References quoted in the ENSDF dataset: 206PB ADOPTED LEVELS, GAMMAS
97 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 92, 514 (1953)
D.E.Alburger, M.H.L.Pryce
Isomerism in Pb206
RADIOACTIVITY 206Bi(EC); measured I(ce). 206Pb deduced levels, isomer T1/2.
Phys.Rev. 99, 112 (1955)
P.H.Stelson, F.K.McGowan
Gamma-Ray Yields from Coulomb Excitation
Arkiv Fysik 12, 237 (1957)
B.Astrom
Half-Lives of Isomeric States in Pb202, Pb203, Pb206, and Tl202
Nucl.Instrum. 1, 95 (1957)
P.A.Tove
Electronic Time Analyzer Applied to the Measurement of the Half-Lives of Metastable States
CEA-1531 (1960)
R.Barloutaud
Contribution a l'Etude des Etats Collectifs des Noyaux Lourds par Excitation Colombienne
NUCLEAR REACTIONS 182,184,186W, 186,188,189,190,192Os, 194,196,198Pt, 198,200,202,204Hg, 206Pb(p, p'), E=5 MeV; measured not given; deduced transition probabilities following Coulomb excitation.
Nucl.Instrum.Methods 8, 151 (1960)
I.Bergstrom, E.C.O.Bonacalza, A.Jech, M.Perez, P.Thieberger
The Oscilloscope Method of Measuring Nuclear Half-Lives
RADIOACTIVITY 205m,206m,203mPb, 181mTa, 85mRb; measured T1/2. Oscilloscope method.
Zhur.Eksptl.I Teoret.Fiz. 40, 341 (1961); Soviet Phys.JETP 13, 232 (1961)
V.N.Guman, L.A.Sliv, G.A.Sogomonova
NUCLEAR STRUCTURE 206Pb; measured not abstracted; deduced nuclear properties.
Phys.Rev. 127, 1284 (1962); Erratum Phys.Rev. 138, AB2 (1965)
P.Mukherjee, B.L.Cohen
Nuclear Structure Studies in the Lead Region with Stripping Reactions
NUCLEAR STRUCTURE 207Pb, 205Pb, 206Pb, 208Pb, 209Pb, 208Bi, 210Bi; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 30, 332 (1962)
O.Nathan
Coulomb Excitation of Lead and Bismuth with 20 MeV α-Particles
NUCLEAR STRUCTURE 209Bi, 206Pb, 207Pb, 204Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90057-3
Arkiv Fysik 22, 127 (1962)
P.Thieberger
Wide Range Time to Pulse Height Converter
NUCLEAR STRUCTURE 206Bi, 60Co, 44Ti, 108Ag, 110Ag, 127Xe, 133Xe; measured not abstracted; deduced nuclear properties.
Ark.Fys. 24, 311 (1963)
B.Sigfridsson
The High Frequency Deflection Method for Measuring Short Half-Lives. Part 3. The Time Calibration, the Shape of a Time-Resolution Curve and a Description of Some of the Electronic Equipment
NUCLEAR STRUCTURE 206Bi; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 71, 348 (1965)
R.J.Lombard
Magnetic Moments of Some Excited States of Sn and Pb Isotopes
NUCLEAR STRUCTURE 202Pb, 200Pb, 206Pb, 204Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(65)90722-4
Nucl.Phys. 87, 1 (1966)
H.L.Acker, G.Backenstoss, C.Daum, J.C.Sens, S.A.De Wit
Measurement and Analysis of Muonic X-Ray Spectra in Spherical Nuclei
NUCLEAR REACTIONS 121Sb(μ-, νnγ), 123Sb(μ-, νnγ), 139La(μ-, νnγ), E > 100 MeV; measured Eγ. 120Sn, 122Sn, 138Ba deduced levels. 66Ga [from zn(p, γ)]; measured Eγ. Cl, Ca, Fe, Sn, Sb, Te, I, Cs, Ba, La, Ce, Pr, Nd, Au, Hg, Tl, 206Pb, Pb, Bi; measured E(X-ray), I(X-ray), deduced nuclear charge distribution parameters.
