References quoted in the ENSDF dataset: 162DY ADOPTED LEVELS, GAMMAS

95 references found.

Clicking on a keynumber will list datasets that reference the given article.

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1959BI10

Phys.Rev. 116, 730 (1959)

M.Birk, G.Goldring, Y.Wolfson

Lifetime of 2⁺ Rotational States

doi: 10.1103/PhysRev.116.730

1961HA23

Phys.Rev. 123, 1758 (1961)

B.Harmatz, T.H.Handley, J.W.Mihelich

Nuclear Levels in a Number of Even-Even Rare Earths (150 < A < 184)

NUCLEAR STRUCTURE ¹⁷²Lu, ¹⁸²Re, ¹⁸⁴Re, ¹⁶⁶Tm, ¹⁵⁰Eu, ¹⁵²Tb, ¹⁴⁹Eu, ¹⁶²Ho, ¹⁵⁶Tb, ¹⁵⁴Tb, ¹⁴⁸Pm; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.123.1758

1961JO10

Nuclear Phys. 24, 443 (1961)

M.Jorgensen, O.B.Nielsen, O.Skilbreid

Levels in Ho¹⁶² and Dy¹⁶²

NUCLEAR STRUCTURE ¹⁶²Ho; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(61)90411-4

1963LI04

Phys.Rev. 129, 2664 (1963)

A.Li, A.Schwarzschild

Lifetimes of 4⁺ and 2⁺ States in the Rotational Nuclei Dy¹⁶⁰, Dy¹⁶², Er¹⁶⁶, Er¹⁶⁸, and Hf¹⁸⁰

NUCLEAR STRUCTURE ¹⁸⁰Hf, ¹⁶⁰Tb, ¹⁶²Ho, ¹⁶⁸Tm, ¹⁶⁶Ho, ⁶⁰Co; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.129.2664

1965BE40

Nucl.Phys. 65, 1 (1965)

D.R.Bes, P.Federman, E.Maqueda, A.Zuker

Properties of the γ-Vibrational State

NUCLEAR STRUCTURE ¹⁵⁰Nd, ^152,154Sm, ^{154,156,158,160}Gd, ^{156,158,160,162,164}Dy, ^{162,164,166,168,170}Er, ^{170,172,174,176}Yb, ^176,178,180Hf, ^182,184,186W, ¹⁸⁶Os, ^{228,230,232,234}Th, ^{230,232,234,236,238}U, ^238,240,242Pu, ^{242,244,246,248}Cm, ^{248,250,252,254}Cf, ^{250,252,254,256}Fm; calculated B(E2).

doi: 10.1016/0029-5582(65)90290-7

1965SO04

At.Energy Rev. 3, No.2, 117 (1965)

V.G.Solovev

Non-Rotational Collective States of Deformed Even-Even Nuclei

NUCLEAR STRUCTURE ¹⁵⁰Nd, ^152,154Sm, ^{154,156,158,160}Gd, ^{158,160,162,164}Dy, ^{164,166,168,170}Er, ^{168,172,174,176}Yb, ^174,176,178Hf, ^{180,182,184,186}W, ^184,186,188Os, ^{228,230,232,234}Th, ^{232,234,236,238}U, ^{236,238,240,242}Pu, ^242,244,246Cm, ^250,252Cf, ^252,254Fm; calculated levels.

1967AS03

Nucl.Phys. A101, 51 (1967)

D.Ashery, N.Bahcall, G.Goldring, A.Sprinzak, Y.Wolfson

Lifetime Measurements of Some Rotational Levels by a New Recoil Method (II)

NUCLEAR REACTIONS ¹⁶¹Dy, ¹⁷¹Yb, ^166,167Er, ^183,184W, ¹⁹⁰Os(¹⁶O, ¹⁶O'γ), E not given; measured σ(E(¹⁶O'), Eγ). ¹⁶¹Dy level deduced gR. ¹⁶¹Dy, ¹⁷¹Yb, ^166,167Er, ¹⁸³W, ¹⁸⁴W, ¹⁸⁶W, ¹⁹⁰Os levels deduced T_1/2.

doi: 10.1016/0375-9474(67)90287-4

1967BA34

Phys.Rev. 160, 1011 (1967)

A.Backlin, A.Suarez, O.W.B.Schult, B.P.K.Maier, U.Gruber, E.B.Shera, D.W.Hafemeister, W.N.Shelton, R.K.Sheline

Nuclear Levels of Dy¹⁶²

NUCLEAR STRUCTURE ¹⁶²Dy, ¹⁶³Dy; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.160.1011

1967HE15

Z.Physik 207, 505 (1967)

W.Henning, D.Heunemann, W.Weber, P.Kienle, H.J.Korner

Mossbauer Effect and Nuclear Moments of the 75 keV State of Dy¹⁶¹ and the 81 keV State of Dy¹⁶²

NUCLEAR REACTIONS ¹⁶¹Dy(γ, γ), E=74.5 keV; measured Mossbauer effect. ¹⁶¹Dy level; deduced μ, quadrupole moment. ¹⁶²Dy(γ, γ), E=80.7 keV; measured Mossbauer effect. ¹⁶²Dy level deduced μ.

1967KU07

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 T_1/2, g. Pulsed beam technique.

doi: 10.1103/PhysRev.161.1185

1968BR03

Z.Physik 209, 197 (1968)

R.Brenn, L.Lehmann, H.Spehl

Hyperfine Fields on Recoil Implanted Nuclei 62 < Z < 74 in a Polarized Fe-, Co- and Ni-Environment

NUCLEAR STRUCTURE ¹⁶⁶Er, ¹⁶⁴Dy, ¹⁶³Dy, ¹⁶⁸Er, ¹⁶⁷Er, ¹⁷⁰Er, ¹⁸⁴W, ¹⁸⁶W, ¹⁸²W, ¹⁸⁰Hf, ¹⁷⁶Hf, ¹⁷⁶Yb, ¹⁷⁸Hf, ¹⁵²Sm, ¹⁵⁴Sm, ¹⁶⁰Gd, ¹⁵⁵Gd, ¹⁵⁸Gd, ¹⁵⁷Gd, ¹⁵⁶Gd, ¹⁶²Dy; measured not abstracted; deduced nuclear properties.

