NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = R.A.Meyer Found 140 matches. Showing 1 to 100. [Next]2005NE12 Nucl.Phys. A758, 174c (2005) C.D.Nesaraja, E.L.Lingerfelt, J.P.Scott, M.S.Smith, W.R.Hix, D.W.Bardayan, J.C.Blackmon, K.Chae, M.W.Guidry, R.A.Meyer A New Computational Infrastructure For Nuclear Astrophysics
doi: 10.1016/j.nuclphysa.2005.05.173
2004SM09 Nucl.Phys. A746, 569c (2004) M.S.Smith, R.A.Meyer, D.W.Bardayan, J.C.Blackmon, K.Chae, M.W.Guidry, W.R.Hix, R.L.Kozub, E.J.Lingerfelt, Z.Ma, J.P.Scott Nuclear data on unstable nuclei for astrophysics
doi: 10.1016/j.nuclphysa.2004.09.092
1997FA18 Nucl.Phys. A624, 401 (1997) M.Fayez-Hassan, Z.Dombradi, Z.Gacsi, J.Gulyas, S.Brant, V.Paar, W.B.Walters, R.A.Meyer Positive Parity Intruder Bands in 116,118Sb NUCLEAR REACTIONS 113,115In(α, n), E=14.5, 16 MeV; analyzed data. 116,118Sb deduced levels, J, π, band structure, intruder states, configurations, ICC, Iγ, γ multipolarity. Interacting boson-fermion-fermion model.
doi: 10.1016/S0375-9474(97)00357-6
1997SC21 Phys.Rev. C56, 1320 (1997) M.Schramm, K.H.Maier, M.Rejmund, L.D.Wood, N.Roy, A.Kuhnert, A.Aprahamian, J.Becker, M.Brinkman, D.J.Decman, E.A.Henry, R.Hoff, D.Manatt, L.G.Mann, R.A.Meyer, W.Stoeffl, G.L.Struble, T.-F.Wang Study of Excited States in 208Pb by Particle-γ Coincidences with the 207Pb(d, p)208Pb and 209Bi(t, α)208Pb Reactions NUCLEAR REACTIONS 207Pb(d, p), E=10 MeV; 209Bi(t, α), E=11.5 MeV; measured Eγ, Iγ, pγ-, αγ-coin. 208Pb deduced levels, J, π, spectroscopic factors, configurations.
doi: 10.1103/PhysRevC.56.1320
1996ME17 Phys.Rev. C54, 2935 (1996) R.A.Meyer, S.V.Jackson, S.Brant, V.Paar Levels of 105Pd Populated in the Decay of 105m,105gAg and Comparison with Interacting Boson-Fermion Model Calculations RADIOACTIVITY 105Cd(EC), (β+) [from 106Cd(n, 2n), E=14 MeV]; 105Ag(EC), (β+) [from 105Cd(EC/β+)-decay]; 105mAg(EC), (IT) [from 105Cd(EC/β+)-decay]; measured γ spectra; deduced log ft. 105Pd deduced levels, J, π, γ-branching, γ multipolarity, μ, quadrupole moment, configuration. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.54.2935
1993CH21 Phys.Rev. C48, 109 (1993) R.E.Chrien, B.K.S.Koene, M.L.Stelts, R.A.Meyer, S.Brant, V.Paar, V.Lopac Neutron-Capture Gamma-Ray Study of Levels in 135Ba and Description of Nuclear Levels in the Interacting-Boson-Fermion Model NUCLEAR REACTIONS Ba, 134Ba(n, γ), E=thermal, resonance; measured Eγ, Iγ. 135Ba deduced levels, J, π, spin cut off parameters. Interacting-boson-fermion, cluster vibration models.
doi: 10.1103/PhysRevC.48.109
1992DR04 Nucl.Phys. A548, 435 (1992) E.Dragulescu, M.Ivascu, C.Petrache, D.Popescu, G.Semenescu, I.Gurgu, M.Ionescu-Bujor, A.Iordachescu, G.Pascovici, R.A.Meyer, V.Lopac, S.Brant, V.Paar, D.Vorkapic, D.Vretenar Nuclear Structure and High-Spin States of 137Pr NUCLEAR REACTIONS 126Te(14N, 3n), E=52-56 MeV; 122Sn(19F, 4n), E=68-76 MeV; measured Eγ, Iγ, σ(E, Eγ, θ), γγ(t), (X-ray)γ(t), γ(t). 137Pr deduced levels, J, π, δ(E2/M1), T1/2. Enriched targets. Ge(Li) detectors. NUCLEAR STRUCTURE 137Pr; calculated levels. Interacting boson-fermion model.
doi: 10.1016/0375-9474(92)90694-F
1991BE03 Nucl.Phys. A522, 483 (1991) J.A.Becker, A.Berger, J.Blomqvist, D.J.Decman, R.Estep, E.Henry, K.H.Maier, L.G.Mann, R.A.Meyer, N.A.F.M.Poppelier, N.Roy, W.Stoffl, G.L.Struble, L.D.Wood Quadrupole Moments of Low-Energy Isomers in 210Po NUCLEAR REACTIONS 209Bi(t, 2n), E=13.5-17 MeV; measured Iγ(θ, t); deduced quadrupole interaction frequencies. 210Po levels deduced quadrupole moments. Shell model, effective charges.
doi: 10.1016/0375-9474(91)90077-J
1991OH03 Z.Phys. A340, 5 (1991) H.Ohm, M.Liang, U.Paffrath, B.De Sutter, K.Sistemich, A.-M.Schmitt, N.Kaffrell, N.Trautmann, T.Seo, K.Shizuma, G.Molnar, K.Kawade, R.A.Meyer The Deformed N = 60 Nucleus 10141Nb RADIOACTIVITY 101Zr(β-); measured Eγ, Iγ, γγ-, γ(X-ray)-coin, βγ(t), βγγ(t); deduced T1/2. 101Nb deduced levels, J, π, T1/2, ICC, band structure, B(λ), δ. Source from fission product separator.
doi: 10.1007/BF01284474
1991SE08 Z.Phys. A339, 269 (1991) H.Seyfarth, H.H.Guven, B.Kardon, W.D.Lauppe, G.Lhersonneau, K.Sistemich, S.Brant, N.Kaffrell, P.Maier-Komor, H.K.Vonach, V.Paar, D.Vorkapic, R.A.Meyer Structure of the Triplet of Low-Lying States in 101Mo NUCLEAR REACTIONS 100Mo(n, γ), E=thermal; measured γγ(t), γ(X-ray)(t). 100Mo(d, p), E=14 MeV; measured σ(θ). 101Mo deduced levels, J, π, δ, T1/2. Model calculations, other data input. RADIOACTIVITY 101Nb(β-); measured γγ(t), γ(X-ray)(t). 101Mo deduced levels, J, π, T1/2, δ. Other data input. Model calculations.