doi: 10.1016/0029-5582(66)90355-5
Phys.Lett. 23, 468 (1966)
R.D.Ehrlich, D.Fryberger, D.A.Jensen, C.Nissim-Sabat, R.J.Powers, B.A.Sherwood, V.L.Telegdi
Energy Shifts and Intensity Ratios in the Muonic X-Ray Spectra of the Pb Isotopes 206, 207 and 208
NUCLEAR STRUCTURE, Mesic-Atoms 208Tl, 206Tl, 207Tl; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90778-5
Nucl.Phys. 79, 495 (1966)
A.Z.Hrynkiewicz, S.Kopta, S.Szymczyk, T.Walczak
Octupole Coulomb Excitation of the 208Pb Nucleus
NUCLEAR REACTIONS 204,206,207,208Pb(12C, 12C'γ), E = 45.5-60.2 MeV; measured Iγ, Eγ, (γ)(12C')-coin 204,206,207,208Pb deduced B(λ).
doi: 10.1016/0029-5582(66)90258-6
CEA-R-2900 (1966)
E.Monnand
Etude de Corps Radioactifs a Vie Tres Breve Produits par Neutrons Rapides
RADIOACTIVITY 12B, 24Na, 88Y, 114In, 202,204Tl, 205,206,207Pb, 208Bi; measured T1/2.
Nucl.Phys. A100, 545 (1967)
T.W.Conlon
High-Resolution Studies of the Gamma Rays from Isomeric States with Half-Lives of 10μs-30ms in Nuclei with Z = 63-83
RADIOACTIVITY 151mEu, 153mGd, 153mTb, 159mDy, 165mTm, 172m,173mLu, 175mHf, 181mTa, 180m,181mW, 187mOs, 187m,189mIr, 191mPt, 199m,200m,201mTl, 206mPb, 207mBi; measured T1/2, Eγ, E(X-ray)-ray; deduced levels, J, π. Natural, enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(67)90123-6
Phys.Rev. 171, 1308 (1968)
P.Richard, N.Stein, C.D.Kavaloski, J.S.Lilley
Two-Neutron-Hole Configurations in Pb206 from Isobaric Analog Measurements
NUCLEAR STRUCTURE 206Pb; measured not abstracted; deduced nuclear properties.
Nucl.Instr.Methods 61, 58 (1968)
M.Tatcher, H.Lindeman
Measurement of Half-Lives of Isomeric Nuclear States by a Method of Time Interval Analysis
RADIOACTIVITY 206mPb; measured T1/2. Integral time interval analysis.
Phys.Rev. 166, 1167 (1968)
R.Tickle, J.Bardwick
Structure of Pb206 Determined by the (d, t) Reactions
NUCLEAR STRUCTURE 206Pb; measured not abstracted; deduced nuclear properties.
Phys.Rev. 168, 1388 (1968)
W.W.True
Shell-Model Theory of Pb206. II
Phys.Rev. 165, 1337 (1968)
J.F.Ziegler, G.A.Peterson
Excitation of Pb206, Pb207, Pb208, and Bi209 by Inelastic Electron Scattering
NUCLEAR REACTIONS 206,207,208Pb, 209Bi(e, e'), E=28-73 MeV; measured σ(Ee'). 206,207,208Pb, 209Bi levels deduced B(EL).
Phys.Rev.Lett. 22, 221 (1969)
H.L.Anderson, C.K.Hargrove, E.P.Hincks, J.D.McAndrew, R.J.McKee, D.Kessler
Muonic X Rays in Pb206 and Possible Observation of Nuclear Polarization
ATOMIC PHYSICS, Mesic-Atoms 206Pb; measured muonic X-rays; deduced nuclear polarization.
doi: 10.1103/PhysRevLett.22.221
Phys.Rev. 187, 1565 (1969)
H.L.Anderson, C.K.Hargrove, E.P.Hincks, J.D.McAndrew, R.J.McKee, R.D.Barton, D.Kessler
Precise Measurement of the Muonic X Rays in the Lead Isotopes
NUCLEAR REACTIONS 206,207,208Pb(μ-, xnγ), E ≈ 0; measured Eγ, Iγ. 203,205,206Tl deduced transitions. 206,207,208Pb; measured muonic X-ray spectra; deduced isotope shift, nuclear charge distributions.
