in 209Po

NUCLEAR REACTIONS 204Hg(9Be, 4n), E=62 MeV; measured Eγ, γγ-coin, Iγ(θ), linear polarisation. 209Po deduced high spin levels J, π, half-life. Comparison with shell model calculations.

doi: 10.1016/S0375-9474(99)00421-2
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

1999LA26      Phys.Rev. C60, 067301 (1999)

G.J.Lane, G.D.Dracoulis, A.P.Byrne, A.R.Poletti, T.R.McGoram

Population of High-Spin States in 234U by an Incomplete-Fusion Reaction

NUCLEAR REACTIONS 232Th(9Be, 3nα), E=52 MeV; measured Eγ, Iγ, γγ-, αγ-coin; deduced incomplete fusion mechanism. 234U deduced levels, possible J, π.

doi: 10.1103/PhysRevC.60.067301
Citations: PlumX Metrics

1998MC03      Nucl.Phys. A637, 469 (1998)

T.R.McGoram, G.D.Dracoulis, A.P.Byrne, A.R.Poletti, S.Bayer

High-Spin Isomers in 211Po and Related Structures in 210Po and 212Po

NUCLEAR REACTIONS 208Pb(9Be, 2nα), E=50 MeV; measured αγγ(t), αγ(t), Eγ, Iγ. 208Pb(7Li, 3np), E=56 MeV; measured γγ(t), Eγ, Iγ. 211Po deduced high-spin levels, isomer T1/2, reduced transition probabilities. Enriched targets, pulsed beam, Compton supressed Ge detectors.

NUCLEAR STRUCTURE 210,211,212Po; calculated levels, J, π, B(λ). Semi-empirical shell model. Yrast configurations, residual interaction.

doi: 10.1016/S0375-9474(98)00227-9
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

1998ST24      Nucl.Phys. A641, 401 (1998)

A.E.Stuchbery, G.D.Dracoulis, T.Kibedi, A.P.Byrne, B.Fabricius, A.R.Poletti, G.J.Lane, A.M.Baxter

Spectroscopy of 215Ra: The shell model and enhanced E3 transitions

NUCLEAR REACTIONS 206Pb(13C, 4n), E=66-84 MeV; measured Eγ, Iγ(θ), Iγ(θ, H, t), γγ(t), (X-ray)γ(t), I(ce)(t). 215Ra deduced levels J, π, g, T1/2, reduced transition probabilities, ICC. Enriched targets, pulsed beam, Ge hyper-pure, planar Ge, Compton-supressed detectors, superconducting solenoidal electron spectrometer, Si(Li) detector.

NUCLEAR STRUCTURE 215Ra; calculated levels, B(λ), g. Semi-empirical shell model, octupole coupling.

doi: 10.1016/S0375-9474(98)00484-9
Citations: PlumX Metrics

1997PO04      Nucl.Phys. A615, 95 (1997)

A.R.Poletti, G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery, B.Fabricius, T.Kibedi, P.M.Davidson

Core-Excited States and the Yrast Line in 208Po

NUCLEAR REACTIONS 204Hg(9Be, 5n), E=55-65 MeV; measured γγ(t), Eγ, Iγ(θ), Iγ(E, t), linear polarization. 208Po deduced high-spin levels, J, π, T1/2, γ-multipolarity, δ. Enriched tatget, pulsed beam, Compton suppressed detectors, Ge hyperpure detectors in linear polarimeter.

NUCLEAR STRUCTURE 208Po; calculated levels. Semi-empirical shell model.

doi: 10.1016/S0375-9474(96)00428-9
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

1994PO20      Nucl.Phys. A580, 43 (1994)

A.R.Poletti, G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery, B.Fabricius, T.Kibedi, P.M.Davidson

Structure of High-Spin Yrast States in 205Pb and 206Pb

NUCLEAR REACTIONS 204Hg(9Be, 4nα), (9Be, 3nα), E=55-65 MeV; measured γγ(t), Eγ, Iγ(θ), Iγ(E, t), linear polarization. 205,206Pb deduced high-spin levels J, π, T1/2. Enriched target, pulsed beam, Ge hyperpure Compton suppressed detectors, Ge hyperpure detectors in linear polarimeter.

NUCLEAR STRUCTURE 205,206Pb; calculated levels. Semi-empirical shell model.

doi: 10.1016/0375-9474(94)90814-1
Citations: PlumX Metrics

1994PO21      Nucl.Phys. A580, 64 (1994)

A.R.Poletti, G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery, B.Fabricius, T.Kibedi, P.M.Davidson

Structure of Low-Lying High-Spin States in 204Hg and 205Hg

NUCLEAR REACTIONS 204Hg(9Be, 9Be'), (9Be, 2α), E=55-65 MeV; measured γγ(t), Eγ, Iγ(θ), Iγ(E, t). 204,205Hg deduced high-spin levels J, π, T1/2. Enriched target, pulsed beam, Ge hyper-pure Compton suppressed detectors, Ge hyper-pure detectors in linear polarimeter.

NUCLEAR STRUCTURE 204,205Hg; calculated levels. Semi-empirical shell model.

doi: 10.1016/0375-9474(94)90815-X
Citations: PlumX Metrics

1993DA10      Nucl.Phys. A560, 822 (1993)

P.M.Davidson, G.D.Dracoulis, A.P.Byrne, T.Kibedi, B.Fabricius, A.M.Baxter, A.E.Stuchbery, A.R.Poletti, K.J.Schiffer

Spectroscopy of 211Rn Approaching the Valence Limit

NUCLEAR REACTIONS 198Pt(18O, 5n), E=96 MeV; measured γγ(t), Eγ, Iγ(E, t), I(ce). 211Rn deduced levels J, π, T1/2, ICC. Enriched target, pulse beam, Ge hyperpure, Compton-suppressed detectors, Si(Li), superconducting electron spectrometer.

NUCLEAR STRUCTURE 211Rn; calculated levels, B(λ). Multi-particle octupole-coupling model, shell model.

doi: 10.1016/0375-9474(93)90173-U
Citations: PlumX Metrics

1992ST09      Nucl.Phys. A548, 159 (1992)

A.E.Stuchbery, G.D.Dracoulis, T.Kibedi, A.P.Byrne, B.Fabricius, A.R.Poletti, G.J.Lane, A.M.Baxter

Spectroscopy and Shell Model Interpretation of High-Spin States in the N = 126 Nucleus 214Ra

NUCLEAR REACTIONS 206Pb(12C, 4n), E=66-84 MeV; 206Pb(13C, 5n), E=66-84 MeV; measured γγ(t), (X-ray)γ(t), Eγ, Iγ(θ), I(ce)(t), Iγ(E, t), Iγ(θ, H, t). 214Ra deduced levels J, π, T1/2, g, B(λ), ICC. Enriched targets, pulsed-beam, Ge hyper-pure, planar Ge, Compton suppressed detectors, superconducting solenoidal electron spectrometer, Si(Li) detector.

