NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = P.Kleinheinz Found 116 matches. Showing 1 to 100. [Next]2010CA08 Phys.Rev. C 81, 031301 (2010) L.Caballero, B.Rubio, P.Kleinheinz, S.W.Yates, A.Algora, A.Dewald, A.Fitzler, A.Gadea, J.Jolie, R.Julin, A.Linnemann, S.Lunardi, R.Menegazzo, O.Moller, E.Nacher, M.Piiparinen, J.Blomqvist Two-phonon octupole excitation in 146Gd NUCLEAR REACTIONS 144Sm(α, 2n), E=26.3 MeV; measured Eγ, Iγ, γγ-coin γ(θ), and linear polarization of γ rays. 146Gd; deduced levels, J, π, multipolarity, and two-phonon octupole excitations.
doi: 10.1103/PhysRevC.81.031301
2006GA33 Phys.Rev.Lett. 97, 152501 (2006) A.Gadea, S.M.Lenzi, S.Lunardi, N.Marginean, A.P.Zuker, G.de Angelis, M.Axiotis, T.Martinez, D.R.Napoli, E.Farnea, R.Menegazzo, P.Pavan, C.A.Ur, D.Bazzacco, R.Venturelli, P.Kleinheinz, P.Bednarczyk, D.Curien, O.Dorvaux, J.Nyberg, H.Grawe, M.Gorska, M.Palacz, K.Lagergren, L.Milechina, J.Ekman, D.Rudolph, C.Andreoiu, M.A.Bentley, W.Gelletly, B.Rubio, A.Algora, E.Nacher, L.Caballero, M.Trotta, M.Moszynski Observation of 54Ni: Cross-Conjugate Symmetry in f7/2 Mirror Energy Differences NUCLEAR REACTIONS 24Mg(32S, 2n), E=75 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 54Ni deduced levels, J, π. Euroball IV, Euclides arrays. Level systematics in neighboring isobars discussed.
doi: 10.1103/PhysRevLett.97.152501
2002IS03 Eur.Phys.J. A 13, 15 (2002) T.Ishii, M.Asai, A.Makishima, I.Hossain, P.Kleinheinz, M.Ogawa, M.Matsuda, S.Ichikawa Gamma-Ray Spectroscopy of the Neutron-Rich Ni Region Through Heavy-Ion Deep-Inelastic Collisions NUCLEAR REACTIONS 198Pt(76Ge, X), E=8 MeV/nucleon; measured Eγ, (recoil)γ-coin. 68Ni deduced levels, J, π, isomeric states T1/2. 78Zn, 80Ge, 82Se, 84Kr, 86Sr, 88Zr, 90Mo, 92Ru, 94Pd; analyzed levels, transitions populated by isomer decay.
doi: 10.1007/s10050-002-8711-7
2001IS02 Acta Phys.Pol. B32, 739 (2001) T.Ishii, M.Asai, M.Matsuda, S.Ichikawa, A.Makishima, I.Hossain, P.Kleinheinz, M.Ogawa Nano-Second Isomers in Neutron-Rich Ni Region Produced by Deep-Inelastic Collisions NUCLEAR REACTIONS 198Pt(76Ge, X)64Cu/66Cu/67Cu/69Cu/66Ni/68Ni/64Co, E=8 MeV/nucleon; measured Eγ, Iγ, (fragment)γ-coin following deep-inelastic collisions. 68Ni deduced isomer T1/2, configuration. Other reactions discussed.
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2001PO18 Phys.Rev. C64, 034302 (2001) Zs.Podolyak, P.G.Bizzeti, A.M.Bizzeti-Sona, A.Gadea, S.Lunardi, D.Bazzacco, G.de Angelis, M.De Poli, D.R.Napoli, C.M.Petrache, C.Rossi Alvarez, C.A.Ur, P.Kleinheinz, J.Blomqvist Shell Model and Octupole Excitations in 147Eu NUCLEAR REACTIONS 124Sn(28Si, 4np), E=125 MeV; measured Eγ, Iγ, γγ-coin. 147Eu deduced high-spin levels, J, π, configurations. GASP array. Comparisons with neighboring nuclides, shell model predictions.
doi: 10.1103/PhysRevC.64.034302
1999AL46 Nucl.Phys. (Supplement) A654, 727c (1999) A.Algora, D.Cano-Ott, B.Rubio, J.L.Tain, J.Agramunt, J.Blomqvist, L.Batist, R.Borcea, R.Collatz, A.Gadea, J.Gerl, M.Gierlik, M.Gorska, O.Guilbaud, H.Grawe, M.Hellstrom, Z.Hu, Z.Janas, M.Karny, R.Kirchner, P.Kleinheinz, W.Liu, T.Martinez, F.Moroz, A.Plochocki, M.Rejmund, E.Roeckl, K.Rykaczewski, M.Shibata, J.Szerypo, V.Wittmann, and the German Euroball Collaboration The GT Resonance Revealed in β+-Decay using New Experimental Techniques RADIOACTIVITY 150Ho(EC), (β+), (β+α); measured Eγ, Eα, β-delayed α emission probability, β-strength. Comparison between results from a Total absorption spectrometer (NAI) and Ge detectors.
doi: 10.1016/S0375-9474(00)88536-X
1998HO15 Phys.Rev. C58, 1318 (1998) I.Hossain, T.Ishii, A.Makishima, M.Asai, S.Ichikawa, M.Itoh, M.Ishii, P.Kleinheinz, M.Ogawa Lifetime Measurement of the πg9/2 Isomer in 79As NUCLEAR REACTIONS 198Pt(76Ge, X), E=550, 635 MeV; 198Pt(74Ge, X), E=625 MeV; measured Eγ, Iγ(t), (projectile-like fragment)γ-coin; deduced isotopic yields. 79As deduced isomeric level T1/2, B(M2), configuration. Systematics of B(M2) values in neighboring isotopes discussed.
doi: 10.1103/PhysRevC.58.1318
1998IS11 Phys.Rev.Lett. 81, 4100 (1998) T.Ishii, M.Asai, I.Hossain, P.Kleinheinz, M.Ogawa, A.Makishima, S.Ichikawa, M.Itoh, M.Ishii, J.Blomqvist The (νg9/22πp3/2)19/2- Isomer in 71Cu and the Prediction of Its E2 Decay from the Shell Model NUCLEAR REACTIONS 198Pt(76Ge, X), E=635 MeV; measured Eγ, Iγ(t), γγ-, (projectile-like fragment)γ-coin, fragment spectra; deduced evidence for 71Cu. 71Cu deduced levels, J, π, isomeric state T1/2, configuration. Deep inelastic collisions. Shell model calculations.
doi: 10.1103/PhysRevLett.81.4100
1997CO21 Z.Phys. A358, 241 (1997) R.Collatz, P.Kleinheinz, B.Rubio, J.L.Tain, M.Piiparinen, H.Keller, R.Kirchner, O.Klepper, E.Roeckl, D.Schardt Gamow-Teller Strength from the β+ Decay of 66147Dy81 RADIOACTIVITY 147Dy(β+); measured Eγ, Iγ; deduced Gamow-Teller strength functions. 147Tb levels deduced feeding Iβ. Total absorption spectrometer.
doi: 10.1007/s002180050319
1997CO23 Z.Phys. A359, 113 (1997) R.Collatz, N.Amzal, Z.Meliani, C.Schuck, Ch.Vieu, J.S.Dionisio, P.Kleinheinz, J.Blomqvist Yrast States in the π-Particle ν-Hole Nucleus 65146Tb81 NUCLEAR REACTIONS 120Sn(31P, 5n), E=150 MeV; measured Eγ, Iγ; 144Sm(6Li, 4n), E=50 MeV; measured Eγ, Iγ, γγ-, (ce)γ-coin. 146Tb deduced levels, J, π, configurations.
