References quoted in the ENSDF dataset: 191IR ADOPTED LEVELS, GAMMAS
57 references found.
Clicking on a keynumber will list datasets that reference the given article.
Naturwissenschaften 37, 397 (1950)
P.Brix, H.Kopfermann, W.v.Siemens
Uber die Kernmomente der Iridium-Isotope
Phys.Rev. 87, 1048 (1952)
K.Murakawa, S.Suwa
Hyperfine Structure in the Spectra of Iridium and Osmium
Ann.Physik 13, 136 (1953)
W.Von Siemens
Hyperfeinstrukturen im Iridium I-Spektrum und die Kernmomente der stabilen Iridium-Isotope
Phys.Rev. 98, 653 (1955)
A.W.Sunyar
Fast E2 Transitions
Phys. Letters 10, 24 (1964); Erratum Phys.Letters 10, 291(1964)
J.A.Cameron, I.A.Campbell, J.P.Compton, R.A.G.Lines
Nuclear Orientation of Ir191m in Iron
NUCLEAR STRUCTURE 191Ir, 191Os, 193Os; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90553-0
Nucl.Phys. 53, 497 (1964)
B.I.Deutch, P.Hornshoj
The Measurement of the L Shell Particle Parameters in the 42 keV E3 Transitions of Ir191
NUCLEAR STRUCTURE 191Os; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90629-7
Z.Naturforsch. 19a, 1409 (1964)
F.Wittmann
Winkelverteilung Resonant Gestreuter γ-Quanten
NUCLEAR STRUCTURE 191Ir; measured not abstracted; deduced nuclear properties.
Phys.Letters 25B, 253 (1967)
F.Wagner, J.Klockner, H.J.Korner, H.Schaller, P.Kienle
Isomer Shift and Quadrupole Splitting in 191Ir and 193Ir
NUCLEAR REACTIONS 191Ir(γ, γ), E=82, 129 keV; 193Ir(γ, γ), E=73, 139 keV; measured Mossbauer effect; deduced isomer shifts. 191,193Ir; deduced quadrupole moment.
doi: 10.1016/0370-2693(67)90002-0
Yadern.Fiz. 7, 735 (1968); Soviet J.Nucl.Phys. 7, 447 (1968)
A.V.Davydov, G.R.Kartashov, Y.V.Khrudev
Resonant Scattering of 129-keV Gamma Rays of Ir191
NUCLEAR REACTIONS 191Ir(γ, γ), E=0.129 MeV; measured Mossbauer effect, γγ(θ, H). 191Ir level deduced μ, γ-mixing. Ge(Li) detector.
Phys.Rev. 165, 506 (1968); Erratum Phys.Rev. 175, 696 (1968)
A.Narath
Magnetic Dipole Moments of 191Ir and 193Ir
NUCLEAR STRUCTURE 191Ir, 193Ir; measured not abstracted; deduced nuclear properties.
J.Phys., C(London) 2, 1405 (1969)
J.J.Davies, J.Owen
The Hyperfine Interactions of Isolated and of Exchange-Coupled Iridium Ions in (NH4)2PtCl6
NUCLEAR MOMENTS 191,193Ir; measured a in (NH4)2PtCl6; deduced μ, quadrupole moment. ENDOR.
