References quoted in the ENSDF dataset: 172OS ADOPTED LEVELS, GAMMAS

25 references found.

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


1971BO06

Nucl.Phys. A162, 407 (1971)

J.Borggreen, E.K.Hyde

Alpha Decay of Neutron-Deficient Osmium Isotopes

NUCLEAR REACTIONS 164Er(16O, xn)172Os/173Os/174Os, E=90-154 MeV; measured σ(E). Enriched target.

RADIOACTIVITY 172,173,174Os; measured Eα, T1/2; deduced Qα, α/(EC+β+).

doi: 10.1016/0375-9474(71)90994-8


1978BE72

Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 2632 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.12, 141 (1978)

R.B.Begzhanov, V.M.Belenkii, E.I.Volmyanskii, V.G.Dubro

The Relationship of the Deformation Energy of the Ground State of a Nucleus to the Experimentally Determined Characteristics of the Rotational Bands

NUCLEAR STRUCTURE 152,154,156,158Gd, 154,156,158Dy, 170,172,174,176,178,180,182W, 172,174,176,180,182,184,186,188,190,192Os; analyzed ground state deformation energy, dependence on inertial parameter. Liquid drop model, Strutinsky method.


1979NE08

Z.Phys. A293, 9 (1979)

B.Nerlo-Pomorska

Microscopic Quadrupole and Hexadecapole Moments of Rare Earth Nuclei

NUCLEAR STRUCTURE 168,170,172,174,176,178,180,182,184Yb, 168,170,172,174,176,178,180,182,184,186Hf, 166,168,170,172,174,176,178,180,182,184,186,188,190W, 170,172,174,176,178,180,182,184,186,188,190,192,194Os, 176,178,180,182,184,186,188,190,192,194,196Pt, 180,182,184,186,188,190Hg; calculated multipole moments, stiffness parameters, deformation energies. Microscopic model, self-consistency condition.


1984BO16

Phys.Rev. C29, 1879 (1984)

D.Bonatsos, A.Klein

Generalized Phenomenological Models of the Yrast Band

NUCLEAR STRUCTURE 122,124,126,130,132,144,146Ba, 156,158,160,162,164,166,168,170Er, 152,154,156,158,160Gd, 158,160,162,164,166,168,170,172,174Yb, 172,174,176,178,180,182,184,186,188,190,192Os, 172,174,176,178,180,182,184,186,188W, 118,120,122,124,126,128Xe; analyzed yrast band systematics; deduced model parameter dependences. Generalized phenomenological models.

doi: 10.1103/PhysRevC.29.1879


1984SA16

Nucl.Phys. A423, 333 (1984)

M.Sambataro, O.Scholten, A.E.L.Dieperink, G.Piccitto

On Magnetic Dipole Properties in the Neutron-Proton IBA Model

NUCLEAR STRUCTURE 144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176Ba, 146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178Ce, 148,150,152,154,156,160,162,164,166,168,170,172,174,176,178,180Nd, 150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182Sm, 152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184Gd, 154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186Dy, 156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Er, 158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190Yb, 160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192Hf, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194W, 164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196Os, 166,168,170,172,178,180,182,184,186,188,190,192,194W, 164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198Pt; calculated 2+ state g. 152Sm; calculated δ(E2/M1). Neutron-proton interacting boson model.

doi: 10.1016/0375-9474(84)90593-1


1985HE14

Hyperfine Interactions 22, 339 (1985)

K.Heyde, P.Van Isacker, J.Jolie

Magnetic Dipole Moments of Collective Quadrupole Excited States

NUCLEAR STRUCTURE 108,110,114,118,122,126,130,134,136Ba, 154,162,170,178,186Dy, 152,160,168,176,184Gd, 150,158,166,174,182Sm, 148,156,164,172,180Nd, 146,154,162,170,178Ce, 144,152,160,168,176Ba, 166,174,182,190,198Pt, 164,172,180,188,196Os, 162,170,178,186,194W, 160,168,176,184,192Hf, 158,166,174,182,190Yb, 156,164,172,180,188Er, 192,194,196,198Pt; calculated μ, low-lying collective quadrupole excitations. Interacting boson model, U(6) representation.