doi: 10.1007/s002180050374
1997CO24 Z.Phys. A359, 115 (1997) R.Collatz, P.Kleinheinz, C.T.Zhang, H.Keller, R.Kirchner, O.Klepper, E.Roeckl Gamma-Decay of the (27/2)- 0.6s E3-Isomer in 68151Er83 RADIOACTIVITY 151mEr(IT) [from 96Mo(58Ni, n2p), E=4.4 MeV/nucleon]; measured Eγ, Iγ, γγ-coin, I(ce). 151Er deduced levels, J, π, configurations. Other N=83 nuclei compared.
doi: 10.1007/s002180050375
1997GA22 Z.Phys. A358, 205 (1997) L.M.Garcia-Raffi, B.Rubio, J.L.Tain, J.Bea, A.Gadea, J.Rico, P.Kleinheinz, R.Menegazzo, R.Wirowski, P.von Brentano, G.Siems, A.Dewald Particle-Quadrupole and Particle-Octupole Coupled States in 145Sm NUCLEAR REACTIONS 142Nd(α, n), E=24.5 MeV; measured Eγ, γγ-coin, Iγ(θ), polarization. 145Sm deduced levels, J, π, configurations.
doi: 10.1007/s002180050309
1996GA24 Z.Phys. A355, 253 (1996) A.Gadea, B.Rubio, J.L.Tain, J.Rico, J.Bea, L.M.Garcia-Raffi, P.Kleinheinz, D.Schardt, E.Roeckl, R.Kirchner, J.Blomqvist Properties of the 69150Tm81 6- β-Decaying Isomer RADIOACTIVITY 148Ho, 150Tm(β-) [from 96Ru, 94Mo(58Ni, X), E=5 MeV/nucleon]; measured γγ-, (X-ray)γ-coin. 148Dy, 150Er deduced levels, J, π, configuration ICC, γ multipolarity. Shell model.
doi: 10.1007/s002180050107
1996ZH09 Phys.Rev. C54, R1 (1996) C.T.Zhang, P.Kleinheinz, M.Piiparinen, R.Broda, R.Collatz, P.J.Daly, K.H.Maier, R.Menegazzo, G.Sletten, J.Styczen, J.Blomqvist Complete Valence Particle Yrast Lines in N = 84 Nuclei Above Gadolinium NUCLEAR STRUCTURE 151Ho, 153Tm, 152Er, 154Yb, 149Tb, 150Dy; calculated levels. Parameter-free shell model, empirical one-, two-body matrix elements.
doi: 10.1103/PhysRevC.54.R1
1995CO12 Z.Phys. A351, 245 (1995) R.Collatz, P.Kleinheinz, C.T.Zhang, A.F.Saad, C.Vieu, J.S.Dionisio, C.Schuck, M.Wilhelm, P.von Brentano, R.Wirowski, J.Blomqvist Particle x Phonon Multiplets in 65147Tb82 NUCLEAR REACTIONS 144Sm(6Li, 3n), E=29 MeV; measured γγ-coin, I(ce). 147Tb deduced levels, J, π, configuration. Other data input.
doi: 10.1007/BF01290904
1995SA31 Z.Phys. A351, 247 (1995) A.F.Saad, C.T.Zhang, R.Collatz, P.Kleinheinz, R.Menegazzo, R.Broda, K.H.Maier, H.Grawe, M.Schramm, R.Schubart, M.Lach, J.Heese, J.Eberth, W.Krolas, S.Hofmann, H.Folger, J.Blomqvist Shell Model Yrast States in the Many-Particle Nucleus 72157Hf85 NUCLEAR REACTIONS 106Cd(54Fe, n2p), E=255 MeV; 102Pd(58Ni, n2p), E > Coulomb barrier; measured γγ-, γγn-, γ(X-ray)-coin. 157Hf deduced high-spin levels, J, π, configuration, isomer, T1/2. Shell model comparison.
doi: 10.1007/BF01290905
1994BR02 Phys.Rev. C49, R575 (1994) R.Broda, C.T.Zhang, P.Kleinheinz, R.Menegazzo, K.-H.Maier, H.Grawe, M.Schramm, R.Schubart, M.Lach, S.Hofmann Collisions between 106Cd and 54Fe at 30 MeV Above the Coulomb Barrier by High Resolution γγ Coincidences NUCLEAR REACTIONS 106Cd(54Fe, X), E=247 MeV; measured γγ-coin, Eγ, Iγ; deduced fusion evaporation σ(Z, N), charge equilibration, relative angular momentum transfer.
doi: 10.1103/PhysRevC.49.R575
1994ME13 Z.Phys. A349, 13 (1994) R.Menegazzo, P.Kleinheinz, R.Collatz, H.Guven, J.Styczen, D.Schardt, H.Keller, O.Klepper, G.Walter, A.Huck, G.Marguier, J.Blomqvist, and the ISOLDE Collaboration The N = 83 Nucleus 149Dy from Gamow-Teller Decay of Its (11/2)- and (1/2)+ 149Ho Parents RADIOACTIVITY 149Ho(β+) [from 94,95Mo(58Ni, X), E=5-4 MeV/nucleon]; measured γγ-, γ(X-ray)-coin; deduced (1/2)+, (11/2)- level decay, T1/2. 149Dy deduced Gamow-Teller decay strength, levels, configuration.
doi: 10.1007/BF01296328
1994ZH08 Z.Phys. A348, 65 (1994) C.T.Zhang, P.Kleinheinz, M.Piiparinen, R.Collatz, T.Lonnroth, G.Sletten, J.Blomqvist Shell Model High-Spin States in 15167Ho84 NUCLEAR REACTIONS 127I(29Si, 5n), E=145 MeV; measured γγ-coin. 151Ho deduced high-spin levels, J, π, configuration, ICC.
doi: 10.1007/BF01291657
1994ZH18 Z.Phys. A348, 249 (1994) C.T.Zhang, P.Kleinheinz, M.Piiparinen, R.Collatz, T.Lonnroth, G.Sletten, J.Blomqvist Seniority Inverted Yrast States Observed in 15369Tm84 NUCLEAR REACTIONS 122Te(35Cl, 4n), E=174 MeV; measured γγ-coin. 153Tm deduced high-spin levels, J, π, band structure, configuration.
doi: 10.1007/BF01305879
1993LA10 Z.Phys. A345, 427 (1993) M.Lach, P.Kleinheinz, J.Blomqvist, A.Ercan, H.J.Hahn, D.Wahner, R.Julin, M.Zupancic, F.Cigoroglu, G.de Angelis Shell Model Yrast States in the N = 79 Nuclei 141Sm and 143Gd NUCLEAR REACTIONS 142Nd, 144Sm(α, 5n), E=77, 80 MeV; measured Eγ, Iγ, γ(θ), I(ce), γγ-coin. 144Sm(α, 6n), E=95 MeV; measured γγ-coin. 141Sm, 143Gd deduced levels, J, π, band structure, configuration. Shell model.
doi: 10.1007/BF01282905
1993PI01 Phys.Rev.Lett. 70, 150 (1993) M.Piiparinen, P.Kleinheinz, J.Blomqvist, A.Virtanen, A.Atac, D.Muller, J.Nyberg, T.Ramsoy, G.Sletten Two- to One -Phonon E3 Transition Strength in 148Gd NUCLEAR REACTIONS 133Cs(19F, 4n), E=73.5 MeV; measured Eγ, Iγ, decay time. 148Gd deduced levels, J, π, mean T1/2, B(λ), configuration.