NUCLEAR STRUCTURE 214Ra; calculated levels, B(λ), g. Semi-empirical shell model, octupole coupling.

doi: 10.1016/0375-9474(92)90081-T
Citations: PlumX Metrics

1990BA31      Nucl.Phys. A515, 493 (1990)

A.M.Baxter, A.P.Byrne, G.D.Dracoulis, R.A.Bark, F.Riess, A.E.Stuchbery, M.C.Kruse, A.R.Poletti

Spectroscopy of High-Spin States of 206Po

NUCLEAR REACTIONS 198Pt(13C, 5n), E=70-80 MeV; measured γγ(t), (13C)γ(t), Eγ, Iγ, Iγ(E), Iγ(θ), I(ce). 206Po deduced levels, J, π, T1/2, B(λ), ICC. Enriched targets, Ge, Si(Li) detectors, pulsed beam. Empirical shell model calculations.

doi: 10.1016/0375-9474(90)90595-D
Citations: PlumX Metrics

1990DR07      Phys.Lett. 246B, 31 (1990)

G.D.Dracoulis, P.M.Davidson, A.P.Byrne, B.Fabricius, T.Kibedi, A.M.Baxter, A.E.Stuchbery, A.R.Poletti, K.J.Schiffer

High-Spin Yrast Isomers in 211Rn and 212Rn with Enhanced E3 Decays

NUCLEAR REACTIONS 198Pt(18O, 5n), (18O, 4n), E ≈ 96 MeV; 204Hg(13C, 5n), E not given; measured γγ-coin, γγ(t), Iγ(θ). 211,212Rn deduced levels, J, π, isomers, T1/2, B(λ), ICC. Multiparticle octupole-vibration coupled model.

doi: 10.1016/0370-2693(90)91303-S
Citations: PlumX Metrics

1990DR12      Nucl.Phys. A520, 353c (1990)

G.D.Dracoulis, P.M.Davidson, A.P.Byrne, B.Fabricius, T.Kibedi, A.M.Baxter, A.E.Stuchbery, A.R.Poletti, K.J.Schiffer

High-Spin Yrast Isomers in 211Rn and 212Rn with Enhanced E3 Decays

NUCLEAR REACTIONS 198Pt(18O, 4n), (18O, 5n), E=96 MeV; 204Hg(13C, 5n), E not given; measured γγ(t), I(ce), Eγ, Iγ. 211,212Rn deduced levels, J, π, yrast isomers, T1/2, ICC, B(λ).

doi: 10.1016/0375-9474(90)91159-O
Citations: PlumX Metrics

1988ST10      Nucl.Phys. A482, 692 (1988)

A.E.Stuchbery, G.D.Dracoulis, A.P.Byrne, S.J.Poletti, A.R.Poletti

Spectroscopy and Octupole Coupling of High-Spin States in 213Rn

NUCLEAR REACTIONS 208Pb(9Be, 4n), E=45-60 MeV; 204Hg(13C, 4n), E=72-75 MeV; measured γγ(t), Xγ(t), E(γ), I(γ)(θ), I(ce), I(γ)(θ, H, t), I(γ)(E, t). 213Rn deduced levels J, π, T1/2, g, reduced transition probabilities, ICC. Enriched targets, pulsed-beam, Ge hyperpure, planar Ge, Si(Li), Compton suppressed detectors.

NUCLEAR STRUCTURE 213Rn; calculated levels, B(E3), g. Semi-empirical shell model.

doi: 10.1016/0375-9474(88)90176-5
Citations: PlumX Metrics

1988ST17      Nucl.Phys. A486, 397 (1988)

A.E.Stuchbery, G.D.Dracoulis, A.P.Byrne, A.R.Poletti

Spectroscopy of 212Rn

NUCLEAR REACTIONS 208Pb(9Be, 5n), E=45-60 MeV; 204Hg(13C, 5n), E=72-75 MeV; measured γγ(t), (X-ray)γ(t), Eγ, Iγ(θ), I(ce), Iγ(θ, H, t), Iγ(E, t). 212Rn deduced levels J, π, T1/2, g, B(λ), ICC. Enriched targets, pulsed beam, Ge hyperpure, planar Ge, Si(Li), Compton suppressed detectors.

NUCLEAR STRUCTURE 212Rn; calculated levels, B(λ), g. Shell model.

doi: 10.1016/0375-9474(88)90243-6
Citations: PlumX Metrics

1987DR08      Nucl.Phys. A467, 305 (1987)

G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery, R.A.Bark, A.R.Poletti

Valence Configurations in 214Rn

NUCLEAR STRUCTURE 214Rn; calculated level energies. Semi-empirical shell model.

NUCLEAR REACTIONS 208Pb(9Be, 3n), E=45-57 MeV; measured γγ(t), γ(t), Eγ, Iγ(θ), I(ce). 214Rn deduced levels, J, π, T1/2, B(λ), ICC. Enriched targets, Ge, Si(Li), Compton suppressed detectors. Pulsed beam.

doi: 10.1016/0375-9474(87)90532-X
Citations: PlumX Metrics

1987PO14      Nucl.Phys. A473, 595 (1987)

A.R.Poletti, G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery

The Low-Lying Yrast Structure of 212Po

NUCLEAR REACTIONS 208Pb(9Be, nα), E=45-57 MeV; measured γγ(t), γ(t), Eγ, Iγ(θ), I(ce). 212Po deduced levels, J, π, T1/2, B(λ), ICC. Enriched targets, Ge, Si(Li), Compton suppressed detectors, pulsed beam.

NUCLEAR STRUCTURE 212Po; calculated level energies. Semi-empirical shell model.

doi: 10.1016/0375-9474(87)90141-2
Citations: PlumX Metrics

1986BY01      Nucl.Phys. A448, 137 (1986)

A.P.Byrne, G.D.Dracoulis, C.Fahlander, H.Hubel, A.R.Poletti, A.E.Stuchbery, J.Gerl, R.F.Davie, S.J.Poletti

Spectroscopy of High-Spin States in 211,212,213Fr

NUCLEAR STRUCTURE 211,212,213Fr; calculated levels, B(E3). Shell model.

NUCLEAR REACTIONS 203,205Tl(12C, xn), (13C, xn), E=77-96 MeV; 198Pt(19F, 5n), E=102 MeV; measured γγ(t), nγ(t), (X-ray)γ(t), Eγ, I(ce), Iγ(θ, H, t), Iγ(E, t). 211Fr, 212Fr, 213Fr deduced levels J, T1/2, g, reduced transition probabilities, ICC. Pulsed-beam, Ge(Li), hyperpure, planar Ge, NE213, Si(Li) detectors.

doi: 10.1016/0375-9474(86)90185-5
Citations: PlumX Metrics

1986DR05      J.Phys.(London) G12, L97 (1986)

G.D.Dracoulis, A.E.Stuchbery, A.P.Byrne, A.R.Poletti, S.J.Poletti, J.Gerl, R.A.Bark

Shape Coexistence in Very Neutron-Deficient Pt Isotopes

NUCLEAR STRUCTURE 176,178,182,184,186,188Pt; analyzed data; deduced shape coexistence evidence.

NUCLEAR REACTIONS 144Sm(35Cl, 2np), (37Cl, 2np), E=173, 170 MeV; measured reaction products, γγ-, γ(X-ray)-coin. 176,178Pt; deduced levels energies, J, π, T1/2, B(E2), yrast band structure, shape coexistence.

doi: 10.1088/0305-4616/12/3/005
Citations: PlumX Metrics

1986PO01      Nucl.Phys. A448, 189 (1986)

S.J.Poletti, G.D.Dracoulis, A.R.Poletti, A.P.Byrne, A.E.Stuchbery, J.Gerl

g-Factors in 210Rn and Octupole Coupling of Core-Excited States in 210Rn, 211Rn and 212Rn

NUCLEAR STRUCTURE 210,211,212Rn; calculated levels, g, B(λ). Semi-empirical shell model, particle-vibration coupling.