1986BE10

At.Data Nucl.Data Tables 35, 15 (1986)

R.Bengtsson, S.Frauendorf, F.-R.May

Quasiparticle Levels in Rotating Rare Earth Nuclei: A cranked shell-model dictionary

NUCLEAR STRUCTURE 152,154,150,156Sm, 152,154,156,158,160Gd, 154,156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 160,162,164,166,168,170,172,174,176Yb, 162,164,166,168,170,172,174,176,178,180,182,184,186Hf, 166,168,170,172,174,176,178,180,182,184,186,188W, 170,172,174,176,178,180,182,184,186,188,190Os, 176,178,180,182,184,186,188,190Pt; calculated quasiparticle levels. Rare earth nuclei, cranked shell model dictionary.

doi: 10.1016/0092-640X(86)90028-8


1987BO05

Phys.Lett. 187B, 1 (1987)

D.Bonatsos

Parameter Systematics of Variable Moment of Inertia Models in the N(p)N(n) Scheme

NUCLEAR STRUCTURE 166,168,170,172,174,176,178,180,182Hf, 172,174,176,178,180,182,184,186W, 172,174,176,178,180,182,184,186,188,190,192Os, 182,184,186,188,190,192,194,196,198Pt; analyzed variable moment of inertia parameters vs valence proton-neutron product; deduced parameter systematics. VMI models.

doi: 10.1016/0370-2693(87)90061-X


1988BH07

Nucl.Phys. A485, 1 (1988)

R.K.Bhaduri, W.Van Dijk

Nuclear Specific Heat and Effective Degrees of Freedom

NUCLEAR STRUCTURE 148,150,152,154,156,158,160,162,164,166Dy, 134,136,138,140,142,144,146,148,150,152,154,156Sm, 182,184,186,188,190,192,194,196,198,200Pt, 172,174,176,178,180,182,184,186,188,190Os; calculated specific heat.

doi: 10.1016/0375-9474(88)90518-0


1988HS01

J.Phys.(London) G14, L31 (1988)

S.T.Hsieh, M.M.King Yen, T.T.S.Kuo

A Three-Band Interpretation of the High-Spin States in Even 172-180Os Isotopes

NUCLEAR STRUCTURE 172,174,176,178,180Os; calculated levels, yrast band characteristics. Interacting boson approximation, two-quasiparticles.

doi: 10.1088/0305-4616/14/2/003


1988PA02

Phys.Rev. C37, 883 (1988)

L.Pauling

Comment on ' Low-Frequency Anomaly in 172Os Moment of Inertia '

NUCLEAR STRUCTURE 172Os; analyzed band structure; deduced quadrupole moment, level frequency anomaly features.

doi: 10.1103/PhysRevC.37.883


1988SA37

Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 838 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 5 (1988)

L.Yu.Sabalyauskas, V.V.Vanagas, T.V.Guseva, J.H.Ruza, Yu.Ya.Tamberg

A Restricted-Dynamics Model for Heavy-Nucleus Levels and Binding Energies

NUCLEAR STRUCTURE 158,160,162,164,166,168,170,172,174,176,178Yb, 162,164,166,168,170,172,174,176,178,180,182Hf, 166,168,170,172,174,176,178,180,182,184W, 170,172,174,176,178,180,182,184,186,188Os, 174,176,178,180,182,184,186,188,190Pt, 180,182,184,186,188,190,192Hg, 190,192,194Pb, 194,196Po, 171Yb, 173Hf, 181Hf, 175W; calculated binding energies. 172,177Yb, 173,176,181Hf, 175,182,183,185W, 186Os, 196Pt; calculated levels; deduced model parameters. Restricted dynamics model.


1990KA24

J.Phys.(London) G16, 1203 (1990)

A.M.Kamchatnov

Classical Model for the Spin Alignment of ' Odd Nucleons '

NUCLEAR STRUCTURE 154Dy, 163Yb, 172Os; calculated yrast band angular velocity vs J. Odd-nucleon spin alignment model.

doi: 10.1088/0954-3899/16/8/015


1990NA14

Nucl.Phys. A512, 61 (1990)

W.Nazarewicz, M.A.Riley, J.D.Garrett

Equilibrium Deformations and Excitation Energies of Single-Quasiproton Band Heads of Rare-Earth Nuclei

NUCLEAR STRUCTURE 148,150,152,154,156,158,160Sm, 150,152,154,156,158,160,162,164,166Gd, 152,154,156,158,160,162,164,166,168Dy, 154,156,158,160,162,164,166,168,170Er, 154,156,158,160,162,164,166,168,170,172,174,176,178,180Yb, 158,160,162,164,166,168,170,172,174,176,178,180,182Hf, 164,166,168,170,172,174,176,178,180,182,184,186,188W, 170,172,174,176,178,180,182,184,186,188,190,192,194Os, 151,153,155,157,159,161Eu, 153,155,157,159,161,163,165Tb, 153,155,157,159,161,163,165,167,169,171Ho, 157,159,161,163,165,167,169,171,173Tm, 161,163,165,167,169,171,173,175,177Lu, 167,169,171,173,175,177,179,181,183,185Ta, 173,175,177,179,181,183,185,187,189Re; calculated equilibrium deformations. Shell correction method, average Woods-Saxon potential, monopole pairing residual interaction.

doi: 10.1016/0375-9474(90)90004-6


1991BA04

Phys.Rev. C43, R926 (1991)

