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2019AU01      Phys.Rev. C 99, 024320 (2019)

S.M.Austin, P.Paul, B.A.Brown, V.Zelevinsky

Reactions leading to the first excited states of 7Li and 7Be and isospin-mixed states in 8Be

NUCLEAR REACTIONS 6Li(d, p), (d, n), E=0.15-7.2 MeV; 7Li(p, p'), (p, n), E=3.0-10.0 MeV; measured Eγ and Iγ from the decays of 7Li (478-keV γ) and 7Be (429-keV γ) at the Stanford 3-MeV Van de Graaff and FN Tandem accelerator; deduced ratios of σ(d, p')/σ(d, n') and σ(p, p')/σ(p, n') as function of incident deuteron and proton energies, effects of isospin mixed states in the compound nucleus. 8Be; calculated levels, J, π using shell model with PJT interaction, and compared with experimental data.

doi: 10.1103/PhysRevC.99.024320
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2001DI01      Phys.Rev. C63, 014611 (2001)

I.Dioszegi, N.P.Shaw, A.Bracco, F.Camera, S.Tettoni, M.Mattiuzzi, P.Paul

Fission Hindrance in 200Pb Measured from Giant Dipole Resonance γ-Ray Emission

NUCLEAR REACTIONS 181Ta(19F, X), E=161, 181 MeV; measured Eγ, Iγ, (fragment)γ-coin following compound nucleus fission. 200Pb deduced GDR decay features, fission hindrance, nuclear viscosity parameter. Statistical model analysis.

doi: 10.1103/PhysRevC.63.014611
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2001DI08      Phys.Rev. C63, 047601 (2001)

I.Dioszegi, I.Mazumdar, N.P.Shaw, P.Paul

Level Densities in Hot 112Sn, 131La, and 134Ce Nuclei from Giant Dipole Resonance γ Decay

NUCLEAR REACTIONS 93Nb, 115In(19F, X), E=75 MeV; 115In(16O, X), E=80 MeV; measured Eγ, Iγ, γ-ray multiplicity. 112Sn, 131La, 134Ce deduced level densities. Comparisons with model predictions. BaF2 detectors.

doi: 10.1103/PhysRevC.63.047601
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2001DI18      Acta Phys.Hung.N.S. 13, 185 (2001)

I.Dioszegi, I.Mazumdar, P.Paul

Nuclear Viscosity of Hot Rotating 240Cf

NUCLEAR REACTIONS 208Pb(32S, X), E=180-285 MeV; measured Eγ, γ-ray and fission fragment multiplicities. 240Cf deduced GDR decay features, saddle-to-scission decay path. Modified statistical model.

doi: 10.1556/APH.13.2001.1-3.24
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2001PA16      Nucl.Phys. A685, 449c (2001)


Commissioning of RHIC and Its Four Detectors

doi: 10.1016/S0375-9474(01)00560-7
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2000DI02      Phys.Rev. C61, 024613 (2000)

I.Dioszegi, N.P.Shaw, I.Mazumdar, A.Hatzikoutelis, P.Paul

Nuclear Viscosity of Hot Rotating 224Th

NUCLEAR REACTIONS 208Pb(16O, F), E=100-177 MeV; measured Eγ, Iγ, (fragment)γ-coin, γ-ray multiplicity; deduced total, fission, evaporation residue σ. 224Th deduced hot GDR features, dissipation coefficient. Statistical model analysis.

doi: 10.1103/PhysRevC.61.024613
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2000SH11      Phys.Rev. C61, 044612 (2000)

N.P.Shaw, I.Dioszegi, I.Mazumdar, A.Buda, C.R.Morton, J.Velkovska, J.R.Beene, D.W.Stracener, R.L.Varner, M.Thoennessen, P.Paul

Nuclear Viscosity of Hot Rotating 240Cf

NUCLEAR REACTIONS 208Pb(32S, X), E=180-285 MeV; measured total fusion σ, Eγ, Iγ, fragment mass distributions following compound nucleus fission. 240Cf deduced dissipation coefficient, temperature and deformation effects. Statistical model calculations.

doi: 10.1103/PhysRevC.61.044612
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1998PA04      Nucl.Phys. A630, 92c (1998)


The GDR and Dissipation in Hot Nuclei

doi: 10.1016/S0375-9474(97)00746-X
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1997BU02      Phys.Rev. C55, 504 (1997)

A.Buda, J.C.Bacelar, S.R.Banerjee, H.Ching, D.J.Hofman, P.Paul, S.Schadmand, A.van der Woude

Dilepton and Photon Decay of Giant Resonances Built on Excited States of 56Ni

NUCLEAR REACTIONS 40Ca(16O, γ), (16O, X), E=82 MeV; measured γ-, pair-production σ. 56Ni deduced isospin mixing, giant resonance photon, dilepton decay parameters.

doi: 10.1103/PhysRevC.55.504
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1997MO30      J.Phys.(London) G23, 1383 (1997)

C.R.Morton, A.Buda, P.Paul, N.P.Shaw, J.R.Beene, N.Gan, M.L.Halbert, D.W.Stracener, R.L.Varner, M.Thoennessen, P.Thirolf, I.Dioszegi

Fission Dynamics using the Decay of the Giant Dipole Resonance

NUCLEAR REACTIONS W, 208Pb(32S, F), E=180-245 MeV; measured Eγ, Iγ, fission(fragment)γ(θ); deduced GDR channel effects. Modified CASCADE calculations.

doi: 10.1088/0954-3899/23/10/028
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1996HO10      Nucl.Phys. A599, 23c (1996)

D.J.Hofman, B.B.Back, P.Paul

Rapid Increase in Prescission GDR γ-Ray Emission with Energy

NUCLEAR REACTIONS 208Pb(16O, X), (16O, F), E ≈ 80-140 MeV; W, 208Pb(32S, X), (32S, F), E ≈ 160-260 MeV; analyzed fission, other reaction data; deduced rapid increase in γ-ray emission from prescission GDR-decay.