1968DE36

Physica 39, 393 (1968)

J.W.M.Dekker, P.F.A.Klinkenberg, J.F.Langkemper

Optical Isotope Shifts and Nuclear Deformation in Dysprosium

NUCLEAR MOMENTS ^{156,158,160,161,162,163,164}Dy; measured isotope shift; deduced quadrupole moment, nuclear deformation parameters.

doi: 10.1016/0031-8914(68)90092-X

1968GR08

Nucl.Phys. A110, 385 (1968)

T.Grotdal, K.Nybo, T.Thorsteinsen, B.Elbek

Collective Vibrational States in Even Dysprosium Nuclei

NUCLEAR REACTIONS ^{156,158,160,162,164}Dy(d, d'). Ed=12 MeV; measured σ(Ed', θ). ^{156,158,160,162,164}Dy deduced levels, J, B(E2), B(E3). Enriched target.

doi: 10.1016/0375-9474(68)90548-4

1968SE02

Phys.Rev. 166, 1227 (1968)

B.Sethi, S.K.Mukherjee

Half-Lives of the Excited States of ⁴⁶Ti, ⁸⁴Rb, ⁹⁹Tc, ¹⁶²Dy, ¹⁶⁴Er, and ¹⁹⁶Au

NUCLEAR STRUCTURE ¹⁶⁴Ho, ¹⁶²Tb, ⁴⁶Sc, ¹⁹⁶Au, ⁸⁴Rb, ⁹⁹Mo; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.166.1227

1969CHZP

Contrib.Intern.Conf.Properties Nucl.States, Montreal, Canada, p.72 (1969)

M.Chen

The Analysis of Muonic X-Ray Spectra of Deformed Nuclei

ATOMIC PHYSICS, Mesic-Atoms ¹⁵⁰Nd, ¹⁵²Sm, ^162,164Dy, ^168,170Er, ^182,184,186W; measured muonic X-ray spectra; deduced quadrupole moment, nuclear charge distributions.

1969HO17

Z.Physik 225, 327 (1969)

V.Honig

Messung von Halbwertszeiten K-Verbotener Ubergange in gg-Kernen der Seltenen Erden

RADIOACTIVITY ¹⁶²Ho, ¹⁷⁶Ta; measured Xγ-delay. ¹⁶²Dy level deduced T_1/2. ¹⁷⁶Hf level deduced J, π, T_1/2.

1970BE36

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, ^{152,154,156,158,160}Gd, ^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 T_1/2. ¹⁴⁸Nd, ¹⁵⁰Sm, ^{152,154,156,158,160}Gd, ^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

1970GA12

Yad.Fiz. 11, 1200 (1970); Sov.J.Nucl.Phys. 11, 667 (1970)

F.A.Gareev, S.P.Ivanova, V.V.Pashkevich

Study of Equilibrium Deformations β₂₀ and β₄₀ of Nuclei of the Rare-Earth and Transuranium Regions as Functions of the Single-Particle Characteristics of the Deformation Parameters

NUCLEAR STRUCTURE ^152,154,156Sm, ^{152,154,156,158,160,162}Gd, ^{156,158,160,162,164}Dy, ^160,162,164Er, ^182,184,186W, ^182,184Os, ^{224,226,228,230,232,234,236}Th, ^{228,230,232,234,236,238,240,242}U, ^{234,236,238,240,242}Pu; calculated quadrupole moment, deformation parameters β₂₀, β₄₀. Saxon-Woods potential.

1970HI03

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.

doi: 10.1103/PhysRevC.1.1184

1970KU06

Phys.Lett. 32B, 29 (1970)

K.Kubo, R.Broglia, C.Riedel, T.Udagawa

Determination of the Y₄ Deformation Parameter from the (p, t) Reaction

NUCLEAR REACTIONS ¹⁵⁸Gd, ¹⁶⁴Dy, ¹⁷²Yb, ¹⁷⁶Hf, ¹⁸⁴W(p, t), E=51.7 MeV; measured nothing; analyzed σ(θ) data. ¹⁵⁶Gd, ¹⁶²Dy, ¹⁷⁰Yb, ¹⁷⁴Hf, ¹⁸²W deduced deformation parameter Y₄.

doi: 10.1016/0370-2693(70)90327-8

1970NE02

Nucl.Phys. A145, 33 (1970)

K.Neergard, P.Vogel

Low-Lying Octupole States of the Doubly Even Deformed Nuclei with 152 < A < 190

NUCLEAR STRUCTURE ^{154,156,158,160}Gd, ^{156,158,160,162,164}Dy, ^{162,164,166,168,170}Er, ^{168,170,172,174,176}Yb, ^{174,176,178,180}Hf, ^182,184,186W, ^186,188,190Os; calculated levels, B(E3), deformation parameters β₃. Quasiparticle RPA, pairing+(octupole-octupole) force.

doi: 10.1016/0375-9474(70)90309-X

1970RA43

Indian J.Phys. 44, 198 (1970)

M.S.Rajput, A.Augusthy

E₂ Transition Probabilities in Even Nuclei

NUCLEAR STRUCTURE ^152,154Sm, ^154,156Gd, ¹⁶²Dy, ^164,166Er, ¹⁶⁸Yb, ¹⁷⁸Hf, ^180,182,184W, ^188,190Os, ^194,196Pt, ¹⁹⁸Hg, ^228,230,232Th, ^234,238U, ^238,240Pu; calculated B(E2) for 2+ - 0+ transitions.

1970SA12

Physica 47, 92 (1970)

G.D.Saksena, S.A.Ahmad

Nuclear Deformation and Optical Isotope Shifts in the Region N = 88-90

NUCLEAR STRUCTURE ^{142,144,146,148,150}Nd, ^{144,146,148,150,152}Sm, ^{150,152,154,156,158,160}Gd, ^{154,156,158,160,162,164}Dy; calculated deformation parameters β, moments of inertia, isotope shift.

doi: 10.1016/0031-8914(70)90102-3

1970VA21

Nucl.Phys. A151, 459 (1970)

C.W.E.van Eijk, F.Schutte

The Kα₁ X-Ray Isotopic Shift for ¹⁶²Dy-¹⁶⁴Dy and the Differences in Nuclear Charge Radii of Dy Isotopes

NUCLEAR MOMENTS ^162,164Dy measured isotope shift of Kα₁ X-ray. ^{156,158,160,161,162,163,164}Dy deduced change in nuclear charge radius.

doi: 10.1016/0375-9474(70)90390-8

1971SU01

J.Phys.Soc.Jap. 30, 602 (1971)

Y.Sugiyama, J.Kokame, T.Seuhiro, Y.Saji, H.Ogata, A.Stricker, I.Nonaka, Y.Ishizaki

The (p, t) Reaction on Even-Even Deformed Nuclei

NUCLEAR REACTIONS ¹⁵⁸Gd, ¹⁶⁴Dy, ¹⁷²Yb, ¹⁷⁶Hf, ¹⁸⁴W(p, t), E=51.7 MeV; measured σ(Et, θ). ¹⁵⁸Gd, ¹⁶⁴Dy, ¹⁷²Yb, ¹⁷⁶Hf, ¹⁸⁴W deduced deformation parameters β₄.

