References quoted in the ENSDF dataset: 168ER ADOPTED LEVELS, GAMMAS
56 references found.
Clicking on a keynumber will list datasets that reference the given article.
Z.Physik 170, 355 (1962)
E.Bodenstedt, H.J.Korner, E.Gerdau, J.Radeloff, L.Mayer, K.Auerbach, J.Braunsfurth, G.Mielken
Der g(R)-Faktor des 2+-Rotationsniveaus von Er168
NUCLEAR STRUCTURE 168Tm; measured not abstracted; deduced nuclear properties.
Phys.Rev. 161, 1185 (1967); R.P.Scharenberg - Priv.Comm. (April 1972)
J.D.Kurfess, R.P.Scharenberg
Pulsed-Beam Measurements of the Nuclear g Factors of the 2+ Rotational States in Neodymium-150, Dysprosium-162 and -164, Erbium-166, -168, and -170, and Tungsten-186
NUCLEAR REACTIONS 150Nd, 162,164Dy, 166,168,170Er, 186W(p, p'γ), E not given; measured pγ(θ, H, t). 150Nd, 162,164Dy, 166,168,170Er, 186W levels deduced T1/2, g. Pulsed beam technique.
Phys.Rev. 158, 1118 (1967)
R.S.Stevens, Jr., J.S.Eck, E.T.Ritter, Y.K.Lee, J.C.Walker
New Mossbauer Levels in the Rare Earths Following Coulomb Excitation
NUCLEAR STRUCTURE 160Gd, 155Gd, 156Gd, 158Gd, 164Dy, 168Er; measured not abstracted; deduced nuclear properties.
Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.731 (1968)
B.I.Deutch, G.B.Hagemann, K.A.Hagemann, S.Ogaza
Larmor Precession for the 4+ States in Some Erbium Isotopes
NUCLEAR REACTIONS 166,168,170Er(16O, 16O'γ), E not given; measured σ(Eγ, E(16O')), γγ(θ, H). 166,168,170Er levels deduced g, Larmor precession.
Z.Physik 208, 184 (1968)
E.Munck
Messung der Magnetischen Momente der Tiefsten 2-zustande fur Einige Dy-, Er- und Yb-Isotope
NUCLEAR REACTIONS 164Dy, 164,166,168Er, 170,172,174Yb(γ, γ), E=73-92 keV; measured Mossbauer effect. 164Dy, 164,166,168Er, 170,172,174Yb levels deduced g.
Nucl.Phys. A151, 401 (1970); G.Goldring - Priv.Comm. (April 1972)
I.Ben-Zvi, P.Gilad, M.B.Goldberg, G.Goldring, K.-H.Speidel, A.Sprinzak
Hyperfine Interaction Studies of Heavy Nuclei in Highly Ionized Atoms
NUCLEAR REACTIONS 148Nd, 150Sm, 152,154,156,158,160Gd, 160,162,164Dy, 168,170Er, 172,174Yb, 178Hf, 182,186W, 188,190Os(16O, 16O'γ), 186W(35Cl, 35Cl'γ), E ≈ 36 MeV; measured σ(θ(γ), pressure). 154Gd(16O, 16O'γ), E ≈ 36 MeV; measured σ(θ(γ), H). 152Gd(α, α'), E=10 MeV; measured σ(Eα'); deduced B(E2). 152Gd level deduced T1/2. 148Nd, 150Sm, 152,154,156,158,160Gd, 160,162,164Dy, 168,170Er, 172,174Yb, 178Hf, 182,186W, 188,190Os deduced g for 2+ levels. Enriched targets.
doi: 10.1016/0375-9474(70)90289-7
Phys.Rev. C1, 1184 (1970)
D.Hitlin, S.Bernow, S.Devons, I.Duerdoth, J.W.Kast, E.R.Macagno, J.Rainwater, C.S.Wu, R.C.Barrett
Muonic Atoms. I. Dynamic Hyperfine Structure in the Spectra of Deformed Nuclei
ATOMIC PHYSICS, Mesic-Atoms 150Nd, 152Sm, 162,164Dy, 168,170Er, 182,184,186W; measured μ-mesic X-ray spectra; deduced isotope shift, nuclear charge distributions.