Phys.Lett. 28B, 415 (1969); Erratum Phys.Lett. 28B, 663 (1969)
P.G.Hansen, P.Hornshoj, H.L.Nielsen, K.Wilsky, H.Kugler, G.Astner, E.Hagebo, J.Hudis, A.Kjelberg, F.Munnich, P.Patzelt, M.Alpsten, G.Andersson, A.Appelqvist, B.Bengtsson, R.A.Naumann, O.B.Nielsen, E.Beck, R.Foucher, J.P.Husson, J.Jastrzebski, A.Johnson, J.Alstad, T.Jahnsen, A.C.Pappas, T.Tunaal, R.Henck, P.Siffert, G.Rudstam
Decay Characteristics of Short-Lived Radio-Nuclides Studied by On-Line Isotope Separator Techniques
RADIOACTIVITY 43Ar, 101Cd, 109Sn, 115I, 115Xe, 205,225,226Rn, 224,225,226Fr; measured T1/2. 75Kr, 119I, 119Xe, 186Pt, 186,188Au, 187,188Hg; measured Eγ. 198,200,202Po; measured Iα. 102,103Cd, 116,117,118I, 116,117,118Xe, 184Pt, 184Au; measured T1/2, Eγ. 79,81Kr, 125,127Xe; measured T1/2, Eγ, I(ce). 103Ag; measured T1/2, Eγ, I(ce), γγ-delay. 187,189,191Pt, 189Au, 206Hg; measured Eγ, γγ-delay. 181Hg; measured T1/2, Eα. 182,183,185Hg; measured T1/2, Eα, Iα. 184,186Hg; measured T1/2, Eα, Iα, Eγ. 202,204,206Rn; measured T1/2, Iα. 103Pd, 187,189,191Ir, 189Pt, 206Tl deduced levels, T1/2.
doi: 10.1016/0370-2693(69)90337-2
Phys.Rev. 185, 1555 (1969)
W.R.Owens, B.L.Robinson, S.Jha
Gyromagnetic Ratio of the 129-keV State in Iridium-191
RADIOACTIVITY 191Pt; measured Xce-, Xγ-delay, γγ(θ, H).
NUCLEAR REACTIONS 191Ir(γ, γ); E = 82.4, 129 keV; measured Mossbauer effect. 191Ir levels deduced T1/2, g, B(M1), μ.
Nucl.Phys. A147, 200 (1970)
R.Avida, I.Ben Zvi, P.Gilad, M.B.Goldberg, G.Goldring, K.H.Speidel, A.Sprinzak
Angular Correlation Measurements on 191,193Ir Following Coulomb Excitation
NUCLEAR REACTIONS 191,193Ir(16O, 16O'γ), E = 40 MeV; measured σ(Eγ, θ(γ)). 191,193Ir levels deduced g, γ-mixing. Natural targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(70)90522-1
Nucl.Phys. A156, 647 (1970)
A.Backlin, V.Berg, S.G.Malmskog
Negative Parity States in Odd-Mass Ir and Au Nuclei
RADIOACTIVITY 193Os[from 192Os(n, γ)], 191,189Pt, 193Hg[from Pb(p, spallation)]; measured E(ce), I(ce), γγ-coin, cece-, γce-delay; deduced log ft. 193Au, 193,191,189Ir deduced levels, J, π, T1/2, γ-multipolarity.
doi: 10.1016/0375-9474(70)90260-5
Nucl.Phys. A143, 160 (1970)
S.G.Malmskog, V.Berg, A.Backlin, G.Hedin
The Low-Energy Level Structure of 191Ir
RADIOACTIVITY 191Pt[from Pb(p, spallation)]; measured Eγ, Iγ, E(ce), I(ce), cece-delay. 191Ir deduced levels, T1/2, J, π, ICC, γ-multipolarities, γ-mixing, B(E2), B(M1), quadrupole moment. Isotope separated sources, Ge(Li) detector.
doi: 10.1016/0375-9474(70)90688-3
Nucl.Phys. A163, 571 (1971)
P.D.Bond, J.D.McGervey, S.Jha
Measurements of Some Nuclear Lifetimes in the Nanosecond Region
RADIOACTIVITY 48Cr[from 47Ti(α, 3n)], 95Tc[from 93Nb(α, 2n)], 99Mo, 101Rh[from 99Tc(α, 2n)], 133Ba, 140La[from 140Ba], 181Hf, 188Ir[from 185Re(α, 3n), from Os(α, xn)188Pt]; measured γγ-delay. 48V, 95Mo, 99Tc, 101Ru, 133Cs, 140Ce, 181Ta, 188Os levels deduced T1/2. 125I; measured XX-delay. 125Te level deduced T1/2. 191Pt[from 193Ir(p, 3n)]; measured γX-, βX-delay. 191Ir level deduced T1/2.