doi: 10.1103/PhysRevLett.70.150
1993RI07 Z.Phys. A345, 245 (1993) J.Rico, B.Rubio, J.L.Tain, A.Gadea, J.Bea, L.M.Garcia-Raffi, O.Tengblad, P.Kleinheinz, R.Menegazzo, R.Wirowski, P.von Brentano, G.Siems, J.Blomqvist Two-Proton Multiplets in the N = 82 Nucleus 14462Sm82 from In-Beam γ-Measurements NUCLEAR REACTIONS 142Nd(α, 2n), E=24.5 MeV; measured γ spectra. 144Sm deduced levels, J, π, configurations. High sensitivity in-beam study.
doi: 10.1007/BF01293352
1993ZH10 Z.Phys. A345, 327 (1993) C.T.Zhang, R.Broda, R.Menegazzo, P.Kleinheinz, R.Collatz, H.Grawe, S.Hofmann, M.Lach, K.H.Maier, M.Schramm, R.Schubart, J.Blomqvist Energy Inversion of the f7/2 and h9/2 Neutrons in Yrast States of 154Yb NUCLEAR REACTIONS 106Cd(54Fe, 2pα), E=4.7 MeV/nucleon; measured γγ(t). 154Yb deduced levels, J, π, configuration. Shell model.
doi: 10.1007/BF01280841
1991KE06 Nucl.Instrum.Methods Phys.Res. A300, 67 (1991) H.Keller, R.Kirchner, O.Klepper, E.Roeckl, D.Schardt, R.S.Simon, P.Kleinheinz, C.F.Liang, P.Paris A Summation-Free β+-Endpoint Spectrometer RADIOACTIVITY 149mTb [from 94,95Mo(58Ni, X), E=5.3 MeV/nucleon]; measured β+γ-coin; deduced β+-endpoint energy. Summation-free β+-endpoint spectrometer.
doi: 10.1016/0168-9002(91)90707-W
1991KE11 Z.Phys. A340, 363 (1991) H.Keller, R.Kirchner, O.Klepper, E.Roeckl, D.Schardt, R.S.Simon, P.Kleinheinz, R.Menegazzo, C.F.Liang, P.Paris, K.Rykaczewski, J.Zylicz β+-Endpoint Measurements Near 100Sn and 146Gd RADIOACTIVITY 104Sn, 147Tb, 148,149Dy, 149Ho, 150Er, 151Tm(β+); measured γ-spectra, Eβ; deduced Q(EC). 104Sn deduced mass excess. Other nuclei discussed.
doi: 10.1007/BF01290323
1991LA17 Z.Phys. A341, 25 (1991) M.Lach, P.Kleinheinz, M.Piiparinen, M.Ogawa, S.Lunardi, M.C.Bosca, J.Styczen, J.Blomqvist Multiparticle- and Particle x Octupole States in 14965Tb84 NUCLEAR REACTIONS 151Eu(α, 6n), E=78 MeV; 144Sm(7Li, 2n), E=32 MeV; measured γγ-coin, Eγ, Iγ, γ-polarization, DCO ratios, γ(θ). 149Tb deduced levels, J, π, configuration, band structure.
doi: 10.1007/BF01281271
1991PI06 Z.Phys. A338, 417 (1991) M.Piiparinen, Y.Nagai, P.Kleinheinz, M.C.Bosca, B.Rubio, M.Lach, J.Blomqvist Three-Nucleon Yrast States in 145Sm NUCLEAR REACTIONS 145Nd(α, 4n), E=55 MeV; measured γγ-coin. 145Sm deduced levels, J, π, γ-multipolarity, ICC. Shell model calculations.
doi: 10.1007/BF01295769
1990DE22 Z.Phys. A336, 375 (1990) G.de Angelis, P.Kleinheinz, B.Rubio, J.L.Tain, K.Zuber, B.Brinkmoller, P.von Rossen, J.Romer, D.Paul, J.Meissburger, G.P.A.Berg, A.Magiera, G.Hlawatsch, L.G.Mann, T.N.Massey, D.Decman, G.L.Struble, J.Blomqvist Collective Excitations in 148Gd Populated in the pp'-Reaction on a Radioactive Target NUCLEAR REACTIONS 148Gd(p, p'), E=25 MeV; measured σ(Ep'), σ(θ). 148Gd deduced levels, B(λ), configuration, J, π. DWBA analysis.
1990MA68 Z.Phys. A337, 301 (1990) L.G.Mann, D.J.Decman, H.E.Martz, T.N.Massey, G.L.Struble, P.Kleinheinz, H.J.Scheerer, D.G.Burke, G.Kajrys Occupancy of Single-Proton Orbitals in 148Gd NUCLEAR REACTIONS 148Gd(3He, d), E=30 MeV; 148Gd(t, α), E=18 MeV; measured σ(θ), σ(Ed), σ(Eα); deduced model parameters. 149Tb levels deduced L, spectroscopic factors. 147Eu deduced levels, L, spectroscopic factors. 148Gd deduced ground state proton pair probability. DWBA analysis.
1990PI17 Z.Phys. A337, 387 (1990) M.Piiparinen, P.Kleinheinz, S.Lunardi, M.Ogawa, G.de Angelis, F.Soramel, W.Meczynski, J.Blomqvist Shell Model and Octupole States in 148Gd from In-Beam Experiments NUCLEAR REACTIONS 148Sm(α, 4n), E=54 MeV; 148Sm(3He, 3n), E=27 MeV; 124Sn(28Si, 4n), E=125 MeV; measured Eγ, Iγ, I(ce), γγ-coin, γ(θ). 148Gd deduced levels, J, π, ICC, γ-multipolarity, B(λ), ratios, T1/2, configurations. Model, other nuclei comparisons.
1989GA11 Z.Phys. A333, 407 (1989) A.Gadea, B.Rubio, J.L.Tain, P.Kleinheinz, C.F.Liang, P.Paris Quasiparticle States in 152Dy Observed in β-Decay of 9+ and 2- 152Ho RADIOACTIVITY 152Ho(β+), (EC) [from 159Tb(3He, 10n), E=280 MeV]; measured γγ-, γ(X-ray)-coin, I(ce). 152Dy deduced levels, J, π, configuration.
1989KA21 Phys.Lett. 227B, 325 (1989) H.Kader, G.Graw, F.J.Eckle, G.Eckle, P.Schiemenz, P.Kleinheinz, B.Rubio, G.de Angelis, T.N.Massey, L.G.Mann, J.Blomqvist Particle-Octupole Coupling in N = 83 Nuclei from Neutron Transfer Studies with Polarized Deuterons NUCLEAR REACTIONS 148Gd, 146Sm(polarized d, t), E=22 MeV; 144Nd(polarized d, t), E=20 MeV; measured σ(θ). 147Gd, 145Sm, 143Nd deduced level, J, π, configuration. Radioactive targets from Ta(p, X) reaction.
doi: 10.1016/0370-2693(89)90938-6
1989ME13 Z.Phys. A334, 525 (1989) R.Menegazzo, H.Guven, J.Styczen, N.Roy, P.Kleinheinz, D.Schardt, R.Barden, G.Walter, A.Huck, G.Marguier, J.Blomqvist, and the ISOLDE Collaboration Gamow-Teller Strength and Particle-Phonon States in 149Dy from Decay of Its (11/2)- and (1/2)+ 149Ho Parents RADIOACTIVITY 149Ho(β+), (EC); measured I(ce). 149Dy deduced levels, J, π, configuration, Gamow-Teller transition strength distribution. Other data input.