ORNL-4513, p.56 (1970)
F.K.McGowan, W.T.Milner, R.O.Sayer, R.L.Robinson, P.H.Stelson
Electric Quadrupole Moments of States in 166,168,170Er, 172,174,176Yb, And 186W
NUCLEAR REACTIONS 166,168,170Er, 172,174,176Yb, 186W(16O, 16O'γ), E=42 MeV; 166,168,170Er, 172,174,176Yb, 186W(α, α'γ), E=12.5-15 MeV; measured (16O')(γ)-coin, α'γ-coin, Iγ. 166,168,170Er, 172,174,176Yb, 186W levels deduced quadrupole moment.
Nucl.Phys. A171, 92 (1971)
J.Lange, R.L.Rasera, H.F.Wagner, W.Schaffer
E2/M1 Mixing Ratios of γ-Transitions from the γ-Vibrational Band to the Ground State Band in 152Sm, 154Gd and 168Er
RADIOACTIVITY 152Eu[from 151Eu(n, γ)]; 154Eu[from 153Eu(n, γ)]; 168Tm[from 168Er(d, 2n)]; measured γγ(θ). 152Sm, 154Gd, 168Er deduced γ-mixing(E2/M1). Enriched targets.
doi: 10.1016/0375-9474(71)90366-6
Nucl.Phys. A180, 600 (1972)
J.M.Domingos, G.D.Symons, A.C.Douglas
Multiple Coulomb Excitation of γ-Vibrational Bands in 162Dy, 166Er, 168Er and 170Er
NUCLEAR REACTIONS 162Dy, 166,168,170Er(16O, 16O'γ), E=45, 59, 60 MeV; measured σ(E), I, (16O)(γ)(θ). 162Dy, 166,168,170Er deduced B(E2), γ-mixing, band-mixing parameters z2. Enriched targets; Ge(Li) detector.
doi: 10.1016/0375-9474(72)90882-2
Rev.Roum.Phys. 19, 233 (1974)
E.A.Ivanov, M.Ionescu-Bujor, C.Stoleriu, M.Zaharcu
Short-Lived Isomeric States Excited by Thermal Neutron Capture
NUCLEAR REACTIONS Ge, Ag, Sb, I, Cs, Eu, Tb, Ho, Er, Tm, Lu, Hf, W, Au(n, γ); measured γγ(t). 71Ge, 108,110Ag, 122Sb, 128I, 134Cs, 152Eu, 160Tb, 166Ho, 168Er, 170Tm, 177Lu, 198Au levels deduced T1/2.
Rev.Roum.Phys. 20, 273 (1975)
A.A.Abdurazakov, M.Budzinski, R.Ion-Mikhai, T.A.Islamov, V.A.Morozov, T.M.Muminov, M.Subotovich, V.I.Fominykh, K.Fuya, I.Kholbaev
New Information on the Decay 168Tm → 168Er
RADIOACTIVITY 168Tm; measured Eγ, Iγ, γγ-coin, I(ce), γγ(θ). 168Er deduced levels, J, π, λ, δ.
Z.Phys. A274, 359 (1975)
M.Behar, L.M.Quinones, Z.W.Grabowski
Multipole Mixing Ratios of Transitions in 168Er
RADIOACTIVITY 168Tm; measured γγ(θ, H, t); deduced attenuation factors. 168Er levels deduced λ, δ.
Nucl.Phys. A297, 51 (1978)
F.K.McGowan, W.T.Milner, R.L.Robinson, P.H.Stelson, Z.W.Grabowski
Coulomb Excitation of Vibrational-Like States in 166-170Er
NUCLEAR REACTIONS 166,168,170Er(α, α'γ), E=14 MeV; measured Iγ, Eγ, γ(θ). 166,168,170Er levels deduced B(E2), B(M1), B(E3), J, π, δ. Enriched targets.
doi: 10.1016/0375-9474(78)90198-7
Phys.Rev. C21, 2575 (1980)
A.Furusawa, M.Kanazawa, S.Hayashibe
g Factors of the 80 and 1094 keV States of 168Er
RADIOACTIVITY 168Tm; measured γγ-coin, γ(θ, t), γγ(θ, H), γγ(θ, H, t), Eγ, Iγ. 168Er levels deduced T1/2, g.