NUCLEAR REACTIONS 202Hg(12C, 4n), E=78 MeV; measured Iγ(θ, H, t). 210Rn deduced g. Semi-empirical shell-model calculations, particle-vibration coupling.

doi: 10.1016/0375-9474(86)90186-7
Citations: PlumX Metrics

1985GE05      Nucl.Phys. A443, 348 (1985)

J.Gerl, G.D.Dracoulis, A.P.Byrne, A.R.Poletti, S.J.Poletti, A.E.Stuchbery

Spectroscopy of 166W and 167W and Alignment Effects in very Neutron-Deficient Tungsten Nuclei

NUCLEAR REACTIONS 142Nd(28Si, 4n), E=150 MeV; 142Nd(28Si, 3n), E=140 MeV; 147Sm(24Mg, 4n), E=128 MeV; measured Eγ, Iγ(θ), γγ-, γX ray-coin. 166,167W deduced levels, J, π, γ-branching, rotational bands. Compton-suppressed detector. Cranked shell model calculations, band crossings, alignment.

doi: 10.1016/0375-9474(85)90267-2
Citations: PlumX Metrics

1985LE17      Nucl.Phys. A443, 210 (1985)

P.M.Lewis, A.R.Poletti, M.J.Savage, C.L.Woods

The Mean Life of the Second 0+ State in 42Ca

NUCLEAR REACTIONS 42Ca(p, p'γ), E=5 MeV; measured pγ-coin. 42Ca level deduced T1/2, B(E2). Enriched target, direct electronic timing.

doi: 10.1016/0375-9474(85)90260-X
Citations: PlumX Metrics

1985PO06      Phys.Lett. 154B, 263 (1985)

A.R.Poletti, G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery, S.J.Poletti, J.Gerl, P.M.Lewis

Magnetic Moments, E3 Transitions and the Structure of High-Spin Core Excited States in 211Rn

NUCLEAR REACTIONS 204Hg(12C, 5n), E=85 MeV; measured γ(θ, H, t). 211Rn deduced levels, J, π, T1/2, g, γ-branching, B(λ), configurations. Shell model.

doi: 10.1016/0370-2693(85)90360-0
Citations: PlumX Metrics

1985PO08      Nucl.Phys. A440, 118 (1985)

A.R.Poletti, G.D.Dracoulis, C.Fahlander, A.P.Byrne

The Yrast Spectroscopy of 209Rn

NUCLEAR REACTIONS 198Pt(16O, 5n), E=81-94 MeV; 198Pt(17O, 6n), E=87-95 MeV; 205Tl(10B, 6n), E=63-75 MeV; measured γγ-, nγ-coin, nγ(t), (16O)γ(t), Eγ, Iγ, Iγ(θ), I(ce). 209Rn deduced levels, J, π, T, configurations, isomers, yrast states, ICC. Ge, Ge(Li), NE213, Si-Li detectors, enriched targets.

doi: 10.1016/0375-9474(85)90045-4
Citations: PlumX Metrics

1985PO13      Nucl.Phys. A442, 153 (1985)

A.R.Poletti, G.D.Dracoulis, S.J.Poletti, A.P.Byrne, A.E.Stuchbery, J.Gerl

Short-Lived Isomers in 211Rn and 210Rn

NUCLEAR REACTIONS 198Pt(18O, 5n), E=92 MeV; 198Pt(17O, 5n), E=95 MeV; measured γ(18O)(t), γ(17O)(t). 211,210Rn deduced T1/2, isomers, yrast states. Ge, NE213 detectors, enriched targets.

doi: 10.1016/0375-9474(85)90139-3
Citations: PlumX Metrics

1984BH03      Nucl.Phys. A420, 96 (1984)

R.K.Bhalla, A.R.Poletti

Accurate Measurements of E2 Lifetimes using the Coincidence Recoil-Distance Method

NUCLEAR REACTIONS 19F, 23Na, 27Al, 35Cl(α, p), E=6.3-7.3 MeV; measured Eγ, Iγ, Doppler shift, recoil, pγ-, pα-coin. 22Ne, 26Mg, 30Si, 38Ar deduced T1/2. Natural targets.

doi: 10.1016/0375-9474(84)90659-6
Citations: PlumX Metrics

1984DA19      Nucl.Phys. A430, 454 (1984)

R.F.Davie, A.R.Poletti, G.D.Dracoulis, A.P.Byrne, C.Fahlander

Isomers and High-Spin States in 205At

NUCLEAR REACTIONS 197Au(13C, 5n), E ≈ 80 MeV; measured γγ-, nγ-coin, nγ(t), Eγ, Iγ, γ(θ). 205At deduced levels, J, π, ICC, configurations. Ge(Li), Ge, NE213, Si(Li) detectors, natural target. Core-polarization calculations.

doi: 10.1016/0375-9474(84)90049-6
Citations: PlumX Metrics

1983TR03      Nucl.Phys. A395, 274 (1983)

W.J.Triggs, A.R.Poletti, G.D.Dracoulis, C.Fahlander, A.P.Byrne

High Spin States in 208Rn

NUCLEAR REACTIONS 196Pt(16O, 4n), E ≈ 89 MeV; measured γγ(t), nγ(t), Eγ, Iγ(θ), I(ce). 208Rn levels deduced J, π, T1/2, ICC, yrast states, isomers. Low energy photon spectrometer, Ge(Li), Si(Li), NE213 detectors, enriched target. Shell-model calculations, configurations.

doi: 10.1016/0375-9474(83)90101-X
Citations: PlumX Metrics

1983VE03      Phys.Rev. C28, 432 (1983)

W.J.Vermeer, R.K.Bhalla, A.R.Poletti

Mean Life of 10B(718 keV) and Its Role in Determining the Giant Dipole Resonance Contribution to Coulomb Excitation of 10B

NUCLEAR REACTIONS 10B(p, p'), E=4.5 MeV; measured pγ-coin. 10B level deduced T1/2. Enriched target.

doi: 10.1103/PhysRevC.28.432
Citations: PlumX Metrics

1982BH06      Nucl.Phys. A390, 189 (1982)

R.K.Bhalla, A.R.Poletti

Mean Lives of the 5.106 and 8.834 MeV Levels of 14N

NUCLEAR REACTIONS 11B(α, n), E=8, 8.8 MeV; measured Eγ(θγ=0°), Doppler shift, recoil. 14N levels deduced T1/2. Enriched target.

doi: 10.1016/0375-9474(82)90156-7
Citations: PlumX Metrics

1982BY01      Nucl.Instrum.Methods 193, 489 (1982)

A.P.Byrne, A.R.Poletti

A Two Crystal Compton Polarimeter using Standard Ge(Li) Detectors

NUCLEAR REACTIONS 50Ti, Cr(α, n), E=11 MeV; measured Eγ, Iγ, linear polarization vs θ, γ(θ). 53Cr levels deduced π, γ-branching, δ. Two crystal Compton polarimeter, sum, difference spectra.

doi: 10.1016/0029-554X(82)90240-3
Citations: PlumX Metrics

1982GO13      J.Phys.(London) G8, 1391 (1982)