doi: 10.1007/BF01284064
1990HE01 Phys.Rev. C41, 280 (1990) Possible Evidence for Four-Particle, Four-Hole Excitations in 146Gd NUCLEAR STRUCTURE 146Gd; calculated levels. Four level model. NUCLEAR REACTIONS 148Gd(p, t), E not given; calculated σ. Four level model.
doi: 10.1103/PhysRevC.41.280
1990HE17 Phys.Rev. C42, 790 (1990) Comment on ' Monopole Strength and Shape Coexistence in the A ≈ 100 Mass Region ' NUCLEAR STRUCTURE A ≈ 100; calculated monopole transition strength vs level energy difference; deduced shape features, role.
doi: 10.1103/PhysRevC.42.790
1990ME01 Phys.Rev. C41, 686 (1990) R.A.Meyer, R.J.Nagle, S.Brant, E.Frlez, V.Paar, P.K.Hopke Interacting Boson Fermion Model Description for the Levels of 71Ge39 Populated in the Beta Decay of 65.30-h 71As RADIOACTIVITY 71As(β+); measured T1/2, Eγ, Iγ, γγ-coin; deduced log ft. 71Ge deduced levels, possible J, π, (EC+β+) branching. NUCLEAR STRUCTURE 71Ge; calculated levels, μ, quadrupole moment, δ. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.41.686
1990ME03 Phys.Rev. C41, 1172 (1990) R.A.Meyer, K.V.Marsh, H.Seyfarth, S.Brant, M.Bogdanovic, V.Paar Interacting-Boson-Fermion-Fermion Model Description of 140La83 and Comparison with Levels Populated by Beta Decay and Neutron Capture RADIOACTIVITY 140Ba(β-); measured Eγ, Iγ. 140La deduced levels, J, π. Other data input. Model calculations. NUCLEAR REACTIONS 139La(n, γ), E=thermal; measured Eγ, Iγ, E(K X-ray), I(K X-ray). 140La deduced levels, J, π. Other data input. Model calculations. NUCLEAR STRUCTURE 140La; calculated levels, μ, γ-branching ratio, T1/2, quadrupole moments. Interacting boson-fermion-fermion model.
doi: 10.1103/PhysRevC.41.1172
1990ME06 Phys.Rev. C41, 2386 (1990) R.A.Meyer, O.Scholten, S.Brant, V.Paar Mixed-Symmetry States in 144Nd: Semimicroscopic accounting within the cluster vibration model and its mapping into the interacting boson model NUCLEAR STRUCTURE 144Nd; calculated levels, J, π, electric quadrupole, magnetic dipole moments, B(E2), B(M1). Cluster-vibration, interacting boson models.
doi: 10.1103/PhysRevC.41.2386
1990ME15 Fizika(Zagreb) 22, 153 (1990) Multigamma-Ray Calibration Standards RADIOACTIVITY 88Br; measured Eγ, Iγ. 56Co, 110mAg; measured Eγ. 44m,44,48Sc, 48V, 28Mg, 52Fe, 52Mn, 56,59Co, 67Ga, 75Se, 82Br, 83Rb, 95Zr, 105,108m,110mAg, 90Nb, 96,99Mo, 103Ru, 113Sn, 121mTe, 124,125Sb, 126,131I, 133,131Ba, 132,134Cs, 149Gd, 143Ce, 150,152,154,155Eu, 182Ta, 168Tm, 183Re, 185Os, 187W; measured Eγ, Iγ, γ-emission probability. Multi-γ-ray calibration standards.
1990SE17 Fizika(Zagreb) 22, 183 (1990) H.Seyfarth, H.H.Guven, B.Kardon, G.Lhersonneau, K.Sistemich, S.Brant, N.Kaffrell, P.Maier-Komor, H.K.Vonach, V.Paar, D.Vorkapic, R.A.Meyer Structure of the Low-Lying Nuclear States of 101Mo RADIOACTIVITY 101Nb(β-) [from fission product separation]; measured Eγ, Iγ, γγ-coin. 101Mo deduced levels, Iγ. NUCLEAR REACTIONS 100Mo(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin. 100Mo(d, p), E=14 MeV; measured σ(θ). 101Mo deduced levels, L, J, π, spectroscopic factors. NUCLEAR STRUCTURE 101Mo; calculated levels, γ-branching ratio, B(λ), μ, quadrupole moments. SU(6) symmetry. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22226. 1989BA14 Phys.Rev. C39, 1514 (1989) E.M.Baum, J.D.Robertson, P.F.Mantica, Jr., S.H.Faller, C.A.Stone, W.B.Walters, R.A.Meyer, D.F.Kusnezov Level Structure of Odd-Mass Pr Isotopes: Decay of 3.0-min 145Ce to levels of 145Pr RADIOACTIVITY 145Ce(β-) [from 235U(n, F)]; measured E(γ), I(γ), γγ(θ), I(ce). 145Pr deduced levels, I(β), ICC, J, π, γ-multipolarity. 145Ce level deduced π. Mass separated source. Interacting boson-fermion model. NUCLEAR STRUCTURE 143,145Pr; calculated levels, wave functions. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.39.1514
1989ES01 Phys.Rev. C39, 76 (1989) R.Estep, R.K.Sheline, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoffl, L.E.Ussery, J.Kantele Levels in 112Pd and 102Mo NUCLEAR REACTIONS 110Pd, 100Mo(t, pγ), E=16 MeV; measured pγ-, pγγ-coin. 102Mo, 112Pd deduced levels, J, π, band structure.
doi: 10.1103/PhysRevC.39.76
1989KU13 Phys.Rev. C40, 924 (1989) D.F.Kusnezov, D.R.Nethaway, R.A.Meyer Level Structure of the Odd Mass Pr Isotopes: Levels of 143Pr84 populated in the beta decay of 143Ce RADIOACTIVITY 143Ce(β-); measured T1/2, Eγ, Iγ, γγ-coin; deduced log ft. 143Pr deduced levels, J, π, ICC, γ-multipolarity. Interacting boson-fermion model. NUCLEAR STRUCTURE 143,145,147Pr; calculated levels. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.40.924
1989KU19 Phys.Lett. 228B, 11 (1989) D.F.Kusnezov, E.A.Henry, R.A.Meyer An Octupole Two-Phonon Multiplet in 96Zr and Its Description within the spdf Interacting Boson Model NUCLEAR STRUCTURE 96Zr; calculated levels, B(λ), γ-branching ratios. spdf interacting boson model, two-phonon octupole vibrational multiplet.
doi: 10.1016/0370-2693(89)90516-9
1989MA12 Z.Phys. A332, 263 (1989) K.H.Maier, A.Aprahamian, J.A.Becker, D.J.Decman, E.A.Henry, R.G.Lanier, L.G.Mann, R.A.Meyer, K.Sale, N.Roy, W.Stoffl, G.L.Struble, J.Blomqvist Decay of the (21/2)- Isomer in 211Bi and Structure of the νg9/22πh9/2 Levels NUCLEAR REACTIONS 209Bi(t, p), E=11.5-17 MeV; measured E(γ), I(γ), γγ-, p(ce)-coin, γ(ce)(t), σ(Eγ). 211Bi deduced isomer decay, ICC ratios, γ-multipolarity, level J, π, configuration, (γ+e-) branching ratios.