1989TA11 Z.Phys. A333, 29 (1989) J.L.Tain, B.Rubio, P.Kleinheinz, D.Schardt, R.Barden, J.Blomqvist Two-Nucleon Excitations in 66148Dy82 from Gamow-Teller Decay of the 67148Ho81 6- Isomer RADIOACTIVITY 148Ho(EC) [from 96Ru, 92,94Mo, 93Nb(58Ni, X), E=5 MeV/nucleon]; measured Eγ, Iγ, γ(X-ray), γγ-coin; deduced isomer T1/2, configuration. 148Dy deduced levels, J, π, T1/2, configurations.
1989WO06 Z.Phys. A333, 413 (1989) H.Wolters, W.Ott, R.Wirowski, A.Dewald, J.Theuerkauf, J.Eberth, K.O.Zell, P.von Brentano, W.Gast, G.Hebbinghaus, P.Kleinheinz, A.Kramer-Flecken, R.M.Lieder, T.Morek, T.Rzaca-Urban, H.Schnare, C.Senff, W.Urban, H.Grawe, H.Kluge, K.H.Maier, S.Heppner, H.Hubel, A.P.Byrne, W.Schmitz High Spin States in Doubly-Closed Shell Nucleus 146Gd NUCLEAR REACTIONS 110Pd(40Ar, 4n), 102Ru(48Ca, 4n), E not given; measured γγ-coin. 146Gd deduced levels, J, π.
1988BA02 Z.Phys. A329, 11 (1988) R.Barden, A.Plochocki, D.Schardt, B.Rubio, M.Ogawa, P.Kleinheinz, R.Kirchner, O.Klepper, J.Blomqvist Beta-Decay of 27/2- Isomers in N = 83 Nuclei NUCLEAR REACTIONS 96Mo(58Ni, n2p), (64Zn, n4p), E=5 MeV/nucleon; measured Eγ, Iγ, γγ-coin. 151Er deduced isomer T1/2, decay features, IT to β-decay branching, B(E3), levels, J, π, γ-multipolarity. 90Zr(64Zn, n4p), 89Y(64Zn, n3p), E=5 MeV/nucleon; measured Eγ, Iγ. 149Dy deduced isomer decay characteristics, β-branching, log ft. 151Ho deduced levels, J, π, γ-multipolarity. 92Mo(64Zn, n2p), E=5 MeV/nucleon; measured Eγ, Iγ, E X-ray, I X-ray. 153Yb deduced T1/2, no E3 isomer. RADIOACTIVITY 151mEr [from 96Mo(58Ni, n2p), (64Zn, n4p), E=5 MeV/nucleon]; measured Eγ, Iγ, γγ-coin; deduced isomer T1/2, decay characteristics, IT to β-decay branching, B(E3). 151Ho deduced levels, J, π, γ-multipolarity. 149mDy [from 90Zr(64Zn, n4p), 89Y(64Zn, n3p), E=5 MeV/nucleon]; measured Eγ, Iγ; deduced isomer decay characteristics, β-branching, log ft.
1988ER02 Z.Phys. A329, 63 (1988) A.Ercan, R.Broda, P.Kleinheinz, M.Piiparinen, R.Julin, J.Blomqvist The Two Particle-Phonon Multiplet (πh11/2νf7/2)x3- and Higher-Lying Four-Nucleon Yrast States in the Doubly-Odd Nucleus 63146Eu83 NUCLEAR REACTIONS 147Sm(α, 4np), E=76 MeV; measured Eγ, Iγ, γ(θ). 146Eu deduced levels, J, π, B(λ), configurations, γ-multipolarity. Model calculations.
1988GU09 Z.Phys. A330, 437 (1988) H.Guven, R.Julin, M.Lach, J.Styczen, M.Muller-Veggian, A.Kramer-Flecken, P.Kleinheinz Proton- and Neutron h11/2 Excitations in 63141Eu78 NUCLEAR REACTIONS 144Sm(α, 6np), E=95, 107 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), oriented nuclei. 141Eu deduced levels, J, π, configuration.
1988LO04 Nucl.Phys. A481, 71 (1988) G.Lovhoiden, S.El-Kazzaz, J.R.Lien, K.Heyde, J.Rekstad, C.Ellegaard, J.H.Bjerregaard, P.Knudsen, P.Kleinheinz Study of High-Spin Hole States in 143Nd NUCLEAR REACTIONS 144Nd(3He, α), E=24 MeV; measured σ(E(α), θ). 143Nd deduced levels, L, J, π, S. Enriched target. Unified model calculations.
doi: 10.1016/0375-9474(88)90473-3
1988MU12 Z.Phys. A330, 343 (1988) M.Muller-Veggian, K.Zuber, H.Guven, G.de Angelis, J.Styczen, M.Lach, G.Hebbinghaus, P.Kleinheinz In-Beam Study of 63143Eu80 NUCLEAR REACTIONS 144Sm(α, 4np), E=95 MeV; measured γγ-coin, Eγ, Iγ, γ(θ). 143Eu deduced levels, J, π, γ-multipolarity.
1988ST02 Phys.Lett. 200B, 419 (1988) W.Starzecki, G.de Angelis, B.Rubio, J.Styczen, K.Zuber, H.Guven, W.Urban, W.Gast, P.Kleinheinz, S.Lunardi, F.Soramel, A.Facco, C.Signorini, M.Morando, W.Meczynski, A.M.Stefanini, G.Fortuna Prolate and Oblate 10+ Isomers in 140Sm78 and 142Gd78 NUCLEAR REACTIONS 142Nd(α, 6n), E=95 MeV; 110Cd(35Cl, 2np), E=148 MeV; measured Eγ, Iγ, γγ-coin, T1/2. 140Sm, 142Gd deduced levels, J, π, B(E2).
doi: 10.1016/0370-2693(88)90145-1
1987HE16 Phys.Rev.Lett. 59, 2024 (1987) G.Hebbinghaus, T.Rzaca-Urban, C.Senff, R.M.Lieder, W.Gast, A.Kramer-Flecken, H.Schnare, W.Urban, G.de Angelis, P.Kleinheinz, W.Starzecki, J.Styczen, P.von Brentano, A.Dewald, J.Eberth, W.Lieberz, T.Mylaeus, A.v.d.Werth, H.Wolters, K.O.Zell, S.Heppner, H.Hubel, M.Murzel, H.Grawe, H.Kluge Observation of Superdeformation in the Doubly Closed-Shell Nucleus 146Gd NUCLEAR REACTIONS 110Pd(40Ar, X), E=180 MeV; measured γγ-energy correlation, DSA. 146Gd deduced levels, moment of inertia, deformation, superdeformation characteristics, quadrupole moment, stretched E2 transitions.
doi: 10.1103/PhysRevLett.59.2024
1987LI09 Phys.Lett. 191B, 245 (1987) C.F.Liang, P.Paris, P.Kleinheinz, B.Rubio, M.Piiparinen, D.Schardt, A.Plochocki, R.Barden Relative Energies of the πh11/2 and πs1/2 β-Decay Isomers RADIOACTIVITY 147Tb(β+) [from 151Ho decay]; 151Ho(β+), (α) [from 159Tb(3He, 11n), E=280 MeV]; measured Eα, Eγ, αγ-coin. 147Tb, 151Ho deduced isomers, T1/2, J, π. Ge(Li), Si detectors.
doi: 10.1016/0370-2693(87)90248-6
1987ST15 Z.Phys. A327, 481 (1987) J.Styczen, R.Menegazzo, W.Starzecki, P.Kleinheinz γ-Rays Draining the Superdeformed Band in 152Dy NUCLEAR REACTIONS 152Gd(α, 4n), E=60 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 152Dy deduced levels, J, π, γ-branching, γ multipolarity, superdeformed band.
