NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = W.F.Piel Found 51 matches. 1996AL16 Z.Phys. A355, 135 (1996) R.Alfier, D.Alber, H.Grawe, H.Kluge, K.H.Maier, R.Schubart, D.B.Fossan, W.F.Piel, Jr. In-Beam γ-Ray Spectroscopy of the Neutron Deficient 100Ag NUCLEAR REACTIONS 46Ti(58Ni, n3p), E=231 MeV; measured γγ-coin, Eγ, Iγ, γ(θ); deduced residual production σ. 64Zn(40Ca, n3p), E=167 MeV; measured nγ-coin. 100Ag deduced high-spin levels, J, π. Shell model comparison.
doi: 10.1007/s002180050090
1993DE26 Phys.Rev. C48, 2246 (1993) M.E.Debray, A.J.Kreiner, J.M.Kesque, M.Ozafran, A.Romo, H.Somacal, M.E.Vazquez, J.Davidson, M.Davidson, K.Ahn, D.B.Fossan, Y.Liang, R.Ma, E.S.Paul, W.F.Piel, Jr., N.Xu Near Yrast States in Doubly Odd 214Fr NUCLEAR REACTIONS 206Pb(11B, 3n), 208Pb(11B, 5n), E=64-80 MeV; measured Eγ, Iγ, γγ-coin, I(ce). 214Fr deduced levels, J, π, isomers T1/2, γ-multipolarity, ICC.
doi: 10.1103/PhysRevC.48.2246
1991PA04 J.Phys.(London) G17, 605 (1991) E.S.Paul, R.Ma, C.W.Beausang, S.A.Forbes, D.B.Fossan, J.Gizon, J.R.Hughes, Y.Liang, S.M.Mullins, P.J.Nolan, W.F.Piel, Jr., R.J.Poynter, P.H.Regan, R.Wadsworth, N.Xu Electromagnetic Properties of N = 75 Isotones: Evidence for triaxiality at low spin NUCLEAR REACTIONS 92Mo(50Cr, n2p), E=220 MeV; measured γγ-coin, γγ(θ). 120Sn(16O, 3n), E=69 MeV; measured γ(θ). 133Ce, 139Gd deduced levels, J, π, δ, B(λ) ratios, shape features. Other nuclei data included.
doi: 10.1088/0954-3899/17/5/009
1991XU01 Phys.Rev. C43, 2189 (1991) N.Xu, C.W.Beausang, J.R.Hughes, Y.Liang, R.Ma, E.S.Paul, W.F.Piel, Jr., S.Shi, D.B.Fossan High Spin States in 141Eu NUCLEAR REACTIONS 110Cd(35Cl, 2n2p), (35Cl, 2np), E ≈ 150-170 MeV; measured σ(Eγ, E), γγ-coin, γ(θ), Eγ, Iγ. 141Eu deduced levels, J, π, band structure, γ-multipolarity.
doi: 10.1103/PhysRevC.43.2189
1990BE28 Phys.Rev. C42, 541 (1990) C.W.Beausang, P.K.Weng, R.Ma, E.S.Paul, W.F.Piel, Jr., N.Xu, D.B.Fossan Rotational Band Structures in Doubly Odd 138Pm NUCLEAR REACTIONS 116Cd(27Al, 5n), E=110-142 MeV; measured σ(Eγ, E), γγ-coin, γ(θ). 138Pm deduced levels, J, π, band structure, configuration.
doi: 10.1103/PhysRevC.42.541
1990DE12 Phys.Rev. C41, R1895 (1990) M.E.Debray, J.Davidson, M.Davidson, A.J.Kreiner, D.Hojman, D.Santos, K.Ahn, D.B.Fossan, Y.Liang, R.Ma, E.S.Paul, W.F.Piel, Jr., N.Xu Evidence for the Onset of Reflection Asymmetry in 216Fr NUCLEAR REACTIONS 208Pb(11B, 3n), E=53-74 MeV; measured Eγ, Iγ, σ(Eγ, E), σ(Eα, E), I(ce), γγ-coin, γγ(θ), oriented nuclei. 216Fr deduced levels, J, π, configuration, B(λ) ratios, band structure.