Phys.Lett. B94, 298 (1980)
K.Schreckenbach, W.Gelletly
The Nature of M1 Admixtures in Intra-Band Transitions in the γ-Vibrational Band
NUCLEAR REACTIONS 167Er(n, e-), E=thermal; measured I(L X-ray), ICC ratios. 168Er levels deduced M1 admixtures, δ in intra-band transitions.
doi: 10.1016/0370-2693(80)90882-5
Hyperfine Interactions 11, 29 (1981)
J.A.Hodges, G.Jehanno, A.Schuhl, Y.Berthier
The Nuclear Magnetic Moment of the I = 2 80.56 keV Mossbauer Level of 166Er
NUCLEAR MOMENTS 166Er; measured Mossbauer effect in ErFe2, ErZn, ErAl2. 167Er; measured NMR in ErFe2, ErZn, ErAl2. 166Er level deduced μ.
NUCLEAR REACTIONS 166Er(γ, γ), E=80.56 keV; measured Mossbauer spectra in ErFe2, ErZn, ErAl2.
J.Phys.Soc.Jpn. 50, 3191 (1981)
T.Iwashita
Gamma-Gamma Directional Correlation in the Decay of 168Tm
RADIOACTIVITY 168Tm(EC); measured γγ(θ), γγ(θ, t), oriented nuclei. 168Er transitions deduced δ, transition probability.
J.Phys.(London) B16, L557 (1983)
V.Pfeufer, W.J.Childs, L.S.Goodman
Crossed-Second-Order Effects in the Isotope Shift of the Ground Configuration 4f126s2 of Er I
NUCLEAR MOMENTS 170,168Er; measured optical isotope shifts. High resolution laser atomic beam spectroscopy.
doi: 10.1088/0022-3700/16/19/001
Z.Phys. A322, 1 (1985)
A.Bernard, H.Bruggemeyer, V.Pfeufer
Changes in Mean-Square Nuclear Charge Radii in Er from Optical Isotope Shifts by Laser-Atomic Beam Spectroscopy
NUCLEAR MOMENTS 164,166,168,170,172,162Er; measured isotope shifts. 167Er deduced magnetic dipole, electric quadrupole constants. 162,164,166,167,168,170Er deduced rms charge radii relative changes.
Nucl.Phys. A442, 424 (1985)
D.G.Burke, B.L.W.Maddaock, W.F.Davidson
Two-Quasineutron States in 168Er Populated by the 167Er(d, p) and 167Er(t, d) Reactions
NUCLEAR REACTIONS 167Er(d, p), E=12 MeV; measured σ(E(p), θ); 167Er(t, d), E=15 MeV; measured σ(E(d), θ). 168Er deduced levels, J, π, band structure two-quasineutron assignments. Enriched targets.
Nucl.Phys. A445, 70 (1985)
D.G.Burke, W.F.Davidson, J.A.Cizewski, R.E.Brown, J.W.Sunier
Two-Quasiproton States in 168Er Studied by the 169Tm(t(pol), α)168Er Reaction
NUCLEAR REACTIONS 169Tm(polarized t, α), E=17 MeV; measured σ(θ), σ(E(α), θ). 168Er deduced levels, J, π, K, two-quasiparticle Nilsson assignments.
doi: 10.1016/0375-9474(85)90361-6
Hyperfine Interactions 24, 159 (1985)
R.Neugart
Collinear Laser Spectroscopy on Unstable Isotopes - A Tool of Nuclear Physics
RADIOACTIVITY 151Dy(EC), (β+), (α); 208,222Ra(α); 232Ra [from 238Ra(p, X), E=600 MeV]; measured hfs. Collinear laser spectroscopy.