doi: 10.1016/0375-9474(71)90509-4
Phys.Lett. 36B, 328 (1971)
G.Eska, E.Hagn, T.Butz, P.Kienle, E.Umlauf
Measurements of NMR on Oriented 192Ir and 191Ir-m in Ni and Fe Host Lattices
NUCLEAR MOMENTS 192Ir, 191mIr; measured g. NMR.
doi: 10.1016/0370-2693(71)90716-7
Nucl.Phys. A176, 338 (1971)
R.H.Price, D.G.Burke, M.W.Johns
Proton States in 191Ir and 193Ir Populated by the (3He, d) and (α, t) Reactions
NUCLEAR REACTIONS 190,192Os(3He, d), E=28 MeV; measured σ(Ed); 190,192Os(α, t), E=28 MeV; measured σ(Et), Q. 191,193Ir deduced levels, J, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(71)90274-0
Nucl.Phys. A180, 321 (1972)
Z.Berant, J.Burde, A.Molchadzki
The Low-Lying States in 191Ir
RADIOACTIVITY 191Pt[from 190Pt(n, γ)]; measured Eγ, Iγ, I(ce), γγ(θ). 191Ir levels deduced J, π, ICC, γ-mixing. Enriched target.
doi: 10.1016/0375-9474(72)90172-8
Nucl.Phys. A181, 207 (1972)
D.S.Brenner, M.L.Perlman
Subshell Conversion-Line Intensity Ratios for Some Pure Transitions
RADIOACTIVITY 103Rh, 107Ag, 109Ag, 125Te, 160Dy, 166Ho, 191Ir, 197Hg; measured I(ce); deduced L-subshell ratios for M1, M4, E3 transitions, M-subshell ratios for E2, E3 transitions, γ-mixing(E2/M1). Enriched targets.
doi: 10.1016/0375-9474(72)90913-X
Z.Phys. 263, 341 (1973)
S.Buttgenbach, M.Herschel, G.Meisel, E.Schrodl, W.Witte, W.J.Childs
Hyperfine Structure Investigations in the 4F9/2 Atomic Ground State of 191Ir and 193Ir
NUCLEAR MOMENTS 191,193Ir; measured hfs, ABMR; deduced quadrupole moment, hyperfine anomaly.
Izv.Akad.Nauk Uzb.SSR, Ser.Fiz.-Mat.Nauk No.4, 79 (1973)
N.A.Ilkhamdzhanov, P.S.Radzhapov, K.T.Salikhbaev
Spectroscopy of 193Ir, 191Ir and 177Lu
RADIOACTIVITY 177Yb, 191Pt, 193Os; measured γγ(θ), γγ(t), γγ(θ, H, t). 177Lu, 191,193Ir deduced levels, J, π, T1/2, g, γ-mixing.
Phys.Rev. C7, 1555 (1973)
K.S.Krane, W.A.Steyert
Nuclear Orientation Studies of the Decays of 187W and 185,191,193Os
RADIOACTIVITY 187W, 185,191,193Os; measured Eγ, γ(θ) from polarized source. 191Ir deduced μ. 187Re, 193Ir deduced μ, γ-mixing.
Phys.Rev. C9, 2063 (1974)
K.S.Krane, W.A.Steyert
Nonalignment of the Magnetic Hyperfine Field of Ir in Fe
RADIOACTIVITY 191mIr; measured γ(θ, t) in Fe; deduced nonalignment of hyperfine field.
Helv.Phys.Acta 47, 482 (1974)
L.A.Schaller, W.Dey
Higher Muonic Transitions in Iridium: Determination of the quadrupole moment
NUCLEAR MOMENTS 191,193Ir; measured quadrupole moment.