Phys.Rev. 185, 1429 (1969)
K.W.Ford, J.G.Wills
Muonic Atoms and the Radial Shape of the Nuclear Charge Distribution
ATOMIC PHYSICS, Mesic-Atoms 206,208Pb; calculated transition energies.
Phys.Rev. C1, 1819 (1970)
P.B.Price, R.L.Fleischer, R.T.Woods
Search for Spontaneously Fissioning Elements in Nature
RADIOACTIVITY 197Au, 204,206,207,208Pb; measured fission tracks. Z=111, Z=114 deduced limit on spontaneous fission T1/2.
Nucl.Phys. A150, 68 (1970)
J.L.Quebert, K.Nakai, R.M.Diamond, F.S.Stephens
Lifetime Measurement of the First Excited State in 206Pb
NUCLEAR REACTIONS 206Pb(40Ar, 40Ar'γ), E=170 MeV; measured recoil-distance, Doppler-shift. 206Pb level deduced T1/2, B(E2).
doi: 10.1016/0375-9474(70)90456-2
Z.Naturforsch. 25a, 975 (1970)
D.Quitmann, J.M.Jaklevic
Measurement of the Magnetic Moments of the Microsecond-Isomers in 73As and 206Pb
RADIOACTIVITY 73mAs, 206mPb; measured Iγ(θ, H). 73As, 206Pb deduced g for isomeric states.
Nucl.Phys. A146, 215 (1970)
F.C.Zawislak, J.D.Bowman
Nuclear g-Factor Measurements of Two Short-Lived States in 206Pb
RADIOACTIVITY 206Bi[from 206Pb(d, 2n)]; measured γγ(θ, H) in Fe lattice. 206Pb levels deduced μ.
doi: 10.1016/0375-9474(70)91099-7
Phys.Scr. 3, 11 (1971)
I.Bergstrom, J.Blomqvist, B.Fant, A.Filevich, G.Linden, K.-G.Rensfelt, J.Sztarkier, K.Wikstrom
E2 Core Polarization by Neutrons in the (i13/2)-2 Configuration in 206Pb
NUCLEAR REACTIONS 204Hg(α, 2nγ), E = 26 MeV; measured Eγ, Iγ, αγ-delay. 206Pb deduced levels, T1/2, B(EL), neutron E2 core polarization charge.
Nucl.Phys. A174, 525 (1971)
E.Grosse, M.Dost, K.Haberkant, J.W.Hertel, H.V.Klapdor, H.J.Korner, D.Proetel, P.von Brentano
Coulomb Excitation of the Lead Isotopes with α and 16O Beams
NUCLEAR REACTIONS 204,206,207,208Pb(α, α'γ), E=15, 18 MeV; 206,207,208Pb(16O, 16O'γ), E=70, 80 MeV; measured Eγ, Iγ, Doppler-shift attenuation. 204,206,207,208Pb deduced B(EL) , B(ML), T1/2. Natural, enriched targets.
doi: 10.1016/0375-9474(71)90400-3
Nucl.Phys. A194, 113 (1972)
O.Hausser, F.C.Khanna, D.Ward
Gamma Decay of Low-Lying States Near the 208Pb Closed Shell
NUCLEAR REACTIONS 204,206,207,208Pb, 209Bi(α, α'γ), E=15-18 MeV; 204,206,207,208Pb, 209Bi(16O, 16O'γ), E=69-80 MeV; measured Eγ, σ(Eγ), DSA. 208Pb(7Li, α2nγ), 208Pb(7Li, 6Li), E=28-31.5 MeV; measured αγ-coin, Eγ, DSA. 204,206,207,208,209Pb, 209Bi deduced B(EL), B(ML), T1/2. Enriched, natural targets.
doi: 10.1016/0375-9474(72)91055-X
Nucl.Phys. A192, 151 (1972)
M.Kanbe, M.Fujioka, K.Hisatake
Level Structure of 206Pb Studied from the Decay of 206Bi
RADIOACTIVITY 206Bi[from 207Pb(p, 2n), Pb(p, xn), 209Bi(p, 4n)]; measured E(ce), I(ce), Iγ, L-subshell ratios; deduced log ft. 206Pb deduced levels, α(K), γ-multipolarity, J, π. Enriched, natural targets, Ge(Li) spectrometers.