1989RO04 Phys.Lett. 221B, 6 (1989) N.Roy, K.H.Maier, A.Aprahamian, J.A.Becker, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoeffl, G.L.Struble Electromagnetic Decay of 10+ States and Yrast Isomers in 208Pb NUCLEAR REACTIONS 209Bi(t, α), E=11.5 MeV; measured αγ-coin. 208Pb levels deduced decay features, γ-branching ratios, configurations.
doi: 10.1016/0370-2693(89)90181-0
1988HE07 Phys.Rev. C37, 2170 (1988) Monopole Strength as a Measure of Nuclear Shape Mixing NUCLEAR STRUCTURE A=50-160; analyzed E0 transition strength; deduced nuclear state mixing effects role.
doi: 10.1103/PhysRevC.37.2170
1988MA01 Phys.Rev. C37, 254 (1988) H.Mach, G.Molnar, S.W.Yates, R.L.Gill, A.Aprahamian, R.A.Meyer Intruder State Collectivity at a Double Subshell Closure from the Beta Decay of 0- 96gY to the Levels of 96Zr RADIOACTIVITY 96Y(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, I(ce), γγ-, γ(ce)-coin, γγ(θ); deduced T1/2. 96Zr deduced levels, J, π, T, band structure, deformation parameter.
doi: 10.1103/PhysRevC.37.254
1988MA32 Phys.Rev. C38, 74 (1988) L.G.Mann, K.H.Maier, A.Aprahamian, J.A.Becker, D.J.Decman, E.A.Henry, R.A.Meyer, N.Roy, W.Stoffl, G.L.Struble Levels of the Four Lowest Two-Particle Configurations in 210Po Studied by In-Beam γ-Ray and Conversion-Electron Spectroscopy with the 209Bi(t, 2n) Reaction NUCLEAR REACTIONS, ICPND 209Bi(t, 2n), E=11.5-17 MeV; measured Eγ, Iγ, I(ce), γγ(t), γ production σ. 210Po deduced levels J, π, γ-branching, ICC, γ-multipolarity, configurations. Shell model.
doi: 10.1103/PhysRevC.38.74
1988ME13 Hyperfine Interactions 43, 331 (1988) Influence of a Strong Proton-Neutron Interaction on Mass 100 Nuclei and Properties of the Octupole Two-Phonon Multiplet in 96Zr NUCLEAR STRUCTURE A=80-120; analyzed data; deduced p-n interaction role. 96Zr; analyzed data; deduced octupole excitations role.
doi: 10.1007/BF02398313
1988YA03 Phys.Rev. C37, 1889 (1988) S.W.Yates, E.M.Baum, E.A.Henry, L.G.Mann, N.Roy, A.Aprahamian, R.A.Meyer, R.Estep Nuclear Structure of 200Pt from In-Beam Conversion-Electron and γ-Ray Spectroscopy NUCLEAR REACTIONS 198Pt(t, pγ), (t, pe-), E=16 MeV; measured Eγ, Iγ, electron spectra, pγ-, pe-, pγγ-coin. 200Pt deduced levels, J, π, ICC, B(E2) ratios, γ-multipolarity, isomer T1/2.
doi: 10.1103/PhysRevC.37.1889
1987BO19 Nucl.Instrum.Methods Phys.Res. B26, 304 (1987) J.W.Borgs, H.-P.Kohl, G.Lhersonneau, H.Ohm, U.Paffrath, K.Sistemich, D.Weiler, R.A.Meyer Improvements at JOSEF and a New Setup for Fission-Product Spectroscopy NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured Eγ, Iγ, γ(107Tc)-coin, fission fragment mass, charge distribution. 131Sb, 97Y levels deduced T1/2, configuration. 107Tc deduced levels. Gas filled separator, electrostatic chopper.
doi: 10.1016/0168-583X(87)90768-3
1987BR38 Fizika(Zagreb) 19, 453 (1987) S.Brant, V.Paar, D.Vorkapic, D.Vretenar, V.Lopac, R.A.Meyer d5/23- and s1/2d3/2g7/2-Parametrization for 101Mo in IBFM/PTQM and the Electromagnetic Properties of Anomalous Triplet NUCLEAR STRUCTURE 101Mo; calculated levels, T1/2, Iγ ratios. Interacting boson-fermion model.
1987DR12 Rev.Roum.Phys. 32, 485 (1987) E.Dragulescu, M.Ivascu, M.Ionescu-Bujor, A.Iordachescu, C.Petrache, D.Popescu, G.Pascovici, G.Semenescu, M.Duma, I.Gurgu, F.Baciu, R.A.Meyer, V.Paar, S.Brant, D.Vorkapic, D.Vretenar, H.Ajazaj High-Spin Spectroscopy of Pr Nuclei NUCLEAR REACTIONS 118,119,120,122,124Sn, 121,123Sb, 125,126,128,130Te, 136,138Ce(19F, X), (16O, X), (14N, X), E not given; measured Eγ, Iγ, γ(θ), γγ(t), X-ray(γ)(t). 133,134,135,136,137,138,139Pr deduced levels, J, π, band structure, γ-branching. In-beam γ-ray spectroscopy. Interacting boson model calculations.
1987ES01 Phys.Rev. C35, 1485 (1987) R.J.Estep, R.K.Sheline, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoffl, L.E.Ussery, J.Kantele Measurement of E0 Transitions in Neutron-Rich Nuclei near A = 100 NUCLEAR REACTIONS 98,100Mo, 104Ru, 106,108,110Pd(t, p), E=16 MeV; measured γp-, (ce)p-coin. 100,102Mo, 106Ru, 108,110,112Pd deduced levels, T1/2, E0 transitions, E0/E2 branching ratios.
doi: 10.1103/PhysRevC.35.1485
1987KU07 Helv.Phys.Acta 60, 456 (1987) D.Kusnezov, A.Bruder, V.Ionescu, J.Kern, M.Rast, K.Heyde, P.Van Isacker, J.Moreau, M.Waroquier, R.A.Meyer Mixing of the Ground Band and Two-Particle Four-Hole Intruder Band in 110Cd NUCLEAR STRUCTURE 110Cd; calculated positive parity levels, J, π. Interacting boson model, configuration mixing calculations.