At.Data Nucl.Data Tables 18, 137 (1976)
K.S.Krane
E2, M1 Multipole Mixing Ratios in Odd-Mass Nuclei, A > 150
COMPILATION A > 150; compiled, evaluated δ.
doi: 10.1016/0092-640X(76)90045-0
Z.Phys. A286, 333 (1978)
S.Buttgenbach, R.Dicke, H.Gebauer, R.Kuhnen, F.Traber
Hyperfine Structure of Six Low-Lying Fine Structure Levels of 191Ir and 193Ir and the 191Δ193 Hyperfine Anomaly
NUCLEAR MOMENTS 191,193Ir; measured hyperfine interaction constants A, B; deduced quadrupole moment.
Nucl.Phys. A313, 191 (1979)
J.Lukasiak, R.Kaczarowski, J.Jastrzebski, S.Andre, J.Treherne
Levels of 191Ir Excited in the (p, 2n) and (d, 3n) Reactions
NUCLEAR REACTIONS 192Os(p, 2nγ), E=12-24 MeV; 192Os(d, 3nγ), E=19-28 MeV; measured Eγ, Iγ, σ(E, Eγ, θ), γγ-coin, γ(t). 191Ir deduced levels, J, π, T1/2. 191mIr deduced T1/2. Enriched target.
doi: 10.1016/0375-9474(79)90575-X
Z.Phys. A290, 301 (1979)
C.Vieu, S.E.Larsson, G.Leander, I.Ragnarsson, W.De Wieclawik, J.S.Dionisio
The Particle Asymmetric Rotor Descriptions of 187-193Ir Positive Parity States
NUCLEAR STRUCTURE 187,189,191,193Ir; calculated energies, electromagnetic properties of positive parity states. Extended version of Hecht-Satchler model for particle plus asymmetric rotor.
J.Phys.(London) G7, 1713 (1981)
W.M.Lattimer, K.S.Krane, N.J.Stone, G.Eska
Nuclear Orientation of 191Pt in Fe
RADIOACTIVITY 191Pt [from 191Ir(d, 2n), E=20 MeV]; measured Iγ(θ), NMR, oriented nuclei; deduced μ. 191Ir transitions deduced δ. Model calculations.
doi: 10.1088/0305-4616/7/12/021
Hyperfine Interactions 15/16, 983 (1983)
I.Berkes, G.Marest, H.Sayouty
The Sign of the Magnetic Moment of 191Pt(g.s.) Determined by Mossbauer Effect on Oriented Nuclei
RADIOACTIVITY 191Pt(EC) [from Ir(d, xn)]; measured resonance absorption spectrum, Mossbauer effect, oriented nuclei. 191Ir transition deduced δ. 191Pt level deduced μ. Polarized split source, dilution refrigerator low temperature orientation.
Phys.Rev.Lett. 51, 1633 (1983)
Y.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro
Precision Muonic-Atom Measurements of Nuclear Quadrupole Moments and the Sternheimer Effect in Rare-Earth Atoms
ATOMIC PHYSICS, Mesic-Atoms 151,153Eu, 155,157Gd, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic X-rays, hfs; deduced 4f, 5d, 6p electronic state Sternheimer shielding factors.
NUCLEAR MOMENTS 151,153Eu, 155,157Gd, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic X-rays, hfs; deduced quadrupole moments.
doi: 10.1103/PhysRevLett.51.1633
Hyperfine Interactions 13, 149 (1983)
F.E.Wagner
Mossbauer Spectroscopy with 191,193Ir
NUCLEAR REACTIONS 191Ir(γ, γ), E=82, 129 keV; 193Ir(γ, γ), E=73, 139 keV; compiled, reviewed Mossbauer data, techniques, source preparation procedures.