NUCLEAR MOMENTS 158,160,162,164,166,168,170,172,174,176Yb, 152,156,158,160,162,164,166,168,170Er, 148,150,152,154,156,158,160,162,164Dy, 136,138,140,142,144,146Ba; measured isotope shifts; deduced rms charge radii. Collinear laser spectroscopy.
Hyperfine Interactions 34, 17 (1987)
S.A.Ahmad, P.M.Rao, A.Venugopalan, G.D.Saksena
Evaluation of Changes in Mean-Square Nuclear Charge Radii of Stable Isotopes of Erbium
NUCLEAR MOMENTS 162,164,166,168,170Er; measured optical isotope shifts; deduced rms charge radii.
Phys.Rev. C35, 1468 (1987)
R.A.Meyer, D.R.Nethaway, A.L.Prindle, R.P.Yaffe
Octupole State Properties in 168Er and the Two-Neutron ([521 1/2][633 7/2]) Configurational Pair
RADIOACTIVITY 168Tm(EC), (β-) [from 169Tm(n, 2n), E=14.8, 40 MeV, Ta spallation]; measured Eγ, Iγ; deduced log ft. 168Er deduced levels, T1/2, B(λ), J, π, K, configurations, octupole band K mixing.
Phys.Rev. C35, 1574 (1987)
H.Okamura, S.Matsuki
Isotope Shift in Erbium I by Laser-Atomic-Beam Spectroscopy
NUCLEAR MOMENTS 162,164,166,167,168,170Er; measured optical isotope shift; deduced field shift, hfs constants. 162,164,166,167,168,170Er deduced relative rms charge radii changes. Laser atomic beam spectroscopy, natural Er target.
J.Phys.(London) G14, Supplement S97 (1988)
P.Petkov, W.Andrejtscheff, Ch.Protochristov, W.D.Hamilton, F.Hoyler, V.V.Martynov
Absolute E0, E1 and E2 Transition Rates in Even-Even Nuclei Obtained in Thermal Neutron Capture
NUCLEAR REACTIONS 167Er, 195Pt, 123Te(n, γ), E=thermal; measured γγ(θ, t), time-related γ-spectra. 168Er, 196Pt, 124Te levels deduced T1/2, B(λ).
NUCLEAR STRUCTURE 172Yb; analyzed data; deduced level characteristics, B(λ).
Phys.Rev. C40, 2035 (1989)
C.E.Doran, A.E.Stuchbery, H.H.Bolotin, A.P.Byrne, G.J.Lampard
Gyromagnetic Ratios in 164Dy and 168Er
NUCLEAR REACTIONS 168Er, 164Dy(58Ni, 58Ni'), E=150, 160, 220 MeV; measured γ(58Ni)-coin, γγ(θ, H). 164Dy, 168Er deduced levels, relative g factors.
NUCLEAR STRUCTURE 164Dy, 166,168Er; calculated levels, g. Semi-empirical aligned quasiparticle model.
At.Data Nucl.Data Tables 42, 189 (1989)
P.Raghavan
Table of Nuclear Moments
COMPILATION Z=1-99; compiled μ, electric quadrupole moments.
doi: 10.1016/0092-640X(89)90008-9
J.Phys.Soc.Jpn. 59, 3148 (1990)
W.G.Jin, T.Horiguchi, M.Wakasugi, Y.Yoshizawa
Hyperfine Structure and Isotope Shift in Er I by the Atomic-Beam Laser Spectroscopy
NUCLEAR MOMENTS 162,164,166,167,168,170Er; measured hfs, isotope shifts; deduced hyperfine parameters. 162,164,166,167,168,170Er deduced rms charge radii, deformation parameter values.