1987ZU02 Z.Phys. A327, 357 (1987) K.Zuber, C.F.Liang, P.Paris, J.Styczen, J.Zuber, P.Kleinheinz, B.Rubio, G.de Angelis, H.Gabelmann, A.Huck, J.Blomqvist, and the ISOLDE Collaboration Gamow-Teller Transitions in β-Decay of 66146Dy80 RADIOACTIVITY 146Dy(β-) [from Gd(3He, xn), E=280 MeV]; measured Eγ, Iγ, E X-ray, I X-ray, γγ-, γ(X-ray)-coin, I(ce); deduced log ft. 146Tb deduced levels, J, π, configuration, γ multipolarity, Gamow-Teller transition characteristics.
1986LU07 Z.Phys. A324, 433 (1986) S.Lunardi, F.Soramel, W.Starzecki, W.Meczynski, R.Julin, M.Lach, A.Ercan, P.Kleinheinz First Observation of Yrast γ-Rays in the N = 78 Nuclei 142Gd and 141Eu NUCLEAR REACTIONS, ICPND 142Nd, 144Sm(α, 6n), (α, 6np), (α, 5n), (α, 4n), (α, 3n), (α, 2n), E=65-107 MeV; measured Eγ, Iγ, σ(E), σ(θ), γ(θ), γγ-coin. 110Cd(35Cl, 2np), (35Cl, 2n2p), E=138 MeV; 112Cd(32S, 2np), (32S, 2n2p), E=132 MeV; 106Pd(37Cl, 2np), (37Cl, 2n2p), (37Cl, 2n), E=148 MeV; measured Eγ, Iγ, γγ-coin. 145Tb, 144Gd, 143Eu deduced exit channel σ ratio. 141Eu, 142Gd deduced levels, yrast cascade. Ge detectors.
1986RU04 Z.Phys. A324, 27 (1986) B.Rubio, A.Ercan, G.de Angelis, P.Kleinheinz, J.L.Tain, B.Brinkmoller, D.Paul, J.Meissburger, L.G.Mann, D.J.Decman, T.N.Massey, G.L.Struble, H.J.Scheerer, J.Blomqvist The Ground State Mass of 147Gd from Single-Neutron-Transfer Reactions and Its Impact on Derived Mass Values NUCLEAR REACTIONS 148Gd(p, d), E=25 MeV; 148Gd(d, t), E=22 MeV; 148Gd(3He, α), E=30 MeV; measured σ(Ed), σ(Et), σ(Eα); deduced Q-value differences. 147Gd deduced mass. 148Gd deduced neutron separation energy. Shell model comparison.
1986YA06 Z.Phys. A324, 417 (1986) S.W.Yates, R.Julin, P.Kleinheinz, B.Rubio, L.G.Mann, E.A.Henry, W.Stoffl, D.J.Decman, J.Blomqvist Particle-Hole Multiplets in 146Gd from In-Beam Studies of Non-Yrast Levels NUCLEAR REACTIONS, ICPND 144Sm(α, 2n), E=23-28 MeV; measured σ(E), Eγ, Iγ, γ(θ), I(ce), γγ-coin. 146Gd deduced levels, γ-multipolarity, ICC, γ-branching, J, π. Ge(Li) detectors, coincidence measurements.
1985KL05 Phys.Rev.Lett. 55, 2664 (1985) P.Kleinheinz, K.Zuber, C.Conci, C.Protop, J.Zuber, C.F.Liang, P.Paris, J.Blomqvist Giant Gamow-Teller Excitation of 148Dy Populated in β+ Decay RADIOACTIVITY 148Dy(EC), (β+) [from Gd(3He, xn), E=240 MeV]; measured γγ-, (X-ray)γ-coin, I(ce); deduced log ft. 148Tb deduced levels, J, π, γ-branching, Gamow-Teller transition strength, ICC, configurations.
doi: 10.1103/PhysRevLett.55.2664
1985KL10 Z.Phys. A322, 705 (1985) P.Kleinheinz, B.Rubio, M.Ogawa, M.Piiparinen, A.Plochocki, D.Schardt, R.Barden, O.Klepper, R.Kirchner, E.Roeckl Beta-Decay of 151Yb RADIOACTIVITY 151Yb(β+) [from 96Ru(56Ni, n2p)]; measured Eγ, Iγ, E X-ray, I X-ray, γ(X-ray)-coin. 151Tm deduced levels, J, π, isomer, T1/2, γ-branching, γ-multipolarity.
doi: 10.1007/BF01415157
1984KL08 Nuovo Cim. 81A, 140 (1984) In-Beam Studies of the Shell Model Nuclei around 146Gd NUCLEAR STRUCTURE 152Dy; analyzed levels, band structure; deduced yrast line, deformed shape coexistence. Discussed other nuclear systematics.
doi: 10.1007/BF02724160
1984LA29 Z.Phys. A319, 235 (1984) M.Lach, J.Styczen, R.Julin, M.Piiparinen, H.Beuscher, P.Kleinheinz, J.Blomqvist The 10+ States of (νh11/2)-2 and (πh11/2)2 Character in the N = 80 Isotones 144Gd and 142Sm NUCLEAR REACTIONS 144Sm(α, 4n), 142Nd(3He, 3n), E not given; measured γγ-coin, σ(Eγ, E), γ(θ). 144Gd, 142Sm deduced levels, γ-branching, isomer T1/2, J, π, B(λ), configuration.
doi: 10.1007/BF01415638
1984LU09 Phys.Rev.Lett. 53, 1531 (1984) S.Lunardi, P.Kleinheinz, M.Piiparinen, M.Ogawa, M.Lach, J.Blomqvist Single- and Double-Octupole Excitations in 148Gd NUCLEAR REACTIONS 148Sm(α, 4n), (3He, 3n), E not given; measured σ(Eγ, E), γ(θ), γγ-coin, I(ce). 148Gd deduced levels, J, π, octupole T1/2, B(E3), configuration, B(λ), γ-branching.
doi: 10.1103/PhysRevLett.53.1531
1983BL04 Z.Phys. A312, 27 (1983) J.Blomqvist, P.Kleinheinz, P.J.Daly Atomic Masses above 146Gd Derived from a Shell Model Analysis of High Spin States NUCLEAR STRUCTURE 146,147,148Gd, 145Sm, 145,146Eu, 147,148,149Tb, 148,149,150Dy, 149,150Ho, 150,151,152Er; analyzed high spin data. 146,147Gd, 144,145Sm; analyzed ground state mass, α-decay mass difference data. 145,146Eu, 147,148Tb, 148,149Dy, 149,150Ho, 150,151Er deduced ground state masses. Shell model.
doi: 10.1007/BF01411658
1983SO13 Z.Phys. A314, 127 (1983) F.Soramel-Stanco, R.Julin, J.Styczen, P.T.Prokofjev, A.Ercan, P.Kleinheinz A 45 ns 8+ Isomer in the Doubly Odd 150Eu Nucleus NUCLEAR REACTIONS 152Sm(p, 3n), E=29 MeV; measured Eγ, Iγ, I(ce), γγ(t). 150Eu deduced levels, J, π, ICC, δ, γ-branching.