1971WO09

Nucl.Phys. A174, 353 (1971)

J.L.Wood, D.S.Brenner

The Decay of ¹⁶²mHo to Levels in ¹⁶²Dy

RADIOACTIVITY ^162mHo[from ¹⁵⁹Tb(α, n)]; measured Eγ, Iγ, T_1/2; deduced log ft. ¹⁶²Dy deduced levels, J, π, γ-multipolarities. Ge(Li) detectors.

doi: 10.1016/0375-9474(71)90668-3

1972DO01

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

1972NE02

J.Inorg.Nucl.Chem. 34, 423 (1972)

B.Neidhart, K.Bachmann

Untersuchung der bei der Wechselwirkung von Hochenergetischen Protonen mit Tantalkernen entstehenden Lanthanidruckstossprodukte-III. Kinetische Energien und Impulse der Lanthanide bei 580 MeV und 19 GeV Protonenenergie

NUCLEAR REACTIONS Ta(p, X), E=0.58, 19 GeV; measured recoil properties of lanthanide nuclides.

doi: 10.1016/0022-1902(72)80418-4

1972NE21

Izv.Akad.Nauk SSSR, Ser.Fiz. 36, 2555 (1972); Bull.Acad.Sci.USSR, Phys.Ser. 36, 2220 (1973)

L.A.Neiburg, P.T.Prokofev, Y.Y.Tamberg

Splitting of Multiplets of Deformed Nuclei in A = 150-190 Region

NUCLEAR STRUCTURE ^156,158Gd, ^156,158,160Tb, ^158,160,162Dy, ^161,164,166Ho, ^166,168Er, ^170,172Tm, ^172,175Yb, ^{170,172,174,175,176,177}Lu, ^178,180Hf, ¹⁸²Ta, ^179,182W, ^182,186,188Re; calculated splitting of 2-, 3-quasiparticle multiplets.

1972WE05

Nucl.Phys. A185, 1 (1972)

L.Weaver, L.C.Biedenharn

Nuclear Rotational Bands and SL(3, R) Symmetry

NUCLEAR STRUCTURE ¹⁵²Sm, ¹⁶⁶Er, ¹⁷²Yb, ¹⁷⁴Yb, ¹⁷⁶Yb, ¹⁵⁴Gd, ¹⁵⁶Gd, ^158,160Gd, ^156,158Dy, ^160,162Dy, ¹⁶⁴Dy, ¹⁶⁸Er, ¹⁵⁸Yb, ^182,184W; calculated B(E2). SL(3, R) symmetry representation.

doi: 10.1016/0375-9474(72)90548-9

1973AB06

Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1007 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.5, 82 (1974)

S.K.Abdulvagabova

Excitation of the 0⁺ States in Two-Nucleon Transfer Reactions in Rare-Earth Nuclei

NUCLEAR STRUCTURE ^150,152Nd, ^152,154,156Sm, ^154,156,158Gd, ^{156,158,160,162}Dy, ^{162,164,166,168,170}Er, ^{168,170,172,174}Yb, ^174,176,178Hf; calculated 0+ levels, B(EL), S(p, t), S(t, p).

1973CH28

Nucl.Phys. A213, 117 (1973)

A.Charvet, R.Chery, R.Duffait, M.Morgue, J.Sau

Lifetimes and Structures of Some Levels Above 1.5 MeV in ¹⁶⁸Yb, ¹⁶⁴Er and ^158,160,162Dy

RADIOACTIVITY ^168g,168mLu [from ¹⁶⁹Tm(α, 5n)]; ^164mTm [from ¹⁶⁵Ho(α, 5n)]; ^{158g,160g,162m}Ho [from ¹⁵⁹Tb(α, xn)]; measured Iγ, Eγ, γγ(t). ¹⁶⁸Yb, ¹⁶⁴Er, ^158,160,162Dy deduced levels, T_1/2. Natural targets; plastic, NaI(Tl), Ge(Li) detectors.

doi: 10.1016/0375-9474(73)90186-3

1973GU09

Phys.Rev. C7, 2476 (1973)

R.K.Gupta

Asymmetric Shape of Nuclei and the Variable Moment-of-Inertia Model

NUCLEAR STRUCTURE ²⁴Mg, ⁵⁶Fe, ¹⁰²Ru, ^104,106Pd, ¹⁵⁰Nd, ^150,152,154Sm, ^154,156,158Gd, ^{156,158,160,162,164}Dy, ^164,166,168Er, ^168,170,174Yb, ^180,184,186W, ^{186,188,190,192}Os, ^192,194,196Pt, ²²⁸Th, ^232,234U calculated nonaxiality parameter for g.S., γ-vibrational band in VMI model.

doi: 10.1103/PhysRevC.7.2476

1973KA25

Phys.Rev. C8, 757 (1973)

R.Kalish, B.Herskind, G.B.Hagemann

g Factor Measurements of High-Spin (Iπ < 10⁺) Rotational States

NUCLEAR REACTIONS ^156,157,158Gd(α, 2nγ), E=27 MeV; measured γ(θ, H). ^158,160,162Dy levels deduced g.

doi: 10.1103/PhysRevC.8.757

1973LE16

Phys.Rev. C8, 819 (1973)

P.L.Lee, F.Boehm

X-Ray Isotope Shifts and Variations of Nuclear Charge-Radii in Isotopes of Nd, Sm, Dy, Yb and Pb

NUCLEAR REACTIONS ^{142,143,144,145,146,148,150}Nd, ^{147,148,149,150,152,154}Sm, ^{161,162,163,164}Dy, ^{170,171,172,173,174,176}Yb, ^{204,206,207,208}Pb(γ, X-ray); measured isotope shift. ^{142,143,144,145,146,148,150}Nd, ^{147,148,149,150,152,154}Sm, ^{161,162,163,164}Dy, ^{170,171,172,173,174,176}Yb, ^{204,206,207,208}Pb deduced nuclear charge radii.

doi: 10.1103/PhysRevC.8.819

1973ME08

Nucl.Phys. A203, 17 (1973)

J.Meyer, J.Speth

Change of Nuclear Radii Due to Rotation; Calculation of Mossbauer and Muonic Isomer Shifts

NUCLEAR STRUCTURE ¹⁵⁰Nd, ^152,154Sm, ^{154,156,158,160}Gd, ^{156,158,160,162,164}Dy, ^{158,160,162,164,166,168,170}Er, ^{164,166,168,170,172,174,176,178}Yb, ^{172,174,176,178,180}Hf, ^{180,182,184,186}W, ^188,190,192Os; calculated Mossbauer, muonic isomer shifts of 2+-70+ transitions.

doi: 10.1016/0375-9474(73)90421-1

1973PR15

Can.J.Phys. 51, 1794 (1973)

V.R.Prakash

A Correction to the Governor Model Moment of Inertia

NUCLEAR STRUCTURE ^152,154Sm, ^{154,156,158,160}Gd, ^{156,158,160,162,164}Dy, ^{162,164,166,168,170}Er, ^{168,170,172,174,176}Yb, ^{174,176,178,180}Hf, ^{180,182,184,186}W, ^186,188,190Os; calculated moment of inertia.