doi: 10.1103/PhysRevC.41.R1895
1990PI01 Phys.Rev. C41, 1223 (1990) W.F.Piel, Jr., D.B.Fossan, R.Ma, E.S.Paul, N.Xu, J.B.McGrory High-Spin Structure of N = 51 96Rh and 97Pd: A shell-model study NUCLEAR REACTIONS 64Zn(40Ca, n3pα), (40Ca, n2pα), E=167 MeV; measured γγ-coin, Iγ(θ). 96Rh, 97Pd deduced levels, J, π. Shell model comparison.
doi: 10.1103/PhysRevC.41.1223
1989HI02 Phys.Rev. C39, 471 (1989) L.Hildingsson, C.W.Beausang, D.B.Fossan, R.Ma, E.S.Paul, W.F.Piel, Jr., N.Xu Properties of Shape-Driving Orbitals: Rotational bands in 131La NUCLEAR REACTIONS 116Cd(19F, 4n), E=76-90 MeV; measured I(γ), E(γ), γ(θ). 131La deduced levels, J, π, T1/2, B(M1)/B(E2) ratios, configurations, shapes. Cranked shell model.
doi: 10.1103/PhysRevC.39.471
1989LO02 Phys.Scr. 39, 56 (1989) T.Lonnroth, C.W.Beausang, D.B.Fossan, L.Hildingsson, W.F.Piel, Jr., E.K.Warburton Very-High-Spin and Core-Coupled States in 213Rn. A Test of the Applicability of the Deformed Independent Particle Model NUCLEAR REACTIONS 204Hg(14C, 6n), (14C, 5n), E=80-90 MeV; measured σ(E(γ), E), γ(θ), γγ(t), I(ce). 213,212Rn deduced levels, J, π, γ-transitions, γ-multipolarity, B(λ).
1989MA32 Phys.Rev. C40, 156 (1989) R.Ma, C.W.Beausang, E.S.Paul, W.F.Piel, Jr., S.Shi, N.Xu, D.B.Fossan, J.Burde, M.A.Deleplanque, R.M.Diamond, A.O.Macchiavelli, F.S.Stephens High-Spin Structures in 137Sm: Role of the β-driving νi13/2 intruder in deformation enhancement NUCLEAR REACTIONS 104Pd(37Cl, 3np), E=170 MeV; measured Eγ, Iγ, γγ(θ), γ(t). 137Sm deduced levels, J, π, band structures, B(λ) ratios. Cranked shell model, quasiparticle configurations.
doi: 10.1103/PhysRevC.40.156
1989PA14 Nucl.Instrum.Methods Phys.Res. A278, 749 (1989) S.Pai, W.F.Piel, Jr., D.B.Fossan, M.R.Maier A Versatile Electronic Pulse-Shape Discriminator NUCLEAR REACTIONS 122Sn(18O, xn), E=89 MeV; measured nγ-timing distribution. New electronic pulse shape discrimination. RADIOACTIVITY 252Cf(SF); measured nγ-timing distribution. New electronic pulse shape discrimination.
doi: 10.1016/0168-9002(89)91199-6
1989XU01 Phys.Rev. C39, 1799 (1989) N.Xu, C.W.Beausang, R.Ma, E.S.Paul, W.F.Piel, Jr., D.B.Fossan, L.Hildingsson High Spin States in 137Pr NUCLEAR REACTIONS 122Sn(19F, 4n), E=81 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), γ(t), σ(Eγ, E). 137Pr deduced levels, J, π, band structure, shape. Cranked shell model.
doi: 10.1103/PhysRevC.39.1799
1988HI04 Phys.Rev. C37, 985 (1988) L.Hildingsson, C.W.Beausang, D.B.Fossan, W.F.Piel, Jr. High Spin Structure in the Odd-Proton Nucleus 133Pr NUCLEAR REACTIONS 118Sn(19F, 4n), 117Sn(19F, 3n), E=72-104 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, Iγ(t), σ(Eγ, E). 133Pr deduced levels, J, π. Enriched targets, Ge, Ge(Li), Si(Li) detectors, bismuth germanate anticompton shields, mini-orange electron spectrometer, cranked shell model.