1983ST03 Phys.Rev.Lett. 50, 1752 (1983) J.Styczen, Y.Nagai, M.Piiparinen, A.Ercan, P.Kleinheinz Deformed Ground-Band States in the N = 86 Nucleus 152Dy NUCLEAR REACTIONS 152Gd(α, 4n), E=60 MeV; measured γγ-coin, γ(θ), I(ce). 156Dy deduced levels, J, π, isomer, γ-multipolarities, γ-branching, backbending characteristics, configurations.
doi: 10.1103/PhysRevLett.50.1752
1983ST07 Z.Phys. A312, 149 (1983) J.Styczen, M.Piiparinen, Y.Nagai, P.Kleinheinz, D.Bazzacco, J.Eberth, J.Blomqvist Seniority-Three Yrast States in the N = 82 Nucleus 147Tb NUCLEAR REACTIONS 144Sm(6Li, 3n), E=22-32 MeV; measured Eγ, Iγ, σ(Eγ), I(ce), γ(θ). 147Tb deduced levels, J, π, γ-branching, γ-multipolarity, configuration.
doi: 10.1007/BF01412157
1982BR13 Z.Phys. A305, 281 (1982) R.Broda, P.Kleinheinz, S.Lunardi, J.Styczen, J.Blomqvist The Decay of the 560 ns Isomer at 8.6 MeV in 14764Gd83 NUCLEAR REACTIONS 140Ce(12C, 5n), E=96 MeV; 148Sm(α, 5n), E=76 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 147Gd deduced isomer decay, levels, J, π, γ-branching, configuration.
doi: 10.1007/BF01419074
1982KL04 Phys.Rev.Lett. 48, 1457 (1982) P.Kleinheinz, J.Styczen, M.Piiparinen, J.Blomqvist, M.Kortelahti Two-Phonon Octupole Excitation in 147Gd RADIOACTIVITY 147Gd [from 147Sm(3He, 3n), E=22, 27 MeV]; measured I(ce), ce(t). 147Gd level deduced T1/2, γ-branching ratio, B(E3), configuration. Si-Li, magnetic lens spectrometers.
doi: 10.1103/PhysRevLett.48.1457
1981KL05 Phys.Scr. 24, 236 (1981) Yrast Octupole Excitations in the 146Gd Region NUCLEAR STRUCTURE 148,149,150,151Dy, 147Gd; calculated yrast line octupole excitations. Particle-phonon exchange coupling.
doi: 10.1088/0031-8949/24/1B/018
1981NA10 Phys.Rev.Lett. 47, 1259 (1981) Y.Nagai, J.Styczen, M.Piiparinen, P.Kleinheinz, D.Bazzacco, P.V.Brentano, K.O.Zell, J.Blomqvist Proton Single-Particle States above Z = 64 NUCLEAR REACTIONS 144Sm(6Li, 3n), E=30 MeV; measured Eγ, Iγ, γ(θ), γγ-, γ(X-ray)-coin, σ(Eγ), I(ce). 147Tb deduced levels, J, π, γ-multipolarity, T1/2 limit, ICC.
doi: 10.1103/PhysRevLett.47.1259
1981PI09 Z.Phys. A300, 133 (1981) M.Piiparinen, R.Pengo, Y.Nagai, E.Hammaren, P.Kleinheinz, N.Roy, L.Carlen, H.Ryde, Th.Lindblad, A.Johnson, S.A.Hjorth, J.Blomqvist High Spin Shell Model Excitations in 149Gd NUCLEAR REACTIONS 150Sm(α, 5n), E=67 MeV; 149Sm(α, 4n), E=51 MeV; 148Sm(α, 3n), E=44 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, linear polarization, I(ce). 149Gd deduced levels, J, π, configuration, ICC, γ-branching, T1/2, B(E2). Shell model.
doi: 10.1007/BF01412290
1981PI10 Z.Phys. A301, 231 (1981) M.Piiparinen, R.Broda, Y.Nagai, P.Kleinheinz, A.Pakkanen The 235 ns 9+ Isomer in 14863Eu85 NUCLEAR REACTIONS 149Sm(p, 2n), E=17 MeV; 150Sm(p, 3n), E=31 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, I(ce). 148Eu deduced levels, isomer T1/2, J, π, ICC, γ-multipolarity, B(M2), configurations.
doi: 10.1007/BF01416298
1980DA18 Z.Phys. A298, 173 (1980) P.J.Daly, P.Kleinheinz, R.Broda, S.Lunardi, H.Backe, J.Blomqvist Proton h211/2 and Octupole Excitations in 14866Dy82 and 14966Dy83 NUCLEAR REACTIONS 152Gd(α, xn), E=70-100 MeV; 136Ce(16O, xn), E=85-95 MeV; measured Eγ, Iγ, γγ-coin, I(ce). 148,149Dy deduced levels, T1/2, J, π, ICC, configuration, γ-multipolarity, yrast cascades.
doi: 10.1007/BF01418655
1980ER04 Z.Phys. A295, 197 (1980) A.Ercan, R.Broda, M.Piiparinen, Y.Nagai, R.Pengo, P.Kleinheinz The 235 μs 9+ Isomer in 146Eu NUCLEAR REACTIONS 147Sm(p, 2n), E=19-22 MeV; measured I(ce), Eγ, Iγ, γγ-coin with, without pulsed beam. 146Eu deduced levels, γ-branching, multipolarity, J, π, configuration.
doi: 10.1007/BF01413077
1980JU04 Phys.Lett. B94, 123 (1980) R.Julin, J.Kantele, M.Lountama, A.Passoja, P.Kleinheinz, J.Blomqvist Electromagnetic Decay of the 0+2 State in the Doubly Closed Shell Nucleus 14664Gd82 NUCLEAR REACTIONS 144Sm(3He, n), E=14-27 MeV; measured I(ce), Eγ, Iγ, (ce)(3He)(t). 146Gd deduced level, T1/2, J, π, γ-multipolarity.
doi: 10.1016/0370-2693(80)90839-4
1980KL09 J.Phys.(Paris), Colloq.C-10, 43 (1980) Particle Octupole Exchange Coupling in the Yrast Lines of Terbium and Dysprosium Nuclei NUCLEAR STRUCTURE 147Tb, 148Dy; analyzed yrast transition data. Particle octupole exchange coupling.
1980LO06 Nucl.Phys. A339, 477 (1980) G.Lovhoiden, J.R.Lien, S.El-Kazzaz, J.Rekstad, C.Ellegaard, J.H.Bjerregaard, P.Knudsen, P.Kleinheinz Studies of Single Neutron Holes in the Transitional Nuclei N = 83-89: The 150,148Nd(d, t) and 150,148,146Nd(3He, α) Pick-up Reactions NUCLEAR REACTIONS 148,150Nd(d, t), E=17 MeV; measured σ(Et, θ). 146,148,150Nd(3He, α), E=24 MeV; measured σ(Eα, θ). 145,147,149Nd deduced levels, L, J. Enriched targets.
doi: 10.1016/0375-9474(80)90028-7
1980NA04 Z.Phys. A296, 91 (1980) Y.Nagai, J.Styczen, M.Piiparinen, P.Kleinheinz The X- (Or Δ) Transition in 152Dy RADIOACTIVITY 152Dy [from 152Gd(α, 4n), E=60 MeV]; measured γγ-coin, T1/2, I(K X-ray)/Iγ, I(L X-ray)/Iγ, Eγ, Iγ; deduced low-energy isomeric E2 transitions, yrast states.
doi: 10.1007/BF01415621
1980RE05 Nucl.Phys. A348, 93 (1980) J.Rekstad, G.Lovhoiden, J.R.Lien, S.El Kazzaz, C.Ellegaard, J.Bjerregaard, P.Knudsen, P.Kleinheinz Studies of Single-Neutron Holes in the Transitional Nuclei N = 83-89: The 148,150,152Sm(3He, α) pick-up reactions NUCLEAR REACTIONS 148,150,152Sm(3He, α), E=24 MeV; measured σ(Eα, θ). 147,149,151Sm deduced levels, L, π, S. Enriched targets.