1987ME04 Phys.Rev. C35, 1468 (1987) R.A.Meyer, D.R.Nethaway, A.L.Prindle, R.P.Yaffe Octupole State Properties in 168Er and the Two-Neutron ([521 1/2][633 7/2]) Configurational Pair RADIOACTIVITY 168Tm(EC), (β-) [from 169Tm(n, 2n), E=14.8, 40 MeV, Ta spallation]; measured Eγ, Iγ; deduced log ft. 168Er deduced levels, T1/2, B(λ), J, π, K, configurations, octupole band K mixing.
doi: 10.1103/PhysRevC.35.1468
1987ME09 Z.Phys. A327, 393 (1987) R.A.Meyer, E.Monnand, J.A.Pinston, F.Schussler, B.Pfeiffer, V.Paar Pseudobands in Non-SU(3) Odd-Mass Nuclei and Coherent State Structures of Quadrupole Phonons NUCLEAR STRUCTURE 99Y, 75Se, 75,77Kr; calculated levels, J. Quadrupole phonon model.
1987YA13 Phys.Rev. C36, 2143 (1987) S.W.Yates, L.G.Mann, E.A.Henry, D.J.Decman, R.A.Meyer, R.J.Estep, R.Julin, A.Passoja, J.Kantele, W.Trzaska E0 Decay of 0+ States in 146Gd: Search for two-phonon octupole excitations NUCLEAR REACTIONS 144Sm(α, 2n), E=25.5 MeV; 144Sm(3He, n), E=15-20 MeV; measured Eγ, Iγ, I(ce). 146Gd deduced levels, J, π, E0 transitions.
doi: 10.1103/PhysRevC.36.2143
1987ZE03 Nucl.Instrum.Methods Phys.Res. A256, 180 (1987) M.Zendel, S.G.Prussin, K.Rengan, T.N.Massey, R.A.Meyer Modification of a Gas Jet Transport System for the Supression of Heavy-Mass Fission Product Homologues NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission product Eγ, Iγ; deduced fission fragment mean penetration depths into Al. Ge(Li) detector.
doi: 10.1016/0168-9002(87)91054-0
1986BR16 Phys.Rev. C34, 341 (1986) S.Brant, V.Paar, D.Vretenar, R.A.Meyer Anomaly in Spectra of 105Pd and 103Ru NUCLEAR STRUCTURE 105Pd, 103Ru; calculated levels; deduced exchange force role. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.34.341
1986LH01 Z.Phys. A323, 59 (1986) G.Lhersonneau, D.Weiler, P.Kohl, H.Ohm, K.Sistemich, R.A.Meyer A New High-Spin Isomer in 9739Y58 RADIOACTIVITY 97mY [from 235U(n, F), E=thermal]; measured Eγ, Iγ, γγ-, γ(X-ray)-, βγ-coin; deduced T1/2. 97Y deduced isomer decay, γ-multipolarity, configuration, levels, possible J, π, γ-branching. Shell model comparison.
1986MA31 Z.Phys. A324, 123 (1986) A.Maj, H.Grawe, H.Kluge, A.Kuhnert, K.H.Maier, R.A.Meyer, J.Recht, N.Roy Observation of Highly Enhanced E3-Transitions in 198,200Po. Evidence for Octupole Instability at Z ≥ 84 and N ≤ 114 ( Question ) NUCLEAR REACTIONS 182,184W(20Ne, 4n), E=105, 112 MeV; measured Eγ, Iγ, γγ-coin. 198,200Po deduced levels, J, π, γ-branching, isomer T1/2, g, B(E3), configurations.
1986ME11 Phys.Lett. 177B, 271 (1986) R.A.Meyer, E.A.Henry, L.G.Mann, K.Heyde Observation of a Full Set of Coexisting Intruder Excitations in 98Zr: Evidence for correlated excitations ( Question ) NUCLEAR REACTIONS 96Zr(t, p), E not given; measured Eγ, Iγ, γγ-coin, pγγ(t). 98Zr deduced levels, J, π. Multiparameter coincidence techniques. Interacting boson model calculations.
doi: 10.1016/0370-2693(86)90751-3
1986MO07 Phys.Rev. C33, 1843 (1986) G.Molnar, S.W.Yates, R.A.Meyer Evidence for a Coexisting Four-Particle, Four-Hole Band in Doubly Closed Subshell 96Zr NUCLEAR REACTIONS 96Zr(n, n'γ), E=2.85, 3.4 MeV; measured σ(θ). 96Zr deduced levels, J, π, γ-branching, γ-multipolarity, B(λ), band structure, configuration.
doi: 10.1103/PhysRevC.33.1843
1986PF02 Z.Phys. A325, 487 (1986) B.Pfeiffer, S.Brant, K.-L.Kratz, R.A.Meyer, V.Paar The K = (3/2)+1 Side-Band in 99Y and Its Description by the IBFM/PTQM Model NUCLEAR STRUCTURE 99Y; calculated levels; deduced rotational band characteristics. Interacting boson-fermion model.
1986SK02 Z.Phys. A323, 407 (1986) G.Skarnemark, K.Broden, N.Kaffrell, S.G.Prussin, N.Trautmann, K.Rengan, D.Eriksen, D.F.Kusnezov, R.A.Meyer Subshell Closure Effects on the Collectivity of 3688Kr52 and the Beta Decay of 88Br to Levels in 88Kr NUCLEAR STRUCTURE 88Kr; calculated levels, B(E2). Neutron-proton interacting boson model. RADIOACTIVITY 88Br(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, γγ-coin, γγ(t). 88Kr deduced levels, J, π, γ-branching, B(E2).
1986WA06 Phys.Rev. C33, 1036 (1986) W.B.Walters, N.K.Aras, C.A.Stone, C.Chung, R.L.Gill, M.Shmid, E.A.Henry, R.A.Meyer Isomerism in 148Pr and the Low-Lying Levels of 148Nd RADIOACTIVITY 148Pr(β-) [from 235U(n, F), 148Nd(n, p)]; measured Eγ, Iγ, γγ(t); deduced isomers, T1/2. 148Nd deduced levels, J, π, γ-branching.
doi: 10.1103/PhysRevC.33.1036
1985CH16 Phys.Rev. C31, 2199 (1985) C.Chung, W.B.Walters, D.S.Brenner, R.L.Gill, M.Shmid, Y.Y.Chu, R.E.Chrien, L.-J.Yuan, F.K.Wohn, R.A.Meyer Decay of 2.2-sec 14656Ba90 to Levels of Odd-Odd 14657La89 RADIOACTIVITY 146Ba(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, T1/2, γγ(t), γγ(θ); deduced log ft. 146La deduced levels, J, π, Iβ, δ. Mass separated 146Ba activity, Ge(Li), Ge, planar detectors.
doi: 10.1103/PhysRevC.31.2199
1985ME09 Nucl.Phys. A439, 510 (1985) R.A.Meyer, E.Monnand, J.A.Pinston, F.Schussler, I.Ragnarsson, B.Pfeiffer, H.Lawin, G.Lhersonneau, T.Seo, K.Sistemich Deformation in Odd-Mass Nuclei near A ≈ 100: One- and three-quasiparticle Nilsson states in 9939Y60 RADIOACTIVITY 99mY [from 235U(n, F), E=thermal]; measured Eγ, Iγ, T1/2, γγ-coin; deduced levels, J, π, K, band structure, γ-branching, Nilsson assignment. Particle-rotor coupling model.