doi: 10.1016/0375-9474(96)00044-9
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1996SC07      Nucl.Phys. A599, 89c (1996)

S.Schadmand, R.Varma, S.R.Banerjee, B.B.Back, D.J.Hofman, C.P.Montoya, P.Paul

Internal Pair Decay Of Giant Resonances in Hot 200Pb

NUCLEAR REACTIONS 181Ta(19F, X), E=95 MeV; measured pair production spectra following compound system decay. 200Pb deduced GDR dominance in pair decay.

doi: 10.1016/0375-9474(96)00050-4
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1995BU29      Phys.Rev.Lett. 75, 798 (1995)

A.Buda, J.C.Bacelar, A.Balanda, Z.Sujkowski, A.van der Woude, R.Bersch, H.Ching, I.Dioszegi, D.J.Hofman, P.Paul, S.Schadmand, R.Varma

Dilepton Decay of Giant Resonances Built on Excited States of 28Si

NUCLEAR REACTIONS 12C(16O, X), E=82 MeV; measured dilepton, photon yields; deduced dilepton production σ. 28Si deduced giant resonance strength function parameters.

doi: 10.1103/PhysRevLett.75.798
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1995HO08      Phys.Rev. C51, 2597 (1995)

D.J.Hofman, B.B.Back, P.Paul

Rapid Increase in Prescission Giant-Dipole-Resonance γ-Ray Emission with Bombarding Energy

NUCLEAR REACTIONS 208Pb(16O, X), E=100-140 MeV; W(32S, X), E=185-230 MeV; 208Pb(32S, X), E=200, 230 MeV; measured Eγ, Iγ, γ-multiplicity; deduced capture, compound nucleus formation σ, linear dissipation strength. 240Cf, 224Th deduced prescission GDR γ-decay features. Statistical model, energy dissipation, viscosity, temperature dependence.

doi: 10.1103/PhysRevC.51.2597
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1995MA54      Acta Phys.Pol. B26, 417 (1995)

A.Maj, T.S.Tveter, J.J.Gaardhoje, B.Herskind, G.Sletten, T.Ramsoy, A.Atac, W.Korten, A.Bracco, F.Camera, M.Mattiuzzi, B.Million, M.Pignanelli, J.Bacelar, A.Buda, H.van der Ploeg, W.Krolas, H.Nifenecker, F.Schussler, J.A.Pinston, A.Menthe, P.Paul, D.J.Hofman, I.Dioszegi, S.Schadmand

Hot Superheavy Nuclei Seen with the GDR γ-Decay

NUCLEAR REACTIONS 232Th(40Ar, F), E=6.8-15 MeV/nucleon; 232Th(37Cl, F), E=7.3 MeV/nucleon; measured fission (fragment)γ-coin. 272Hs, 269Bh deduced GDR γ-decay features. Other reaction data, aspects reviewed.

1995NE03      Phys.Rev. C51, 2218 (1995)

J.Nestler, B.B.Back, K.S.Drese, D.J.Hofman, S.Schadmand, R.Varma, P.Paul

Time Scale of Quasifission from Giant Dipole Resonance γ-Ray Yield

NUCLEAR REACTIONS 165Ho(58Ni, X), E=368 MeV; measured γ(fragment)-coin; deduced weak GDR γ-decay evidence, quasifission time scale.

doi: 10.1103/PhysRevC.51.2218
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1995SC26      J.Phys.(London) G21, 821 (1995)

S.Schadmand, R.Varma, S.R.Banerjee, B.B.Back, D.J.Hofman, C.P.Montoya, P.Paul

Internal Pair Decay of Giant Resonances in Hot 200Pb

NUCLEAR REACTIONS 181Ta(19F, X), E=95 MeV; measured cascade pair spectra, pair-, γ-spectra ratio. 200Pb deduced giant resonances internal pair decay features. Statistical model, hot nuclei.

doi: 10.1088/0954-3899/21/6/010
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1995ZA10      Phys.Lett. 357B, 515 (1995)

N.V.Zamfir, G.Hering, R.F.Casten, P.Paul

Hexadecapole Deformations in Actinide and Trans-Actinide Nuclei

NUCLEAR STRUCTURE Z=28-98; analyzed B(E2) data. Z=92-114; calculated B(λ). 250,252Cf deduced β4.

doi: 10.1016/0370-2693(95)00978-T
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1994HO03      Phys.Rev.Lett. 72, 470 (1994)

D.J.Hofman, B.B.Back, I.Dioszegi, C.P.Montoya, S.Schadmand, R.Varma, P.Paul

Viscosity of Saddle-to-Scission Motion in Hot 240Cf from Giant Dipole Resonance γ Yield

NUCLEAR REACTIONS 208Pb(32S, F), E=230 MeV; measured fission (fragment)γ-coin, Eγ, Iγ, γ-anisotropy. 240Cf deduced saddle to scission motion viscosity, time.

doi: 10.1103/PhysRevLett.72.470
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1994PA06      Nucl.Phys. A569, 73c (1994)


The GDR as Clock for Fission Dynamics in Hot Actinide Nuclei

NUCLEAR REACTIONS 208Pb(16O, F), E=140 MeV; 208Pb(32S, F), E=200, 230 MeV; 232Th(28Si, F), E=223 MeV; analyzed γ-spectra, fission (fragment)γ(θ). 224Th, 240Cf, 260Rf deduced fisson associated friction coefficients. GDR as fission dynamics clock, hot actinide nuclei.

