References quoted in the ENSDF dataset: 154SM 154SM(G,G'),(E,E')
34 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Lett. 31B, 206 (1970)
R.M.Wheeler, U.Atzmony, K.A.Hardy, J.C.Walker
Isomer Shift in the 82 keV Transition of 154Sm
NUCLEAR REACTIONS 154Sm(γ, γ), E=82 keV; measured Mossbauer effect; deduced isomer shift.
doi: 10.1016/0370-2693(70)90105-X
Phys.Rev. C13, 1083 (1976)
T.Cooper, W.Bertozzi, J.Heisenberg, S.Kowalski, W.Turchinetz, C.Williamson, L.Cardman, S.Fivozinsky, J.Lightbody, Jr., S.Penner
Shapes of Deformed Nuclei as Determined by Electron Scattering: 152Sm, 154Sm, 166Er, 176Yb, 232Th, and 238U
NUCLEAR REACTIONS 152,154Sm, 166Er, 176Yb, 232Th, 238U(e, e'); measured σ(Ee'). 152,154Sm, 166Er, 176Yb, 232Th, 238U deduced shape parameters.
Phys.Rev. C14, 543 (1976)
F.R.Metzger
Low-Lying El Transitions in the Stable Even Sm Isotopes
NUCLEAR REACTIONS 144,148,150,154Sm(γ, γ), E=1.2-3.8 MeV bremsstrahlung; measured σ, linear polarization. 144Sm deduced level, B(E1), J, π, Γ. 148,150,154Sm levels deduced Γ, B(E1). Enriched 144,150Sm targets.
Nucl.Phys. A276, 221 (1977)
Z.Berant, J.Tenenbaum, R.Moreh
Nuclear Resonance Fluorescence in 146Nd and 154Sm
NUCLEAR REACTIONS 146Nd, 154Sm(γ, γ'); measured Eγ, Iγ(θ). 146Nd, 154Sm deduced levels, J, π, M2/E1, Γ.
doi: 10.1016/0375-9474(77)90380-3
Proc.Int.Conf.Nucl.Structure, Tokyo, Japan, Int.Academic Printing Co., Ltd.Japan, Vol.1, p.387 (1977)
R.Hofmann, H.G.Andresen, B.Dreher, S.Gluckert, K.Merle, H.Miessen, R.Neuhausen, H.Scheib
Investigation of the Ground State Rotational Band of 152Sm and 154Sm by High Resolution Electron Scattering
NUCLEAR REACTIONS 148,152,154Sm(e, e'), E=80-300 MeV; measured σ(E). 152,154Sm deduced rms radii, B(E2), B(E4), B(E6), transition radii.
Nucl.Instrum.Methods 166, 69 (1979)
R.Moreh
Studies in Nuclear Spectroscopy Using the (γ, γ') and the (γ, n) Reactions. Part II. Nuclear Physics and Fundamental Scattering Processes
COMPILATION 15N, 50Cr, 55Mn, 62Ni, 65Cu, 66Zn, 69Ga, 74Ge, 75As, 80Se, 86Sr, 90Zr, 93Nb, 100Mo, 112Cd, 118,120Sn, 126,130Te, 139La, 140Ce, 141Pr, 142,144,146Nd, 144,154Sm, 202Hg, 203,205Tl, 208Pb, 209Bi; compiled total, ground state Γγ. Elastic, inelastic scattering data, monochromatic photons.
Phys.Lett. 148B, 260 (1984)
D.Bohle, G.Kuchler, A.Richter, W.Steffen
Further Evidence for the New Collective Magnetic Dipole Mode in Heavy Deformed Nuclei
NUCLEAR REACTIONS 154Sm, 164Dy, 168Er, 174Yb(e, e'), E=29 MeV; measured σ(E(e'), θ=165°), from factors, B(M1).
doi: 10.1016/0370-2693(84)90084-4
J.Phys.(London) G12, L47 (1986)
A.Faessler, Z.Bochnacki, R.Nojarov
Restoring Force for the 1+ Collective Mode in Deformed Nuclei
NUCLEAR STRUCTURE 154Sm, 156,158Gd, 164Dy, 168Er, 174Yb; calculated levels, B(M1). Deformed nuclei, collective mode, restoring force.
doi: 10.1088/0305-4616/12/2/002
Z.Phys. A324, 289 (1986)
R.Nojarov, Z.Bochnacki, A.Faessler
Microscopic Calculation of the Restoring Force for Scissor Isovector Vibrations
NUCLEAR STRUCTURE 154Sm, 156,158Gd, 164Dy, 168Er, 174Yb; calculated levels, B(λ), moment of inertia. Scissor isovector vibration restoring force, microscopic model.