doi: 10.1016/0375-9474(85)90424-5
1985ME20 Hyperfine Interactions 22, 385 (1985) Deformation and Shape Coexistence in Medium Mass Nuclei NUCLEAR STRUCTURE Z=38-50; N=59; compiled, reviewed, analyzed level data; deduced deformation, shape coexistence features. Nuclear vibron model, quadrupole phonon model.
doi: 10.1007/BF02064011
1985SE02 Z.Phys. A320, 393 (1985) T.Seo, H.Lawin, G.Lhersonneau, R.A.Meyer, G.Menzen, K.Sistemich The Nilsson-Potential Parameters for Neutrons at A ≈ 100 and New Deformation Values for 103Mo and 105Mo RADIOACTIVITY 105,103Nb(β-); measured γγ(t), centroid shift. 105,103Mo deduced level T1/2, ground state band B(λ), (g(k)-g(R)/Q0), quadrupole moment, Nission assignments.
doi: 10.1007/BF01415715
1985TO10 Nucl.Phys. A439, 427 (1985) Y.Tokunaga, H.Seyfarth, R.A.Meyer, O.W.B.Schult, H.G.Borner, G.Barreau, H.R.Faust, K.Schreckenbach, S.Brant, V.Paar, M.Vouk, D.Vretenar Low-Lying Levels of 77Se Studied by Thermal Neutron Capture and Evidence for a New Term in the E2 Operator of TQM(IBM) NUCLEAR REACTIONS 76Se(n, γ), E=thermal; measured Iγ, Eγ, I(ce); deduced Q, neutron separation energy. 77Se deduced levels J, π, population probability. Enriched target, crystal-, β-, pair-spectrometers. Statistical, particle-vibration model analyses.
doi: 10.1016/0375-9474(85)90420-8
1984ME04 Phys.Rev. C29, 1839 (1984) R.A.Meyer, J.Lin, G.Molnar, B.Fazekas, A.Veres, M.Sambataro Influence of Cross Subshell Excitations on the Collective States of 98Mo Observed by β Decay and (n, n'γ) Reaction Spectroscopy RADIOACTIVITY 98mNb(β-) [from 98Mo(n, p), E=14 MeV]; measured Eγ, Iγ, γγ(t), γγ-coin; deduced log ft. 98Mo deduced levels, J, π, γ-branching, Iβ, absolute Iγ, δ. Compton suppression. NUCLEAR REACTIONS 98Mo(n, n'γ), E=14 MeV; measured γ(θ), Eγ, Iγ, γγ-coin, γγ(θ). 98Mo deduced levels, δ, J, π. Enriched target. NUCLEAR STRUCTURE 98Mo; calculated levels, γ-branching ratios, cross subshell excitations. Interacting boson model.
doi: 10.1103/PhysRevC.29.1839
1984ME09 Phys.Lett. 140B, 159 (1984) R.A.Meyer, K.Heyde, P.Van Isacker, M.Waroquier, J.Moreau, J.L.Wood Interaction between Neutron Particle-Hole and Octupole Core-Coupled States in N = 83 Nuclei NUCLEAR STRUCTURE 147Gd, 145Sm; calculated levels; deduced neutron particle-hole, octupole core coupled state interaction, intruder state role. RADIOACTIVITY 145Eu(EC), (β+) [from mass separation]; measured Eγ, Iγ. 145Sm deduced levels, J, π, γ-multipolarity data.
doi: 10.1016/0370-2693(84)90911-0
1984SE05 Z.Phys. A315, 251 (1984) T.Seo, A.-M.Schmitt, H.Ahrens, J.P.Bocquet, N.Kaffrell, H.Lawin, G.Lhersonneau, R.A.Meyer, K.Shizuma, K.Sistemich, G.Tittel, N.Trautmann Evidence of Rotational Bands in 103Nb RADIOACTIVITY 103Zr(β-) [from fission product separation]; measured Eγ, Iγ, γγ-, (X-ray)γ-coin, γγ(t). 103Nb deduced levels, J, π, T1/2, Nilsson assignments, rotational bands, (g(k)-g(R)/Q0) magnitude.
doi: 10.1007/BF01419388
1984SH03 Z.Phys. A315, 65 (1984) K.Shizuma, H.Ahrens, J.P.Bocquet, N.Kaffrell, B.D.Kern, H.Lawin, R.A.Meyer, K.Sistemich, G.Tittel, N.Trautmann Odd Neutron Nuclei near A = 100: Rotational bands in 103Mo and 105Mo populated in the β- decays of 103Nb and 105Nb RADIOACTIVITY 103,105Nb(β-) [from fission product isotope separation]; measured Eγ, Iγ, γγ-, (X-ray)γ-coin, γγ(θ); deduced T1/2. 103,105Mo deduced levels, γ-branching, δ, B(E2), quadrupole moment.
doi: 10.1007/BF01436210
1984TO11 Nucl.Phys. A430, 269 (1984) Y.Tokunaga, H.Seyfarth, O.W.B.Schult, S.Brant, V.Paar, D.Vretenar, H.G.Borner, G.Barreau, H.Faust, Ch.Hofmeyr, K.Schreckenbach, R.A.Meyer A Study of 75Se by Neutron Capture and the SU(3)-SU(5) Transition in the Quadrupole-Phonon Representation NUCLEAR REACTIONS 74Se(n, γ), E=thermal; measured Iγ, Eγ, I(ce); deduced Q. 75Se, 75As deduced levels, J, π. Enriched target, crystal, pair β-spectrometers.
doi: 10.1016/0375-9474(84)90041-1
1984WA04 Phys.Rev. C29, 991 (1984) W.B.Walters, E.A.Henry, R.A.Meyer Gamma-Ray Cascade Population of the (19/2)- Isomer in the Decay of 133mTe to Levels of 133I RADIOACTIVITY 133mTe(β-), (IT) [from 235U(n, F), E=thermal]; measured T1/2, Eγ, Iγ, γγ-coin; deduced log ft. 133I deduced levels, J, π, T1/2, ICC. Ge detectors, three parameter coincidences.
doi: 10.1103/PhysRevC.29.991
1983BR24 Nucl.Phys. A408, 285 (1983) D.S.Brenner, D.Barkey, S.Blair, D.D.Warner, R.A.Meyer The Level Scheme of 183Re and Systematics of Odd-A Re Isotopes: Interplay of ϵ2 and ϵ4 deformations in the W-Re region RADIOACTIVITY 183,183mOs(EC), (β+) [from 182W(α, 3n), W(α, xn)]; measured Eγ, Iγ, T1/2, γγ-coin. 183Re deduced levels, J, π, ICC, γ-multipolarity. Ge(Li) detectors, enriched, natural targets.