RADIOACTIVITY 252Cf(SF); analyzed neutron spectra, multiplicity vs fragment mass data following SF-decay. GDR as fission dynamics clock, hot actinide nuclei.

doi: 10.1016/0375-9474(94)90097-3
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1993HO05      Phys.Rev. C47, 1103 (1993)

D.J.Hofman, B.B.Back, C.P.Montoya, S.Schadmand, R.Varma, P.Paul

High Energy γ Rays from 252Cf Spontaneous Fission

RADIOACTIVITY 252Cf(SF); analyzed γ-, neutron decay data following SF-decay. Statistical model.

doi: 10.1103/PhysRevC.47.1103
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1993MO28      Nucl.Instrum.Methods Phys.Res. A334, 437 (1993)

C.P.Montoya, S.Schadmand, R.Varma, P.H.Zhang, R.Butsch, I.Dioszegi, D.J.Hofman, P.Paul

An Electron-Positron Pair Spectrometer for High Energy Decays of Nuclei

RADIOACTIVITY 8Li(β-) [from 7Li(d, p)]; measured β-decay end point energy; deduced detector calibration. Segmented phoswich plastic scintillator array (e+, e-) pair spectrometer.

NUCLEAR REACTIONS 19F(p, α), E=5.2 MeV; measured Eγ, Iγ, for GDR region in 20Ne; deduced spectrometer efficiency. Segmented phoswich plastic scintillator array (e+, e-) pair spectrometer.

doi: 10.1016/0168-9002(93)90805-R
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1993RI03      Phys.Rev.Lett. 70, 533 (1993); Erratum Phys.Rev.Lett. 70, 2659 (1993)

J.Ritman, F.-D.Berg, W.Kuhn, V.Metag, R.Novotny, M.Notheisen, P.Paul, M.Pfeiffer, O.Schwalb, H.Lohner, L.Venema, A.Gobbi, N.Herrmann, K.D.Hildenbrand, J.Mosner, R.S.Simon, K.Teh, J.P.Wessels, T.Wienold

First Observation of the Coulomb-Excited Double Giant Dipole Resonance in 208Pb via Double-γ Decay

NUCLEAR REACTIONS 208Pb(209Bi, 209Bi'), E=1 GeV/nucleon; measured γγ-coin sum spectra following Coulomb excitation. 208Pb deduced single, double GDR, energy, width, decay features. Relativistic Coulomb excitation.

doi: 10.1103/PhysRevLett.70.533
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1992DI03      Phys.Rev. C46, 627 (1992)

I.Dioszegi, D.J.Hofman, C.P.Montoya, S.Schadmand, P.Paul

Giant Dipole Resonance Decay from Fusion-Fission and Quasifission of Hot Thorium Nuclei

NUCLEAR REACTIONS 208Pb(16O, F), E=140 MeV; W(32S, F), E=185-230 MeV; measured fission (fragment)γ(θ), Eγ, Iγ, fragment mass, total kinetic energy distributions. 224Th deduced shape features, quasifission T1/2, GDR decay.

doi: 10.1103/PhysRevC.46.627
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1991BU08      Phys.Rev. C44, 1515 (1991)

R.Butsch, D.J.Hofman, C.P.Montoya, P.Paul, M.Thoennessen

Time Scales for Fusion-Fission and Quasifission from Giant Dipole Resonance Decay

NUCLEAR REACTIONS 208Pb(16O, F), E=120, 140 MeV; 196Pt(24Mg, F), E=150 MeV; W(28Si, F), E=185 MeV; measured fission (fragment)γ-coin, γ(θ), anisotropy; deduced fission σ, fission time, friction coefficient. 224,226Th deduced fissility parameters.

doi: 10.1103/PhysRevC.44.1515
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1991MO21      Z.Phys. A340, 371 (1991)

C.P.Montoya, S.Schadmand, I.Dioszegi, D.J.Hofman, P.H.Zhang, P.Paul

Giant Monopole Resonances in the Statistical Model

NUCLEAR STRUCTURE 110Sn; calculated (e+e-)-pair decay of isoscalar, isovector giant monopole resonance decay; deduced GDR role.

doi: 10.1007/BF01290324
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1990BU05      Phys.Rev. C41, 1530 (1990)

R.Butsch, M.Thoennessen, D.R.Chakrabarty, M.G.Herman, P.Paul

Nuclear Deformation in Excited Pb Isotopes from Giant Dipole γ-Ray-Fission Angular Correlations

NUCLEAR REACTIONS 181Ta(19F, X), (19F, F), E=105, 141 MeV; measured Eγ, Iγ, fission (fragment)γ-coin. 200Pb deduced GDR energy, width, deformation parameter. Statistical model analysis.

doi: 10.1103/PhysRevC.41.1530
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1989VO10      Phys.Rev. C40, R2441 (1989)

R.J.Vojtech, R.Butsch, V.M.Datar, M.G.Herman, R.L.McGrath, P.Paul, M.Thoennessen

High Energy Photon Production in Low Energy 12C + 112,124Sn Collisions

NUCLEAR REACTIONS 112,124Sn(12C, X), E=7.5, 10.5 MeV/nucleon; measured γ yield, σ(θγ, Eγ); deduced source velocity, γ yield isotopic dependence. Statistical model calculations.

doi: 10.1103/PhysRevC.40.R2441
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1988BL01      Z.Phys. A329, 103 (1988)

K.Blatt, K.Becker, B.Heck, H.Jansch, H.Leucker, D.Fick, R.Caplar, R.Butsch, K.-H.Mobius, W.Ott, P.Paul, E.Steffens, J.Pochodzalla, G.Tungate

23Na + 23Na Fusion with Unpolarized and Aligned Beams

NUCLEAR REACTIONS, ICPND 23Na(23Na, X), E=80-177 MeV; measured fusion σ(E), σ(θ), σ(A), tensor analyzing power. Tof, unpolarized, aligned beams. Model calculations.

