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NSR database version of May 21, 2024.

Search: Author = G.Jung

Found 27 matches.

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1986RO16      J.Phys.(London) G12, 903 (1986)

S.J.Robinson, W.D.Hamilton, P.Hungerford, B.Pfeiffer, G.Jung, D.M.Snelling

Levels and Transitions in 140Ba Populated following the β Decay of 140Cs

NUCLEAR STRUCTURE 140,142,144,146Ba; calculated levels, B(E2). Interacting boson model.

RADIOACTIVITY 140Cs(β-) [from 235U(n, F), mass separation]; measured Eγ, Iγ, γγ(θ), oriented nuclei; deduced log ft, Iβ. 140Ba deduced levels, J, π, δ, γ-branching. Interacting boson model.

doi: 10.1088/0305-4616/12/9/013
Citations: PlumX Metrics

1984BE50      Z.Phys. A319, 193 (1984)

K.Becker, G.Jung, K.-H.Kobras, H.Wollnik, B.Pfeiffer

Gamma-Gamma Angular Correlation Measurements of Transitions in 98Sr and 98Zr and Confirmation of Shape Coexistence in 98Sr

RADIOACTIVITY 98Rb(β-n) [from 235U(n, F), E=thermal]; 98Y(β-) [following 98Sr decay]; measured γγ(θ), γγ-coin. 98Sr, 98Zr deduced levels, J, π, γ-branching, δ, shape coexistence evidence.

doi: 10.1007/BF01415633
Citations: PlumX Metrics

1983KR11      Z.Phys. A312, 43 (1983)

K.-L.Kratz, H.Ohm, A.Schroder, H.Gabelmann, W.Ziegert, B.Pfeiffer, G.Jung, E.Monnand, J.A.Pinston, F.Schussler, G.I.Crawford, S.G.Prussin, Z.M.de Oliveira

The Beta-Decay of 95Rb and 97Rb

RADIOACTIVITY 95,97Rb(β-); 95,97Sr(β-n) [from 95,97Rb(β-decay)]; measured Eγ, Iγ, I(ce), β-delayed En, In, β-delayed nγ-coin, βγ(t); deduced β-strength function. 95,97Sr deduced levels, T1/2, γ-multipolarity, ICC, neutron unbound level density.

doi: 10.1007/BF01411659
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23242.

1982DE08      Nucl.Instrum.Methods 192, 261 (1982)

R.Decker, K.-D.Wunsch, H.Wollnik, G.Jung, E.Koglin, G.Siegert

A Hyperpure Germanium Detector for Precise Beta Endpoint Energy Determinations

RADIOACTIVITY 28Al, 20F, 38Cl, 88Rb [from 27Al, 19F, 37Cl, 87Rb(d, p), E=1-6.5 MeV]; measured Eβ, βγ-coin, β-endpoint energies, Qβ. Hyperpure Ge detector, on-line separation.

doi: 10.1016/0029-554X(82)90831-X
Citations: PlumX Metrics

1982KA03      Z.Phys. A304, 293 (1982)

K.Kawade, G.Battistuzzi, H.Lawin, H.A.Selic, K.Sistemich, F.Schussler, E.Monnand, J.A.Pinston, B.Pfeiffer, G.Jung

Excited 0+-Levels in 98Zr

RADIOACTIVITY 98Rb [from isotope separator]; 98Sr [from 98Rb(β-decay), isotope separator]; 98Y [from 98Sr(β-decay), isotope separator]; measured Eγ, Iγ, I(ce), γγ(θ), βγ(t). 98Zr deduced levels, T1/2, γ-branching, B(E2), B(E0), J, π, shape coexistence.

doi: 10.1007/BF01421511
Citations: PlumX Metrics

1982KR07      Z.Phys. A305, 93 (1982)

K.-L.Kratz, H.Ohm, H.Gabelmann, G.I.Crawford, G.Jung, B.Pfeiffer

Evidence for Excited 0+ States in 94Sr

RADIOACTIVITY 95Rb [from mass separator]; measured β-delayed nγ-coin, Eγ, γγ-coin. 94Sr deduced levels, J, π, γ-branching. Tof, 3He ionization chamber, Ge(Li) spectrometer.

doi: 10.1007/BF01415087
Citations: PlumX Metrics

1982KR11      Z.Phys. A306, 239 (1982)

K.-L.Kratz, A.Schroder, H.Ohm, M.Zendel, H.Gabelmann, W.Ziegert, P.Peuser, G.Jung, B.Pfeiffer, K.D.Wunsch, H.Wollnik, C.Ristori, J.Crancon

Beta-Delayed Neutron Emission from 93-100Rb to Excited States in the Residual Sr Isotopes.