Phys.Lett. 140B, 17 (1984)
K.H.Burger, S.Buttgenbach, R.Dicke, G.Golz, F.Traber
Direct Measurement of the Nuclear Magnetic Dipole Moments of 191Ir and 193Ir by High-Precision Atomic Beam Magnetic Resonance
NUCLEAR MOMENTS 191,193Ir; measured hfs; deduced hfs constants, atomic diamagnetism uncorrected μ. ABMR technique, high precision.
doi: 10.1016/0370-2693(84)91038-4
Nucl.Phys. A426, 144 (1984)
S.J.Mundy, J.Lukasiak, W.R.Phillips
The Spin(6) Scheme and Electromagnetic Transitions in 191Ir and 193Ir
NUCLEAR STRUCTURE 191,193Ir, 192,194,196,198Pt; calculated levels, B(λ). Interacting boson-fermion model, Spin(6) scheme.
NUCLEAR REACTIONS Ir, Pt(p, p'), (α, α'), E=5-6 MeV; measured σ(Eγ, θ), Eγ, Iγ, Coulomb excitation. 191,193Ir, 192,194,196,198Pt deduced levels, B(λ), δ. Natural targets.
doi: 10.1016/0375-9474(84)90070-8
Phys.Rev. C29, 1830 (1984)
Y.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro
Systematics of Ground-State Quadrupole Moments of Odd-A Deformed Nuclei Determined with Muonic M X Rays
NUCLEAR MOMENTS 151,153Eu, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic hfs, E(M X-ray), I(M X-ray); deduced ground state quadrupole moments, β2. 151,153Eu deduced large deformation change.
ATOMIC PHYSICS, Mesic-Atoms 151,153Eu, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic hfs, E(M X-ray), I(M X-ray); deduced implication on Steinheimer correction factors.
Hyperfine Interactions 24, 223 (1985)
R.M.Steffen
Precision Measurements of Nuclear Quadrupole Moments by Muonic X-Rays
ATOMIC PHYSICS, Mesic-Atoms 151,153Eu, 155,157Gd, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic X-rays.
NUCLEAR MOMENTS 151,153Eu, 155,157Gd, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic hfs, X-rays; deduced ground state quadrupole moment. High precision.
Nucl.Phys. A456, 349 (1986)
W.R.Kolbl, J.Billowes, J.Burde, J.A.G.De Raedt, M.A.Grace, A.Pakou
g-Factor and Lifetime Measurements in 191,193Ir
NUCLEAR REACTIONS 191,193Ir(32S, 32S'), E=89, 118 MeV; measured Coulomb excitation, γ(θ, H), γ(θ, t), recoil. 191,193Ir levels deduced g, T1/2. Transient field method, IMPAC technique.
doi: 10.1016/0375-9474(86)90398-2
Phys.Rev. C33, 855 (1986)
F.K.McGowan, N.R.Johnson, I.Y.Lee, W.T.Milner, C.Roulet, J.Hattula, M.P.Fewell, Y.A.Ellis-Akovali, R.M.Diamond, F.S.Stephens, M.W.Guidry
Test of the Triaxial Rotor Model and the Interacting Boson Fermion Approximation Model Description of Collective States in 191Ir
NUCLEAR REACTIONS 191Ir(40Ar, 40Ar'), E=160 MeV; 191Ir(136Xe, 136Xe'), E=617 MeV; measured Eγ, Iγ(θ) following Coulomb excitation. 191Ir deduced levels, J, π, B(λ).
Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 1889 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.11, 14 (1987)
P.T.Prokofev, G.L.Rezvaya, L.I.Simonova
Study of the Excited States for 191,193Ir in (n, n'γ) Reactions
NUCLEAR REACTIONS 191,193Ir(n, n'γ), E=fast; measured Eγ, Iγ. 191,193Ir deduced levels, J, π.