doi: 10.1103/PhysRevC.37.985
1988MA20 Phys.Rev. C37, 1926 (1988) R.Ma, E.S.Paul, S.Shi, C.W.Beausang, W.F.Piel, Jr., N.Xu, D.B.Fossan, T.Chapuran, D.P.Balamuth, J.W.Arrison Band Structure in Doubly Odd 130Pr NUCLEAR REACTIONS 110Cd(28Si, 3npα), E=160 MeV; 106Pd(31P, 3nα), E=155 MeV; measured Eγ, Iγ, γγ(θ), γα-, γp-coin. 130Pr deduced levels, J, π, B(M1)/B(E2) ratios, configuration. Cranked shell model analysis.
doi: 10.1103/PhysRevC.37.1926
1988PA09 Phys.Rev.Lett. 61, 42 (1988) E.S.Paul, R.Ma, C.W.Beausang, D.B.Fossan, W.F.Piel, Jr., S.Shi, N.Xu, J.-Y.Zhang Deformation-Driving Properties of the vi13/2[660](1/2)+ Intruder Orbital for A ≈ 130 Nuclei NUCLEAR REACTIONS 104Pd(37Cl, 3np), E=170 MeV; measured γγ-coin, γ-multiplicity. 137Sm deduced levels, J, π, Nilsson assignments, band structure.
doi: 10.1103/PhysRevLett.61.42
1988PI03 Phys.Rev. C37, 1067 (1988) W.F.Piel, Jr., C.W.Beausang, D.B.Fossan, R.Ma, E.S.Paul, P.K.Weng, N.Xu, G.Scharff-Goldhaber High-Spin States of 99Ag and 100Cd NUCLEAR REACTIONS 64Zn(40Ca, 2n2p), (40Ca, 2n3p), E=167 MeV; measured Eγ, Iγ, σ(Eγ, E), γ(θ), γγ-coin. 99Ag, 100Cd deduced levels, J, π, δ, T1/2. Ge detectors, enriched targets, bismuth germanate anti-Compton shields, NE213 liquid scintillator detectors. VMI model.
doi: 10.1103/PhysRevC.37.1067
1987BE22 Phys.Rev. C36, 602 (1987) C.W.Beausang, L.Hildingsson, E.S.Paul, W.F.Piel, Jr., P.K.Weng, N.Xu, D.B.Fossan Collective Band Structures in the Odd-Proton Nuclei 135,137Pm NUCLEAR REACTIONS 116Sn(24Mg, 4np), E=144 MeV; 114Cd(27Al, 4n), E=131 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, σ(Eγ, E). 135,137Pm deduced levels, J, π, γ multipolarity. Enriched targets. Cranked shell model calculations.
doi: 10.1103/PhysRevC.36.602
1987BE50 Phys.Rev. C36, 1810 (1987) C.W.Beausang, L.Hildingsson, E.S.Paul, W.F.Piel, Jr., N.Xu, D.B.Fossan Similar Rotational Band Structures in Doubly-Odd 136Pm and 134Pr NUCLEAR REACTIONS 114Cd(27Al, 5n), (27Al, 3nα), E=131, 134 MeV; 116Sn(24Mg, 3np), E=133 MeV; measured Eγ, Iγ, γ(θ). 134,136Pm deduced levels, J, π, B(λ) ratios, band characteristics. Semi-classical model.
doi: 10.1103/PhysRevC.36.1810
1987BI07 Phys.Lett. 189B, 277 (1987) J.Billowes, K.P.Lieb, J.W.Noe, W.F.Piel, Jr., S.L.Rolston, G.D.Sprouse, O.C.Kistner Observation of Proton Alignment at the Backbend in 136Nd NUCLEAR REACTIONS 110Pd(30Si, 4n), E=235 MeV; measured Eγ, Iγ, nγ-coin, recoil distance, γγ(θ, H). 136Nd levels deduced T1/2, B(λ), g. Recoil implantation method.
