References quoted in the ENSDF dataset: 154GD 152SM(A,2NG),154SM(A,4NG)
25 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Letters 18, 314 (1965)
H.Ejiri, M.Ishihara, M.Sakai, K.Katori, T.Inamura
Anisotropy of Conversion Electrons from (p, 2n) and (α, 4n) Reactions
NUCLEAR STRUCTURE 196Hg, 186Os, 126Xe, 138Ce, 102Pd, 108Cd, 106Cd, 154Gd; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90352-5
Nucl.Phys. 88, 624 (1966)
O.Lonsjo, G.B.Hagemann
Vibrational States of 152Sm and 154Gd Populated by the (α, 2n) Reaction
NUCLEAR REACTIONS 150Nd, 152Sm, 154Sm(α, 2n), Eα = 18-20.5 MeV; measured E(ce), I(ce), γce- coin. 152Sm, 154Gd, 156Gd deduced levels, J, π. Enriched targets.
doi: 10.1016/0029-5582(66)90420-2
J.Phys.Soc.Japan 24, 1189 (1968)
H.Ejiri, M.Ishihara, M.Sakai, K.Katori, T.Inamura
Conversion Electrons from (α, xn) Reactions on Sm Isotopes and Nuclear Structures of Gd Nuclei
NUCLEAR REACTIONS 150,152,154Sm(α, xnγ), E=36, 40 MeV; measured I(ce), Iγ, σ(Eγ, θ(γ)), ce anisotropy. 150,152,154,156Gd deduced levels.
Phys.Rev. 174, 1544 (1968)
C.F.Williamson, S.M.Ferguson, B.J.Shepherd, I.Halpern
Intensities and Angular Distributions of Ground-State Rotational Transitions Excited in (α, 3n) and (α, 4n) Reactions
NUCLEAR STRUCTURE 154Gd, 156Dy, 160Dy, 162Er, 168Yb, 152Gd, 170Yb, 176Hf; measured not abstracted; deduced nuclear properties.
RLO-1388-120 (1969)
S.M.Ferguson, R.Heffner, H.Ejiri
Gamma Transitions from High Spin States in the Beta-Vibrational Band of 154Gd
NUCLEAR REACTIONS 154Sm(α, 4nγ), E=42 MeV; measured Iγ, σ(Eγ, θ(γ)). 154Gd transitions deduced B(E2), γ-mixing. Ge(Li) detector, enriched target.
Phys.Lett. 35B, 214 (1971)
S.M.Ferguson, R.Heffner, H.Ejiri
Electric Quadrupole Transitions from High Spin States in the Beta-Vibrational Band of 154Gd
NUCLEAR REACTIONS 154Sm(α, 4nγ), E=42 MeV; measured Eγ, Iγ, B(E2) 154Gd deduced B(E2), branching ratios.
doi: 10.1016/0370-2693(71)90177-8
Nucl.Phys. A188, 1 (1972)
S.M.Ferguson, H.Ejiri, I.Halpern
De-Excitation of Rare-Earth Compound Nuclei Formed in Bombardments with 40 MeV α-Particles
NUCLEAR REACTIONS 154Sm, 157,158,160Gd, 163,164Dy, 167,168Er, 173,174,176Yb, 179,180Hf(α, xnγ), E=40.5 MeV;αγ-delay, Iγ, σ. 154Gd, 158,160Dy, 164Er, 168Yb, 174,176Hf, 180W deduced ground band transition intensities.
doi: 10.1016/0375-9474(72)90175-3
Nucl.Phys. A179, 51 (1972)
I.Rezanka, F.M.Bernthal, J.O.Rasmussen, R.Stokstad, I.Fraser, J.Greenberg, D.A.Bromley
High-Spin States in 153Gd and 154Gd from (α, xnγ) Studies
NUCLEAR REACTIONS 152Sm(α, 3nγ), (α, 2nγ), E=27-32 MeV; measured Eγ, Iγ(θ), γγcoin. 153Gd, 154Gd deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(72)90104-2
Bull.Amer.Phys.Soc. 18, 1404, DB3 (1973)
Y.Gono, D.R.Zolnowski, D.R.Haenni, T.T.Sugihara
In-beam electron measurements from 154Sm(α, 4nγ)154Gd and 148Sm(C, 4nγ)156Er
NUCLEAR REACTIONS 148Sm(12C, 4nγ), 154Sm(α, 4nγ); measured Eγ, I(ce). 154Gd, 156Er levels deduced J.