1973ST07

Czech.J.Phys. 23B, 25 (1973)

F.Sterba, J.Sterbova, M.Rozkos

Angular Distributions of 12 MeV Deuterons Inelastically Scattered by the ¹⁶²Dy

NUCLEAR REACTIONS ¹⁶²Dy(d, d'), E=12.1 MeV; measured σ(Ed', θ). ¹⁶²Dy deduced levels, L, J, π.

1973TR03

Phys.Lett. 44B, 41 (1973)

N.Trautner, G.Lovhoiden, P.R.Christensen

Elastic and Inelastic Deuteron Scattering from ¹⁵²Sm and ¹⁶²Dy

NUCLEAR REACTIONS ¹⁵²Sm, ¹⁶²Dy(d, d'), E=12 MeV; measured σ(E, θ). ¹⁵²Sm, ¹⁶²Dy levels deduced β.

doi: 10.1016/0370-2693(73)90295-5

1973WE10

Z.Phys. 262, 425 (1973)

F.Weller

Doublet Splitting in Even-A Deformed Nuclei

NUCLEAR STRUCTURE ¹⁶²Dy, ^166,168Er, ^172,174Yb; calculated doublet splitting between excited two-quasiparticle states with parallel, antiparallel L-coupling.

1974BE69

Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 93 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.1, 81 (1974)

R.B.Begzhanov, V.M.Belenkii, V.K.Usharov

Negative Parity States in Even-Even Nuclei

NUCLEAR STRUCTURE ¹⁶²Dy, ¹⁶⁸Er, ^228,230Th, ²³²U; calculated levels.

1974DA03

Phys.Rev.Lett. 32, 337 (1974)

J.P.Davidson, D.A.Close, J.J.Malanify

Evidence for Higher Shape Deformations in Muonic X Rays

NUCLEAR REACTIONS ²³²Th, ²³⁸U(μ, X-ray); measured muonic X-rays. ²³²Th, ²³⁸U, ¹⁵²Sm, ¹⁶²Dy, ¹⁷⁰Er, ¹⁸²W deduced deformation parameters.

doi: 10.1103/PhysRevLett.32.337

1974QUZW

JOUR NUKLA 19 637

NUCLEAR STRUCTURE ¹⁶O, ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ³⁶Ar, ⁴⁰Ca, ²⁴²Pu; calculated quadrupole moment. ¹⁵²Sm, ¹⁵⁸Gd, ¹⁶²Dy, ¹⁶⁶Er, ¹⁷⁴Yb, ¹⁷⁸Hf, ¹⁸⁴W, ¹⁹⁰Os; calculated quadrupole moment, deformation β.

1975BI13

Nucl.Phys. A251, 169 (1975)

B.L.Birbrair, N.A.Voinova, N.S.Smirnova

The 0⁺ States in Doubly Even Deformed Nuclei

NUCLEAR STRUCTURE ^150,152Nd, ^152,154,156Sm, ^{154,156,158,160}Gd, ^{156,158,160,162,164,166}Dy, ^{158,160,162,164,166,168,170,172}Er, ^{164,166,168,170,172,174,176}Yb, ^{170,172,174,176,178,180,182}Hf, ^{174,176,178,180,182,184,186,188}W, ^{182,184,186,188,190}Os; calculated transition energies, B(λ).

doi: 10.1016/0375-9474(75)90708-3

1975KA17

Phys.Scr. 11, 190 (1975)

R.Kalish

New Methods and Results in Nuclear Moment Measurements Reported at the Uppsala Conference (June 10-14, 1974)

COMPILATION ¹⁶N, ^18,20O, ²²Ne, ^22,25Na, ^24,26Mg, ²⁸Si, ^39,41K, ^41,42Ca, ⁵¹Cr, ^53,54Mn, ⁵⁵Fe, ⁵⁹Ni, ⁷⁷As, ⁷⁸Br, ^80,85Rb, ^103,103m,105Rh, ¹⁰⁸Ag, ¹¹¹Cd, ¹¹³Sn, ^126,130I, ^{126,128,130,132}Xe, ¹⁵¹Gd, ^162,164Dy, ^181,182,184Re, ^{194,195,196,197,198,198m,199,200,201,202}Tl, ¹⁹⁷Hg, ²⁰⁰Pb, ²⁰⁵Po, ²⁰⁸Bi, ^237mPu; compiled g. ⁷¹Ge, ^102,103Ru, ¹¹⁰Pd, ^{113,115,116,118}Sn, ²⁰⁵Pb, ^206,208Po; compiled quadrupole moment.

1977HO11

Phys.Rev. C15, 1665 (1977)

H.R.Hooper, J.M.Davidson, P.W.Green, D.M.Sheppard, G.C.Neilson

Gamma-Ray Angular Distribution Measurements from the ^162,164Dy(n, n'γ) Reactions

NUCLEAR REACTIONS ^162,164Dy(n, n'γ), E=1.5-2.4 MeV; measured σ(E, Eγ, θ). ^162,164Dy deduced levels, J, π, δ. Enriched targets, Ge(Li) detectors.

doi: 10.1103/PhysRevC.15.1665

1977KE06

Nucl.Phys. A278, 109 (1977)

F.Kearns, G.Varley, G.D.Dracoulis, T.Inamura, J.C.Lisle, J.C.Willmott

Lifetimes of High Spin Rotational States

NUCLEAR REACTIONS ^152,154Sm, ^156,158Gd, ^160,162,164Dy, ^{164,166,168,170}Er, ^170,172,174Yb(⁵⁶Fe, ⁵⁶Fe'), (⁸⁴Kr, ⁸⁴Kr'), E232, 348 MeV; measured Eγ, Doppler broadened lineshapes. ^152,154Sm, ^156,158Gd, ^160,162,164Dy, ^{164,166,168,170}Er, ^170,172,174Yb levels deduced T_1/2, B(E2). Enriched targets. Ge(Li) detectors.

doi: 10.1016/0375-9474(77)90188-9

1978GE03

J.Phys.(London) G4, 575 (1978)

W.Gelletly, W.F.Davidson, J.Simic, H.G.Borner, A.F.Diggory, W.Mampe, K.Schreckenbach, D.D.Warner

Intraband Transition Rates in the Gamma-Vibrational Bands of ¹⁶²Dy and ¹⁶⁸Er

NUCLEAR REACTIONS ¹⁶⁷Er, ¹⁶¹Dy(n, γ); measured γ-spectrum. ¹⁶⁸Er, ¹⁶²Dy deduced transition rates, δ.