doi: 10.1016/0370-2693(87)91431-6
1987BI13 Phys.Rev. C36, 974 (1987) J.Billowes, K.P.Lieb, J.W.Noe, W.F.Piel, Jr., S.L.Rolston, G.D.Sprouse, O.C.Kistner, F.Christancho Lifetime and g-Factor Measurements of Yrast States in 134Nd and 136Nd NUCLEAR REACTIONS 110Pd(28Si, 4n), (30Si, 4n), E=120-125 MeV; measured nγ-coin, recoil distance Doppler shift. 76Ge(62Ni, 4n), (62Ni, 3n), (64Ni, 4n), (64Ni, 5n), E=235 MeV; measured nγ-coin vs H, γ-anisotropy. 136,134Nd deduced levels, J, π, T1/2, transition quadrupole moment, B(λ), g-factors. 135Nd level deduced g. 146,148Nd(16O, 16O'), E=38 MeV; measured γ correlation anisotropy following Coulomb excitation; deduced Nd paramagnetic relaxation time in Ni.
doi: 10.1103/PhysRevC.36.974
1987BI14 Hyperfine Interactions 34, 65 (1987) J.Billowes, K.P.Lieb, J.W.Noe, W.F.Piel, Jr., S.L.Rolston, G.D.Sprouse, O.C.Kistner, F.Christancho Lifetime and g-Factor Measurements in 136Nd NUCLEAR REACTIONS 110Pd(30Si, 4n), E=121 MeV; measured nγ-coin, Doppler shifted recoil distance. 76Ge(64Ni, 4n), E=235 MeV; measured γγ(θ, H, t). 136Nd deduced yrast levels, J, π, B(E2), T1/2, g, configuration, band structure.
doi: 10.1007/BF02072680
1987CO11 Phys.Rev. C35, 1939 (1987) P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., S.M.Sterbenz, D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton Yrast States of 216Rn and the Extent of a Region of Possible Static Intrinsic Reflection Asymmetry NUCLEAR REACTIONS 208Pb(14C, 2nα), E=67-68 MeV; measured Eγ, Iγ, γ(θ), γγ-, γ(X-ray)-coin. 216Rn deduced levels, J, π, yrast scheme. Hyperpure Ge, Ge(Li) detectors.
doi: 10.1103/PhysRevC.35.1939
1987CO36 Phys.Rev. C36, 2286 (1987) P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton Level Spectrum of 219Ra and Weak Coupling in the Light Actinide Region NUCLEAR REACTIONS, ICPND 208Pb(14C, 3n), E=60-78 MeV; measured Eγ, Iγ, γ(θ), I(ce), thick target yield, σ(E). 219Ra deduced levels, J, π, ICC, B(λ) ratios, γ-multipolarity. Weak coupling model.
doi: 10.1103/PhysRevC.36.2286
1987PA02 Phys.Rev.Lett. 58, 984 (1987) E.S.Paul, C.W.Beausang, D.B.Fossan, R.Ma, W.F.Piel, Jr., N.Xu, L.Hildingsson, G.A.Leander Collective Oblate Band in 131La Due to the Rotational Alignment of h11/2 Neutrons NUCLEAR REACTIONS 116Cd(19F, 4nγ), E=76 MeV; measured γγ-coin. 131La deduced levels, J, π, band structure, shape characteristics. Ge detectors. Cranked shell model calculations.
doi: 10.1103/PhysRevLett.58.984
1987PA17 Phys.Rev. C36, 153 (1987) E.S.Paul, C.W.Beausang, D.B.Fossan, R.Ma, W.F.Piel, Jr., P.K.Weng, N.Xu Band Crossings in the γ-Soft Nucleus 136Nd NUCLEAR STRUCTURE 136Nd; calculated levels, band crossing frequencies. Cranked shell model. NUCLEAR REACTIONS 116Cd(24Mg, 4n), E=106 MeV; measured Eγ, Iγ, γγ(θ), γ(θ), γγ-coin, σ(Eγ, E). 136Nd deduced levels, J, π, band structures, rotational bands, band crossing frequencies, configurations, γ-multipolarity. Cranked shell model analysis.