D.R.Gordon, A.R.Poletti

E2/M1 Mixing Ratio of the 4.28 → 2.23 MeV Transition in 32S

NUCLEAR REACTIONS 32S(p, p'), E=7.5 MeV; measured pγ-coin, pγ(θ), Eγ, Iγ. 32S transitions deduced δ.

doi: 10.1088/0305-4616/8/10/009
Citations: PlumX Metrics

1982PO03      Nucl.Phys. A380, 335 (1982)

A.R.Poletti, G.D.Dracoulis, C.Fahlander, I.Morrison

Yrast Traps and High-States in 210Rn

NUCLEAR REACTIONS 205Tl(10B, 5n), E ≈ 70 MeV; 198Pt(16O, 4n), E ≈ 90 MeV; 198Pt(17O, 5n), E ≈ 96 MeV; measured γγ-, nγ-coin, nγ(t), Eγ, Iγ, γ(θ), ICC. 210Rn deduced levels J, π, T, configurations, yrast traps. Ge(Li), Ge, NE213, Si-Li detectors, enriched targets. Shell-model.

doi: 10.1016/0375-9474(82)90109-9
Citations: PlumX Metrics

1982SJ01      Phys.Rev. C25, 889 (1982)

T.P.Sjoreen, D.B.Fossan, U.Garg, A.Neskakis, A.R.Poletti, E.K.Warburton

High-Spin States in 205At

NUCLEAR REACTIONS 197Au(12C, 4n), E=77 MeV; measured γγ-coin, γ(θ), γ(t), Eγ, Iγ. 205At deduced levels, J, π, T1/2, B(λ), γ-multipolarity.

doi: 10.1103/PhysRevC.25.889
Citations: PlumX Metrics

1982VE04      J.Phys.(London) G8, 743 (1982)

W.J.Vermeer, A.R.Poletti

Determination of Partial Decay Widths for the 2-, 8.87 MeV Level in 16O

NUCLEAR REACTIONS 19F(p, α), E=7.4 MeV; measured Eγ, Iγ, αγ-coin. 16O levels deduced transition strength, γ-branching, δ.

doi: 10.1088/0305-4616/8/5/014
Citations: PlumX Metrics

1982VE05      J.Phys.(London) G8, 851 (1982)

W.J.Vermeer, A.R.Poletti

Branching Ratio for the Isoscalar Transition 2+, T=1, 1.95 MeV → 0+, T=1, 0.66 MeV in 22Na

NUCLEAR REACTIONS 19F(α, n), (α, α'), E=5 MeV; measured γγ-coin. 19F deduced γ-branching upper limits. 22Na transition deduced branching ratio, B(E2).

doi: 10.1088/0305-4616/8/6/014
Citations: PlumX Metrics

1981DR10      Phys.Rev. C24, 2386 (1981)

G.D.Dracoulis, C.Fahlander, A.R.Poletti

High-Spin Isomer in 211Rn, and the Shape of the Yrast Line

NUCLEAR REACTIONS 198Pt(18O, 5n), E=96 MeV; measured σ(E, Eγ), γγ-, nγ-coin, I(ce), γ(θ). 211Rn deduced yrast levels, J, π, T1/2, γ-multipolarity, γ-branching, configurations.

doi: 10.1103/PhysRevC.24.2386
Citations: PlumX Metrics

1981PO07      Phys.Rev. C23, 1550 (1981)

A.R.Poletti, E.K.Warburton, J.W.Olness

Nuclear Structure of High-Spin States in 46Ti and 46V

NUCLEAR REACTIONS 40Ca(9Be, n2p), (9Be, p2n), E=20-45 MeV; measured σ(E, Eγ), γγ-coin, Iγ(θ), DSA, recoil. 46V, 46Ti deduced levels, J, π, γ-multipolarity, transition strengths, T1/2.

doi: 10.1103/PhysRevC.23.1550
Citations: PlumX Metrics

1981PO08      Nucl.Phys. A359, 180 (1981)

A.R.Poletti, G.D.Dracoulis, C.Fahlander, I.Morrison

High-Spin States and Yrast Isomers in 211Rn

NUCLEAR REACTIONS 205Tl(11B, 5n) E ≈ 70 MeV; 198Pt(18O, 5n), E ≈ 95 MeV; measured γγ-, nγ-coin, nγ(t), γγ(t), Eγ, Iγ, γ(θ). 211Rn deduced levels J, π, T, ICC, configurations. Ge, Ge(Li), NE213 detectors, enriched targets. Shell-model calculations.

doi: 10.1016/0375-9474(81)90218-9
Citations: PlumX Metrics

1980FI07      J.Phys.(London) G6, 723 (1980)

L.K.Fifield, A.R.Poletti, D.C.Radford

Isovector Magnetic Dipole Transition in 22Na

NUCLEAR REACTIONS 19F(α, n), E=5.4 MeV; measured DSA, recoil. 22Na levels deduced T1/2, B(M1). Natural CaF2 target, Ge(Li) detector.

doi: 10.1088/0305-4616/6/6/009
Citations: PlumX Metrics

1980PO07      Phys.Rev.Lett. 45, 1475 (1980)

A.R.Poletti, G.D.Dracoulis, C.Fahlander

Low-Lying Yrast States in 210Rn and 211Rn and the Competition between Neutron-Hole and Proton Excitations

NUCLEAR REACTIONS 205Tl(11B, 5n), (10B, 5n), E=70 MeV; measured γ(t), γγ(t), γ(θ). 210,211Rn deduced yrast states, J, π, T1/2, ICC, B(E2), competing neutron-hole, proton excitations.

doi: 10.1103/PhysRevLett.45.1475
Citations: PlumX Metrics

1979BE41      Aust.J.Phys. 32, 195 (1979)

D.J.Beale, A.R.Poletti, J.R.Southon

Gamma-Ray Studies Using a Solid Argon Target: Properties of States in 40K and 40Ar

NUCLEAR REACTIONS 40Ar(p, n), (p, p'), E=5.75 MeV; measured Eγ, Iγ, DSA, Iγ(θ). 40K levels deduced T1/2, J, δ. 40Ar levels deduced T1/2. Solid Ar target. Weak coupling, delta function interaction model.

doi: 10.1071/PH790195
Citations: PlumX Metrics

1979PO01      J.Phys.(London) G5, 575 (1979)

A.R.Poletti, L.K.Fifield, J.Asher, B.E.Cooke

Precision Doppler-Shift Attenuation Lifetime Measurements in 28Si and 31P

NUCLEAR REACTIONS 4He(28Si, α), (28Si, p), E=46.8, 48.0, 48.2 MeV; measured DSA. 28Si level deduced T1/2, B(λ). 31P levels deduced T1/2, B(λ). Compared with shell model. Implanted target.

doi: 10.1088/0305-4616/5/4/021
Citations: PlumX Metrics

1979PO19      Phys.Rev. C20, 1768 (1979)

A.R.Poletti, R.P.Sjoreen, D.B.Fossan, U.Garg, A.Neskakis, E.K.Warburton

High-Spin States in 210Rn: The Effect of the Neutron Holes on the Four-Proton Configurations

NUCLEAR REACTIONS 204Pb(9Be, 3nγ), E=40-55 MeV; measured γγ-coin, σ(E), Iγ(θ). 210Rn deduced levels, T1/2, γ-multipolarities, J. Pulsed beam.