doi: 10.1016/0375-9474(72)90011-5
Nucl.Phys. A186, 97 (1972)
K.H.Maier, K.Nakai, J.R.Leigh, R.M.Diamond, F.S.Stephens
Stroboscopic Measurement of the g-Factors of the 7- Isomer in 206Pb and the 21/2+ Isomer in 207Bi
NUCLEAR REACTIONS 204Hg(α, 2nγ), E=26 MeV; 204Hg(7Li, 4nγ), E=41 MeV; measured αγ(θ, H, t). 206mPb, 207mBi deduced μ. Stroboscopic method.
doi: 10.1016/0375-9474(72)90127-3
Phys.Rev. C6, 1870 (1972)
J.C.Manthuruthil, D.C.Camp, A.V.Ramayya, J.H.Hamilton, J.J.Pinajian, J.W.Doornebos
Excited States in 206Pb from the Decay of 206Bi
RADIOACTIVITY 206Bi; measured Eγ, Iγ, γγ-coin; deduced log ft. 206Pb deduced levels, J, π, ICC, γ-branching, γ-multipolarity.
Nucl.Phys. A189, 526 (1972)
K.Nakai, B.Herskind, J.Blomqvist, A.Filevich, K.-G.Rensfelt, J.Sztarkier, I.Bergstrom, S.Nagamiya
The g-Factor of the 12+ Isomeric State in 206Pb and the Effective Orbital g-Factor of the Neutron
NUCLEAR REACTIONS 204Hg(α, 2nγ), E=27 MeV; measured αγ(θ, H, t). 206mPb deduced g, neutron effective orbital g.
doi: 10.1016/0375-9474(72)90311-9
Phys.Rev.Lett. 29, 878 (1972)
J.W.Tape, E.G.Adelberger, D.Burch, L.Zamick
Lifetime of the 0+2 State of 206Pb and the State Dependence of the Monopole Effective Charge
NUCLEAR REACTIONS 206Pb(p, p'γ), E=12.25 MeV; measured E(ce), I(ce), p'ce-delay. 206Pb level deduced T1/2.
doi: 10.1103/PhysRevLett.29.878
LYCEN-7301, p.55 (1973)
J.Daniere, R.Rougny
Application de L'intercorrelation Digitale a L'etude des Niveaux Nucleaires Excites de vie Moyenne Superieure a 1μ s
RADIOACTIVITY 206Pb level measured T1/2.
KFK-1783, p.65 (1973)
N.Brauer, B.Focke, A.Goldmann, J.Hadijuana, M.v.Hartrott, K.Nishiyama, D.Quitmann, D.Riegel, W.Zeitz
Quadrupolrelaxation von 206Pb in Flussigeon Hg
NUCLEAR REACTIONS 204Hg(α, 2nγ); measured γγ(θ, H). 206Pb levels deduced quadrupole moment.
Nucl.Phys. A212, 478 (1973)
M.Kaplan, P.D.Johnston, P.Kittel, N.J.Stone
Gamma-Ray Multipolarity Studies by the Nuclear Orientation of 206Bi in Nickel; Perturbation in the 120 μs 2.2 MeV State of 206Pb
RADIOACTIVITY 206Bi; measured Iγ(θ, t); deduced Heff, γ-ray multipolarities, Pb intermediate state reorientation. 206Pb transitions deduced γ-mixing.
doi: 10.1016/0375-9474(73)90819-1
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 142,143,144,145,146,148,150Nd, 147,148,149,150,152,154Sm, 161,162,163,164Dy, 170,171,172,173,174,176Yb, 204,206,207,208Pb(γ, X-ray); measured isotope shift. 142,143,144,145,146,148,150Nd, 147,148,149,150,152,154Sm, 161,162,163,164Dy, 170,171,172,173,174,176Yb, 204,206,207,208Pb deduced nuclear charge radii.
Phys.Rev. C8, 2313 (1973)
C.W.Ma, W.W.True
Shell Model in the Lead Region
NUCLEAR STRUCTURE 206,210Pb, 210Po, 208,210Bi, 206,208Tl, 206Hg; calculated levels, J, π, binding energies, γ-branching, γ-mixing, S.