doi: 10.1016/0375-9474(83)90585-7
1983HI03 Phys.Rev. C27, 2203 (1983) H.G.Hicks, J.H.Landrum, E.A.Henry, R.A.Meyer, S.Brant, V.Paar Population of 133I from the Beta Decay of Fission Product 133gTe and the Cluster-Vibration Model NUCLEAR STRUCTURE 133I; calculated levels, B(λ), branching ratios, static quadrupole moment, μ. RADIOACTIVITY 133Te(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, γγ-coin; deduced log ft. 133I deduced levels, J, π, β-branching, γ-branching, B(λ). Cluster vibration model. Hyperpure Ge, Ge(Li) detectors.
doi: 10.1103/PhysRevC.27.2203
1983ME08 Phys.Rev. C27, 2217 (1983) R.A.Meyer, J.F.Wild, K.Eskola, M.E.Leino, S.Vaisala, K.Forssten, U.Kaup, A.Gelberg Collective Excitations of 82Kr Observed by In-Beam and Decay Spectroscopy and Their Characterization by the Interacting Boson Model RADIOACTIVITY 82,82mBr(β-); 82,82mRb(β+), (EC); measured Eγ, Iγ, γγ-coin. 82Kr deduced levels, J, π. NUCLEAR REACTIONS 80Se(α, 2nγ), E=16-21.3 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 82Kr deduced levels, J, π, γ-multipolarity, δ, γ-branching, band structure configuration. Interacting boson model.
doi: 10.1103/PhysRevC.27.2217
1983ME17 Int.J.Appl.Radiat.Isotop. 34, 1073 (1983) Multigamma-Ray Calibration Sources RADIOACTIVITY 88Br(β-); 152Eu(β-), (β+), (EC); 56Co(EC), (β+); 110mAg(β-); 168Tm(EC), (β-); measured Iγ. Automated multi-spectrometer γ-ray counting, large volume hyperpure Ge detectors, mass separated sources.
doi: 10.1016/0020-708X(83)90173-4
1982HE06 Phys.Rev. C25, 3193 (1982) K.Heyde, J.Sau, E.A.Henry, R.A.Meyer Influence of the M1 Tensor Term for Transitions between Levels of the Two-Proton Nucleus 134Te Populated in the Beta Decay of 10-s 134Sb NUCLEAR STRUCTURE 134Te; calculated levels, B(λ), electromagnetic transition rates; deduced tensor M1 operator role. Shell model, 134Sb decay data analysis.
doi: 10.1103/PhysRevC.25.3193
1982LI09 Radiochem.Radioanal.Lett. 50, 399 (1982) Ground-State Decay Branchings for 85,86,87,88Se Isotopes with a Gas-Phase Rapid Chemistry System RADIOACTIVITY 85,86,87,88Se [from fission]; measured Eγ, Iγ following β-decay. 85,86,87,88Br, 85,86,87,88Kr levels deduced γ-branching, absolute Iγ.
1982ME01 Phys.Rev. C25, 682 (1982) R.A.Meyer, O.G.Lien III, E.A.Henry Coexisting Intruder Bands in 83Se and Evidence for the Role of Proton Subshell Closure in Inhibiting Formation of Odd-Neutron Intruder Bands RADIOACTIVITY 83As; measured Eγ, Iγ, T1/2. 83Se deduced levels, J, π. Ge(Li) detectors. NUCLEAR STRUCTURE 81Ge, 83Se, 85Kr, 87Sr; analyzed data; deduced intruder states in N=49 nuclei.
doi: 10.1103/PhysRevC.25.682
1982ME10 J.Phys.(London) G8, 1413 (1982) R.A.Meyer, J.W.T.Meadows, E.S.Macias Opposing Properties of Particle-Hole and Intruder-Hole Bands in N = 87 Nuclei and 149Sm Levels Populated by 149Pm(β-) and 149Eu(EC) RADIOACTIVITY 149Eu(EC) [from Sm(p, xn), 149Sm(α, 4n)149Gd(EC-decay)]; 149Pm(β-) [from 148Nd(n, γ)149Nd(β-decay)]; measured Eγ, Iγ, γγ-coin, I(ce). 149Sm deduced levels, ICC, γ-multipolarity, band structure, configuration. Compton suppression, Ge(Li), Si detectors.
doi: 10.1088/0305-4616/8/10/012
1982RE08 Nucl.Instrum.Methods 197, 427 (1982) K.Rengan, J.Lin, M.Zendel, R.A.Meyer On-Line System for the Isolation and Study of 0.5 to 30 Second Selenium Fission Products with Simulataneous Suppression of Daughter Bromine Activity RADIOACTIVITY 85,86,87,88,89Se [from 235U(n, F)]; measured Eγ, Iγ, T1/2. 89Se deduced transition. On-line, fast gas jet systems.
doi: 10.1016/0167-5087(82)90338-6
1982RE10 Radiochem.Radioanal.Lett. 51, 339 (1982) Measurement of Yields of Fission Products with Half Lives of 1 to 30 Sec by Continuous Chemistry Techniques RADIOACTIVITY 85,86,87,88Se [from fission]; measured Eγ, Iγ; deduced cumulative yields. Gas jet system.
1982WA21 Phys.Rev. C26, 2273 (1982) W.B.Walters, S.M.Lane, N.L.Smith, R.J.Nagle, R.A.Meyer Shell Model Description of N = 81 Five-Excition 135Xe and the Decay of 135I NUCLEAR STRUCTURE 135Xe; calculated levels; deduced configurations. Shell model. RADIOACTIVITY 135I(β-) [from fission product radiochemical separation]; measured Eγ, Iγ, T1/2, γγ-coin; deduced Iβ, log ft. 135Xe deduced levels, J, π, γ-branching. Shell model.
doi: 10.1103/PhysRevC.26.2273
1981WA05 Phys.Rev. C23, 1113 (1981) R.W.Waldo, R.A.Karam, R.A.Meyer Delayed Neutron Yields: Time dependent measurements and a predictive model RADIOACTIVITY, Fission 233,234,236,239U, 238Np, 239,240,242,243Pu, 242,243Am, 246Cm, 250Cf, 233Th [from thermal neutron irradiation]; measured delayed neutron yield; deduced delayed neutron characteristics. Fission product yield model. NUCLEAR REACTIONS, Fission 232,233,235,238U, 237Np, 238,239,241,242Pu, 241,242Am, 245Cm, 249Cf, 232Th(n, F), E=thermal; measured delayed neutron yield; deduced delayed neutron characteristics. Fission product yield model.
doi: 10.1103/PhysRevC.23.1113
1980ME06 Phys.Rev. C21, 2590 (1980) R.A.Meyer, J.E.Fontanilla, N.L.Smith, C.F.Smith, R.C.Ragaini, V.Paar Level Properties of 85Rb from the Decay of the 85Kr and 85Sr Isomers and the Cluster-Vibration Model NUCLEAR STRUCTURE 85Rb; calculated levels, B(λ); deduced role of M1 tensor term. Cluster-vibration model. RADIOACTIVITY 85Kr [from fission products], 85Sr [from 84Sr+n, 85Rb(α, n)]; measured Eγ, Iγ, I(ϵ)/Iβ+, Eβ, Iβ; deduced Q(ϵ), log ft. 85Rb deduced levels, J, π, γ-branching. Ge(Li) detector. Compton-suppression spectrometer.