doi: 10.1103/PhysRevC.20.1768
Citations: PlumX Metrics

1979RA05      J.Phys.(London) G5, 409 (1979)

D.C.Radford, A.R.Poletti

Lifetimes of Excited States in 54Mn and 53Cr

NUCLEAR REACTIONS 50Ti(α, n), E=9.0, 11.0 MeV; 51V(α, n), E=7.8, 10.5 MeV; measured Eγ, Iγ, Doppler shift, recoil distance. 53Cr, 54Mn levels deduced T1/2. Enriched, natural targets, Ge(Li) detector.

doi: 10.1088/0305-4616/5/3/011
Citations: PlumX Metrics

1978DR06      J.Phys.(London) G4, 1323 (1978)

G.D.Dracoulis, D.C.Radford, A.R.Poletti

Gamma Decay and Band Structures in 46Ti

NUCLEAR REACTIONS 43Ca(α, nγ), E=8-15 MeV; measured Eγ, σ(E, Eγ), γγ-coin, DSA, Iγ, γ(θ). 46Ti deduced levels, J, π, T1/2. Enriched targets, Ge(Li) detectors.

doi: 10.1088/0305-4616/4/8/014
Citations: PlumX Metrics

1978FI04      J.Phys.(London) G4, L65 (1978)

L.K.Fifield, J.Asher, A.R.Poletti

A Precise Measurement of the Lifetime of the Lowest 4+ State in 22Ne

NUCLEAR REACTIONS 4He(19F, p), E=28.2 MeV; measured DSA. 22Ne level deduced T1/2. Implanted target.

doi: 10.1088/0305-4616/4/3/005
Citations: PlumX Metrics

1978RA13      Nucl.Phys. A303, 134 (1978)

D.C.Radford, J.R.Southon, A.R.Poletti

Lifetime Measurements in 41Ar and 41K

NUCLEAR REACTIONS 40Ar(d, p), (d, n), E=2.99 MeV; measured Doppler shift. 41Ar, 41K levels deduced T1/2, transition strengths. Solid, gas targets, pγ-coin.

doi: 10.1016/0375-9474(78)90047-7
Citations: PlumX Metrics

1978WA09      Phys.Rev. C18, 1637 (1978)

E.K.Warburton, J.W.Olness, A.M.Nathan, A.R.Poletti

Yrast Decay Schemes from Heavy-Ion + 48Ca Fusion-Evaporation Reactions: IV. 53Cr, 54V, 62Co, and 61-63Ni

NUCLEAR REACTIONS 40Ca(9Be, xn), (9Be, xp), 48Ca(18O, xn), (18O, 3n), (18O, p), E=25-55 MeV; measured σ(E, Eγ), γγ-coin, γ(θ), recoil distance, DSA. 53Cr, 54V, 62Co, 61,62,63Ni deduced levels, J, π, T1/2, δ, B(λ), γ-branching. Enriched targets, Ge(Li) detectors.

doi: 10.1103/PhysRevC.18.1637
Citations: PlumX Metrics

1977PO07      J.Phys.(London) G3, 945 (1977)

A.R.Poletti, J.R.Southon

The Strength of the M2 Transition from the 7/2- Hole State in 43K

NUCLEAR REACTIONS 40Ar(α, p), E=10.4 MeV; measured γ(t) electronic timing. 43K level deduced T1/2, M2 strength.

doi: 10.1088/0305-4616/3/7/008
Citations: PlumX Metrics

1977RA01      Nucl.Phys. A275, 141 (1977)

D.C.Radford, A.R.Poletti

Recoil-Distance Lifetime Measurements in 22Na, 22Ne, 30P and 30Si

NUCLEAR REACTIONS 19F(α, nγ), (α, pγ), E=5.65 MeV; 27Al(α, nγ), E=6.18 MeV; 27Al(α, pγ), E=3.92 MeV; measured Eγ(θ(γ)=0), Doppler shift, recoil distance. 22Ne, 22Na levels deduced T1/2. 30Si, 30P levels deduced T1/2, B(λ). Natural targets.

doi: 10.1016/0375-9474(77)90280-9
Citations: PlumX Metrics

1977SO07      Aust.J.Phys. 30, 23 (1977)

J.R.Southon, A.R.Poletti, D.J.Beale

Angular Correlation Measurements in 33Si

NUCLEAR REACTIONS 32S(d, pγ), E=3.5 MeV; measured pγ(θ). 33S levels deduced J, π, δ, γ-branching.

doi: 10.1071/PH770023
Citations: PlumX Metrics

1976BA45      Phys.Rev. C14, 1782 (1976)

T.T.Bardin, J.G.Pronko, R.E.McDonald, A.R.Poletti, J.B.McGrory

Gamma-Ray Spectroscopy of Low-Lying States in 56Cr

NUCLEAR REACTIONS 54Cr(t, pγ), E=2.9 MeV; measured Eγ, Iγ, pγ-coin, γ(t), pγ(θ). 56Cr deduced levels, γ-branching, J, π, T1/2, δ. Shell model analysis.

doi: 10.1103/PhysRevC.14.1782
Citations: PlumX Metrics

1976BE14      Nucl.Phys. A261, 238 (1976)

D.J.Beale, A.R.Poletti, J.R.Southon

Lifetimes of Levels in 54Mn

NUCLEAR REACTIONS 54Cr(p, n), E=2.72-4.65 MeV; measured Doppler shift, σ(Eγ, θγ). 54Mn deduced levels, T1/2, δ, γ-branching. Enriched target.

doi: 10.1016/0375-9474(76)90567-4
Citations: PlumX Metrics

1976BR08      Phys.Rev. C13, 1194 (1976)

B.A.Brown, D.B.Fossan, P.M.S.Lesser, A.R.Poletti

Isomeric 17/2- Level and Parity Mixing in 93Tc

NUCLEAR REACTIONS 90Zr(6Li, 3n), E=34 MeV; measured γγ-coin, γ(θ, t). 93Tc deduced levels, parity mixing, T1/2, B(E2).

doi: 10.1103/PhysRevC.13.1194
Citations: PlumX Metrics

1976BR24      Phys.Rev. C14, 602 (1976)

B.A.Brown, D.B.Fossan, P.M.S.Lesser, A.R.Poletti

High-Spin States in 92Zr

NUCLEAR REACTIONS 88Sr(7Li, 2np), E=34 MeV; measured γγ-coin, γ(θ, t), Eγ, Iγ. 92Zr deduced levels, J, π, λ. Natural target. Ge(Li) detectors.

doi: 10.1103/PhysRevC.14.602
Citations: PlumX Metrics

1976BR29      Phys.Rev. C14, 1016 (1976)

B.A.Brown, D.B.Fossan, A.R.Poletti, E.K.Warburton

Lifetimes of Yrast States in 51Ti, 52Ti, and 52V

NUCLEAR REACTIONS 48Ca(6Li, 2npγ), E=26 MeV; 48Ca(7Li, 3npγ), (7Li, 2npγ), (7Li, 3nγ), E=28 MeV; measured recoil distance, σ(Eγ). 51,52Ti, 52V deduced levels, T1/2, B(E2).

doi: 10.1103/PhysRevC.14.1016
Citations: PlumX Metrics

1976KO10      Phys.Rev. C13, 1944 (1976)