doi: 10.1103/PhysRevC.36.153
1987PA27 Phys.Rev. C36, 1853 (1987) E.S.Paul, C.W.Beausang, D.B.Fossan, R.Ma, W.F.Piel, Jr., N.Xu, L.Hildingsson High-Spin States in Doubly-Odd 130La NUCLEAR REACTIONS 116Cd(19F, 5n), E=76 MeV; measured Eγ, Iγ, γ(θ), γγ(θ), γ(t). 130La deduced levels, J, π, band characteristics, B(M1)/B(E2), configuration. Cranked shell model.
doi: 10.1103/PhysRevC.36.1853
1987PA30 Phys.Rev. C36, 2380 (1987) E.S.Paul, S.Shi, C.W.Beausang, D.B.Fossan, R.Ma, W.F.Piel, Jr., N.Xu, P.K.Weng Band Crossings in Even-Even 138Sm and 134Nd NUCLEAR REACTIONS 104Pd(37Cl, 2np), (37Cl, 2npα), E=170 MeV; 110Cd(28Si, 2n2p), E=162 MeV; 112Cd(27Al, 4np), E=140 MeV; measured Eγ, Iγ, γ(θ), γγ(θ). 138Sm, 134Nd deduced levels, J, π, band structure, shapes.
doi: 10.1103/PhysRevC.36.2380
1987PI05 Phys.Rev. C35, 959 (1987) W.F.Piel, Jr., C.W.Beausang, D.B.Fossan, L.Hildingsson, E.S.Paul Collective Band Structures in the γ-Soft Nucleus 135Nd NUCLEAR REACTIONS 112Cd(27Al, 3np), E=110-142 MeV; measured γ(θ), γγ-coin. 116Sn(24Mg, 3n2p), E=124-144 MeV; measured γγ-coin. 135Nd deduced levels, J, π, δ, band structure, B(λ) ratios, configuration. Enriched targets, n-type Ge detectors, bismuth germanate anti-Compton shields. Cranked shell model calculations.
doi: 10.1103/PhysRevC.35.959
1987XU01 Phys.Rev. C36, 1649 (1987) N.Xu, C.W.Beausang, E.S.Paul, W.F.Piel, Jr., P.K.Weng, D.B.Fossan, E.Gulmez, J.A.Cizewski Observation of Both h11/2 Proton and Neutron Alignments in 139Pm NUCLEAR REACTIONS 116Cd(27Al, 4n), E=122, 124 MeV; measured γ(θ), γ(t), Eγ, Iγ, γγ(θ), γγ-coin. 139Pm deduced levels, J, π, rotational band characteristics.
doi: 10.1103/PhysRevC.36.1649
1986CH01 Phys.Rev. C33, 130 (1986) T.Chapuran, K.Dybdal, D.B.Fossan, T.Lonnroth, W.F.Piel, Jr., D.Horn, E.K.Warburton High-Spin γ-Ray Spectroscopy in 197Bi NUCLEAR REACTIONS, ICPND 192Pt(10B, 5n), E=50-80 MeV; measured σ(Eγ, E), γγ-coin, γ(θ), γγ(t), gamma-ray yields. 197Bi deduced levels, J, π, isomers, T1/2, configurations, B(λ), yrast sequence.
doi: 10.1103/PhysRevC.33.130
1986CO05 Phys.Rev. C33, 1855 (1986) P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton Intermediate and Weak Coupling in 219Ra NUCLEAR REACTIONS 208Pb(14C, 3n), E=60-78 MeV; measured Eγ, Iγ, γ(θ). 219Ra deduced levels, γ-branching, J, π, rotational band. Weak coupling model.