Ann.Phys.(New York) 171, 253 (1986)
P.Van Isacker, K.Heyde, J.Jolie, A.Sevrin
The F-Spin Symmetric Limits of the Neutron-Proton Interacting Boson Model
NUCLEAR STRUCTURE 154Sm, 156,158Gd, 164Dy, 168Er, 174Yb; A=148-198; calculated levels, B(λ), M1, E2, M3 excitation strengths, g systematics, dipole, quadrupole moments; deduced F-spin conditions, consequences. F-spin symmetric limits, interacting boson model.
doi: 10.1016/0003-4916(86)90002-3
Nucl.Phys. A473, 494 (1987)
O.Castanos, J.P.Draayer, Y.Leschber
Collective 1+ States in Rare Earth and Actinide Nuclei
NUCLEAR STRUCTURE 152,154,156,158,160Gd, 156,158,160,164,166,168,170Er, 234,236,238,240U, 236,238,240,242Pu; calculated ground band level μ. 154Sm, 156,158,160Gd, 164Dy, 168Er, 174Yb, 232Th, 238,234,236,240U, 242Pu; calculated interband B(M1). Deformed nuclei, shell model.
doi: 10.1016/0375-9474(87)90137-0
Ann.Phys.(New York) 180, 290 (1987)
O.Castanos, J.P.Draayer, Y.Leschber
Towards a Shell-Model Description of the Low-Energy Structure of Deformed Nuclei II. Electromagnetic Properties of Collective M1 Bands
NUCLEAR STRUCTURE 154Sm, 156,160Gd, 164Dy, 168Er, 174Yb, 232Th, 234,236,238,240U, 242Pu; calculated levels, δ, B(λ). Shell model, deformed nuclei.
doi: 10.1016/0003-4916(87)90047-9
Phys.Rev. C35, 2310 (1987)
O.Civitarese, A.Faessler, R.Nojarov
Theoretical Description of Low-Lying K(π) = 1+ States in Deformed Nuclei
NUCLEAR STRUCTURE 154Sm, 156,158Gd, 164Dy, 168Er, 174Yb; calculated B(M1). Quasiparticle random phase approximation.
Phys.Lett. 194B, 6 (1987)
I.Hamamoto, C.Ronstrom
Form-Factor of Low-Lying K(π) = 1+ Excitations in Rare-Earth Nuclei
NUCLEAR STRUCTURE 154Sm, 156,158,164Dy, 168Er, 174Yb; calculated B(M1), transition densities. Microscopic model.
NUCLEAR REACTIONS 154Sm, 156,158,164Dy, 168Er, 174Yb(e, e'), E=10-60 MeV; calculated σ(E, θ). DWBA, microscopic transition densities.
doi: 10.1016/0370-2693(87)90759-3
Nucl.Phys. A465, 25 (1987)
U.Hartmann, D.Bohle, T.Guhr, K.-D.Hummel, G.Kilgus, U.Milkau, A.Richter
Excitation Energy and Transition Strength Systematics of Mixed Symmetric J(π) = 1+ States from Inelastic Electron Scattering
NUCLEAR STRUCTURE 46,48Ti, 110Pd, 154Sm, 154,156,158Gd, 164Dy, 168Er, 174Yb, 232Th, 238U; calculated levels, B(M1) strength distribution. Interacting boson models.
doi: 10.1016/0375-9474(87)90297-1
FRCEA-TH-79 (1987)
V.Meot
Etude des Excitations Collectives Quadrupolaires dans les Isotopes 144, 148, 150, 152, 154 du Samarium et du Cerium 140 par Diffusion Inelastique d'Electrons
NUCLEAR REACTIONS 144,148,150,152,154Sm, 140Ce(e, e'), E < 700 MeV; measured spectra, form factors. 144,148,150,152,154Sm, 140Ce deduced collective states excitation, transition charge density. Model comparison.