J.J.Kolata, J.W.Olness, E.K.Warburton, A.R.Poletti

Investigation of High-Spin States in 38Ar

NUCLEAR REACTIONS 27Al(14N, n2pγ), E=40 MeV; measured γγ-coin, recoil distance. 38Ar deduced levels, J, π, T1/2, δ.

doi: 10.1103/PhysRevC.13.1944
Citations: PlumX Metrics

1976PO03      Phys.Rev. C13, 1180 (1976)

A.R.Poletti, E.K.Warburton, J.W.Olness, J.J.Kolata, P.Gorodetzky

Heavy-Ion Fusion-Evaporation Reactions: High Spin States in 43Ca and 43Sc

NUCLEAR REACTIONS 27Al(19F, n2pγ), (19F, 2pγ), (19F, 2nγ), (19F, αγ), (19F, 2nαγ), 27Al(19F, n3pγ), (19F, pαγ), (19F, npαγ), (19F, 2pαγ), (19F, 2αγ), 27Al(19F, n2αγ), (19F, p2αγ), (19F, 2nαγ), (19F, 2npγ), (19F, npγ), E=40 MeV; measured σ(Eγ, θ), γγ-coin, recoil distance, polarization. 43Ca, 43Sc deduced levels, J, π, λ, δ, T1/2. 40,44Ca, 44Sc levels deduced T1/2, λ. 40,41K, 38,40Ar, 41,42Ca calculated yrast levels.

doi: 10.1103/PhysRevC.13.1180
Citations: PlumX Metrics

1976SO03      J.Phys.(London) G2, 117 (1976)

J.R.Southon, L.K.Fifield, A.R.Poletti

Lifetimes of Excited States in 40Ar

NUCLEAR REACTIONS 40Ar(p, p'γ), E=6.75 MeV; measured p'γ-coin, DSA. 40Ar levels deduced T1/2, J, B(λ).

doi: 10.1088/0305-4616/2/2/008
Citations: PlumX Metrics

1976SO05      Nucl.Phys. A267, 263 (1976)

J.R.Southon, A.R.Poletti, D.J.Beale

Angular Correlation Measurements in 40Ar

NUCLEAR REACTIONS 40Ar(p, p'), E=6.4, 7.0 MeV; measured pγ(θ). 40Ar deduced δ, γ-branching ratios, levels, J, transition strengths. Gas target.

doi: 10.1016/0375-9474(76)90659-X
Citations: PlumX Metrics

1976SO08      Aust.J.Phys. 29, 355 (1976)

J.R.Southon, A.R.Poletti, D.J.Beale

Angular Correlations in 19O

NUCLEAR REACTIONS 18O(d, pγ), E=5 MeV; measured pγ(θ). 19O levels deduced J, π, δ, B(λ).

doi: 10.1071/PH760355
Citations: PlumX Metrics

1976WA03      Phys.Rev. C13, 1762 (1976)

E.K.Warburton, J.W.Olness, J.J.Kolata, A.R.Poletti

High-Spin Yrast Levels in 39Ar

NUCLEAR REACTIONS 24Mg(18O, n2pγ), (18O, nαγ), 27Al(18O, npαγ), E=20-60 MeV; measured polarization, γγ-coin, Doppler shift. 39Ar deduced levels, J, π, T1/2.

doi: 10.1103/PhysRevC.13.1762
Citations: PlumX Metrics

1976WA11      Phys.Rev. C14, 996 (1976)

E.K.Warburton, J.W.Olness, A.R.Poletti, J.J.Kolata

Decay Schemes for High-Spin States in 35,36,37Cl and 37Ar from Heavy-Ion Fusion-Evaporation

NUCLEAR REACTIONS 25,24,26Mg, 27Al, 18O, 10Be(18O, X), 24,26Mg, 27Al, 28Si(19F, X), 26Mg, 27Al(14N, X), 27Al, 18O(16O, X), 26Mg, 18,16O, 10Be(13C, X), 25,26Mg, 19F, 18O(12C, X), 12C(11B, X), E=20-60 MeV; measured fusion evaporation, γγ-coin, polarization, recoil distance. 35,36,37Cl, 37Ar deduced levels, J, π, T1/2. Ge(Li) detectors, natural, enriched targets.

doi: 10.1103/PhysRevC.14.996
Citations: PlumX Metrics

1975PO13      Phys.Rev. C12, 1407 (1975)

A.R.Poletti, D.C.Radford, J.R.Southon

Lifetime of the 3463-keV Level in 40Ar

NUCLEAR REACTIONS 37Cl(α, pγ), E=10.6 MeV; measured pγ(t). 40Ar level deduced J, π, T1/2, B(E2).

doi: 10.1103/PhysRevC.12.1407
Citations: PlumX Metrics

1975RA29      Nucl.Phys. A254, 183 (1975)

D.C.Radford, A.R.Poletti

Lifetime of the 3.854 MeV State in 13C by the Recoil-Distance Method

NUCLEAR REACTIONS 12C(d, pγ), E=2.51 MeV; measured Eγ(theta(γ)=0), Doppler shift, recoil distance. 13C level deduced T1/2. Natural target.

doi: 10.1016/0375-9474(75)90590-4
Citations: PlumX Metrics

1974FI02      Nucl.Phys. A220, 183 (1974)

L.K.Fifield, A.R.Poletti

A Study of Excited States in 33Cl by Elastic Proton Scattering on 32S

NUCLEAR REACTIONS 32S(p, p), E=3.36-3.40 MeV, 3.8-5.0 MeV; measured σ(Ep, θ(p)). 33Cl deduced levels, J, π, level-width. Natural targets.

doi: 10.1016/0375-9474(74)90761-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0784.

1974KO04      Phys.Rev. C9, 953 (1974)

J.J.Kolata, P.Gorodetzky, J.W.Olness, A.R.Poletti, E.K.Warburton

High-Spin States in 39K from 24Mg(18O, p2nγγ...)39K

NUCLEAR REACTIONS 24Mg(18O, Xγ), E=20-61.5 MeV; measured σ(E, Eγ, θ), recoil distance. 39K deduced levels, J, π, T1/2, λ.

doi: 10.1103/PhysRevC.9.953
Citations: PlumX Metrics

1974PO10      Phys.Rev. C10, 997 (1974)

A.R.Poletti, B.A.Brown, D.B.Fossan, P.Gorodetzky, J.J.Kolata, J.W.Olness, E.K.Warburton

Lifetimes of the (f7/2)3 15/2- States in 51V and 43Ca and (f7/2)2 4+ States in 50Ti and 42Ca via Heavy-Ion Recoil-Distance-Method Measurements

NUCLEAR REACTIONS 48Ca(6Li, 3n), (6Li, 3np), E=26 MeV; 48Ca(7Li, 4n), E=28 MeV; 27Al(18O, np), (18O, 2np), E=30, 35 MeV; 27Al(19F, n2p), E=36 MeV; measured recoil distance. 42,43Ca, 50Ti, 51V levels deduced T1/2, B(E2).

doi: 10.1103/PhysRevC.10.997
Citations: PlumX Metrics

1974PO14      Phys.Rev. C10, 2312 (1974)

A.R.Poletti, B.A.Brown, D.B.Fossan, E.K.Warburton

Nuclear Spectroscopy with Lithium Beams. I. High-Spin States in 55Fe, 55Mn, and 53Cr