Phys.Rev.Lett. 31, 1146 (1973)
T.L.Khoo, F.M.Bernthal, J.S.Boyno, R.A.Warner
Experimental Demonstration of Backbending Behavior from a Band Crossing in 154Gd
NUCLEAR REACTIONS 152Sm(α, 2nγ), E=24 MeV; 154Sm(α, 4nγ), E=41, 45, 48, 50 MeV; measured Eγ, γγ-coin. 154Gd deduced levels, J, π, B(E2), γ-branching.
doi: 10.1103/PhysRevLett.31.1146
Phys.Lett. 44B, 39 (1973)
D.Ward, R.L.Graham, J.S.Geiger, H.R.Andrews
Anomalous Moments of Inertia for High-Spin Levels in the Beta Vibrational Band of 154Gd
NUCLEAR REACTIONS 154Sm(α, 4nγ), E=38, 41 MeV; measured σ(E;Eγ, θ), γγ-coin. 154Gd deduced levels, J, π.
doi: 10.1016/0370-2693(73)90294-3
Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1786 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 1 (1974)
D.Ward, R.L.Graham, J.S.Geiger, G.R.Andrews
Band Crossing and Anomalous Moments of Inertia of High-Spin States in 154Gd
NUCLEAR REACTIONS 154Sm(α, 4nγ), E=38, 41 MeV; measured Eγ, Iγ(E;θ), γγ-coin. 154Gd deduced levels, J, π, γ-branching, band parameters, moments of inertia.
Phys.Rev. C10, 2460 (1974)
Y.Gono, T.T.Sugihara
Electric Monopole Admixtures in Interband Transitions of 154Gd
NUCLEAR REACTIONS 154Sm(α, 4n), E=45 MeV, enriched target; measured in-beam I(ce), Iγ. 154Gd transitions deduced ICC, B(E0)/B(E2).
Texas A and M Univ.Cyclotron Inst.Ann.Rept., p.29 (1975)
D.R.Zolnowski, T.Kishimoto
Theoretical Interpretation of Negative-Parity States: A Quadrupole-Octupole Model
NUCLEAR STRUCTURE 150Sm, 154Dy, 154Gd, 162Er; calculated negative parity levels.
Bull.Amer.Phys.Soc. 21, No.4, 657, JF3 (1976)
R.L.West, E.G.Funk, J.W.Mihelich
In-Beam γ-Ray Spectroscopy of 154Gd Using the (α, 2n) Reaction
NUCLEAR REACTIONS 152Sm(α, 2nγ), E=24 MeV; measured σ(Eγ, θ), γγ(t). 154Gd deduced levels, K, J, π.
Phys.Rev. C18, 679 (1978)
R.L.West, E.G.Funk, J.W.Mihelich
Levels in 154Gd Populated by the (α, 2nγ) Reaction and the Decay of the Isomers of 154Tb
NUCLEAR REACTIONS 152Sm(α, 2nγ), E=24 MeV; measured Eγ, Iγ, γγ(t), γ(θ), γγ(θ). 154Gd deduced levels, K, J, π, δ, quadrupole moment. Enriched targets, Ge(Li) detectors.
RADIOACTIVITY 154m,154Tb; measured γγ(θ). 154Gd levels deduced J, π, δ. Ge(Li) detectors.