doi: 10.1103/PhysRevC.33.1855
1986HI03 Phys.Rev. C33, 2200 (1986) L.Hildingsson, C.W.Beausang, D.B.Fossan, W.F.Piel, Jr. Rotational Band Structure in 133Pr NUCLEAR REACTIONS 118Sn(19F, 4n), E=72-104 MeV; measured γ(θ), γγ(t), γγ-coin, σ(Eγ, E), I(ce). 133Pr deduced levels, J, π, T1/2, ICC, γ-branching. Enriched targets, Ge, Si(Li) detector, bismuth germanate anti-Compton shields, mini-orange electron spectrometer. Cranked shell model.
doi: 10.1103/PhysRevC.33.2200
1986LO05 Phys.Rev. C33, 1641 (1986) T.Lonnroth, C.W.Beausang, D.B.Fossan, L.Hildingsson, W.F.Piel, Jr., M.A.Quader, S.Vajda, T.Chapuran, E.K.Warburton Excited States in Neutron-Deficient 195Bi NUCLEAR REACTIONS, ICPND 182W(19F, 6n), E=85-135 MeV; 169Tm(30Si, 4n), E=142 MeV; measured Eγ, Iγ, γγ(t), γ(t), I(ce), relative γ yields. 195Bi deduced levels, J, π, δ, ICC. Enriched targets, Ge(Li), Si(Li) detectors, mini-orange magnetic spectrometer. Shell model comparison.
doi: 10.1103/PhysRevC.33.1641
1986PI03 Phys.Rev. C33, 512 (1986) W.F.Piel, Jr., G.Scharff-Goldhaber, C.J.Lister, B.J.Varley High-Spin States of 97Rh NUCLEAR REACTIONS 60Ni(40Ca, 3p), E=120-150 MeV; measured γγ-coin, γ(θ), σ(Eγ, E). 66Zn(35Cl, 2n2p), E=165 MeV; 70Ge(32S, 2n3p), E=130 MeV; measured γ(θ). 97Rh deduced levels, J, π, δ. Enriched targets, Ge(Li) detectors.
doi: 10.1103/PhysRevC.33.512
1986WA19 Phys.Rev. C34, 136 (1986) E.K.Warburton, C.W.Beausang, D.B.Fossan, L.Hildingsson, W.F.Piel, Jr., J.A.Becker High-Spin (f7/2)(A-40) States in 47Ti, 47Sc, 44Ca, 45Ca, and 48Ti via 36S + 14C Fusion-Evaporation Reactions NUCLEAR REACTIONS, ICPND 36S(14C, 2n), (14C, 3n), (14C, np), (14C, 2np), (14C, nα), (14C, 2nα), E=18-38 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), DSA, σ(Eγ, E); deduced residual production σ. 47,48Ti, 47Sc, 44,45Ca deduced levels, J, π, γ-branching, B(λ), T1/2, γ-multipolarity, δ, B(λ), configuration.
doi: 10.1103/PhysRevC.34.136
1985PI02 Phys.Rev. C31, 456 (1985) W.F.Piel, Jr., P.Chowdhury, U.Garg, M.A.Quader, P.M.Stwertka, S.Vajda, D.B.Fossan Collective Structures in the Odd-Z Transitional Nuclei 115,117I and 121,123Sb NUCLEAR REACTIONS 106Cd(12C, 2np), E=58-63 MeV; 106Cd(14N, n2p), E=62 MeV; 112Sn(12C, 2npα), E=86 MeV; 120,122Sn(7Li, 2nα), E=27 MeV; measured γγ-coin, γ(θ), γ(t). 115,117I, 121,123Sb deduced levels, J, π, T1/2. Enriched targets, Ge(Li), Ge detectors.
doi: 10.1103/PhysRevC.31.456
1985PI05 Phys.Rev. C31, 2087 (1985) W.F.Piel, Jr., T.Chapuran, K.Dybdal, D.B.Fossan, T.Lonnroth, D.Horn, E.K.Warburton High-Spin γ-Ray Spectroscopy in Z = 83 Isotopes: 199,201Bi NUCLEAR REACTIONS 194,196Pt(10B, 5n), E=57-72 MeV; measured Eγ, Iγ, γγ-coin, Iγ(t), Iγ(θ), γγ(θ). 199,201Bi deduced levels, J, π, T1/2, δ, configurations, B(λ), yrast sequence. Enriched targets, Ge(Li), Ge detectors.