Phys.Rev.Lett. 66, 691 (1991)
H.G.Borner, J.Jolie, S.J.Robinson, B.Krusche, R.Piepenbring, R.F.Casten, A.Aprahamian, J.P.Draayer
Evidence for the Existence of Two-Phonon Collective Excitations in Deformed Nuclei
NUCLEAR REACTIONS Er(n, γ), E=thermal; measured γ Doppler shift. 168Er levels deduced T1/2, B(λ), collectivity features. GRID technique.
doi: 10.1103/PhysRevLett.66.691
J.Phys.(London) G17, 1683 (1991)
W.F.Davidson, W.R.Dixon
Identification of Rotational Bands at Intermediate Excitation in 168Er
NUCLEAR REACTIONS 167Er(n, γ), E=thermal; measured Eγ, Iγ. 168Er deduced levels, radiative decay, transition γ-multipolarity, J, π, band structure. Curved-crystal spectometers, intrinsic Ge spectrometer.
doi: 10.1088/0954-3899/17/11/015
PIRS-0288/NRC (1991)
W.F.Davidson, W.R.Dixon
Identification of Rotational Bands at Intermediate Excitation in 168Er
NUCLEAR REACTIONS 167Er(n, γ), E not given; measured Eγ, Iγ. 168Er deduced levels, J, π, band structure. Curved-crystal spectrometer.
Phys.Rev. C44, 2213 (1991)
C.C.Dey, B.K.Sinha, R.Bhattacharya, S.K.Basu
Measurements of Subnanosecond Nuclear Lifetimes
RADIOACTIVITY 133Ba, 177,175Hf, 177Lu, 168Tm [from 165Ho(α, n), E=35 MeV]; 95Zr; measured γγ-coin, βγ-coin. 95Nb, 133Cs, 175Lu, 168Er deduced level T1/2. 177Hf deduced level T1/2, μ.
Nucl.Phys. A533, 49 (1991)
P.Petkov, W.Andrejtscheff, J.Copnell, S.J.Robinson
E1 and M1 Transition Strengths from Two-Quasiparticle Structures in 168Er
NUCLEAR REACTIONS 167Er(n, γ), E=thermal; measured Eγ, Iγ, γγ(t). 168Er levels deduced T1/2, B(λ). Natural target, Ge detectors, generalized centroid-shift analysis, E1 systematics.
doi: 10.1016/0375-9474(91)90819-R
Phys.Rev. C45, 1549 (1992)
F.Brandolini, P.Pavan, D.Bazzacco, C.Rossi-Alvarez, R.V.Ribas, M.De Poli, A.M.I.Haque
g Factors for Yrast States in Isotopic Doublets 156,158Gd and 166,168Er
NUCLEAR REACTIONS 156,158Gd(58Ni, 58Ni'), 166,168Er(58Ni, 58Ni'), E=130-217 MeV; measured γ(θ, H, T) in polarized Gd, Fe, (particle)γ-coin, following Coulomb excitation. 156,158Gd, 166,168Er levels deduced g-factors of ground state rotational bands. Cranked shell model and cranked HFB calculations. Thin foil transient-field IMPAC technique.
Z.Phys. D22, 569 (1992)
H.-D.Kronfeldt, D.Ashkenasi, H.M.Nikseresht
Crossed-Second-Order Effects in the Isotope Shift for 170-166Er and 168-166Er in the Configuration 4f126s2
NUCLEAR MOMENTS 170,168,166Er; measured isotope shifts; deduced J, term dependence, cross-second-order effects parameters. High resolution interference, intermodulated optogalvanic saturation spectroscopy.
Z.Phys. A355, 277 (1996)
I.Alfter, E.Bodenstedt, W.Knichel, J.Schuth
Observation of a Strong Correlation between g(2+γvib) and g(2+rot) in Strongly deformed nuclei
RADIOACTIVITY 154Eu(β-) [from 153Eu thermal neutron irradiation]; 166mHo(β-) [from 165Ho thermal neutron irradiation]; 168Tm(EC), (β+) [from 168Er(d, 2n)]; measured γγ-directional correlations. 154Gd, 166,168Er deduced γ-vibrational bands δ(E2/M1), B(λ).