1988CH11      Phys.Rev. C37, 1437 (1988)

D.R.Chakrabarty, M.Thoennessen, S.Sen, P.Paul, R.Butsch, M.G.Herman

Giant Dipole Resonances in Excited Er Isotopes

NUCLEAR REACTIONS 141Pr(19F, X), E=94.1, 96.5, 111.1, 129 MeV; measured γ spectra. 160Er deduced GDR energies, widths, deformation parameters, shape evolution. Statistical model analysis.

doi: 10.1103/PhysRevC.37.1437
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1988OT08      Nucl.Phys. A489, 329 (1988)

W.Ott, R.Butsch, H.J.Jansch, K.-H.Mobius, P.Paul, G.Tungate, E.Steffens, K.Rusek, Z.Moroz, I.M.Turkiewicz, K.Becker, K.Blatt, H.Leucker, D.Fick

Elastic and Inelastic Scattering of Polarized 7Li Ions from a 26Mg Target

NUCLEAR REACTIONS 26Mg(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; measured σ(θ), analyzing powers (τ)T10(θ), (τ)T20(θ), T20(θ), T21(θ), (τ)T30(θ).

doi: 10.1016/0375-9474(88)90156-X
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1988TH01      Phys.Rev. C37, 1762 (1988)

M.Thoennessen, D.R.Chakrabarty, R.Butsch, M.G.Herman, P.Paul, S.Sen

Onset of Deformation in Pb Isotopes at High Excitation Energies

NUCLEAR REACTIONS 181Ta(19F, X), E=93, 105 MeV; measured Eγ, Iγ. 200Pb deduced GDR, width, deformation parameter, shape transition. Statistical model.

doi: 10.1103/PhysRevC.37.1762
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1987BU16      Phys.Rev. C36, 1351 (1987)

R.Butsch, H.Jansch, D.Kramer, K.-H.Mobius, W.Ott, E.Steffens, G.Tungate, A.Weller, K.Becker, K.Blatt, H.Leucker, W.Luck, D.Fick, P.Paul

Fusion Evaporation and Fusion-Fission with Aligned 23Na Ions at Energies near and below the Fusion Barrier

NUCLEAR REACTIONS, ICPND 48Ti(polarized 23Na, X), E=48-72.5 MeV; measured σ(fragment θ); 206Pb(polarized 23Na, F), E=108-120 MeV; measured fission fragment σ(θ); deduced fusion σ(E), T20(E), barrier parameters. Coupled-channels calculations.

doi: 10.1103/PhysRevC.36.1351
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1987CH03      Phys.Rev.Lett. 58, 1092 (1987)

D.R.Chakrabarty, M.Thoennessen, N.Alamanos, P.Paul, S.Sen

Evidence for Prolate Deformation in Highly Excited Neutron-Deficient Pb Isotopes

NUCLEAR REACTIONS W(16O, X), E=100, 140 MeV; 181Ta(19F, X), E=105, 126 MeV; measured γ-spectra. 198,199,200,201,202Pb deduced GDR energies, width, dipole strength distributions, deformation parameter. γ-ray multiplicity filter. Theoretical analyses.

doi: 10.1103/PhysRevLett.58.1092
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1987CH31      Phys.Rev. C36, 1886 (1987)

D.R.Chakrabarty, S.Sen, M.Thoennessen, N.Alamanos, P.Paul, R.Schicker, J.Stachel, J.J.Gaardhoje

Giant Resonances in Excited Sn Isotopes

NUCLEAR REACTIONS 93Nb(19F, X), E=80, 100, 160 MeV; 94Mo(16O, X), E=140 MeV; measured Eγ, Iγ, γ-multiplicity. 110,112Sn deduced GDR energies, width, strength distribution. Statistical model analyses, isovector GQR.

doi: 10.1103/PhysRevC.36.1886
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1987TH07      Phys.Rev.Lett. 59, 2860 (1987)

M.Thoennessen, D.R.Chakrabarty, M.G.Herman, R.Butsch, P.Paul

Giant Dipole Resonance in Highly Excited Thorium: Evidence for strong fission hindrance

NUCLEAR REACTIONS 208Pb(16O, X), E=100, 120, 140 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ), yield ratios. 224Th deduced giant dipole resonance, level density parameters, fission hindrance factors.

doi: 10.1103/PhysRevLett.59.2860
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1986AL09      Phys.Lett. 173B, 392 (1986)

N.Alamanos, P.Braun-Munzinger, R.F.Freifelder, P.Paul, J.Stachel, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young

Observation of High Energy Electromagnetic Dipole Radiation in 14N + Ni Reactions at E(lab)/A = 35 MeV

NUCLEAR REACTIONS Ni(14N, X), E=35 MeV/nucleon; measured σ(θ, Eγ), γ(θ); deduced high energy dipole radiation.

doi: 10.1016/0370-2693(86)90401-6
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1986BL08      Phys.Rev.Lett. 57, 819 (1986)

K.Blatt, K.Becker, B.Heck, H.Jansch, H.Leucker, D.Fick, R.Caplar, R.Butsch, D.Kramer, K.-H.Mobius, Z.Moroz, W.Ott, P.Paul, E.Steffens, G.Tungate, I.M.Turkiewicz, A.Weller

Limitation of Heavy-Ion Fusion: Fusion of aligned 23Na with 23Na

NUCLEAR REACTIONS 23Na(23Na, X), (polarized 23Na, X), E(cm)=40-88.5 MeV; measured fusion σ(E), tensor analyzing power vs E; deduced reaction mechanism.

doi: 10.1103/PhysRevLett.57.819
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1986BU15      Phys.Rev.Lett. 57, 2002 (1986)