Nucl.Phys. A475, 439 (1987)
A.A.Raduta, I.I.Ursu, D.S.Delion
Simultaneous GCSM Description of the M1 State and the Major Collective Bands
NUCLEAR STRUCTURE 154Gd, 154Sm, 164Dy, 168Er, 174Yb, 232Th, 238U; calculated levels, B(M1). Generalized coherent state model.
NUCLEAR REACTIONS 156Gd, 232Th, 238U(e, e'), E not given; calculated M1 form factor. Generalized coherent state model.
doi: 10.1016/0375-9474(87)90073-X
Nucl.Phys. A484, 1 (1988)
R.Nojarov, A.Faessler
Symmetry-Restoring Interactions for K(π) = 1+ Isovector Vibrations
NUCLEAR STRUCTURE 154Sm, 156,158Gd, 164Dy, 168Er, 174Yb; calculated levels, B(M1). Symmetry restoring RPA.
doi: 10.1016/0375-9474(88)90138-8
Nucl.Phys. A491, 24 (1989)
A.A.Raduta, D.S.Delion
Description of Magnetic Properties of the Proton-Neutron Asymmetric States within the Generalized Coherent States Model
NUCLEAR STRUCTURE 156Gd, 164Dy, 238U; calculated M3 form factor. 154,156,158,160Gd, 154Sm, 164Dy, 168Er, 174Yb, 232Th, 238U; calculated levels, B(λ).
doi: 10.1016/0375-9474(89)90204-2
Nucl.Phys. A515, 237 (1990)
A.Faessler, R.Nojarov, F.G.Scholtz
Magnetic Dipole Electroexcitations in Rare-Earth Nuclei
NUCLEAR REACTIONS 154Sm, 154,156,158Gd, 168Er, 164Dy(e, e'), E not given; calculated form factors, magnetic dipole excitation. Quasiparticle RPA, DWBA.
doi: 10.1016/0375-9474(90)90368-V
Nucl.Phys. A509, 509 (1990)
P.O.Lipas, M.Koskinen, H.Harter, R.Nojarov, A.Faessler
Microscopic IBA Calculations of (e, e') M1 Form Factors
NUCLEAR STRUCTURE 154Sm, 154,156,158Gd, 164Dy, 168Er; calculated B(M1), g-factors. 164Dy; calculated form factors. Microscopic interacting boson model.
doi: 10.1016/0375-9474(90)90089-5
Nucl.Phys. A507, 99c (1990)
A.Richter
Shell Model and Magnetic Dipole Modes in Deformed Nuclei
NUCLEAR STRUCTURE 46,48Ti, 156Gd, 168Er, 164Dy, 148,150,152,154Sm; analyzed reaction data; deduced magnetic dipole mode features.
doi: 10.1016/0375-9474(90)90571-3
Yad.Fiz. 52, 364 (1990); Sov.J.Nucl.Phys. 52, 233 (1990)
D.M.Vladimirov
Spin and Spin-Isospin 1+ States of Deformed Nuclei in the SU(4) Symmetry Scheme
NUCLEAR STRUCTURE 154Sm, 154,156,158,160Gd, 160,162,164Dy, 168Er, 174Yb, 232Th, 238U; calculated B(λ), levels. Deformed nuclei, SU(4) symmetry scheme.
Phys.Rev.Lett. 65, 2515 (1990)
W.Ziegler, C.Rangacharyulu, A.Richter, C.Spieler
Orbital Magnetic Dipole Strength in 148, 150, 152, 154Sm and Nuclear Deformation
NUCLEAR REACTIONS 148,150,152,154Sm(γ, γ'), E=4.6 MeV bremsstrahlung; measured γ-spectra. 148,150,152,154Sm deduced deformation, transition B(λ). Nuclear resonance fluorescence.
doi: 10.1103/PhysRevLett.65.2515
Phys.Rev.Lett. 66, 2456 (1991); Erratum Phys.Rev.Lett. 69, 2999 (1992)
C.De Coster, K.Heyde
Magnetic Dipole Spin Resonance in Rare-Earth Nuclei
NUCLEAR STRUCTURE 148Nd, 154Sm, 164Dy, 174Yb; calculated B(M1). Quasiparticle RPA.
doi: 10.1103/PhysRevLett.66.2456
Phys.Scr. 43, 460 (1991)
C.Magnusson
The Effect of the Presence of Quadrupole Pairing on the Properties of K(π) = 1+ States in Doubly Even Nuclei
NUCLEAR STRUCTURE 156Gd, 164Dy, 154Sm; calculated B(M1). Quasiparticle RPA.