Nucl.Instrum.Methods 193, 647 (1982)
R.Daniel, J.F.Sharpey-Schafer
The Use of a fast Counting System in a 5 GeLi γ-Ray Polarimeter
NUCLEAR REACTIONS 152Sm(α, 2n), E=19.5 MeV; measured Eγ, Iγ, linear polarization vs θ. 154Gd deduced levels, J, π, vibrational band characteristics, γ-multipolarity, δ. Fast counting Ge(Li) polarimeter, in-plane, out-of-plane sum, difference spectra.
J.Phys.(London) G15, 1871 (1989)
J.D.Morrison, J.Simpson, M.A.Riley, H.W.Cranmer-Gordon, P.D.Forsyth, D.Howe, J.F.Sharpey-Schafer
Rotational Band Structure in 154Gd
NUCLEAR REACTIONS 150Nd(9Be, 5n), E=55 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 154Gd deduced levels, J, π, decay features. Enriched targets, Ge(Li)-NaI(Tl) and Ge-NaI(Tl) escape-suppressed spectrometers. Cranked shell model calculations, systematic comparisons of N=90 isotones.
doi: 10.1088/0954-3899/15/12/012
Proc.6th Intern.Conf.on Nuclei Far from Stability + 9th Intern.Conf.on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R.Neugart, A.Wohr, Eds., p.585 (1993)
A.Aprahamian, X.Wu, S.Fischer, W.Reviol, J.X.Saladin
Vibrations in Deformed Nuclei
NUCLEAR STRUCTURE 154,156Gd, 162Dy; analyzed data; deduced multi-phonon vibrations evidence.
Phys.Lett. 316B, 235 (1993)
X.Wu, A.Aprahamian, J.Castro-Ceron, C.Baktash
Identical Bands and Multi-Phonon Vibrations
NUCLEAR REACTIONS 152Sm(α, 2n), E=26 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 154Gd deduced levels, J, π, B(λ), band structure, Iγ.
NUCLEAR STRUCTURE 168Er, 156Gd, 170Yb, 178Hf; analyzed Eγ data; deduced band characteristics.
doi: 10.1016/0370-2693(93)90319-D
Phys.Rev. C49, 1837 (1994)
X.Wu, A.Aprahamian, S.M.Fischer, W.Reviol, G.Liu, J.X.Saladin
Multiphonon Vibrational States in Deformed Nuclei
NUCLEAR REACTIONS 152Sm(α, 2n), E=26 MeV; measured Eγ, Iγ, γγ(θ). 154Gd deduced levels, J, π, K, relative B(E2) values, configuration, band structure.
Nucl.Phys. A688, 716 (2001)
D.G.Burke, J.C.Waddington, O.P.Jolly
(3He, d) and (α, t) Reaction Studies of 154Gd: Nature of Kπ = 4+ Bands in Heavy Deformed Nuclei
NUCLEAR REACTIONS 153Eu(3He, d), E=24 MeV; measured σ(E, θ=30° and 60°). 153Eu(α, t), E=27 MeV; measured σ(E, θ=45° and 60°). 154Gd deduced levels, two-quasiproton admixtures. Enriched targets, magnetic spectrograph. Double-γ-phonon vs hexadecapole interpretations compared.
doi: 10.1016/S0375-9474(00)00597-2
Nucl.Data Sheets 110, 2257 (2009)
C.W.Reich
Nuclear Data Sheets for A = 154
COMPILATION 154Ce, 154Pr, 154Nd, 154Pm, 154Sm, 154Eu, 154Gd, 154Tb, 154Dy, 154Ho, 154Er, 154Tm, 154Yb, 154Lu, 154Hf; compiled, evaluated structure data.