doi: 10.1103/PhysRevC.31.2087
1984PI11 Phys.Rev. C30, 902 (1984) W.F.Piel, Jr., G.Scharff-Goldhaber Level Scheme of 98Pd and 96Ru NUCLEAR REACTIONS 70Ge(32S, 2n2p), E=120 MeV; 90Zr(12C, 2nα), E=71 MeV; 66Zn(35Cl, 2n3p), E=170 MeV; 60Ni(40Ca, 4p), E=120 MeV; 70Ge(32S, 2pα), E=120 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ), γγ-coin. 96Ru, 98Pd deduced levels, γ-branching, yrast scheme, J, π, configuration.
doi: 10.1103/PhysRevC.30.902
1984QU02 Phys.Rev. C30, 1772 (1984) M.A.Quader, W.F.Piel, Jr., S.Vajda, W.A.Watson III, F.C.Yang, D.B.Fossan Proton-Hole-Induced Bands in Odd-Odd 116,118,120,122I Nuclides NUCLEAR REACTIONS 106Cd(12C, np), E=58, 63 MeV; 112,114,116Cd(10B, 4n), E=51, 54 MeV; 114,116,118Sn(7Li, 3n), E=34 MeV; measured γγ-coin, γ(θ), σ(Eγ, E), γγ(θ). 116,118,120,122I deduced levels, J, π, band structure, configuration.
doi: 10.1103/PhysRevC.30.1772
1983DY02 Phys.Rev. C28, 1171 (1983) K.Dybdal, T.Chapuran, D.B.Fossan, W.F.Piel, Jr., D.Horn, E.K.Warburton High-Spin States in 201,203At and the Systematic Behavior of Z = 85 Isotopes NUCLEAR REACTIONS, ICPND 192,194Pt(14N, 5n), E=58-100 MeV; measured γγ-coin, σ(Eγ, E), γ(θ), γ(t), Eγ, Iγ, γ yields. 201,203At deduced levels, J, π, T1/2, γ-branching, configurations.
doi: 10.1103/PhysRevC.28.1171
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
1983PI05 Phys.Rev. C28, 209 (1983) W.F.Piel, Jr., G.Scharff-Goldhaber, C.J.Lister, B.J.Varley High-Spin States of 94Ru and 96Pd NUCLEAR REACTIONS 60Ni(40Ca, 2n2p), (40Ca, 2pα), E=120-150 MeV; measured γγ-, γp-, γα-, γn-coin, nγ(t), σ(Eγ). 70Ge(32S, 2n2pα), E=130 MeV; 66Zn(35Cl, 2npα), E=165 MeV; measured γ(θ). 96Pd, 94Ru deduced levels, J, π, T1/2. Ge(Li), Si surface barrier, NE213 liquid scintillator detectors. NUCLEAR STRUCTURE 96Pd, 94Ru; calculated levels, T1/2. Shell model.
doi: 10.1103/PhysRevC.28.209
1983VA14 Phys.Rev. C27, 2995 (1983) S.Vajda, W.F.Piel, Jr., M.A.Quader, W.A.Watson III, F.C.Yang, D.B.Fossan Proton-Hole Induced Bands in Odd-Odd 118,120Sb NUCLEAR REACTIONS 114,116Cd(7Li, 3n), E=29 MeV; 110Pd(11B, 3n), E=51 MeV; measured γγ(t). 118,120Sb deduced levels, J, π, T1/2, γ-multipolarity, band structure, configuration, isomer.
doi: 10.1103/PhysRevC.27.2995
1982CH01 Phys.Rev. C25, 813 (1982) P.Chowdhury, W.F.Piel, Jr., D.B.Fossan Collective Properties of 1g9/2 Proton-Hole Excitations: High-spin states in 116,118,120,122Te and 120Xe nuclei NUCLEAR REACTIONS 117Sn(α, n), E=16, 18, 20 MeV; 119Sn(α, n), E=18 MeV; 114Sn(α, 2n), E=22, 24 MeV; 116Sn(α, 2n), E=22 MeV; 106Pd(12C, 2n), E=58 MeV; 110Pd(13C, 3n), E=40, 45, 49, 52 MeV; 110Cd(13C, 3n), E=52 MeV; measured γγ-coin, γ(θ), σ(Eγ). 116,118,120,122Te, 120Xe deduced levels, J, π. Enriched targets, Ge(Li) detectors.