doi: 10.1016/0375-9474(80)90547-3
1979BR28 Z.Phys. A293, 135 (1979) R.Broda, M.Behar, P.Kleinheinz, P.J.Daly, J.Blomqvist Particle Plus Octupole M2/E3 Isomers and High-Spin Particle-Hole States in 147Tb and 148Tb NUCLEAR REACTIONS 151Eu(α, xn), E=68-110 MeV; measured I(ce), Eγ, Iγ, σ(E) for X=5-8, ICC. 147,148Tb deduced levels, T1/2, γ multipolarities. Particle phonon coupling model.
doi: 10.1007/BF01559755
1979FA01 Phys.Lett. 80B, 190 (1979) T.Faestermann, H.Bohn, F.v.Feilitzsch, A.W.Sunyar, R.Broda, P.Kleinheinz, M.Ogawa Shell Model Isomers Near Z = 64, N = 82: g-Factors of Yrast States in 146Gd and 147Gd NUCLEAR MOMENTS 146mGd, 147mGd [from 122,124Sn(28Si, X), E=119, 132 MeV]; measured γ(θ, H, t); deduced nuclear g-factors. Compared with shell model.
doi: 10.1016/0370-2693(79)90195-3
1979KL04 Z.Phys. A290, 279 (1979) P.Kleinheinz, R.Broda, P.J.Daly, S.Lunardi, M.Ogawa, J.Blomqvist Particle Hole Yrast States in 146Gd and 147Gd and the Z=64 Shell Closure NUCLEAR REACTIONS 148,149Sm(α, 6n), 148Sm(α, 5n), E=70-90 MeV; 144Sm(α, 2n), E=30 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, I(ce). 146Gd deduced levels, ICC, T1/2, γ-branching, multipolarity, B(E2) configurations. 147Gd deduced levels, T1/2, γ-branching, B(M2), B(E3), configuration.
doi: 10.1007/BF01408545
1979LI12 Nucl.Phys. A324, 141 (1979) J.R.Lien, G.Lovhoiden, K.Aareskjold, S.El Kazzaz, C.Ellegaard, K.Heyde, M.Waroquier, P.Van Isacker, H.Vincx, J.R.Rekstad, P.Kleinheinz Studies of Single-Neutron Holes in the Transitional Nuclei N = 83-89: The 142Ce(d, t)141Ce and 142Ce(3He, α)141Ce Pick-up Rections NUCLEAR REACTIONS 142Ce(d, t), E=17 MeV; 142Ce(3He, α), E=24 MeV; measured σ(Et, θ), σ(Eα, θ). 141Ce deduced levels, L, π, S. Enriched target. Unified model calculations.
doi: 10.1016/0375-9474(79)90084-8
1979PI07 Z.Phys. A290, 337 (1979) M.Piiparinen, S.Lunardi, P.Kleinheinz, H.Backe, J.Blomqvist High Spin Isomers in 151Dy NUCLEAR REACTIONS 152Gd(α, 5n), E=72 MeV; 136Ce(18O, 3n), E=83 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, ceγ-coin, E(ce). 151Dy deduced levels, transition multipolarities, T1/2, shell-model configurations.
doi: 10.1007/BF01408552
1978BE22 Z.Phys. A285, 405 (1978) D.Benson, Jr., P.Kleinheinz, R.K.Sheline, E.B.Shera Nuclear Levels in 193Os NUCLEAR REACTIONS 192Os(d, p), E=12.0 MeV; measured σ(Ep, θ). 192Os(n, γ), E=th; measured σ(Eγ); deduced Q. 193Os deduced levels, K, J, π.
doi: 10.1007/BF01813241
1978BR15 Z.Phys. A285, 423 (1978) R.Broda, M.Ogawa, S.Lunardi, M.R.Maier, P.J.Daly, P.Kleinheinz Production of High Multiplicity Yrast Isomers in 147Gd and 146Gd in α-Particle Induced Reactions NUCLEAR REACTIONS Sm(α, xnγ), E=70-90 MeV; measured γ-spectra, γ(t). 146,147Gd deduced levels, T1/2, J, π.
doi: 10.1007/BF01813243
1978DA14 Z.Phys. A288, 103 (1978) P.J.Daly, P.Kleinheinz, R.Broda, A.M.Stefanini, S.Lunardi, H.Backe, L.Richter, R.Willwater, F.Weik A 0.5 μs 10+ Isomer in 148Dy and the πh11/2 Effective E2 Charge NUCLEAR REACTIONS 152Gd(α, 8nγ), E=90-120 MeV; 136Ce(16O, 4nγ), E=85-92 MeV; measured σ(E, Eγ), γγ-coin. 148Dy deduced levels, J, π, T1/2, B(E2).
doi: 10.1007/BF01408208
1978KL01 Z.Phys. A284, 351 (1978) P.Kleinheinz, S.Lunardi, M.Ogawa, M.R.Maier The 3- State in the Doubly Closed Shell Nucleus 146Gd NUCLEAR REACTIONS 148Sm(α, 6nγ), E=82 MeV; measured Eγ, Iγ(θ), γγ-coin. 146Gd deduced levels, J, π.
doi: 10.1007/BF01406808
1978KL04 Z.Phys. A286, 27 (1978) P.Kleinheinz, M.Ogawa, R.Broda, P.J.Daly, D.Haenni, H.Beuscher, A.Kleinrahm Properties of the 3- First Excited State in the Doubly Closed Shell Nucleus 146Gd NUCLEAR REACTIONS 149Sm(α, 7nγ), E=90 MeV; measured γ, ce spectra, γγ(t). 144Sm(α, 2nγ), E=90 MeV; measured γce(t). 146Gd levels deduced T1/2, λ, B(λ).
doi: 10.1007/BF01434610
1978OG01 Z.Phys. A284, 271 (1978) M.Ogawa, P.Kleinheinz, S.Lunardi, O.W.B.Schult, M.Fenzl Gamma-Ray Multiplicities in α-Induced Compound and Precompound Reactions NUCLEAR REACTIONS 150Sm(α, xnγ), E=40-140 MeV; measured γ-multiplicities.
doi: 10.1007/BF01406797
1978OG03 Phys.Rev.Lett. 41, 289 (1978) M.Ogawa, R.Broda, K.Zell, P.J.Daly, P.Kleinheinz Lowest 2+ State in 146Gd and the Energy Gap at Z=64 NUCLEAR REACTIONS 144Sm(α, 2nγ), E=22.4-25.1 MeV; measured σ(E, Eγ). 146Gd deduced levels, J, π.
doi: 10.1103/PhysRevLett.41.289
1977BE15 Z.Phys. A281, 145 (1977) D.Benson, Jr., P.Kleinheinz, R.K.Sheline, E.B.Shera Nuclear Levels and Spectroscopy of 191Os NUCLEAR REACTIONS 190Os(d, p), 192Os(d, t), E=12 MeV; measured σ(θ); deduced Q. 190Os(n, γ), E=th; measured Eγ, Iγ; deduced Q. 191Os deduced levels, J, π, L, S.
doi: 10.1007/BF01408626
1977EL02 Nucl.Phys. A280, 1 (1977) S.El-Kazzaz, J.R.Lien, G.Lovhoiden, P.Kleinheinz, C.Ellegaard, J.Bjerregaard, P.Knudsen, J.Rekstad A Study of Levels in 141Nd with the (d, t) and (3He, α) Reactions NUCLEAR REACTIONS 142Nd(d, t), E=17 MeV; measured σ(Et, θ). 142Nd(3He, α), E=24.0 MeV; measured σ(Eα, θ). 141Nd deduced levels, L, S. Enriched targets.