R.Butsch, H.Jansch, D.Kramer, K.-H.Mobius, Z.Moroz, W.Ott, K.Rusek, E.Steffens, R.Suntz, G.Tungate, I.Turkiewicz, A.Weller, K.Becker, K.Blatt, D.Fick, H.Leucker, W.Luck, P.Paul

Subbarrier Fusion with Aligned 23Na Ions

NUCLEAR REACTIONS, ICPND 48Ti(polarized 23Na, X), E=48-72.5 MeV; 208Pb(polarized 23Na, X), E=108-120 MeV; measured fragment energy vs mass spectrum, fusion σ(E); deduced second rank tensor analyzing power vs E. (δE-E) Si telescopes, TOF. Coupled-channels calculations.

doi: 10.1103/PhysRevLett.57.2002
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1986ST03      Phys.Rev. C33, 1420 (1986)

J.Stachel, P.Braun-Munzinger, R.H.Freifelder, P.Paul, S.Sen, P.DeYoung, P.H.Zhang, T.C.Awes, F.E.Obenshain, F.Plasil, G.R.Young, R.Fox, R.Ronningen

Pion Production: A probe for coherence in medium-energy heavy-ion collisions

NUCLEAR REACTIONS Ni, 27Al(14N, π0X), E=35 MeV/nucleon; 27Al, Ni(16O, π0X), E=25 MeV/nucleon; measured inclusive pion production σ(θ(π), E(π)), invariant pion mass; deduced pion production, reabsorption mechanisms.

doi: 10.1103/PhysRevC.33.1420
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1986TU01      J.Phys.(London) G12, 1001 (1986)

G.Tungate, D.Kramer, R.Butsch, O.Karban, K.H.Mobius, W.Ott, P.Paul, A.Weller, E.Steffens, K.Becker, K.Blatt, D.Fick, B.Heck, H.Jansch, H.Leucker, K.Rusek, I.M.Turkiewicz, Z.Moroz

Elastic and Inelastic Scattering of Polarized 7Li from 120Sn

NUCLEAR REACTIONS 120Sn(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; measured σ(θ), analyzing power vs θ. Polarimeter, ΔE, E counters. Coupled channels calculations.

doi: 10.1088/0305-4616/12/10/011
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1986YO02      Phys.Rev. C33, 742 (1986)

G.R.Young, F.E.Obenshain, F.Plasil, P.Braun-Munzinger, R.Freifelder, P.Paul, J.Stachel

Production of Neutral Pions in Heavy-Ion Collisions at E(lab)/A = 25 MeV

NUCLEAR REACTIONS 27Al, Ni(16O, π0X), E=402 MeV; measured inclusive σ(θ(π), E(π)); deduced collective pion production mechanism.

doi: 10.1103/PhysRevC.33.742
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1984BR01      Phys.Rev.Lett. 52, 255 (1984)

P.Braun-Munzinger, P.Paul, L.Ricken, J.Stachel, P.H.Zhang, G.R.Young, F.E.Obenshain, E.Grosse

Pion Production in Heavy-Ion Collisions at E(Lab)/A = 35 MeV

NUCLEAR REACTIONS 27Al, Ni, W(14N, π0X), E=35 MeV/nucleon; measured γγ-coin following pion decay, pion production σ vs mass; deduced many nucleon role in reaction mechanism.

doi: 10.1103/PhysRevLett.52.255
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1983FR01      Nucl.Instrum.Methods 204, 445 (1983)

W.S.Freeman, W.F.Piel, Jr., H.W.Wilschut, T.Chapuran, P.Paul

Electron-Pair Detector for In-Beam Nuclear Studies

NUCLEAR REACTIONS 19F(p, α), E=3.96 MeV; measured σ(θ), (e+)(e-)-coin. 12C(16O, 16O'), E=78 MeV; measured (e+)(e-)-coin. Double, triple coincidence technique, E-ΔE scintillator pair detectors.

doi: 10.1016/0167-5087(83)90072-8
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1980FR10      Phys.Rev.Lett. 45, 1479 (1980)

W.S.Freeman, H.W.Wilschut, T.Chapuran, W.F.Piel, Jr., P.Paul

Heavy-Ion Resonances in Angular-Momentum-Unfavored Channels

NUCLEAR REACTIONS 16O(16O, 16O'), E=50-80 MeV; 12C(16O, 16O'), E=39-65 MeV; measured σ(E, Eγ), σ(E, pairproduction); deduced wave reflection in ion-ion potential. 32S, 28Si deduced resonances, exit channel reduced width ratio.

doi: 10.1103/PhysRevLett.45.1479
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1979FA12      Nucl.Phys. A330, 333 (1979)

A.Faessler, D.J.Millener, P.Paul, D.Strottman

Alpha and Proton Decay of the Isoscalar E2 Resonance in 16O and 40Ca

NUCLEAR STRUCTURE 16O, 40Ca; calculated Γα/Γp for T=0, GQR. SU(3) framework, 1p-1h excitations.

doi: 10.1016/0375-9474(79)90058-7
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1979JA25      Phys.Lett. 87B, 354 (1979)

C.M.Jachcinski, P.Braun-Munzinger, G.M.Berkowitz, R.H.Freifelder, M.Gai, R.L.McGrath, P.Paul, T.Renner, C.D.Uhlhorn

Angular Correlation Studies of Intermediate Width Structures in 16O + 12C

NUCLEAR REACTIONS 12C(16O, 12C), E(cm)=19-23 MeV; measured σ(θ), 12C'γ-coin, 12C-, 16O(θ). 28Si resonances deduced J, π, intermediate structure.

doi: 10.1016/0370-2693(79)90553-7
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1978GO10      Z.Phys. A287, 171 (1978)

U.Goerlach, D.Habs, M.Just, V.Metag, P.Paul, H.J.Specht, H.J.Maier

Resonances in the Isomeric and Prompt Fission Probabilities of 240Pu

NUCLEAR REACTIONS 239Pu(d, p), E=11 MeV; measured proton-fragment time distributions, prompt, delayed fission σ; deduced fission probability.