doi: 10.1016/j.nds.2009.09.001
Eur.Phys.J. A 47, 5 (2011)
J.F.Sharpey-Schafer, S.M.Mullins, R.A.Bark, J.Kau, F.Komati, E.A.Lawrie, J.J.Lawrie, T.E.Madiba, P.Maine, A.Minkova, S.H.T.Murray, N.J.Ncapayi, P.A.Vymers
Congruent band structures in 154Gd : Configuration-dependent pairing, a double vacuum and lack of β-vibrations
NUCLEAR REACTIONS 152Sm(α, 2n), E=25 MeV;154Sm(α, 4n), E=45 MeV; measured Eγ, Iγ, γγ-coin, polarization using spectrometer array AFRODITE; deduced levels, J, π, bands, rotational bands. Levels and bands compared to 152Sm.
doi: 10.1140/epja/i2011-11005-8
Phys.Rev. C 100, 044324 (2019)
S.N.T.Majola, Z.Shi, B.Y.Song, Z.P.Li, S.Q.Zhang, R.A.Bark, J.F.Sharpey-Schafer, D.G.Aschman, S.P.Bvumbi, T.D.Bucher, D.M.Cullen, T.S.Dinoko, J.E.Easton, N.Erasmus, P.T.Greenlees, D.J.Hartley, J.Hirvonen, A.Korichi, U.Jakobsson, P.Jones, S.Jongile, R.Julin, S.Juutinen, S.Ketelhut, B.V.Kheswa, N.A.Khumalo, E.A.Lawrie, J.J.Lawrie, R.Lindsay, T.E.Madiba, L.Makhathini, S.M.Maliage, B.Maqabuka, K.L.Malatji, P.L.Masiteng, P.I.Mashita, L.Mdletshe, A.Minkova, L.Msebi, S.M.Mullins, J.Ndayishimye, D.Negi, A.Netshiya, R.Newman, S.S.Ntshangase, R.Ntshodu, B.M.Nyako, P.Papka, P.Peura, P.Rahkila, L.L.Riedinger, M.A.Riley, D.G.Roux, P.Ruotsalainen, J.J.Saren, C.Scholey, O.Shirinda, M.A.Sithole, J.Sorri, M.Stankiewicz, S.Stolze, J.Timar, J.Uusitalo, P.A.Vymers, M.Wiedeking, G.L.Zimba
β and γ bands in N=88, 90, and 92 isotones investigated with a five-dimensional collective Hamiltonian based on covariant density functional theory: Vibrations, shape coexistence, and superdeformation
NUCLEAR REACTIONS 136Xe(18O, 4n)150Sm, E=75 MeV; 148Nd(α, 2n)150Sm, E=25 MeV; 152Sm(α, 4n)152Gd, E=45 MeV; 152Sm(α, 2n)154Gd, E=25 MeV; 155Gd(3He, 4n)154Dy, E=37.5 MeV; 147Sm(12C, 3n)156Er, E=65 MeV; 155Gd(α, 3n)156Dy, E=25 MeV; 144Sm(18O, 4n)158Yb, E=78 MeV; 150Sm(12C, 4n)158Er, E=65 MeV; 156Gd(α, 2n)158Dy, E=27 MeV; 147Sm(16O, 3n)160Yb, E=73 MeV; 152Sm(12C, 4n)160Er, E=64 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization) using the AFRODITE array at the cyclotron facility of the iThemba Labs for 11 reactions, and JUROGAM II array at Jyvaskyla for 148Nd(α, 2n)150Sm and 155Gd(α, 3n)156Dy reactions. 150Sm, 152,154Gd, 154,156,158Dy, 156,160Er, 158,160Yb; deduced levels, J, π, multipolarities, β, γ and 0+ bands, B(E2) ratios. 150,152,154Sm, 152,154,156Gd, 154,156,158Dy, 156,158,160Er, 158,160,162Yb; calculated potential energy surfaces (PES) and probability density distribution contours in (β, γ) plane; deduced staggering parameters, in-band B(E2) values, absolute transition strengths of E0 transitions, X(E0/E2) values from present and previous experimental data. Comparison with 5DCH-CDFT calculations with PC-PK1 density functional.
doi: 10.1103/PhysRevC.100.044324