RADIOACTIVITY 93,94,95,96,97,98,99,100Rb [from 235U(n, F)]; measured Eγ, Iγ, β-delayed nγ-, βγ-, γγ-coin; deduced β-strength function role. 92,93,94,95,96,97,98Sr levels deduced delayed neutron branching ratios.

doi: 10.1007/BF01415126
Citations: PlumX Metrics

1982MI01      J.Phys.(London) G8, 111 (1982)

E.Michelakakis, W.D.Hamilton, P.Hungerford, G.Jung, P.Pfeiffer, S.M.Scott

Levels and Transitions in 142,144Ce Populated following the β Decay of 142,144La

RADIOACTIVITY 142,144La [from fission product Cs decay]; measured Eγ, Iγ, γγ(θ), oriented nuclei, γγ-coin; deduced Qβ. 142,144Ce deduced levels, J, π, δ. Ge(Li) detectors.

doi: 10.1088/0305-4616/8/1/013
Citations: PlumX Metrics

1981DE25      Z.Phys. A301, 165 (1981)

R.Decker, K.D.Wunsch, H.Wollnik, G.Jung, J.Munzel, G.Siegert, E.Koglin

Prazise Qβ-Wert-Messungen mit einem Intrinsic-Germanium-Detektor an schweren, Neutronenreichen Spaltprodukten (Precise Q(β-) Values with an Intrinsic Germanium Detector for Heavy, Neutron-Rich Fission Products)

RADIOACTIVITY 138,139,140,141,142,143,144,145,146Cs, 139,141,143,146Ba, 146La [from on-line fission product separation]; measured βγ-coin, β-end point energies; deduced Qβ. Intrinsic Ge detector.

doi: 10.1007/BF01419247
Citations: PlumX Metrics

1981JU02      Nucl.Phys. A352, 1 (1981)

G.Jung, B.Pfeiffer, P.Hungerford, S.M.Scott, F.Schussler, E.Monnand, J.A.Pinston, L.J.Alquist, H.Wollnik, W.D.Hamilton

The Level Structure of 96Y from the Decay of 96Sr

RADIOACTIVITY 96Sr [from 235U(n, F)]; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced log ft. 96Y deduced levels, J, π, γ-multipolarity, ICC. Mass-separated 96Rb activity, Si(Li) and Ge(Li) detectors.

doi: 10.1016/0375-9474(81)90554-6
Citations: PlumX Metrics

1981KR11      Phys.Lett. 103B, 305 (1981)

K.-L.Kratz, A.Schroder, H.Ohm, G.Jung, B.Pfeiffer, F.Schussler

Observation of Beta-Delayed Neutron Decay to Excited 0+ States in the Residual Nucleus: The case 97Rb(βnγ)96Sr

RADIOACTIVITY 97Rb; measured β-delayed neutron emission, γγ-, βγ-, nγ-coin, I(ce). 96Sr levels deduced neutron branching ratio, different structure characteristics.

doi: 10.1016/0370-2693(81)90229-X
Citations: PlumX Metrics

1980AL08      Nucl.Phys. A338, 1 (1980)

L.J.Alquist, H.Wollnik, G.Jung, B.Pfeiffer, P.Hungerford, S.M.Scott, W.D.Hamilton

Gamma-Gamma Angular Correlations of Transitions in 92Sr

RADIOACTIVITY 92Rb; measured γγ(θ). 92Sr levels deduced J, π. Mass-separated 92Rb activity.

doi: 10.1016/0375-9474(80)90117-7
Citations: PlumX Metrics

1980DE02      Z.Phys. A294, 35 (1980)

R.Decker, K.D.Wunsch, H.Wollnik, E.Koglin, G.Siegert, G.Jung

Prazise Qβ-Wert-Messungen mit einem Intrinsic-Germanium Detektor an leichten, neutronenreichen Spaltprodukten