doi: 10.1007/BF01408087
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1978GO13      Phys.Rev. C18, 1706 (1978)

P.D.Goldstone, F.Hopkins, R.E.Malmin, P.Paul

Subbarrier Resonances in Fission of 234U, 236U, and 240Pu

NUCLEAR REACTIONS 233,235U, 239Pu(d, p), E=11-17 MeV; measured σ(E), pF-coin; deduced vibrational spectrum.

doi: 10.1103/PhysRevC.18.1706
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1978KN02      Phys.Lett. 74B, 191 (1978)

K.T.Knopfle, G.J.Wagner, P.Paul, H.Breuer, C.Mayer-Boricke, M.Rogge, P.Turek

Dominance of α Decay from the Isoscalar Giant Quadrupole Resonance in 16O

NUCLEAR REACTIONS 16O(α, X), E=155 MeV; measured scattered α charged particle angular correlation. 16O isoscalar GQR deduced particle decay.

doi: 10.1016/0370-2693(78)90550-6
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1978MA22      Phys.Rev. C17, 2097 (1978)

R.E.Malmin, F.Kahn, P.Paul

Observation of Intermediate Structure Resonances in the 12C(16O, 16O(0+, 6.05)) Reaction

NUCLEAR REACTIONS 12C(16O, 16O'), E=46-56 MeV; measured pair γ-coin, σ(E). 16O deduced resonances, reduced Γ.

doi: 10.1103/PhysRevC.17.2097
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1978MA32      Phys.Rev. C18, 163 (1978)

R.E.Malmin, J.W.Harris, P.Paul

Intermediate Structure Resonances in the Inelastic Scattering of 12C on 16O

NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E=33-54 MeV; measured σ(E, θ). 28Si deduced resonances, J, π, reduced widths.

doi: 10.1103/PhysRevC.18.163
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1977PA26      Phys.Lett. 71B, 71 (1977)

P.Paul, M.Suffert, P.Gorodetzky

Remeasurement of the ΔT = 1 γ-Decay from the 16.6-16.9 MeV States in 8Be

NUCLEAR REACTIONS 4He(α, γ), E=33.4-35 MeV; measured Eγ, Iγ(E). 8Be level deduced Γγ.

doi: 10.1016/0370-2693(77)90742-0
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1977SN01      Nucl.Phys. A285, 189 (1977)

K.A.Snover, P.Paul, H.M.Kuan

Radiative Proton Capture to the Ground State and First Three Excited States of 12C

NUCLEAR REACTIONS 11B(p, γ), E=6-23 MeV; measured σ(90°) for transitions to the 01+, 2+, 02+, , 3- levels in 12C. 11B(p, γ), E=12.4, 14.4 MeV; measured σ(θ). Enriched target.

doi: 10.1016/0375-9474(77)90245-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0351.

1976FI05      Phys.Rev. C14, 28 (1976)

G.A.Fisher, P.Paul, F.Riess, S.S.Hanna

Giant E1 Resonances in 8Be from the Reaction 7Li(p, γ)8Be

NUCLEAR REACTIONS 7Li(p, γ), E=0.8-17.6 MeV; measured σ(E, Eγ, θ). 8Be deduced giant resonances, Γγ.

doi: 10.1103/PhysRevC.14.28
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0022.

1976GO13      Phys.Lett. 62B, 280 (1976)

P.D.Goldstone, F.Hopkins, R.E.Malmin, P.Von Brentano, P.Paul

Vibrational Resonances below 5 MeV in the Fission of 240Pu

NUCLEAR REACTIONS 239Pu(d, pF), E=13 MeV; measured σ, fission probability. 240Pu deduced resonance, K, π.

doi: 10.1016/0370-2693(76)90074-5
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1976NO07      Phys.Lett. 65B, 125 (1976)

J.W.Noe, D.F.Geesaman, P.Paul, M.Suffert

Radiative Width of the First T = 2 State in 8Be

NUCLEAR REACTIONS 6Li(d, γ), E=6.85-7.10 MeV; measured yields. 8Be deduced resonance, Γ, T.

doi: 10.1016/0370-2693(76)90010-1
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1975GO23      Phys.Rev.Lett. 35, 1141 (1975)

P.D.Goldstone, F.Hopkins, R.E.Malmin, P.Paul

Sequence of Subbarrier Fission Resonances in 236U

NUCLEAR REACTIONS 235U(d, pF), E=13, 15, 17 MeV; measured σ, pf-coin. 236U deduced resonances, K, π.

doi: 10.1103/PhysRevLett.35.1141
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2450.

1975HA06      Phys.Rev. C11, 998 (1975)

M.N.Harakeh, P.Paul, K.A.Snover

E1 Transitions in 17F. I. The Low-Lying T = 3/2 States

NUCLEAR REACTIONS 16O(p, γ), E=14.8 MeV; measured σ(Eγ, θ). 17F deduced resonances, level-width, B(E1).

doi: 10.1103/PhysRevC.11.998
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1975HA07      Phys.Rev. C11, 1008 (1975)

M.N.Harakeh, P.Paul, P.Gorodetzky

E1 Transitions in 17F. II. The Region of the Giant Resonances

NUCLEAR REACTIONS 16O(p, γ), E=15.75-31.66 MeV; measured σ(E, Eγ, θ). 17F deduced resonances, T.

doi: 10.1103/PhysRevC.11.1008
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1975HA39      Phys.Rev. C12, 1410 (1975)

M.H.Harakeh, P.Paul, H.M.Kuan, E.K.Warburton

E1 Excitaions in A = 15 Nuclei

NUCLEAR REACTIONS 14C(p, γ), E=2.8-30 MeV; measured σ(E, Eγ, θ). 14N(p, γ), E=24-33.5 MeV; measured σ(E, Eγ). 15N deduced resonances, T1/2, B(E1).

