NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = P.Paul Found 94 matches. 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
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
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
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
2001PA16 Nucl.Phys. A685, 449c (2001) Commissioning of RHIC and Its Four Detectors
doi: 10.1016/S0375-9474(01)00560-7
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
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
1998PA04 Nucl.Phys. A630, 92c (1998) The GDR and Dissipation in Hot Nuclei
doi: 10.1016/S0375-9474(97)00746-X
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
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
1996HO10 Nucl.Phys. A599, 23c (1996) 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
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
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
1995HO08 Phys.Rev. C51, 2597 (1995) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1978MA22 Phys.Rev. C17, 2097 (1978) 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
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
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
1977SN01 Nucl.Phys. A285, 189 (1977) 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
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
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
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
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
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
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
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
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
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
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
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
1973DI02 Phys.Rev. C7, 695 (1973) 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
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
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
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
1971PA30 Phys.Rev.Lett. 27, 1013 (1971) 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
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
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
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
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
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
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
1968PA09 Phys.Rev. 173, 919 (1968) Magnetic Dipole Transitions and Isospin in Be8 NUCLEAR STRUCTURE 8Be, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.173.919
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
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
1967PA01 Phys.Letters 24B, 51 (1967) 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
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
1966FI01 Phys.Rev.Letters 16, 850 (1966) 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
1966PA11 Phys.Rev. 147, 774 (1966) 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
1966PA15 Z.Naturforsch. 21a, 914 (1966) Isospin in Be8 NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
1965KO05 Phys.Letters 15, 157 (1965) 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
1965PA02 Phys.Rev. 137, B493 (1965) Radiative Capture of He3 by Li7 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B493
1965PA03 Phys.Rev. 137, B499 (1965) 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
1964PA04 Bull.Am.Phys.Soc. 9, No.4, 391, BA13 (1964) 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) 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
1964PA13 Phys.Letters 10, 201 (1964) 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
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) 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
1963PA14 Conf.Low Medium Energy Nucl.Phys., Univ.Manchester, p.19 (1963) The 2.8 MeV State in Si26 NUCLEAR STRUCTURE 26Si; measured not abstracted; deduced nuclear properties.
1959PA05 Nuclear Phys. 13, 576 (1959) Gamma Resonance Scattering at the 17.22 MeV Levels in C12
doi: 10.1016/0029-5582(59)90337-2
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