Nucl.Phys. A600, 272 (1996)
F.Brandolini, C.Cattaneo, R.V.Ribas, D.Bazzacco, M.De Poli, M.Ionescu-Bujor, P.Pavan, C.Rossi-Alvarez
g-Factors in the Ground State and γ-Bands in 164,166,168Er
NUCLEAR REACTIONS 164,166,168Er(58Ni, 58Ni'), E=165, 210, 225 MeV; measured γ(θ, H, T) in polarized Gd, (particle)-γ-coin following Coulomb excitation. 164,166,168Er levels deduced g factors. Enriched targets, thin foil transient field IMPAC technique. Cranked Hartree-Fock-Bogoliubov, interacting boson, geometrical collective model, projected angular momentum shell models.
doi: 10.1016/0375-9474(96)00003-6
Phys.Rev. C53, 2749 (1996)
H.Maser, S.Lindenstruth, I.Bauske, O.Beck, P.von Brentano, T.Eckert, H.Friedrichs, R.D.Heil, R.-D.Herzberg, A.Jung, U.Kneissl, J.Margraf, N.Pietralla, H.H.Pitz, C.Wesselborg, A.Zilges
Systematics of Low-Lying Dipole Excitations in the Deformed Even-Even Nuclei 164,166,168,170Er
NUCLEAR REACTIONS 164,166,168,170Er(γ, γ'), E ≤ 4.1 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry. 164,166,168,170Er deduced levels, J, π, K, Γ0, B(λ). Enriched targets.
Nucl.Phys. A635, 273 (1998)
I.Alfter, E.Bodenstedt, W.Knichel, J.Schuth
Multipole Mixing Parameters of γ-Transitions between the γ-Vibrational Band and the Ground State Rotational Band of 168Er and F-Spin Violation
RADIOACTIVITY 168Tm(EC) [from 168Er(d, 2n)]; measured Eγ, Iγ, γγ(θ). 168Er deduced interband transitions δ. Data from other nuclei compared.
doi: 10.1016/S0375-9474(98)00150-X
Phys.Rev. C57, 569 (1998)
H.Lehmann, J.Jolie, F.Corminboeuf, H.G.Borner, C.Doll, M.Jentschel, R.F.Casten, N.V.Zamfir
Lifetimes of the Lowest 2+(K(π) = 0+) Levels in 168Er and 164Dy
NUCLEAR REACTIONS 167Er, 163Dy(n, γ), E=reactor; measured Eγ, Iγ. 168Er, 164Dy deduced levels T1/2, B(E2)B(M1), excited K(π)=0+ band configurations. Gamma-ray induced Doppler broadening technique. Several models compared.
Nucl.Phys. A651, 323 (1999)
J.L.Wood, E.F.Zganjar, C.De Coster, K.Heyde
Electric Monopole Transitions from Low Energy Excitations in Nuclei
NUCLEAR STRUCTURE A=12-238; compiled, analyzed electric monopole transition strengths; deduced role of deformation, shape coexistence.
doi: 10.1016/S0375-9474(99)00143-8
Eur.Phys.J. D 11, 197 (2000)
D.Ashkenasi, S.Kroger, H.-D.Kronfeldt
Finestructure, Hyperfine Structure and Isotope Shift of 4f126d7s in Er I
NUCLEAR MOMENTS 164,166,167,168,170Er; measured hfs, isotope shifts. Doppler-reduced saturation absorption spectroscopy.
Phys.Rev. C62, 034313 (2000)
L.Genilloud, J.Jolie, H.G.Borner, H.Lehmann, F.Becvar, M.Krticka, N.V.Zamfir, R.F.Casten
Lifetimes of Negative Parity States in 168Er
NUCLEAR REACTIONS 167Er(n, γ), E=reactor; measured Doppler-broadened Eγ, Iγ. 168Er levels deduced T1/2, B(E1). Gamma-ray induced Doppler broadening technique. Comparison with IBA model predictions.
doi: 10.1103/PhysRevC.62.034313
Fiz.Elem.Chastits At.Yadra 31, 1496 (2000); Phys.Part.Nucl. 31, 764 (2000)
E.P.Grigoriev
Structure of Even Erbium Isotopes
NUCLEAR STRUCTURE 150,152,154,156,158,160,162,164,166,168,170Er; analyzed levels, J, π, rotational bands features; deduced parameters. Neighboring isotones also discussed. Quasiparticle vibrational model.