doi: 10.1103/PhysRevC.12.1410
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1975NA12      Phys.Rev.Lett. 35, 1137 (1975)

A.M.Nathan, G.T.Garvey, P.Paul, E.K.Warburton

M1 Decay Rates and Second-Class Currents in Mass 8

NUCLEAR REACTIONS 4He(α, γ), E=33-36 MeV; measured σ(E, Eγ). 8Be levels deduced M1 Γ.

doi: 10.1103/PhysRevLett.35.1137
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1975PA18      Nucl.Phys. A254, 1 (1975)

P.Paul, H.S.Kuan, E.K.Warburton

Study of T = 0 and T = 2 Giant Dipole Resonances in 14N

NUCLEAR REACTIONS 13C(p, γ), E=23-33 MeV; measured σ(E, Eγ). 14N deduced resonance. Enriched target.

doi: 10.1016/0375-9474(75)90577-1
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1974GO23      Phys.Rev. C10, 1525 (1974)

D.R.Goosman, D.F.Geesaman, F.E.Cecil, R.L.McGrath, P.Paul

Lowest T = 2, Jπ = 0+ State in 12C

NUCLEAR REACTIONS 10Be(3He, n), E=13 MeV; measured σ(En, θ). 12C deduced level.

doi: 10.1103/PhysRevC.10.1525
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1974SN01      Phys.Rev.Lett. 32, 317 (1974)

K.A.Snover, K.Ebisawa, D.R.Brown, P.Paul

Evidence for a Collective E2 Resonance in the Reaction 208Pb(p, γ)209Bi

NUCLEAR REACTIONS 208Pb(p, γ), E=17.5-25 MeV; measured γ(θ). 209Bi deduced resonance.

doi: 10.1103/PhysRevLett.32.317
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1973DI02      Phys.Rev. C7, 695 (1973)

E.M.Diener, J.F.Amann, P.Paul

Proton Capture into the Giant Dipole Resonance of 40Ca

NUCLEAR REACTIONS 39K(p, γ), E=6.5-17 MeV; measured σ(E;Eγ, θ); deduced autocorrelation functions. 40Ca deduced giant dipole resonance, level-width.

doi: 10.1103/PhysRevC.7.695
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1563.

1973DI03      Phys.Rev. C7, 705 (1973)

E.M.Diener, J.F.Amann, P.Paul, J.D.Vergados

Isospin Effects in the Giant Dipole Resonance of 42Ca

NUCLEAR REACTIONS 41K(p, γ), E=4-13 MeV; measured σ(E;Eγ, θ). 42Ca deduced giant dipole resonance structure, level-width.

doi: 10.1103/PhysRevC.7.705
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1972WA18      Phys.Rev. C6, 375 (1972)

E.K.Warburton, H.M.Kuan, D.E.Alburger, P.Paul, K.A.Snover

Comment on a Possible Jπ = 0+, T = 2 Resonance in Be9(He3, γγ)C12

NUCLEAR REACTIONS 9Be(3He, γ), E approx 1.74 MeV; measured σ(E;Eγ). 12C deduced no T=2 resonance, upper limit for level-width.

doi: 10.1103/PhysRevC.6.375
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1971DI04      Phys.Rev. C3, 2303 (1971)

E.M.Diener, J.F.Amann, P.Paul, S.L.Blatt

Isospin Splitting of the Giant Dipole Resonance in 60Ni

NUCLEAR REACTIONS 59Co(p, γ), E=4.4-13.6 MeV; measured σ(E;Eγ, θ(γ)). 60Ni deduced giant dipole resonance structure.

doi: 10.1103/PhysRevC.3.2303
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1971PA30      Phys.Rev.Lett. 27, 1013 (1971)

P.Paul, J.F.Amann, K.A.Snover

Symmetry Energy for Collective Dipole Excitation

NUCLEAR REACTIONS 48Ca(p, γ), E=4-18 MeV; 63Cu(p, γ), E=2-18 MeV; measured σ(E;Eγ). 49Sc, 64Zn deduced giant dipole resonance structure, separation energies of T+1, T components.

doi: 10.1103/PhysRevLett.27.1013
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1971RI13      Nucl.Phys. A175, 462 (1971)

F.Riess, W.J.O'Connell, P.Paul

Radiative Proton Capture into 14N

NUCLEAR REACTIONS 13C(p, γ0), E=3-18 MeV; measured σ(E, θ), 13C(p, γ1), E=5.5-18 MeV; measured σ(E, θ); 13C(p, p'γ), E=3-17 MeV; measured σ(E). 14N deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(71)90442-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2679.

1971SN03      Phys.Lett. 37B, 29 (1971)

K.A.Snover, J.F.Amann, W.Hering, P.Paul

Proton Radiative Capture into 209Bi Through Giant Resonances and Analog Resonances

NUCLEAR REACTIONS 208Pb(p, γ), E=8-18 MeV; calculated σ(E;Eγ). 209Bi deduced giant dipole/analog resonance interference, E1 strengths.

doi: 10.1016/0370-2693(71)90561-2
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1970DI09      Nucl.Instrum.Methods 83, 115 (1970)

E.M.Diener, J.F.Amann, S.L.Blatt, P.Paul

An Improved High-Energy Gamma Spectrometer

NUCLEAR REACTIONS 3H(p, γ), E=4 MeV; 12C(p, γ), E=14.2 MeV; 88Sr(p, γ), E=9.4 MeV; measured σ(Eγ).

doi: 10.1016/0029-554X(70)90543-4
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1970OL03      Phys.Rev. C1, 958 (1970)