doi: 10.1103/PhysRevC.25.813
1982TH01 Phys.Rev. C25, 331 (1982) C.E.Thorn, W.F.Piel, Jr., M.J.LeVine, P.D.Bond, A.Gallman Masses of 98Pd, 99Pd, and 100Pd NUCLEAR REACTIONS 96Ru(16O, 14C), (16O, 13C), (16O, 12C), 104Pd(16O, 14C), E=70 MeV; measured σ(E(12C)), σ(E(13C)), σ(E(14C)). 98,99,100Pd deduced level, Q, mass excess. 106Cd deduced mass excess. Q3D magnetic spectrometer.
doi: 10.1103/PhysRevC.25.331
1981PI02 Phys.Rev. C23, 708 (1981) W.F.Piel, Jr., G.Scharff-Goldhaber, A.H.Lumpkin, Y.K.Lee, D.C.Stromswold Level Schemes of 102Pd and 100Pd NUCLEAR REACTIONS 92Zr(13C, 3nγ)102Pd, E=56 MeV; 94Zr(12C, 4nγ)102Pd, E=69 MeV; 91Zr(12C, 3nγ)100Pd, E=56, 63 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ), γ(t), γγ-coin, linear polarization. 102,100Pd deduced levels, γ branching, J, π, δ, T1/2 limits. Enriched 91,92,94Zr targets, Ge(Li) detectors, Ge(Li) Compton polarimeter. Variable moment of inertia model, interacting boson approximation, rotation alignment models.
doi: 10.1103/PhysRevC.23.708
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
1977PI01 Phys.Rev. C15, 287 (1977) W.F.Piel, Jr., G.Scharff-Goldhaber Level Scheme of 99Pd and a Possible High-Spin Cascade in 99Rh NUCLEAR REACTIONS 70Ge(32S, X), E=110-140 MeV; measured γγ-coin, γX-ray coin, σ(E). 91Zr(12C, X), E=56-66 MeV; measured σ(E), γ(t). 92Zr(10B, X), E=40-55 MeV; measured σ(E). 99Pd, 99Rh deduced levels, J, π. Enriched targets, Ge(Li), Si(Li) detectors.
doi: 10.1103/PhysRevC.15.287
1973PI01 Nucl.Phys. A203, 369 (1973) The β-Decay of Tritium RADIOACTIVITY 3H, 195Au; measured Eβ; deduced end-point energy, log ft, Q, upper limit for rest mass of electron antineutrino, for Fermi energy of neutrino sea.
doi: 10.1016/0375-9474(73)90141-3
1973SC14 Phys.Lett. 44B, 416 (1973) G.Scharff-Goldhaber, M.McKeown, A.H.Lumpkin, W.F.Piel, Jr. 'Forking' of Ground State Bands in 102Pd and 100Pd NUCLEAR REACTIONS 90Zr(13C, 3nγ), E=58 MeV; 91Zr(12C, 3nγ), E=64 MeV; 92Zr(13C, 3nγ), E=55 MeV; 94Zr(12C, 4nγ), E=65 MeV; measured Eγ, Iγ(θ). 100,102Pd deduced levels, J, π.
doi: 10.1016/0370-2693(73)90322-5
1968HS02 Nucl.Phys. A117, 686 (1968) S.T.Hsue, M.U.Kim, L.M.Langer, W.F.Piel, Jr., E.J.Spejewski The Negaton Decay of 122Sb RADIOACTIVITY 122Sb; measured Eβ, Iβ, β-spectrum shapes; deduced Qβ, nuclear matrix elements.
doi: 10.1016/0375-9474(68)90839-7
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