doi: 10.1103/PhysRevC.21.2590
1979GL09 Phys.Rev. C20, 2370 (1979) M.D.Glascock, E.W.Schneider, W.B.Walters, S.V.Jackson, R.A.Meyer Level Structure of Odd-Mass In Nuclei and the Unified Model. II. 117In Levels Populated in the Decay of 117Cd Isomers RADIOACTIVITY 117,117mCd [from 116Cd(n, γ)]; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced β-branching, log ft. 117In deduced levels, J, π. NUCLEAR REACTIONS 116Cd(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced σ.
doi: 10.1103/PhysRevC.20.2370
1979PA03 J.Phys.(London) G5, L75 (1979) A Possible Semimicroscopic Mechanism to Generate Two 0+ Bands and their Band Mixing: 110Cd as an Example NUCLEAR STRUCTURE 110Cd; calculated energy levels; deduced semi-microscopic band-mixing theory. Ground-state band mixed with cluster combination.
doi: 10.1088/0305-4616/5/1/010
1979SC06 Phys.Rev. C19, 1025 (1979) E.W.Schneider, M.D.Glascock, W.B.Walters, R.A.Meyer Collective Excitations in 128Xe Observed Following the Decay of 128Cs And 128I RADIOACTIVITY 128Cs [from 133Cs(d, 7n), E=80 MeV], 128I [from 127I(n, γ), E=th]; measured Eγ, Iγ, γγ(θ). 128Xe deduced levels, J, π, log ft, branching ratios. Ge(Li) detectors.
doi: 10.1103/PhysRevC.19.1025
1979SC12 Z.Phys. A291, 77 (1979) E.W.Schneider, M.D.Glascock, W.B.Walters, R.A.Meyer Radioactive Decay of 1.7-h 149Nd to Levels of Transitional 149Pm NUCLEAR REACTIONS 148Nd(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin. 149Nd deduced levels, J, π. Compton suppression Ge(Li) detector. Enriched targets. Core-coupling model interpretation.
doi: 10.1007/BF01415819
1978AN11 Phys.Rev. C18, 383 (1978) D.L.Anderson, D.S.Brenner, R.A.Meyer Collective Excitations in 158Dy as Populated in Radioactive Decay of 158Ho-g, m RADIOACTIVITY 158m,158Ho [from 149Sm(12C, 3n)(2.3-H, EC, β+)158Ho]; measured Eγ, Iγ, γγ-coin; deduced log ft. 158Dy deduced levels, J, π, ICC, γ multipolarities. Ge(Li) detectors, enriched targets.
doi: 10.1103/PhysRevC.18.383
1978HE08 Phys.Rev. C17, 1219 (1978) K.Heyde, M.Waroquier, R.A.Meyer Unified Description of Odd-Mass Indium Nuclei I. General Theory and Comparison to 113In and 115In Levels Populated in the Decay of 113Sn and 115Cd-m, g RADIOACTIVITY 113Sn, 115m,115Cd; measured Eγ, Iγ; deduced log ft. 113,115In deduced levels. Unified model analysis, Compton suppression.
doi: 10.1103/PhysRevC.17.1219
1978HE16 Phys.Rev. C18, 1814 (1978) Systematic Study of the Structure of Odd-Mass Lanthanum Nuclei. III. Levels in 133La from the Decay of 5-h 133Ce RADIOACTIVITY 133Ce [from Ba(α, xn)]; measured Eγ, Iγ, I(ce), γγ-coin; deduced log ft. 133La deduced levels, J, π, ICC, λ, B(λ). Mass separation, chemical purification.
doi: 10.1103/PhysRevC.18.1814
1978JA14 Phys.Rev. C18, 1840 (1978) S.V.Jackson, J.W.Starner, W.R.Daniels, M.E.Bunker, R.A.Meyer N = 85 Nuclei. II. Decay of 4.15-h 149Tb-g to Levels of 149Gd RADIOACTIVITY 149Tb [from 181Ta(p, X), 141Pr(12C, 4n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 149Gd deduced levels, J, π, λ. Mass separated, chemically purified sources, Ge(Li) detectors.
doi: 10.1103/PhysRevC.18.1840
1978ME10 Phys.Rev. C17, 1822 (1978) R.A.Meyer, A.L.Prindle, W.A.Myers, P.K.Hopke, D.Dieterly, J.E.Koops Multiparticle Configurations in the Odd-Neutron Nuclei 61Ni and 67Zn Populated by Decay of 61Cu, 67Cu, and 67Ga RADIOACTIVITY 61,67Cu; measured Eγ, Iγ. 67Ga; measured absolute Iγ, T1/2, Eγ. 61Ni, 67Zn deduced levels, J, π, γ-branching.
doi: 10.1103/PhysRevC.17.1822
1978NE09 Int.J.Appl.Radiat.Isotop. 29, 188 (1978) D.Newton, A.E.R.Toureau, A.L.Anderson, R.A.Meyer Relative High-Energy Gamma- and X-Ray Emissions Following the Decay of 103Pd RADIOACTIVITY 103Pd; measured abundance ratio of γ to X-ray.
doi: 10.1016/0020-708X(78)90143-6
1977BR22 Phys.Rev. C16, 747 (1977) D.S.Brenner, M.Lindner, R.A.Meyer Unique First Forbidden Beta Decay of 183Re and 185Os RADIOACTIVITY 183Re, 185Os; measured Eγ, Iγ, T1/2; deduced log ft. 183W, 185Re deduced levels, J, π. Ge(Li) detectors.
doi: 10.1103/PhysRevC.16.747
1977GL06 Z.Phys. A283, 415 (1977) M.D.Glascock, E.W.Schneider, W.B.Walters, R.A.Meyer The Lifetime of the 376.7-keV Level and Shape Coexistence in 111Ag RADIOACTIVITY 111mPd; measured Eγ, Iγ, γγ(t). 111Ag level deduced T1/2, J, π.
doi: 10.1007/BF01409524
1977JA04 Phys.Rev. C15, 1806 (1977) Population of 0+ States in 126Te by Decay of 126I and γ Softness in Even-Even Te Nuclei RADIOACTIVITY 126I [from 127I(n, 2n)]; measured Eγ, Iγ; deduced log ft. 126Xe, 126Te deduced levels. Ge(Li) detectors, Compton suppression.
doi: 10.1103/PhysRevC.15.1806
1977ME03 Phys.Rev. C15, 390 (1977) High-Spin Three-Quasiparticle States of 93Nb Populated in the Beta Decay of 21/2+ 93Mo-m RADIOACTIVITY 93mMo [from 90Zr(α, n), 92Zr(α, 3n)]; measured Eγ, Iγ; deduced log ft. 93Nb deduced levels, J, π. Ge(Li), Compton suppression spectrometer.