J.W.Olness, W.R.Harris, P.Paul, E.K.Warburton

Nuclear Structure of Na22. VI. Some Results for Levels with E(ex) > 2.9 MeV

NUCLEAR REACTIONS 20Ne(3He, pγ), E=6.92 MeV; measured σ(Ep, Eγ, θ(pγ)), γ-linear polarization, Doppler shifts. 22Na deduced levels, J, π, γ-multipolarity, γ-branching, T1/2.

doi: 10.1103/PhysRevC.1.958
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1969HE22      Phys.Rev. 188, 1967 (1969)

S.H.Henson, D.B.Fossan, P.Paul, K.W.Jones

Lifetime of the 3.86-MeV State in C13

NUCLEAR REACTIONS 10B(α, p), E=4.5 MeV; measured σ(Eγ, E(13C)). 13C level deduced T1/2. Recoil distance method.

doi: 10.1103/PhysRev.188.1967
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1968FI09      Phys.Rev. 176, 1130(1968)

T.R.Fisher, S.S.Hanna, D.C.Healey, P.Paul

Lifetimes of Levels in A = 10 Nuclei

NUCLEAR REACTIONS 9Be(d, p), (d, n), E=1.7 MeV; 10B(p, n), (p, p'), E=2-9.5 MeV; measured Doppler-shift attenuation. 10Be, 10B, 10C levels deduced T1/2.

doi: 10.1103/PhysRev.176.1130
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1968PA09      Phys.Rev. 173, 919 (1968)

P.Paul, D.Kohler, K.A.Snover

Magnetic Dipole Transitions and Isospin in Be8

NUCLEAR STRUCTURE 8Be, 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.173.919
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1968PA11      Phys.Rev. 173, 1063 (1968)

P.Paul, J.W.Olness, E.K.Warburton

Nuclear Structure of Na22. V. Doppler-Shift Attenuation Measurements

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

doi: 10.1103/PhysRev.173.1063
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1968RI16      Phys.Rev. 176, 1140(1968)

F.Riess, P.Paul, J.B.Thomas, S.S.Hanna

Lifetimes of Levels in 12C, 13C, and 13N

NUCLEAR REACTIONS 13C(p, p'), E=4.1, 4.125, 4.55 MeV; 12C(d, p), E=1.79, 2.715, 3.60 MeV; 12C(p, γ), E approx. 0.459 MeV; 10B(α, p), E=2.9 MeV; measured Doppler - shift attenuation. 12,13C, 13N levels, deduced T1/2.

doi: 10.1103/PhysRev.176.1140
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1967PA01      Phys.Letters 24B, 51 (1967)

P.Paul, T.R.Fisher, S.S.Hanna

Transition Rates of Analog Levels in A = 10 Nuclei

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

doi: 10.1016/0370-2693(67)90337-1
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1967PA19      Phys.Rev. 164, 1332 (1967)

P.Paul, N.G.Puttaswamy, D.Kohler

Excited States in B11 Observed in the Li7(αγ) Reaction

NUCLEAR STRUCTURE 11B, 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1332
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1525.

1966FI01      Phys.Rev.Letters 16, 850 (1966)

T.R.Fisher, S.S.Hanna, P.Paul

Transition Rates in B10 and the β Decay of C10

NUCLEAR STRUCTURE 9Be, 10B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.16.850
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1966PA11      Phys.Rev. 147, 774 (1966)

P.Paul, J.B.Thomas, S.S.Hanna

Lifetimes of the First Excited States of Li7 and Be7

NUCLEAR STRUCTURE 7Li, 7Be; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.147.774
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1966PA15      Z.Naturforsch. 21a, 914 (1966)


Isospin in Be8

NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.

1965KO05      Phys.Letters 15, 157 (1965)

D.Kohler, P.Paul

Gamma Transitions to the 16.6- and 16.9-MeV States in Be8

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)91322-3
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1965PA02      Phys.Rev. 137, B493 (1965)

P.Paul, S.L.Blatt, D.Kohler

Radiative Capture of He3 by Li7

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.137.B493
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1965PA03      Phys.Rev. 137, B499 (1965)

P.Paul, S.L.Blatt, D.Kohler

Search for Resonances in the Reaction Li7(He3, α)Li6

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.137.B499
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1500.

1964PA04      Bull.Am.Phys.Soc. 9, No.4, 391, BA13 (1964)

P.Paul, S.L.Blatt, D.Kohler

7Li(3He, γ)10B and 7Li(3He, α)6Li Reactions

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.

1964PA06      Nucl.Phys. 53, 465 (1964)

P.Paul, K.P.Lieb

The Excited State at 25 MeV in Be8

NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90626-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1385.

1964PA13      Phys.Letters 10, 201 (1964)

P.Paul, S.L.Blatt, D.Kohler

Evidence for the Isotopic Spin Assignment T=0 for the Level at 16.93 MeV in Be8

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90169-6
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1964PA16      Bull.Am.Phys.Soc. 9, No.7, 704, B7 (1964)

P.Paul, S.S.Hanna, G.D.Sprouse

Measurement of Doppler Shifts with Solid-State Detectors

NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.

1963PA04      Phys.Rev. 129, 2698 (1963)

P.Paul, D.Kohler

Alpha-Particle Spectra Produced in the Reactions of Deuterons on Li7

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.129.2698
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1963PA14      Conf.Low Medium Energy Nucl.Phys., Univ.Manchester, p.19 (1963)

P.Paul, B.Povh, G.Schork

The 2.8 MeV State in Si26

NUCLEAR STRUCTURE 26Si; measured not abstracted; deduced nuclear properties.

1959PA05      Nuclear Phys. 13, 576 (1959)

P.Paul, U.Stierlin

Gamma Resonance Scattering at the 17.22 MeV Levels in C12

doi: 10.1016/0029-5582(59)90337-2
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