NUCLEAR REACTIONS 51V(7Li, 3nγ), (7Li, 2npγ), (7Li, nαγ), E=25 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, DSA, recoil distance. 55Fe, 55Mn, 53Cr levels deduced J, π, T1/2, B(E2).

doi: 10.1103/PhysRevC.10.2312
Citations: PlumX Metrics

1974PO15      Phys.Rev. C10, 2329 (1974)

A.R.Poletti, B.A.Brown, D.B.Fossan, E.K.Warburton

Nuclear Spectroscopy with Lithium Beams. II. High-Spin States in 52Cr, 54Mn, 54Fe, and 56Fe

NUCLEAR REACTIONS 51V(7Li, 2nαγ), (7Li, 3npγ), (7Li, 4nγ), (7Li, 2nγ), 51V(6Li, 2npγ), (6Li, 3nγ), E=25 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, DSA, recoil distance. 52Cr, 54Mn, 54,56Fe deduced levels, J, π, T1/2, B(E2).

doi: 10.1103/PhysRevC.10.2329
Citations: PlumX Metrics

1974PR04      Phys.Rev. C9, 1430 (1974); Erratum Phys.Rev. C10, 1249 (1974)

J.G.Pronko, T.T.Bardin, J.A.Becker, T.R.Fisher, R.E.McDonald, A.R.Poletti

Gamma-Ray Spectroscopy Studies of 52Ti

NUCLEAR REACTIONS 50Ti(t, pγ), E=2.9 MeV; measured Eγ, Iγ, DSA, γγ(θ). 52Ti levels deduced J, π, T1/2, γ-mixing.

doi: 10.1103/PhysRevC.9.1430
Citations: PlumX Metrics

1974PR11      Phys.Rev. C10, 1345 (1974)

J.G.Pronko, T.T.Bardin, J.A.Becker, R.E.McDonald, A.R.Poletti

γ-Ray Deexcitation of 50Ti States in the Region of 4-MeV Excitation

NUCLEAR REACTIONS 48Ti(t, pγ), E=2.9 MeV; measured pγ-coin, pγ(θ), Eγ, Iγ, DSA. 50Ti deduced levels, T1/2, γ-branching ratios, J, π, γ-mixing.

doi: 10.1103/PhysRevC.10.1345
Citations: PlumX Metrics

1974WA07      At.Data Nucl.Data Tables 14, 147 (1974)

E.K.Warburton, J.J.Kolata, J.W.Olness, A.R.Poletti, Ph.Gorodetzky

Gamma Rays from Fusion-Evaporation Reactions in 32 ≤ A < 46 Nuclei

NUCLEAR REACTIONS 24,26Mg, 27Al, 28Si(14N, X), (16O, X), (18O, X), (19F, X), E=20-60 MeV; compiled Eγ, Iγ, γ-emitting nuclei list.

doi: 10.1016/S0092-640X(74)80021-5
Citations: PlumX Metrics

1973FI03      Phys.Rev. C7, 1878 (1973)

T.R.Fisher, T.T.Bardin, J.A.Becker, L.F.Chase, Jr., D.Kohler, R.E.McDonald, A.R.Poletti, J.G.Pronko

Gamma-Ray Spectroscopy of Low-Lying Levels in 28Mg

NUCLEAR REACTIONS 26Mg(t, pγ), E=2.9 MeV; measured σ(Ep, Eγ), pγ(θ), DSA. 28Mg deduced transitions, levels, T1/2, γ-branching, γ-mixing, J.

doi: 10.1103/PhysRevC.7.1878
Citations: PlumX Metrics

1973FI09      Phys.Rev. C8, 1837 (1973)

T.R.Fisher, A.R.Poletti, B.A.Watson

Measurement of the 59Co Quadrupole Moment by Observation of the Deformation Effect in the 59Co + n Total Cross Section

NUCLEAR REACTIONS 59Co(n, X), E=1, 1.2, 1.4, 1.6, 2, 15.2 MeV; measured σ for non-aligned, aligned target, deformation effect. 59Co deduced quadrupole moment.

doi: 10.1103/PhysRevC.8.1837
Citations: PlumX Metrics

1973GO31      Phys.Rev.Lett. 31, 1067 (1973)

P.Gorodetzky, J.J.Kolata, J.W.Olness, A.R.Poletti, E.K.Warburton

Gamma-Ray Spectroscopy in A = 40 Nuclei via Heavy-Ion-Induced Reactions; High-Spin States in 41K and 41Ca

NUCLEAR REACTIONS 24,26Mg, 27Al(16O, Xγ), (18O, Xγ), (19F, X), E=20-60 MeV; measured γ(θ), γγ-coin, Eγ, recoil distance. 41K, 41Ca levels deduced J, π, γ-multipolarities, γ-branching, T1/2.

doi: 10.1103/PhysRevLett.31.1067
Citations: PlumX Metrics

1973PO02      Phys.Rev. C7, 1433 (1973)

A.R.Poletti, T.T.Bardin, J.G.Pronko, R.E.McDonald

Lifetimes in 33P by the Doppler-Shift-Attenuation Method

NUCLEAR REACTIONS 31P(t, pγ), E=2.9 MeV; measured σ(Ep), Eγ, Doppler-shift attenuation; 33P deduced levels, T1/2, J, π.

doi: 10.1103/PhysRevC.7.1433
Citations: PlumX Metrics

1973PO03      Phys.Rev. C7, 1479 (1973)

A.R.Poletti, T.T.Bardin, R.E.McDonald, J.G.Pronko

33P; Angular Correlation Studies of Excited States

NUCLEAR REACTIONS 31P(t, pγ), E=2.9 MeV; measured σ(Ep), pγ(θ), Eγ, Iγ. 33P deduced levels, γ-mixing, J, π.

doi: 10.1103/PhysRevC.7.1479
Citations: PlumX Metrics

1973PO11      Phys.Rev. C8, 1285 (1973)

A.R.Poletti, J.G.Pronko

Beta Decay of 17N

RADIOACTIVITY 17N; measured βγ-coin, nβ(t), Eβ, Eγ. Deduced β-branching, log ft. 17O deduced levels.

doi: 10.1103/PhysRevC.8.1285
Citations: PlumX Metrics

1972BR45      Phys.Rev. C6, 1298 (1972)

J.E.Brock, I.A.Luketina, A.R.Poletti

Lifetime Measurements in 35Cl and 37Cl

NUCLEAR REACTIONS 35,37Cl(p, p'), (p, α), 37Cl(p, n), E=6 MeV; measured DSA, Eγ. 35,37Cl deduced levels, T1/2, level-width.

doi: 10.1103/PhysRevC.6.1298
Citations: PlumX Metrics

1972LU02      Phys.Rev. C6, 196 (1972)

I.A.Luketina, J.E.Brock, A.R.Poletti

Lifetime Measurements in Ar37

NUCLEAR REACTIONS 37Cl(p, nγ), E=3.45-6.0 MeV; measured DSA, Eγ, Iγ. 35Cl(p, p'γ), E=3.45-6.0 MeV; measured Eγ. 37Ar deduced levels, J, π, γ-branching, T1/2. 35Cl deduced transition.

doi: 10.1103/PhysRevC.6.196
Citations: PlumX Metrics

1971MC11      Phys.Rev. C4, 377 (1971)