RADIOACTIVITY 88,89,90,91,92,93,94,95,96,97Rb, 91,94,96Sr, 94,95,96Y [from on-line fission product separation]; measured Eβ, βγ-coin; deduced Q(β). Intrinsic Ge detector.

doi: 10.1007/BF01473120
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1980JU03      Phys.Rev. C22, 252 (1980)

G.Jung, B.Pfeiffer, L.J.Alquist, H.Wollnik, P.Hungerford, S.M.Scott, W.D.Hamilton

Gamma-Gamma Angular Correlations of Transitions in 94Sr and 96Sr

RADIOACTIVITY 94,96Rb; measured γγ(θ). 94,96Sr deduced levels, J, π. Mass-separation.

doi: 10.1103/PhysRevC.22.252
Citations: PlumX Metrics

1980SC05      Phys.Lett. 90B, 57 (1980)

A.Schroder, H.Ohm, W.Rudolph, K.Summerer, K.-L.Kratz, K.D.Wunsch, G.Jung, J.Crancon, C.Ristori

Spectroscopy of Beta-Delayed Neutrons in Coincidence with Gamma-Rays Depopulating Excited States in 93Sr

RADIOACTIVITY 94Rb; measured β-delayed nγ(t). 94Sr deduced resonance in β-strength function. 93Sr levels deduced p-wave n-branching. Optical model analysis.

doi: 10.1016/0370-2693(80)90050-7
Citations: PlumX Metrics

1980SC13      Nucl.Phys. A339, 415 (1980)

F.Schussler, J.A.Pinston, E.Monnand, A.Moussa, G.Jung, E.Koglin, B.Pfeiffer, R.V.F.Janssens, J.van Klinken

Discovery of a Very Low-Lying 0+ State in 98Sr and Shape Coexistence Implication in 98Sr

RADIOACTIVITY 98Rb [from 235U(n(th), F)]; measured T1/2, Eγ, Iγ, I(ce), γγ(t), γce(t), βγ(t). 98Sr deduced levels, J, π. On-line separation of fission products.

doi: 10.1016/0375-9474(80)90024-X
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1980SC16      J.Phys.(London) G6, 1291 (1980)

S.M.Scott, W.D.Hamilton, P.Hungerford, D.D.Warner, G.Jung, K.D.Wunsch

The Neutron-Rich Barium Isotopes

RADIOACTIVITY 142,144,146Cs [from 235U(n, F), mass separation]; measured Eγ, Iγ, γγ(θ). 142,144,146Ba levels deduced J, π, δ. Interacting boson model.

doi: 10.1088/0305-4616/6/10/016
Citations: PlumX Metrics

1979BA62      Phys.Rev. C20, 2244 (1979)

S.J.Balestrini, R.Decker, H.Wollnik, K.D.Wunsch, G.Jung, E.Koglin, G.Siegert

Independent Yields of Rb and Cs Isotopes from Thermal-Neutron Induced Fission of 235U

NUCLEAR REACTIONS 235U(n, F), E=thermal; measured relative abundancies of Rb, Cs isotopes. 88,89,90,91,92,93,94,95,96,97Rb, 137,138,139,140,141,142,143,144,145,146Cs deduced independent, fractional yields. Rb, Cs deduced charge displacement, dispersion, enhancement factor. Even-odd Z effect model. Mass separator, fast neutron detector.

doi: 10.1103/PhysRevC.20.2244
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21641.

1979KR10      Phys.Lett. 86B, 21 (1979)

K.-L.Kratz, H.Ohm, K.Summerer, M.Zendel, G.Jung, K.D.Wunsch, C.Ristori, J.Crancon, S.G.Prussin

Systematic Trends in the Beta Minus Strength Functions of Neutron-Rich Rubidium Isotopes

RADIOACTIVITY 89,91,93,95,97Rb; analyzed data on β-decay properties, γ, neutron spectroscopy; deduced resonances in β-strength function.

doi: 10.1016/0370-2693(79)90611-7
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1979RI09      Z.Phys. A290, 311 (1979)

C.Ristori, J.Crancon, K.D.Wunsch, G.Jung, R.Decker, K.-L.Kratz

Half-Lives and Delayed Neutron Emission Probabilities of Short-Lived Rb and Cs Precursors