Hyperfine Interactions 43, 493 (1988)
E.Scheidemann, R.Eder, E.Hagn, E.Zech
A Transmission γ-Ray Polarimeter for Sign Measurements of Magnetic Moments of Radioactive Nuclei
RADIOACTIVITY 60Co, 193Os, 191m,192,194Ir, 195mPt; measured γ(θ), γ CP, oriented nuclei; deduced μ sign. Transmission γ-ray polarimeter, low temperature nuclear orientation.
Z.Phys. D14, 9 (1989)
G.Sawatzky, R.Winkler
Isotope Shift and Hyperfine Structure in the Iridium I Spectrum
NUCLEAR MOMENTS 191,193Ir; measured hfs, isotope shifts; deduced hyperfine, isotope shift, nuclear parameters.
Z.Phys. A340, 235 (1991)
E.Scheidemann, R.Eder, E.Hagn, E.Zech
A Mini Transmission γ-Ray Compton Polarimeter and Measurements of the Sign of Magnetic Moments of Radioactive Nuclei
RADIOACTIVITY 193Os;191mIr, 192,194Ir, 195mPt; measured sign of μ. Low temperature nuclear orientation, mini-transmission γ-ray Compton polarimeter.
Hyperfine Interactions 97/98, 409 (1996)
E.Hagn
Recent Developments and New Trends in NMR on Oriented Nuclei
NUCLEAR MOMENTS 169,171,172,173,174,177,177mLu; compiled, reviewed hfs, μ, quadrupole moments, quadrupole interaction in Co. 184,186,186m,188,186,191,193,195,197,198,199Au, 185,187,189Pt, 189,191,192,193Ir; compiled reviewed quadrupole moments, ratio. 90,95,96Nb, 90m,95Zr, 111In, 193m,195m,197mAu, 197mHg; compiled, reviewed quadrupole interaction changes. 90Nb, 90mZr; compiled, reviewed NMR data, oriented nuclei.
Phys.Rev. C54, 1129 (1996)
S.Ohya, T.Ohtsubo, K.Komatsuzaki, D.J.Cho, S.Muto
Measurements for Spin Inversion and Noninversion in Successive Decays Via Nuclear Magnetic Resonance on Oriented Nuclei
RADIOACTIVITY 89Zr(β+), (EC); 89mY(IT) [from 89Zr decay]; 191Os(β-); 191mIr(IT) [from 191Os decay]; measured Iγ(θ, T, H), NMR, oriented nuclei; deduced μ, related features.
Hyperfine Interactions 97/98, 479 (1996)
A.E.Stuchbery, S.S.Anderssen, E.Bezakova
IMPAC In-Beam and Out-of-Beam; g-Factors and pre-equilibrium effects following ion-implantation
NUCLEAR REACTIONS 188,190,192Os, 194,196,198Pt(16O, 16O'), E=36 MeV; 194,196,198Pt(28Si, 28Si'), E=60 MeV; 194,196,198Pt(34S, 34S'), E=80 MeV; 188,190,192Os(32S, 32S'), E=80 MeV; 191,193Ir(58Ni, 58Ni'), E=155, 180 MeV; measured γγ(θ, H), implanted recoil nuclei. 191,193Ir, 188,190,192Os levels deduced g factors.
Nucl.Phys. A669, 241 (2000)
E.Bezakova, A.E.Stuchbery, H.H.Bolotin, W.A.Seale, S.Kuyucak, P.Van Isacker
Electromagnetic Properties of Low-Excitation States in 191Ir and 193Ir and Supersymmetry Schemes
NUCLEAR REACTIONS 191,193Ir(58Ni, 58Ni'), E=155, 180 MeV; 191,193Ir(65Cu, 65Cu'), E=130 MeV; 191,193Ir(32S, 32S'), E=100 MeV; 191,193Ir(16O, 16O'), E=40 MeV; measured Eγ, Iγ(θ, H, T) in polarized Gd, Fe following Coulomb excitation, (recoil)γ-, (particle)γ-coin. 191,193Ir levels deduced g-factors, δ, T1/2. Thin-foil transient-field IMPAC technique, recoil-distance lifetime measurement.