R.E.McDonald, J.A.Becker, A.D.W.Jones, A.R.Poletti

Radiative Decay of the 1.472-MeV State of O19

NUCLEAR REACTIONS 18O(d, pγ), E=2.68 MeV; measured σ(Ep, Eγ, θ(γ)), Doppler shift attenuation. 19O deduced levels, T1/2, γ-branching.

doi: 10.1103/PhysRevC.4.377
Citations: PlumX Metrics

1970JO06      Phys.Rev. C1, 1000 (1970)

A.D.W.Jones, J.A.Becker, R.E.McDonald, A.R.Poletti

Beta Decay of Na25 and Al29

RADIOACTIVITY 25Na, 29Al[from 23Na, 27Al(t, p)]; measured Eγ, Iγ; deduced log ft. 25Mg, 29Si deduced γ-branching.

doi: 10.1103/PhysRevC.1.1000
Citations: PlumX Metrics

1970PO08      Phys.Rev. C2, 964 (1970)

A.R.Poletti, J.A.Becker, R.E.McDonald

Angular-Correlation Study of Na23 Using the Mg24(t, αγ)Na23 Reaction

NUCLEAR REACTIONS 24Mg(t, αγ), E=2.80 MeV; measured σ(Eα, Eγ, θ(γ), θ(αγ)). 23Na levels deduced J, π, γ-branching, γ-mixing.

doi: 10.1103/PhysRevC.2.964
Citations: PlumX Metrics

1969MC12      Phys.Rev. 181, 1631 (1969)

R.E.McDonald, J.A.Becker, A.D.W.Jones, A.R.Poletti

Beta Decay of Ne24

RADIOACTIVITY 24Ne[from 22Ne(t, p)]; measured T1/2, Eγ, Iγ; deduced β-branching. 24Na levels deduced J, π. Ge(Li) detector.

doi: 10.1103/PhysRev.181.1631
Citations: PlumX Metrics

1969PO03      Phys.Rev. 182, 1054 (1969)

A.R.Poletti, J.A.Becker, R.E.McDonald

Some Properties of the States at 1.346, 1.459, and 1.554 MeV in F19

NUCLEAR REACTIONS 19F(p, p'γ) , E=2.8, 2.9, 5 MeV; measured σ(E;Eγ, θ(γ)), Doppler shift attenuation. 19F deduced levels, T1/2, γ-mixing, γ-branching. Ge(Li) detector.

doi: 10.1103/PhysRev.182.1054
Citations: PlumX Metrics

1969PO04      Phys.Rev. 181, 1606 (1969)

A.R.Poletti, A.D.W.Jones, J.A.Becker, R.E.McDonald

Lifetimes of Excited States in Ca40 by the Doppler-Shift Attenuation Method

NUCLEAR REACTIONS 40Ca(p, p'γ), E = 8.5-9.0 MeV; measured σ(E;Eγ, θ(γ)), Doppler shift attenuation. 40Ca deduced levels J, π, T1/2, level-width, γ-branching. Ge(Li) detector.

doi: 10.1103/PhysRev.181.1606
Citations: PlumX Metrics

1969PO06      Phys.Rev. 184, 1130 (1969)

A.R.Poletti, A.D.W.Jones, J.A.Becker, R.E.McDonald, R.W.Nightingale

Doppler-Shift Measurements of Lifetimes of Low-Lying Levels in Na23

NUCLEAR REACTIONS 23Na(p, p'γ), E = 3.75-5.25 MeV; measured σ(E;Eγ), Doppler shift attenuation. 23Na deduced levels, T1/2.

doi: 10.1103/PhysRev.184.1130
Citations: PlumX Metrics

1968FO02      Phys.Rev. 168, 1228 (1968)

D.B.Fossan, A.R.Poletti

Magnetic Moment and Core Excitation of the d3/2 Hole State in Sc47

NUCLEAR STRUCTURE 47Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.168.1228
Citations: PlumX Metrics

1968WA07      Phys.Rev. 168, 1232 (1968)

E.K.Warburton, A.R.Poletti, J.W.Olness

Nuclear Structure of Na22. IV. Gamma-Ray Correlation Measurements

NUCLEAR STRUCTURE 22Na, 19F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.168.1232
Citations: PlumX Metrics

1968WA15      Phys.Rev. 171, 1178 (1968)

E.K.Warburton, J.W.Olness, S.D.Bloom, A.R.Poletti

E2 and M1 Matrix Elements in B10

NUCLEAR STRUCTURE 11B, 10B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.171.1178
Citations: PlumX Metrics

1967FO01      Phys.Letters 24B, 38 (1967)

D.B.Fossan, A.R.Poletti

Analogous 3/2- Levels in 43Ca and 41Ar

NUCLEAR STRUCTURE 43Ca, 41Ar; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90332-2
Citations: PlumX Metrics

1967OL02      Phys.Rev. 154, 971 (1967)

J.W.Olness, A.R.Poletti, E.K.Warburton

Electromagnetic Decay of the N14 3.95- and 7.03-MeV Levels

NUCLEAR STRUCTURE 14N, 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.154.971
Citations: PlumX Metrics

1967OL05      Phys.Rev. 161, 1131 (1967)

J.W.Olness, A.R.Poletti, E.K.Warburton

Energies and Decay Modes of Ne19 States: Energies of First Excited States of Ne21, Na21, and Mg22

NUCLEAR STRUCTURE 19Ne, 20Ne, 22Mg, 21Na, 21Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.161.1131
Citations: PlumX Metrics

1967PO02      Phys.Rev. 153, 1108 (1967)

A.R.Poletti

Parity of the 2.10- and 1.08-MeV Levels in F18

NUCLEAR STRUCTURE 16O, 18F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.153.1108
Citations: PlumX Metrics

1967PO09      Phys.Rev. 160, 883 (1967)

A.R.Poletti, D.B.Fossan

Measurement of the Magnetic Moment and Lifetime of the 1.131-MeV Level in F18

NUCLEAR STRUCTURE 18F, 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.160.883
Citations: PlumX Metrics

1967PO10      Phys.Rev. 162, 1040(1967)

A.R.Poletti, E.K.Warburton, J.W.Olness, S.Hechtl

Nuclear Structure of Na22. II. Some Gamma-Ray Doppler-Shift and Correlation Measurements

NUCLEAR REACTIONS 19F(α, nγ), E=4-7 MeV; 20Ne(3He, pγ), E=6.56 MeV; measured Doppler shift attenuation, σ(Eγ, Ep, θ(pγ)), γγ-coin. 22Na deduced levels, J, π, T1/2, γ-branching, γ-mixing.

doi: 10.1103/PhysRev.162.1040
Citations: PlumX Metrics

1967PO14      Phys.Rev. 164, 1479 (1967)

A.R.Poletti, E.K.Warburton, J.W.Olness

Nuclear Structure of Na22. III. Spins and Parities from the Linear Polarization of Gamma Rays

NUCLEAR STRUCTURE 22Na, 19F, 22Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1479
Citations: PlumX Metrics

1967WA06      Phys.Rev. 155, 1164 (1967)

E.K.Warburton, J.W.Olness, A.R.Poletti

Gamma-Ray Transitions Between the Low-Lying Levels of F18

NUCLEAR STRUCTURE 16O, 18F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.155.1164
Citations: PlumX Metrics

Back to query form    [Next]