RADIOACTIVITY 94,95,96,97,98Rb, 143,144,145,146,147Cs [from on-line separator]; measured T1/2, delayed-neutron emission probabilities.

doi: 10.1007/BF01408548
Citations: PlumX Metrics

1979SC11      Z.Phys. A290, 359 (1979)

F.Schussler, J.Blachot, E.Monnand, B.Fogelberg, S.H.Feenstra, J.van Klinken, G.Jung, K.D.Wunsch

Nuclear Spectroscopy of Neutron-Rich A = 143 Nuclei

RADIOACTIVITY 143Cs, 143Ba [from fission]; measured Eγ, Iγ, I(ce), γγ-, βγ-coin; deduced Qβ, Iβ, log ft. 143Ba, 143La deduced levels, ICC, T1/2, J, π, multipolarity, configurations. Mass separation.

doi: 10.1007/BF01408397
Citations: PlumX Metrics

1979SC24      J.Phys. (London) G5, L187 (1979)

S.M.Scott, D.D.Warner, W.D.Hamilton, P.Hungerford, G.Jung, K.D.Wunsch, B.Pfeiffer

The Onset of Deformation in the Neutron-Rich Ba Isotopes

RADIOACTIVITY 142,144,146Cs; measured γγ(θ). 142,144,146Ba levels deduced J, π. Mass separation, Ge(Li) detectors.

doi: 10.1088/0305-4616/5/10/008
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1978KO29      Z.Phys. A288, 319 (1978)

E.Koglin, G.Jung, G.Siegert, R.Decker, K.D.Wunsch, H.Wollnik

Half-Lives of the New Isotopes 100Rb, 100Sr, 145Cs and of 99Rb, 99Sr and 147Cs

RADIOACTIVITY 100Rb, 100Sr, 148Cs, 99Rb, 99Sr, 147Cs [from 235U+n]; measured activity build-up, decay with β-multi-scaling, γ-multispectra; deduced T1/2.

doi: 10.1007/BF01415200
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1978MO33      Verh.Deut.Phys.Ges. No4/1978, 845 F4-10 (1978)

E.Monnand, J.Blachot, J.P.Bocquet, F.Schussler, H.Lawin, G.Sadler, K.Sistemich, G.Jung, K.D.Wunsch

Evidence for a new isomer in 146La and level scheme of 146Ce

RADIOACTIVITY 146La(β-); measured Eγ, Iγ(t), γγ-coin.; deduced isomer T1/2. Mass-separators OSTIS, LOHENGRIN, JOSEF.

1978WO09      Phys.Rev. C17, 2185 (1978)

F.K.Wohn, K.D.Wunsch, H.Wollnik, R.Decker, G.Jung, E.Koglin, G.Siegert

Identification of 147Cs and Half-Life Determinations for Cs and Ba Isotopes with A = 144-147 and Rb and Sr Isotopes with A = 96-98

RADIOACTIVITY 96,97,98Rb, 96,97,98Sr, 144,145,146,147Cs, 144,145,146,147Ba [from 235U(n, F)]; measured T1/2. Ge(Li), plastic scintillation detectors, mass separated activities.

doi: 10.1103/PhysRevC.17.2185
Citations: PlumX Metrics

1978WU04      Z.Phys. A288, 105 (1978)

K.D.Wunsch, R.Decker, H.Wollnik, J.Munzel, G.Siegert, G.Jung, E.Koglin

Precision Beta Endpoint Energy Measurements of Rubidium and Cesium Fission Products with an Intrinsic Ge-Detector

RADIOACTIVITY 88,89,90,91,92,93,94Rb, 138,139,140,141,142,143,144Cs; measured βγ-coin, Eβ; deduced Q.

1977WO07      Nucl.Phys. A291, 355 (1977)

H.Wollnik, F.K.Wohn, K.D.Wunsch, G.Jung

Experimental Indication of the Onset of Nuclear Deformation in Neutron-Rich Sr Isotopes at Mass 98

RADIOACTIVITY 98Rb [from 235U(n, fission)]; measured Eγ, Iγ. 98Sr deduced levels. Mass-separated Rb activity.

doi: 10.1016/0375-9474(77)90325-6
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