doi: 10.1088/0305-4616/4/4/014

1978HO09

Phys.Lett. 65A, 220 (1978)

W.Hogervorst, G.J.Zaal, J.Bouma, J.Blok

Isotope Shifts and Hyperfine Structure of Natural Dysprosium

NUCLEAR MOMENTS ^{156,158,160,161,162,163,164}Dy; measured hfs, isotope shift.

doi: 10.1016/0375-9601(78)90154-8

1978HU03

Phys.Rev. C17, 622 (1978)

P.Hubert, N.R.Johnson, E.Eichler

Lifetime Measurements and Multiple Coulomb Excitation in ¹⁶²Dy

NUCLEAR REACTIONS ¹⁶²Dy(⁴⁰Ar, ⁴⁰Ar'γ), E=148.6 MeV; measured recoil distance DSA, Coulomb excitation. ¹⁶²Dy levels deduced T_1/2, B(E2).

doi: 10.1103/PhysRevC.17.622

1978RA14

Yad.Fiz. 27, 1501 (1978); Sov.J.Nucl.Phys. 27, 792 (1978)

P.P.Raichev, R.P.Rusev

Energy Levels and Reduced E2-Transition Probabilities of Deformed Even-Even Nucleu in the SU(3) Scheme

NUCLEAR STRUCTURE ^152,154Sm, ^154,156,158Gd, ^160,162,164Dy, ^{160,164,166,168}Er; calculated levels, B(E2). SU(3) model.

1979GU15

Phys.Rev. C20, 1814 (1979)

M.W.Guidry, I.Y.Lee, N.R.Johnson, P.A.Butler, D.Cline, P.Colombani, R.M.Diamond, F.S.Stephens

Reduced Transition Probabilities and Energies of High-Spin States in ¹⁶²Dy

NUCLEAR REACTIONS ¹⁶²Dy(¹³⁶Xe, ¹³⁶Xe'), E(lab)=547, 612 MeV; measured T_1/2, Eγ. ¹⁶²Dy levels deduced B(E2).

doi: 10.1103/PhysRevC.20.1814

1980HU06

J.Phys.(London) G6, 741 (1980)

P.Hungerford, W.D.Hamilton, S.M.Scott, D.D.Warner

Gamma-Gamma Directional Correlation Measurements in ^162,164Dy Following Thermal Neutron Capture

NUCLEAR REACTIONS ^161,163Dy(n, γ), E=th; measured Eγ, Iγ, γγ(θ). ^162,164Dy deduced levels, J, π, δ. Deformed rotor model.

doi: 10.1088/0305-4616/6/6/011

1980KO22

Nucl.Phys. A343, 210 (1980)

W.K.Koo

Sum-Rule Approach to the Static Quadrupole Moments of Arbitrary Excited States in Even-Even Nuclei

NUCLEAR STRUCTURE ¹⁸Ne, ^32,34S, ⁵⁶Fe, ^58,60,62Ni, ^70,72,74,76Ge, ^116,124Sn, ^148,150,152Sm, ^160,162,164Dy; calculated static quadrupole moments of 2⁺, 4⁺ states. Sum-rule approach.

doi: 10.1016/0375-9474(80)90650-8

1980KU15

Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 942 (1980); Bull.Acad.Sci.USSR, Phys.Ser. 44, No.5, 36 (1980)

N.K.Kuzmenko, V.M.Mikhailov

Relation of the Level Distribution of Particles to the Density of One-Quasi-Particle States near the Fermi Surface

NUCLEAR STRUCTURE ^167,169Er, ^{169,171,173,175}Yb; calculated neutron one-quasiparticle energies; ¹⁵⁶Gd, ^162,164Dy, ^166,168Er, ¹⁷⁴Yb, ^176,178,180Hf; calculated two-quasiparticle energies. Number projection.

1981BI14

Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 23 (1981)

B.L.Birbrair, I.A.Mitropolsky

Self-Consistent Pairing and Collective State Structure in Deformed Nuclei

NUCLEAR STRUCTURE ^{154,156,158,160}Gd, ^{156,158,160,162}Dy, ^{160,162,164,166,168,170}Er, ^168,170,172Yb; calculated levels, B(E0)/B(E2).

1981WA28

Phys.Rev.Lett. 47, 1819 (1981)

D.D.Warner

Description of M1 Transitions in Deformed Even-Even Nuclei with the Interacting Boson Approximation

NUCLEAR STRUCTURE ¹⁵⁴Gd, ¹⁶²Dy, ^166,168Er; calculated δ(E2/M1) for intrabrand transitions. Interacting boson approximation.

doi: 10.1103/PhysRevLett.47.1819

1982CL04

Phys.Rev. C26, 1636 (1982)

D.L.Clark, G.W.Greenlees

Changes of Charge Radii and Hyperfine Interactions of the Dy Isotopes

NUCLEAR MOMENTS ^{156,158,160,161,162,163,164}Dy; measured hfs, optical isotope shifts; deduced rms charge radii differences, hyperfine anomaly, hyperfine constants. Atomic beams, laser spectroscopy.

doi: 10.1103/PhysRevC.26.1636

1982FI15

Nucl.Phys. A389, 218 (1982)

C.A.Fields, K.H.Hicks, R.A.Ristinen, F.W.N.De Boer, P.M.Walker, J.Borggreen, L.K.Peker

A Study of the Rotational Side-Bands in ¹⁶²Dy

NUCLEAR REACTIONS ¹⁶⁰Gd(α, 2n), E=24, 28 MeV; measured E(γ), I(γ)(E, t, θ), γγ-coin, ICC. ¹⁶²Dy deduced levels, K, J, π. Enriched targets, Ge(Li), hyperpure Ge detectors, mini-orange spectrometer. Two-quasiparticle plus rotor analysis.

doi: 10.1016/0375-9474(82)90517-6

1982WA04

Phys.Rev. C25, 2019 (1982)

D.D.Warner, R.F.Casten

Interacting-Boson-Approximation E2 Operator in Deformed Nuclei

NUCLEAR STRUCTURE ^156,158,160Gd, ^{158,160,162,164}Dy, ^{162,164,166,168,170}Er, ^178,180Hf, ^182,184W; calculated B(E2), branching ratios; deduced E2 operator parameters. Interacting boson approximation.

doi: 10.1103/PhysRevC.25.2019

1983JA03

Nucl.Phys. A394, 39 (1983)

J.Janecke, E.H.L.Aarts, A.G.Drentje, M.N.Harakeh, C.Gaarde

Isobaric Analog States in Rare-Earth Nuclei Studied with the (³He, t) Charge Exchange Reaction at θ(L) = 0°