doi: 10.1016/0375-9474(77)90289-5
1977KL04 Nucl.Phys. A283, 189 (1977) P.Kleinheinz, A.M.Stefanini, M.R.Maier, R.K.Sheline, R.M.Diamond, F.S.Stephens Different Structure Collective Bands in the N = 87 Nuclei 149Sm, 151Gd And 153Dy NUCLEAR REACTIONS 148Nd, 150Sm, 152Gd(α, 3nγ), E=35-45 MeV; measured σ(E, Eγ, θ), γ linear polarization, γγ-coin. 149Sm, 151Gd, 153Dy deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(77)90428-6
1976BE50 Phys.Rev. C14, 2095 (1976) D.Benson, Jr., P.Kleinheinz, R.K.Sheline, E.B.Shera Nuclear Spectroscopy of 189Os NUCLEAR REACTIONS 188Os(d, p), E=12 MeV; measured σ(Ep, θ). 190Os(d, t), E=12 MeV; measured σ(Et, θ); deduced Q. 188Os(n, γ), E=th; measured σ(Eγ); deduced Q. 189Os deduced levels, K, L, J, π, evidence for triaxiality. Nilsson model.
doi: 10.1103/PhysRevC.14.2095
1976ST01 Nucl.Phys. A258, 34 (1976) A.M.Stefanini, P.J.Daly, P.Kleinheinz, M.R.Maier, R.Wagner Isomers in the N = 83 Nucleus 149Dy NUCLEAR REACTIONS 152Gd(α, 7n), E=90-116 MeV; measured Eγ, Iγ(θ), αγ-, γγ-delay. 149Dy deduced levels, J, π, T1/2. Enriched target. Ge detectors.
doi: 10.1016/0375-9474(76)90525-X
1976ST08 Phys.Lett. 62B, 405 (1976) A.M.Stefanini, P.Kleinheinz, M.R.Maier A 500 ms Three-Particle Isomer in 149Dy NUCLEAR REACTIONS 152Gd(α, 7n), E=106 MeV; measured γγ(θ, t). 149Dy deduced level, J, π, T1/2.
doi: 10.1016/0370-2693(76)90669-9
1975KL01 Phys.Lett. 53B, 442 (1975) P.Kleinheinz, M.R.Maier, R.M.Diamond, F.S.Stephens, R.K.Sheline Revised Single-Particle Energies in N = 83 Nuclei NUCLEAR REACTIONS 139La(7Li, nαγ), (7Li, 3nγ), E=30 MeV; 144Nd(α, 3nγ), E=40 MeV; 147Sm(α, 4nγ), E=57 MeV; measured reaction products, Eγ, Iγ, σ(Eγ), γγ-coin, γγ(t). 141Ce, 143Nd, 145Sm, 147Gd levels. 142Nd; deduced T1/2.
doi: 10.1016/0370-2693(75)90213-0
1975SH03 Phys.Rev.Lett. 34, 535 (1975) E.B.Shera, E.T.Ritter, G.A.Rinker, Jr., M.J.Bennett, R.B.Perkins, H.D.Wohlfahrt, G.Fricke, L.K.Wagner, P.Kleinheinz, R.K.Sheline, R.M.Steffen, J.W.Negele Muonic Isotope Shifts in the Even Fe Nuclei ATOMIC PHYSICS 54,56,58Fe; measured muonic isotope shift.
doi: 10.1103/PhysRevLett.34.535
1975TH02 Phys.Lett. 55B, 447 (1975) R.C.Thompson, A.Ikeda, P.Kleinheinz, R.K.Sheline, P.J.Daly Nucleon Transfer Cross Sections for Mixed Odd-A Targets NUCLEAR REACTIONS 189Os(d, t); calculated σ.
doi: 10.1016/0370-2693(75)90552-3
1975WA12 Nucl.Phys. A246, 43 (1975) L.K.Wagner, D.G.Burke, H.E.Cheung, P.Kleinheinz, R.K.Sheline A Nuclear Structure Study of 165Ho Using the (t, α), (α, t) and (3He, d) Reactions NUCLEAR REACTIONS 164Dy(α, t), E=27 MeV; measured σ(Et); 164Dy(3He, d), E=24 MeV; measured σ(Ed); 166Er(t, α), E=15 MeV; measured σ(Eα). 165Ho deduced levels, J, π, L. Enriched targets.
doi: 10.1016/0375-9474(75)90562-X
1974BA26 Nucl.Phys. A222, 377 (1974) B.B.Back, J.Bang, S.Bjornholm, J.Hattula, P.Kleinheinz, J.R.Lien Neutron Strength Functions in Rare Earth Nuclei NUCLEAR REACTIONS 156,158,160Gd, 160,162,164Dy, 166,168,170Er, 170,172,174,176Yb(d, p), E=9 MeV; measured σ(Ep). 157,159,161Gd, 161,163,165Dy, 167,169,171Er, 171,173,175,177Yb deduced neutron strength functions.
doi: 10.1016/0375-9474(74)90397-2
1974KL01 Phys.Rev.Lett. 32, 68 (1974) P.Kleinheinz, R.K.Sheline, M.R.Maier, R.M.Diamond, F.S.Stephens Shape Coexistence and its Cause in 151Gd NUCLEAR REACTIONS 150Sm(α, 3nγ), E=35-45 MeV; measured σ(E;Eγ), γγ-coin, γ(θ). 151Gd deduced levels, J, π.
doi: 10.1103/PhysRevLett.32.68
1974KL03 Priv.Comm. (March 1974) P.Kleinheinz, G.Lovhoiden, A.Mogelvang NUCLEAR REACTIONS 174,176,178,180Hf(3He, α); measured σ(Eα, θ). 173,175,177,179Hf deduced levels, J, π.
1974ST06 Nucl.Phys. A222, 235 (1974) F.S.Stephens, P.Kleinheinz, R.K.Sheline, R.S.Simon Backbending and Rotation Alignment NUCLEAR STRUCTURE 161,162Er, 171,172Hf; calculated rotational band parameters.
doi: 10.1016/0375-9474(74)90390-X
1973KL06 Nucl.Phys. A208, 93 (1973) P.Kleinheinz, P.J.Daly, R.F.Casten Two-Quasiparticle States and the Microscopic Composition of Kπ = 2+ Collective Excitations in 182W and 184W NUCLEAR REACTIONS 183W(d, t), 183W(d, p), 183W(3He, α), Ed=12.1 MeV, E(3He)=20.3 MeV; measured σ(Et, θ), σ(Ep, θ), σ(Eα, 60°). 182,184W deduced levels, J, K, π, two-quasiparticle configurations. Enriched targets.
doi: 10.1016/0375-9474(73)90737-9
1973KL07 Nucl.Phys. A203, 539 (1973) P.Kleinheinz, R.F.Casten, B.Nilsson Hexadecapole Deformation in the Wolfram Nuclei NUCLEAR REACTIONS 182,184,186W(3He, α), E=20.3 MeV; 180,182,184,186W(d, t), E=12.1 MeV; measured σ(Eα), σ(Et, θ). 179,181,183,185W deduced levels, J, π, L, E4 deformation. Enriched target.
doi: 10.1016/0375-9474(73)90363-1
1973LI06 Nucl.Phys. A201, 369 (1973) T.Lindblad, H.Ryde, P.Kleinheinz High-Spin States and Rotation-Particle Coupling in 179W NUCLEAR REACTIONS 181Ta(p, 3n)179W, Ep=30 MeV; 178Hf(α, 3n)179W, Eα=26-43 MeV; measured σ(Eα, Eγ, θ(γ)), αγ-delay, γγ-coin. 179W deduced levels, J, π, γ-branching, γ-mixing, K-mixing; calculated μ. Natural, enriched targets.
doi: 10.1016/0375-9474(73)90072-9
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