NUCLEAR STRUCTURE 191,193Ir; calculated g-factors, B(M1), B(E2). Particle-triaxial-rotor model, supersymmetry models.
doi: 10.1016/S0375-9474(99)00565-5
Hyperfine Interactions 127, 79 (2000)
D.Verney, F.Le Blanc, L.Cabaret, J.Crawford, H.T.Duong, J.Genevey, G.Huber, F.Ibrahim, M.Krieg, J.K.P.Lee, D.Lunney, J.Obert, J.Oms, J.Pinard, J.C.Putaux, B.Roussiere, J.Sauvage, V.Sebastian, and the ISOLDE Collaboration
Nuclear moments of neutron-deficient iridium isotopes from laser spectroscopy
NUCLEAR MOMENTS 182,183,184,185,186,186m,187,188,189,191,193Ir; measured hfs, isotope shifts; deduced μ, quadrupole moments, radii, deformation parameters. Multiple-step laser ionization.
Yad.Fiz. 64, No 6, 1123 (2001); Phys.Atomic Nuclei 64, 1048 (2001)
B.Roussiere, F.Ibrahim, J.Libert, J.Sauvage, D.Verney, L.Cabaret, J.E.Crawford, J.Genevey, D.Hojman, G.Huber, A.Knipper, F.Le Blanc, J.K.P.Lee, G.Marguier, J.Oms, J.Pinard, A.Wojtasiewicz
Properties of the Low-Lying Levels in the Transitional Ir and Au Nuclei
NUCLEAR STRUCTURE 183,185,187,189,191,193Ir, 183,185,187,189,191,193,195,197Au; calculated levels, J, π, μ, quadrupole moments. Axial rotor plus one or two quasiparticles, comparisons with data.
doi: 10.1134/1.1383615
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
Eur.Phys.J. A 30, 489 (2006)
D.Verney, L.Cabaret, J.E.Crawford, H.T.Duong, B.Fricke, J.Genevey, G.Huber, F.Ibrahim, M.Krieg, F.Le Blanc, J.K.P.Lee, G.Le Scornet, D.Lunney, J.Obert, J.Oms, J.Pinard, J.C.Putaux, K.Rashid, B.Roussiere, J.Sauvage, V.Sebastian, and the ISOLDE Collaboration
Deformation change in light iridium nuclei from laser spectroscopy
NUCLEAR MOMENTS 182,183,184,185,186,186m,187,188,189,191,193Ir; measured hfs, isotope shift; deduced μ, quadrupole moments, radii, β2. Laser spectroscopy.
NUCLEAR STRUCTURE 180,184,186,192Os; calculated potential energy surfaces. 183,185,187,189,191,193Ir; calculated β2, μ, quadrupole moments. 182,184,186Ir; calculated single-particle level energies. 183,185,186Ir; calculated rotational band level energies, configurations. Axial rotor plus one or two quasiparticles.
doi: 10.1140/epja/i2006-10140-7
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
At.Data Nucl.Data Tables 111-112, 1 (2016)
N.J.Stone
Table of nuclear electric quadrupole moments
COMPILATION Z=1-99; compiled experimental values of nuclear electric quadrupole moments.
doi: 10.1016/j.adt.2015.12.002
INDC(NDS)-0794 (2019)
N.J.Stone
Table of Recommended Nuclear Magnetic Dipole Moments: Part I - Long-lived States
COMPILATION Z=0-99; compiled experimental values of nuclear magnetic moments.
INDC(NDS)-0816 (2020)
N.Stone
Table of Recommended Nuclear Magnetic Dipole Moments: Part II, Short-Lived States
COMPILATION Z=5-95; compiled experimental values of nuclear magnetic moments.
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.