NUCLEAR REACTIONS ^{152,154,156,158,160}Gd, ^160,162Dy, ^{162,164,166,168,170}Er, ^{170,172,174,176}Yb, ^176,178,180Hf(³He, t), E=60.5 MeV; measured σ(E(t), θ=0°). ^{152,154,156,158,160}Tb, ^160,162Ho, ^{162,164,166,168,170}Tm, ^{170,172,174,176}Lu, ^176,178,180Ta deduced IAS, Γ, Coulomb displacement energies. Enriched targets, magnetic spectrometer.

doi: 10.1016/0375-9474(83)90160-4

1984DR08

Ann.Phys.(New York) 156, 41 (1984)

J.P.Draayer, K.J.Weeks

Towards a Shell Model Description of the Low-Energy Structure of Deformed Nuclei. I. Even-Even Systems

NUCLEAR STRUCTURE ^160,162,164Dy, ^164,166,168Er, ^166,168Yb, ²³²Th, ^234,236,238U; calculated levels, B(E2), quadrupole moments. Shell model, deformed nuclei.

doi: 10.1016/0003-4916(84)90210-0

1985NE09

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 ^{158,160,162,164,166,168,170,172,174,176}Yb, ^{152,156,158,160,162,164,166,168,170}Er, ^{148,150,152,154,156,158,160,162,164}Dy, ^{136,138,140,142,144,146}Ba; measured isotope shifts; deduced rms charge radii. Collinear laser spectroscopy.

1986BE09

Phys.Lett. 172B, 277 (1986)

R.Bengtsson, S.Aberg

g Factors as a Probe of Correlated Changes of the Nuclear Deformation and Pair Field in Ground-State Rotational Bands

NUCLEAR STRUCTURE ¹⁵⁴Dy; calculated g-band transitional quadrupole moments, g proton, neutron pairing gap energy vs ground state deformation. ¹⁶⁴Dy, ^158,168Yb; calculated proton pairing gap energy vs ground state deformation. ¹⁶⁰Yb; calculated neutron pairing gap energy vs ground state deformation, g. ^156,160,162Dy; calculated neutron, proton energy gaps, g. ^{154,156,158,160,162,164}Dy deduced correlation between Δ(n), Δ(p), g.

doi: 10.1016/0370-2693(86)90251-0

1986NE06

Yad.Fiz. 44, 1443 (1986)

V.O.Nesterenko, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova

Hexadecapole States in Deformed Nuclei

NUCLEAR STRUCTURE ^158,160Gd, ^{158,160,162,164}Dy, ^166,168,170Er, ^{168,170,172,174}Yb, ^174,176,178Hf, ¹⁸⁴W, ^186,188Os; calculated hexadecapole states, B(E4), wave functions. ¹⁶⁸Er; calculated B(E2).

1987LI11

Nucl.Phys. A469, 348 (1987)

P.O.Lipas, P.Toivonen, E.Hammaren

IBA-1 Calculations of E2/M1 Mixing Ratios

NUCLEAR STRUCTURE ^{146,148,150,152}Sm, ^152,154,156Gd, ¹⁶²Dy, ^{162,164,166,168}Er, ¹⁷²Yb, ¹⁹⁰Os; calculated levels, δ(E2/M1). Interacting boson approximation.

doi: 10.1016/0375-9474(87)90115-1

1987RA01

At.Data Nucl.Data Tables 36, 1 (1987)

S.Raman, C.H.Malarkey, W.T.Milner, C.W.Nestor, Jr., P.H.Stelson

Transition Probability, B(E2), from the Ground to the First-Excited 2⁺ State of Even-Even Nuclides

COMPILATION A=6-254; compiled, evaluated 2⁺ level energies, B(E2), T_1/2, β₂, β₂/β₂(sp), EWSR, intrinsic quadrupole moments.

doi: 10.1016/0092-640X(87)90016-7

1988BA17

Ann.Phys.(New York) 182, 344 (1988)

A.F.Barfield, B.R.Barrett, J.L.Wood, O.Scholten

An Interacting Boson Model Description of Octupole States in Nuclei

NUCLEAR STRUCTURE ¹⁵⁴Sm, ^156,158Gd, ^158,162Dy, ¹⁶⁸Er, ¹⁷²Yb, ¹⁷⁸Hf, ¹⁸²W; calculated levels, B(λ). Interacting boson model.

doi: 10.1016/0003-4916(88)90016-4

1988BH04

J.Phys.(London) G14, 717 (1988)

S.Bhattacharya, S.Sen

The Anharmonic Vibrator Model and the Electromagnetic Properties of the Ground-State Bands of Even-Even Nuclei

NUCLEAR STRUCTURE ^104,106,110Pd, ^126,128Xe, ¹²⁸Ba, ^150,152,154Sm, ^{152,154,156,158,160}Gd, ^{156,158,160,162,164}Dy, ^{156,158,160,162,164,166,168,170}Er, ^{160,162,164,166,168,170,172,174,176}Yb, ^{166,168,170,172,174,176,178,180}Hf, ^{180,182,184,186}W, ^{182,184,186,188,190,192}Os, ^{190,192,194,196}Pt, ^230,232,234Th, ^{232,234,236,238}U, ^238,240,242Pu, ^244,246,248Cm; calculated levels, B(E2); deduced model parameter, B(λ) correlation. Anharmonic vibrator.

doi: 10.1088/0305-4616/14/6/011

1988BO02

Phys.Lett. 200B, 1 (1988)

D.Bonatsos

Systematics of Odd-Even Staggering in γ-Bands as a Test for Phenomenological Collective Models

NUCLEAR STRUCTURE ^{152,154,158,160}Gd, ^{154,156,158,160,162}Dy, ^{146,148,150,152,154}Sm, ^{156,158,160,162,164,166,168}Er, ^{160,162,164,166,168,170,172,174}Yb, ^{190,188,186,184,182}Os; analyzed levels, band structure; deduced γ-band staggering systematics. ²³²Th, ¹⁶⁶Yb, ¹⁶⁴Er, ¹⁷⁸Hf; calculated odd spin to even spin level displacements. Phenomenological collective models.

doi: 10.1016/0370-2693(88)91098-2

1988CH26

Phys.Rev. C38, 960 (1988)

D.S.Chuu, S.T.Hsieh

Structure of Even-Even Dy Nuclei in the Interacting Boson Model with Two-Quasiparticle States

NUCLEAR STRUCTURE ^{154,156,158,160,162}Dy; calculated levels, yrast B(E2). Interacting boson model, two-quasiparticle states.

doi: 10.1103/PhysRevC.38.960

1988DE17

Nucl.Instrum.Methods Phys.Res. A268, 155 (1988)

P.P.J.Delheij, G.L.Morgan

Magnetic Moments of Low-Energy Neutron Resonances in ¹⁶¹Dy

NUCLEAR REACTIONS ¹⁶¹Dy(n, X), E=low; measured transmission spectra. ¹⁶²Dy deduced resonances, μ. Polarized target, tof.