Phys.Rev. C63, 044308 (2001)
J.B.Gupta, J.H.Hamilton, A.V.Ramayya
Microscopic Study of the 168Er Multiphonon Band Structure
NUCLEAR STRUCTURE 168Er; calculated levels, J, π, B(E2); deduced multiphonon band structure. Dynamic deformation theory.
doi: 10.1103/PhysRevC.63.044308
Yad.Fiz. 65, 673 (2002); Phys.Atomic Nuclei 65, 641 (2002)
E.P.Grigoriev
Band Interaction in 162Dy, 168Er, and 172Yb
NUCLEAR STRUCTURE 162Dy, 168Er, 172Yb; calculated rotational band level energies, Coriolis interaction strength between bands. Comparisons with data.
doi: 10.1134/1.1471266
Z.Naturforsch. 57a, 591 (2002)
P.Thakur, M.S.Behra, R.Dogra, A.K.Bhati, S.C.Bedi
Static Electric Quadrupole Moments in the Ground State and K = 4-1 Bands in 168Er
RADIOACTIVITY 168Tm(EC) [from 168Er(p, n), E=12 MeV]; measured Eγ, Iγ(θ, t), γγ-coin, Time Dependent Perturbed Angular Correlation. 168Er; deduced ratios of quadrupole moments and deformation parameters.
Nucl.Phys. A729, 337 (2003)
G.Audi, A.H.Wapstra, C.Thibault
The AME2003 atomic mass Evaluation (II). Tables, graphs, and references
COMPILATION A=1-293; compiled, evaluated atomic mass data.
doi: 10.1016/j.nuclphysa.2003.11.003
Phys.Rev. C 68, 044305 (2003)
C.Y.Wu, D.Cline, M.W.Simon, R.Teng, K.Vetter, M.P.Carpenter, R.V.F.Janssens, I.Wiedenhover
Kπ=4- isomers and their rotational bands in 168, 170Er
NUCLEAR REACTIONS 168,170Er(238U, 238U'), E=1358 MeV; measured prompt and delayed Eγ, Iγ, γγ-, (particle)γ-coin. 168,170Er deduced levels, J, π, rotational bands, B(E1), configurations. Gammasphere, Chico arrays.
doi: 10.1103/PhysRevC.68.044305
At.Data Nucl.Data Tables 87, 185 (2004)
I.Angeli
A consistent set of nuclear rms charge radii: properties of the radius surface R(N, Z)
COMPILATION A=1-248; compiled, analyzed charge radii.
doi: 10.1016/j.adt.2004.04.002
IAEA-STI/PUB/1263 (2007)
H.D.Choi, R.B.Firestone, R.M.Lindstrom, G.L.Molnar, S.F.Mughabghab, R.Paviotti Corcuera, Z.Revay, A.Trkov, V.Zerkin, C.Zhou
Database of Prompt Gamma Rays from Slow Neutron Capture for Elemental Analysis
COMPILATION Z=1-92; compiled Eγ, Iγ from neutron capture.
Priv.Comm. (2009)
G.Audi, W.Meng, D.Lunney, B.Pfeiffer
Atomic Mass Evaluation 2009
Phys.Rev. C 81, 054313 (2010)
G.D.Dracoulis, G.J.Lane, F.G.Kondev, H.Watanabe, D.Seweryniak, S.Zhu, M.P.Carpenter, C.J.Chiara, R.V.F.Janssens, T.Lauritsen, C.J.Lister, E.A.McCutchan, I.Stefanescu
Two-quasiparticle structures and isomers in 168Er, 170Er, and 172Er
NUCLEAR REACTIONS 170Er(136Xe, X)168Er/170Er/172Er, E=830 MeV; measured Eγ, Iγ, γγ, γγ(t), and isomer half-lives using Gammasphere array. 168,170,172Er; deduced levels, J, π, rotational bands, multipolarities, B(E1), B(M1), B(E2), K-hindrance factors, configurations, quasiparticle structures, and gK-gR.
doi: 10.1103/PhysRevC.81.054313
Chin.Phys.C 36, 1603 (2012)
M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer
The AME2012 atomic mass evaluation (II). Tables, graphs and references
COMPILATION A=1-295; compiled, evaluated atomic mass data.