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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1984KL08      Nuovo Cim. 81A, 140 (1984)

P.Kleinheinz

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
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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
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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
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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
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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
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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
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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
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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
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1981KL05      Phys.Scr. 24, 236 (1981)

P.Kleinheinz

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
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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
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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
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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
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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
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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
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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
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1980KL09      J.Phys.(Paris), Colloq.C-10, 43 (1980)

P.Kleinheinz

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1801.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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