doi: 10.1016/0168-9002(88)90601-8

1988JA12

Nucl.Phys. A487, 77 (1988)

M.K.Jammari, R.Piepenbring

Anharmonicities of γ-Vibrations in Deformed Nuclei

NUCLEAR STRUCTURE ^124,126Ba, ^130,132Ce, ^162,164Dy, ^164,166,168Er, ^{186,188,190,192}Os; calculated levels; deduced anharmonicities. Multiphoton method.

doi: 10.1016/0375-9474(88)90130-3

1988KU21

Phys.Rev. C38, 2482 (1988)

S.Kuyucak, I.Morrison

β-Band Moment of Inertia Anomaly

NUCLEAR STRUCTURE ^{158,160,162,164}Dy, ^{162,164,166,168,170}Er, ^{166,168,170,172,174}Yb, ^{170,172,174,176,178,180}Hf; calculated ground, (β^-), (γ)-band moment of inertia; deduced moment of inertia anomaly. Interacting boson model.

doi: 10.1103/PhysRevC.38.2482

1989HU05

Phys.Rev. C39, 1617 (1989)

H.X.Huang, C.S.Wu, J.Y.Zeng

Calculation of Rotational Spectra of Well-Deformed Nuclei Up to Very High Spins

NUCLEAR STRUCTURE ²⁴⁸Cm, ^{244,242,240,238,236}Pu, ^{238,236,230,234,232}U, ^232,230,228Th, ^{178,176,174,172,170}Hf, ^{176,174,172,170,168}Yb, ^166,164Er, ^164,162Dy, ¹⁵⁶Gd; calculated levels. Three-parameter formula.

doi: 10.1103/PhysRevC.39.1617

1989SU15

Phys.Lett. 229B, 327 (1989)

K.Sugawara-Tanabe, A.Arima

The Structure of Dipole Modes in Dy Isotopes from A = 160 to 164

NUCLEAR STRUCTURE ^160,162,164Dy; calculated levels, B(λ). Self-consistent cranked HFB field based RPA.

doi: 10.1016/0370-2693(89)90412-7

1990WA25

J.Phys.Soc.Jpn. 59, 2700 (1990)

M.Wakasugi, T.Horiguchi, W.G.Jin, H.Sakata, Y.Yoshizawa

Changes of the Nuclear Charge Distribution of Nd, Sm, Gd and Dy from Optical Isotope Shifts

NUCLEAR MOMENTS ^{142,144,146,148,150,143,145}Nd, ^{144,148,150,152,154,147,149}Sm, ^{152,154,156,158,160,155,157}Gd, ^{156,158,160,162,164,161,163}Dy; measured isotope shifts, hfs; deduced rms charge radii changes, nuclear parameter. Atomic beam laser spectroscopy.

1993MI18

Bull.Rus.Acad.Sci.Phys. 57, 15 (1993)

I.N.Mikhailov, P.N.Usmanov, A.A.Okhunov, S.Brianson, R.Kulessa

Magnetic Properties of Collective States for ^{156,158,160,162,164}Dy Isotopes

NUCLEAR STRUCTURE ^{156,158,160,162,164}Dy; calculated levels, g(R) factor, B(λ) vs spin, δ. Phenomenological model, Coriolis mixing.

1993SO20

Bull.Rus.Acad.Sci.Phys. 57, 1668 (1993)

V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova

γ-Transitions between Excited States of Even-Even Deformed Nuclei

NUCLEAR STRUCTURE ¹⁶⁸Er, ¹⁶²Dy, ^156,158Gd; calculated B(λ). Quasiparticle phonon model.

1995BE02

Nucl.Phys. A584, 413 (1995)

J.Berzins, P.Prokofev, R.Georgii, R.Hucke, T.von Egidy, G.Hlawatsch, J.Klora, H.Lindner, U.Mayerhofer, H.H.Schmidt, A.Walter, V.G.Soloviev, N.Yu.Shirikova, A.V.Sushkov

¹⁶²Dy Studied with (n, γ), (n, n'γ), (d, p) and (d, t) Reactions

NUCLEAR REACTIONS ¹⁶¹Dy(n, γ), ¹⁶²Dy(n, n'γ), E=fast, thermal; measured γ-spectra. ¹⁶¹Dy(d, p), E=15, 22 MeV; ¹⁶³Dy(d, t), E=22 MeV; measured spectra. ¹⁶²Dy deduced levels, configurations. Quasiparticle-phonon nuclear model.

NUCLEAR STRUCTURE ¹⁶²Dy; calculated levels, B(λ). Quasiparticle-phonon nuclear model.

doi: 10.1016/0375-9474(94)00522-O

1996SO19

Fiz.Elem.Chastits At.Yadra 27, 1643 (1996); Phys.Part.Nucl. 27, 667 (1996)

V.G.Solovev, A.V.Sushkov, N.Yu.Shirikova

Low-Lying Nonrotational States in Strongly Deformed Even-Even Nuclei of the Rare-Earth Region

NUCLEAR STRUCTURE ^156,158,160Gd, ^160,162,164Dy, ^166,168Er; calculated low-lying nonrotational levels E, π, transitions B(λ). Quasiparticle-phonon model.

1997AL04

Z.Phys. A357, 13 (1997)

I.Alfter, E.Bodenstedt, W.Knichel, J.Schuth

g-Factors of the Ground-State Rotational Bands of ^158,160,162Dy Derived from Perturbed γ-γ Directional Correlations following (α, 2n)-Reactions

NUCLEAR REACTIONS ^156,158,160Gd(α, 2n), E=27 MeV; measured Eγ, Iγ, γγ-coin, directional correlations. ^158,160,162Dy deduced ground state rotational bands g-factors.

doi: 10.1007/s002180050208

1997SO26

Int.J.Mod.Phys. E6, 437 (1997)

V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova

Quadrupole and Hexadecapole Vibrational Excitations in Deformed Nuclei

NUCLEAR STRUCTURE ^156,158,160Gd, ^160,162,164Dy, ^166,168Er; calculated levels, configurations, B(λ); deduced quasiparticle-phonon, one-, two-phonon coupling roles. Quasiparticle-phonon nuclear model.

doi: 10.1142/S0218301397000251

1999BR43

Eur.Phys.J. A 6, 149 (1999)

F.Brandolini, M.De Poli, P.Pavan, R.V.Ribas, D.Bazzacco, C.R.Rossi-Alvarez

g-Factors in the Ground State and the γ-Bands in ^{160, 162, 164}Dy

NUCLEAR REACTIONS ^160,162,164Dy(⁵⁸Ni, ⁵⁸Ni'), E ≈ 220 MeV; measured Eγ, Iγ(θ, H) following Coulomb excitation. ^160,162,164Dy deduced g-factors for ground-state band, vibrational bands transitions. Transient field technique.