doi: 10.1103/PhysRevC.15.390
1977ME12 Phys.Rev. C16, 417 (1977) R.A.Meyer, K.V.Marsh, D.S.Brenner, V.Paar Cluster-Vibrational-Field Model for 95Mo and Levels Populated in the Decay of 95mTc, 95gTc RADIOACTIVITY 95,95mTc [from Mo(p, xn), 93Nb(α, 2n)]; measured Eγ, Iγ, I(ce), T1/2; deduced β-branching, log ft. 95Mo deduced levels, J, π, B(λ), δ. Enriched, natural targets.
doi: 10.1103/PhysRevC.16.417
1977ME15 Z.Phys. A283, 379 (1977) Evidence for the Coexistence of Shapes in Even-Mass Cd Nuclei RADIOACTIVITY 110m,110Ag, 110m,110In; measured Eγ, Iγ, γγ-coin. 110Cd deduced levels, K, J, π. 112,114Cd deduced band parameters.
doi: 10.1007/BF01409518
1977NA18 Phys.Rev. C16, 1683 (1977) Half-Life of 52Mn RADIOACTIVITY 52Mn; measured T1/2.
doi: 10.1103/PhysRevC.16.1683
1977YA08 Phys.Rev. C16, 1581 (1977) Levels of 52Cr Populated in the Decay of 52V, 52Mn-g and in the Sequence 52Fe → 52Mn-m → 52Cr RADIOACTIVITY 52Mn; measured T1/2. 52m,52Mn, 52V; measured Eγ, Iγ. 52Cr deduced levels, J, π. Compton suppression.
doi: 10.1103/PhysRevC.16.1581
1976BR09 Phys.Rev. C13, 1288 (1976) Decay of 187W and the 1/2+[411] Band in Odd-Mass Re Isotopes RADIOACTIVITY 187W [from 186W(n, γ)]; measured Eγ, Iγ, T1/2; deduced log ft. 187Re deduced levels, J, π, Nilsson assignments.
doi: 10.1103/PhysRevC.13.1288
1976BU05 Phys.Rev. C13, 1577 (1976) R.L.Bunting, W.L.Talbert, Jr., J.R.McConnell, R.A.Meyer Decays of 88Kr and 88Rb RADIOACTIVITY 88Kr, 88Rb [from 235U(n, F)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 88Rb, 88Sr deduced levels, J, π.
doi: 10.1103/PhysRevC.13.1577
1976CO06 Phys.Rev. C13, 847 (1976) Coupled Quadrupole-Octupole Excitations in 44Ca and the Decay of 44K, 44Sc-m, and 44Sc-g RADIOACTIVITY 44K, 44,44mSc; measured Eγ, Iγ, γγ-coin; deduced log ft. 44Ca deduced levels, J, π, γ-branching, T1/2. 44mSc deduced transition.
doi: 10.1103/PhysRevC.13.847
1976DE35 J.Inorg.Nucl.Chem. 38, 2135 (1976) Decay of 113Sn to Levels of 113In RADIOACTIVITY 113Sn; measured Eγ, Iγ; deduced β-branching. 113In deduced levels.
doi: 10.1016/0022-1902(76)80179-0
1976HE09 Phys.Rev. C13, 2063 (1976) Odd Parity Levels in 133La and the Particle-Plus-Triaxial-Rotor Model RADIOACTIVITY 133Ce; measured Eγ, Iγ, I(ce); deduced log ft. 133La deduced levels, J, π, ICC, λ. Enriched targets, mass separation, Ge(Li), Si(Li) detectors.
doi: 10.1103/PhysRevC.13.2063
1976HE11 Phys.Rev. C13, 2501 (1976) Decay of 3.912-h 133La to 133Ba and Level Structure of the N = 77 Nuclei RADIOACTIVITY 133La; measured Eγ, Iγ, γγ-coin; deduced log ft, ICC. 133Ba deduced levels, J, π.
doi: 10.1103/PhysRevC.13.2501
1976HI07 Phys.Rev. C13, 2512 (1976) Decay of 179Lu to Levels in the 107-Neutron Nucleus 179Hf RADIOACTIVITY 179Lu [from 180Hf(γ, p), 179Hf(n, p)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 179Hf deduced levels, J, π.
doi: 10.1103/PhysRevC.13.2512
1976HO04 Phys.Rev. C13, 434 (1976) Hindered Beta Decay of 95mNb and the Decay Sequence 95Zr → 95mNb, 95gNb → 95Mo RADIOACTIVITY 95Zr, 95m,95Nb; measured Eγ, Iγ; deduced log ft. 95Mo deduced levels.
doi: 10.1103/PhysRevC.13.434
1976JA01 Phys.Rev. C13, 339 (1976) N=85 Nuclei. I. Decay of 145Pr to Levels of 145Nd RADIOACTIVITY 145Pr [from 235U(n, F), E=thermal; 146Nd(n, p), E=14 MeV]; measured Eγ, Iγ, γγ-coin; deduced log ft. 145Nd deduced levels, J, π.
doi: 10.1103/PhysRevC.13.339
1976JA05 Phys.Rev. C13, 803 (1976); Erratum Phys.Rev. C13, 2596 (1976) S.V.Jackson, W.B.Walters, R.A.Meyer Levels in the Three-Hole Nucleus 105Ag and the Decay of 55.5-min 105Cd RADIOACTIVITY 105Cd [from 106Cd(n, 2n)]; measured Eγ, Iγ, γγ-coin, Eβ, Iβ, I(EC); deduced log ft, β/EC. 105Ag deduced levels, J, π.
doi: 10.1103/PhysRevC.13.803
1976JA07 J.Inorg.Nucl.Chem. 38, 1099 (1976) S.V.Jackson, E.A.Henry, R.A.Meyer Decay of 48Sc and 48V to Levels of 48Ti RADIOACTIVITY 48V, 48Sc; measured Eγ, Iγ, γγ-coin; deduced log ft. 48Ti deduced levels.
doi: 10.1016/0022-1902(76)80228-X
1976MA35 Phys.Rev. C14, 1141 (1976) L.G.Mann, W.B.Walters, R.A.Meyer Levels of 129I Populated in the Decay of 129mTe and 129gTe RADIOACTIVITY 129,129mTe [from 128Te(n, γ)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 129I deduced levels, J, π, B(E2). Ge(Li) detectors, enriched targets.
doi: 10.1103/PhysRevC.14.1141
1976MA37 Phys.Rev. C14, 639 (1976) E.S.Macias, M.E.Phelps, D.G.Sarantites, R.A.Meyer Decay of 39-Day 103Ru and 17-Day 103Pd to the Levels of 103Rh RADIOACTIVITY 103Ru, 103Pd; measured Eγ, Iγ, γX-ray coin, I(X-ray); deduced log ft. 103Rh deduced levels, J, π, ICC, δ, B(E2), B(M1). Ge(Li), Si(Li) detectors, anti-Compton spectrometer.
doi: 10.1103/PhysRevC.14.639
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