B.R.Barrett, G.D.Dracoulis, R.A.Bark

Intruder Bands as F-Spin Analog States

NUCLEAR STRUCTURE A=168-182; analyzed band structure; deduced intruder band, F-spin analog relationship. 172,174Os, 180,182Hg, 176,178Pb; calculated uncoupled band moments of inertia, quadrupole moments. F-spin, interacting boson model.

doi: 10.1103/PhysRevC.43.R926


1991BA31

J.Phys.(London) G17, 1209 (1991)

R.A.Bark

A Shape Coexistence Interpretation of the Phenomenology of Alignment Curves in Os and Re Isotopes

NUCLEAR STRUCTURE 172,174,176,178,180,182Os, 171,172,175,177,179,181Re; analyzed data; deduced low-frequency unbending mechanism. Shape coexistence model, intruder configuration excitation.

doi: 10.1088/0954-3899/17/8/011


1993AU05

Nucl.Phys. A565, 1 (1993)

G.Audi, A.H.Wapstra

The 1993 Atomic Mass Evaluation. (I). Atomic Mass Table

COMPILATION A=1-266; compiled, evaluated mass excess, binding energy, β-decay data; deduced atomic masses.

doi: 10.1016/0375-9474(93)90024-R


1993AU07

Nucl.Phys. A565, 66 (1993)

G.Audi, A.H.Wapstra

The 1993 Atomic Mass Evaluation. (II). Nuclear-Reaction and Separation Energies

COMPILATION A=1-266; compiled, evaluated two-neutron, two-proton separation energies, Q(α), Q(2β-), Q(β-n), other reaction data.


1993CH09

J.Phys.(London) G19, 299 (1993)

H.C.Chiang, S.T.Hsieh, M.M.King Yen, D.S.Chuu

Anomalies of Moment of Inertia in 170-180Os

NUCLEAR STRUCTURE 170,172,174,176,178,180Os; calculated levels, quadrupole moments, moment of inertia, backbending plots. Interacting boson plus fermion-pair model.

doi: 10.1088/0954-3899/19/2/012


1994DA02

Nucl.Phys. A568, 90 (1994)

P.M.Davidson, G.D.Dracoulis, T.Kibedi, A.P.Byrne, S.S.Anderssen, A.M.Baxter, B.Fabricius, G.J.Lane, A.E.Stuchbery

Non-Yrast States and Shape Co-Existence in 172Os

RADIOACTIVITY 172Ir(α), (EC) [from 144Sm(31P, 3n), E=150 MeV]; measured Eγ, Iγ, γγ(t), γγ(θ), I(ce), (ce)γ-coin. 172Os deduced levels, J, π, ICC, B(λ), branching ratios, configurations, band structure.

doi: 10.1016/0375-9474(94)90005-1


1994DR04

Phys.Rev. C49, 3324 (1994)

G.D.Dracoulis

Properties of Intruder Bands in the Os-Pt-Hg-Pb Region

NUCLEAR STRUCTURE 180,182,184Hg, 172,174Os, 174,176Pt, 186,188Pb; analyzed levels; deduced intruder bands features. Restricted 2-component model, interacting proton, neutron shells.

doi: 10.1103/PhysRevC.49.3324


1994VIZY

Priv.Comm. (1994)

A.Virtanen, N.R.Johnson, F.K.McGowan, I.Y.Lee, C.Baktash, M.A.Riley, J.C.Wells, J.Dudek

Transition Quadrupole Moments of High-Spin States of 172Os

NUCLEAR REACTIONS 144Nd(32S, 4n), E=162 MeV; measured γγ-coin, Doppler shift recoil distance. 172Os deduced levels, J, π, T1/2, transition quadrupole moments, high-spin band structure.


1995CH01

Phys.Rev. C51, 136 (1995)

W.-T.Chou, S.T.Hsieh

Interacting Boson Approximation Studies of the Negative Parity States of 172-180Os Isotopes

NUCLEAR STRUCTURE 172,174,176,178,180Os; calculated levels, B(λ). Interacting boson approximation.

doi: 10.1103/PhysRevC.51.136


1995HI02

Phys.Rev. C51, 1736 (1995)

T.Hild, W.-D.Schmidt-Ott, V.Kunze, F.Meissner, C.Wennemann, H.Grawe

α and β Decays of 169-173Os and the Nuclear Structure of the Daughter Isotopes

RADIOACTIVITY 168,169Os(α) [from 114Cd(58Ni, xn), E=212-267 MeV]; measured Eα, Iα, T1/2, αγ-coin. 170,171,172,173Os(α), (β+), (EC) [from 140Ce(36Ar, xn), E=178-210 MeV]; measured Eα, Iα, Eγ, Iγ, T1/2, γγ-, αγ-coin. 170,171,172,173Os deduced α-branching. 165,167W deduced levels, J, π, configuration. 170,172Re deduced levels. 171,173Re deduced levels, probable J, π, configuration. Ge(Si) detectors.

doi: 10.1103/PhysRevC.51.1736


2012WA38

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.