doi: 10.1007/s100500050329

2001WU05

Phys.Rev. C64, 064317 (2001)

C.Y.Wu, D.Cline, M.W.Simon, G.A.Davis, R.Teng, A.O.Macchiavelli, K.Vetter

Electromagnetic Properties of the Rotationally Aligned Band in ¹⁶²Dy

NUCLEAR REACTIONS ¹¹⁸Sn(¹⁶²Dy, ¹⁶²Dy'), (¹⁶⁴Dy, ¹⁶⁴Dy'), E=780, 790 MeV; measured Eγ, Iγ, γγ-, (particle)γ-coin. ^162,164Dy deduced high-spin levels, J, π, B(M1), B(E2), deformation. Gammasphere, Chico arrays.

doi: 10.1103/PhysRevC.64.064317

2002GO15

Yad.Fiz. 65, 819 (2002); Phys.Atomic Nuclei 65, 785 (2002)

L.I.Govor, A.M.Demidov, V.A.Kurkin

Multipole Mixtures in γ Transitions Accompanying the (n, n'γ) Reaction on ¹⁶²Dy

NUCLEAR REACTIONS ¹⁶²Dy(n, n'), E=fast; measured Eγ, Iγ(θ). ¹⁶²Dy deduced transitions δ. Comparisons with previous results.

doi: 10.1134/1.1481469

2002JU08

Phys.Rev. C66, 014312 (2002)

A.Jungclaus, B.Binder, A.Dietrich, T.Hartlein, H.Bauer, Ch.Gund, D.Pansegrau, D.Schwalm, J.L.Egido, Y.Sun, D.Bazzacco, G.de Angelis, E.Farnea, A.Gadea, S.Lunardi, D.R.Napoli, C.Rossi-Alvarez, C.Ur, G.B.Hagemann

Backbending Region Study in ^{160, 162}Dy using Incomplete Fusion Reactions

NUCLEAR REACTIONS ¹⁶⁰Gd(⁷Li, X)¹⁶⁰Ho/¹⁶¹Ho/¹⁶²Ho/¹⁶³Ho/¹⁶⁰Dy/¹⁶¹Dy/¹⁶²Dy/¹⁶³Dy/¹⁶⁴Dy/¹⁶⁰Gd, E=35-67 MeV; measured production σ, charged particle angular distributions. ^158,160Gd(⁷Li, X)¹⁶⁰Dy/¹⁶²Dy, E=56 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. ^160,162Dy deduced high-spin levels, J, π, configurations. GASP, ISIS arrays, incomplete fusion, comparison with model predictions.

doi: 10.1103/PhysRevC.66.014312

2005ST24

At.Data Nucl.Data Tables 90, 75 (2005)

N.J.Stone

Table of nuclear magnetic dipole and electric quadrupole moments

NUCLEAR MOMENTS Z=0-99; A=1-255; compiled μ, electric quadrupole moments.

COMPILATION Z=0-99; A=1-255; compiled μ, electric quadrupole moments.

doi: 10.1016/j.adt.2005.04.001

2006AP01

Nucl.Phys. A764, 42 (2006)

A.Aprahamian, X.Wu, S.R.Lesher, D.D.Warner, W.Gelletly, H.G.Borner, F.Hoyler, K.Schreckenbach, R.F.Casten, Z.R.Shi, D.Kusnezov, M.Ibrahim, A.O.Macchiavelli, M.A.Brinkman, J.A.Becker

Complete spectroscopy of the ¹⁶²Dy nucleus

NUCLEAR REACTIONS ¹⁶¹Dy(n, γ), E=0.03-2 MeV; measured Eγ, Iγ, E(ce), I(ce). ¹⁶⁰Gd(α, 2n), E=256 MeV; measured Eγ, Iγ, γγ-coin. ¹⁶²Dy deduced levels, K, J, π, ICC, configurations, collective features. Complete spectroscopy, Ritz combination principle.

doi: 10.1016/j.nuclphysa.2005.09.020

2008KI07

Nucl.Instrum.Methods Phys.Res. A589, 202 (2008)

T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr.

Evaluation of theoretical conversion coefficients using BrIcc

COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.

doi: 10.1016/j.nima.2008.02.051

2011SW02

Phys.Rev. C 83, 034322 (2011), Publishers Note Phys.Rev. C 83, 049903 (2011)

T.P.D.Swan, P.M.Walker, Zs.Podolyak, M.W.Reed, G.D.Dracoulis, G.J.Lane, T.Kibedi, M.L.Smith

Discovery of a nonyrast K^π = 8⁺ isomer in ¹⁶²Dy, and the influence of competing K-mixing mechanisms on its highly forbidden decay

NUCLEAR REACTIONS ¹⁶⁰Gd(⁹Be, 3nα), E=57 MeV; measured Eγ, Iγ, γγ-coin, γγ(t), pulsed beam, isomer half-lives. ¹⁶²Dy; deduced levels, J, π, isomer, bands, multipolarity, hindrance factors, alignment plots, configurations. Analyzed small deviations from N_pN_n dependence.

doi: 10.1103/PhysRevC.83.034322

2013AN02

At.Data Nucl.Data Tables 99, 69 (2013)

I.Angeli, K.P.Marinova

Table of experimental nuclear ground state charge radii: An update

COMPILATION Z=0-96; compiled nuclear radii, rms nuclear charge radii.

doi: 10.1016/j.adt.2011.12.006

2014STZZ

REPT INDC(NDS)-0658 (2014)

N.J.Stone

Table of nuclear magnetic dipole and electric quadrupole moments

COMPILATION Z=0-99; A=1-254; compiled μ, electric quadrupole moments, J, π, T_1/2, experimental methods.

2017AP01

Phys.Rev. C 95, 024329 (2017)

A.Aprahamian, S.R.Lesher, C.Casarella, H.G.Borner, M.Jentschel

Lifetime measurements in ¹⁶²Dy

NUCLEAR REACTIONS Dy(n, γ), E=thermal neutrons from high flux reactor at the ILL-Grenoble; measured Eγ, Iγ, level half-lives by Gamma-Ray-Induced Doppler (GRID) broadening technique. ¹⁶²Dy; deduced levels, bands, B(E2), B(E1), B(M1), collective quadrupole and octupole vibrational excitations. Comparison with Alaga rule predictions. Systematics of energies and B(E2) values for second 0+ and 2+ states in even-even Z=62-72 and N=84-100 nuclei.

doi: 10.1103/PhysRevC.95.024329

2021WA16

Chin.Phys.C 45, 030003 (2021)

M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi

The AME 2020 atomic mass evaluation (II). Tables, graphs and references

ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.

doi: 10.1088/1674-1137/abddaf