NUCLEAR REACTIONS 164Dy, 158,156Gd, 154Sm, 168Er, 174Yb(e, e'), E not given; calculated σ(θ). DWBA.
Phys.Rev. C43, R949 (1991)
C.Rangacharyulu, A.Richter, H.J.Wortche, W.Ziegler, R.F.Casten
Strong Correlation and Saturation of E2 and M1 Transition Strengths in Even-Even Rare-Earth Nuclei
NUCLEAR STRUCTURE 142,146,148,150Nd, 144,148,150,152,154Sm, 154,156,158,160Gd, 160,162,164Dy, 168Er; analyzed B(λ) data; deduced strong correlation between E2 and M1 strengths, strengths saturation.
Nucl.Phys. A522, 139c (1991)
A.Richter
Electron Scattering and Elementary Excitations
NUCLEAR REACTIONS 154Sm(γ, γ'), E ≈ 3.8-4.6 MeV; measured Eγ, Iγ. 144,148,150,152,154Sm levels deduced B(M1), K-mixing. Other data included.
doi: 10.1016/0375-9474(91)90055-B
Nucl.Phys. A564, 366 (1993)
W.Ziegler, N.Huxel, P.von Neumann-Cosel, C.Rangacharyulu, A.Richter, C.Spieler, C.De Coster, K.Heyde
Low-Energy Dipole-Strength Distributions in 148, 150, 152, 154Sm
NUCLEAR REACTIONS 148,150,152,154Sm(γ, γ'), E=2-4 MeV; measured nuclear resonance fluorescence spectra. 148,150,152,154Sm deduced levels, J, π, B(λ). Comparison QRPA, QTDA model calculations.
doi: 10.1016/0375-9474(93)90510-5
J.Phys.(London) G20, 315 (1994)
P.Sarriguren, E.Moya de Guerra, R.Nojarov, A.Faessler
Spin- and Deformation-Dependent Orbital M1 Strength in Rare-Earth Nuclei
NUCLEAR STRUCTURE 142,146,148,150Nd, 144,148,150,152,154Sm, 156,158Gd; calculated levels, B(λ), quadrupole moments, proton rms radii. Quasiparticle RPA, deformed Woods-Saxon potential, quadrupole-quadrupole, spin-spin residual interactions.
doi: 10.1088/0954-3899/20/2/010
Phys.Rev. C52, 3259 (1995)
R.Nojarov, A.Faessler, M.Dingfelder
Competing Electric and Magnetic Excitations in Backward Electron Scattering from Heavy Deformed Nuclei
NUCLEAR STRUCTURE 154Sm, 154,156,158Gd, 168Er; calculated B(λ), transition densities. Quasiparticle RPA.
NUCLEAR REACTIONS 154Sm, 154,156,158Gd, 168Er(e, e'), E not given; calculated σ(θ). DWBA, PWBA, quasiparticle RPA.
Nucl.Phys. A600, 335 (1996)
R.Nojarov, A.Faessler, M.Dingfelder
Orbital Response to Backward (e, e') Scattering at Low and High Excitation Energies
NUCLEAR STRUCTURE 154Sm; calculated levels, B(λ), transition densities. RPA.
NUCLEAR REACTIONS 154Sm(e, e'), E not given; calculated σ(θ). Plane wave, DWBA approaches, RPA transition densities.
doi: 10.1016/0375-9474(96)00031-0
J.Phys.(London) G25, 1023 (1999)
V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova, N.Lo Iudice
Dipole Strength Distribution in Doubly Even Deformed Nuclei
NUCLEAR STRUCTURE 154Sm, 168Er, 178Hf, 238U; calculated E1, M1 strength distributions; deduced orbital, spin contributions. RPA. Comparisons with data.
doi: 10.1088/0954-3899/25/5/307
Int.J.Mod.Phys. E9, 249 (2000)
A.A.Kuliev, R.Akkaya, M.Ilhan, E.Guliyev, C.Salamov, S.Selvi
Rotational-Invariant Model of the States with Kπ = 1+ and Their Contribution to the Scissors Mode
NUCLEAR STRUCTURE 144,148,150,152,154Sm; calculated B(M1) strength distributions; deduced scissors mode features. RPA, self-consistent calculations.
doi: 10.1016/S0218-3013(00)00017-9