Phys.Rev. C8, 2453 (1973)
P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins, R.J.Powers, A.R.Kunselman
Nuclear Polarization and Charge Parameters Using the Muonic 2s State
ATOMIC PHYSICS 120Sn, 138Ba, 140,142Ce, 206Pb; measured muonic X-rays. Deduced nuclear polarization.
J.Inorg.Nucl.Chem. 35, 2139 (1973)
G.N.Salaita, P.K.Eapen
Isomeric Cross Sections for (n, 2n) Reactions in Thallium, Lead, and Bismuth at 14.8 MeV
RADIOACTIVITY 202,202mTl, 205m,206m,207mPb, 208mBi; measured T1/2, Eγ.
NUCLEAR REACTIONS 203,205Tl, 206,207,208Pb, 209Bi(n, 2nγ), E=14.8 MeV; measured σ(Eγ).
doi: 10.1016/0022-1902(73)80276-3
Phys.Rev. C9, 2444 (1974)
K.W.Ford, G.A.Rinker, Jr.
Comparison of Muonic-Atom and Electronic X-Ray Isotope Shifts in Lead
NUCLEAR STRUCTURE, Mesic-Atoms 208,207,206,204Pb; analyzed muonic isotopic shifts, compared electronic shifts.
Nucl.Phys. A221, 555 (1974)
A.Olin, O.Hausser, T.K.Alexander, A.J.Ferguson, W.Witthuhn
Static Moments of the First Excited States of 32,34S and 204,206Pb
NUCLEAR REACTIONS 204Pb(32S, 32S'γ), E=100, 112.5, 125 MeV; 206Pb(34S, 34S'γ), E=122 MeV; measured σ(E, θ(p), θ(γ), phi(γ)). 32,34S, 204Pb levels deduced B(E2), quadrupole moment. 204,206Pb levels deduced g. NaI(Tl) detectors. Enriched targets.
doi: 10.1016/0375-9474(74)90482-5
Phys.Rev. C11, 1719 (1975)
D.Kessler, H.Mes, A.C.Thompson, H.L.Anderson, M.S.Dixit, C.K.Hargrove, R.J.McKee
Muonic X Rays in Lead Isotopes
ATOMIC PHYSICS, Mesic-Atoms 204,206,207,208Pb(μ-, X-ray), E approx 0; measured muonic transition energies, L-linewidth. 204,206,207,208Pb deduced nuclear polarization, Fermi parameters, anomalous fs splitting, isotope shift.
Phys.Scr. 11, 228 (1975)
D.Riegel
Relaxation Rates of Excited Nuclei in Liquid Metals
NUCLEAR REACTIONS 71Ga(p, nγ), 130Te(α, 3nγ); measured γ(θ, H). 71Ge, 132Xe levels deduced g.
Phys.Lett. 65B, 337 (1976)
R.Julin, J.Kantele, M.Luontama, T.Poikolainen, V.Rahkonen
Half-Lives of Two-Neutron-Hole 0+2 States in 206Pb and 208Po
NUCLEAR REACTIONS 209Bi(p, 2n), E=14.8 MeV; measured γ(t). 208Po, 206Pb deduced levels, λ, T1/2.
doi: 10.1016/0370-2693(76)90236-7
Phys.Rev. C16, 1594 (1977)
J.E.Draper, R.J.McDonald, N.S.P.King
In-Beam Study of 206Pb Level Scheme Including Conversion Electrons ≥ 40 keV
NUCLEAR REACTIONS 204Hg(α, 2nγ), E=30 MeV; measured I(ce), Eγ, Iγ, γγ-coin, γ(t). 206Pb deduced levels, J, π, ICC. Ge(Li), Si(Li) detectors.
Can.J.Phys. 55, 456 (1977)
P.R.H.McConnell, P.W.Martin, B.G.Turrell
Nuclear Orientation of 206Bi in Nickel
RADIOACTIVITY 206Bi; measured γ-spectra, γ(θ, t); deduced hyperfine field. 206Pb transitions deduced δ.
Z.Phys. A281, 355 (1977)
G.Vanden Berghe
Interplay of Valence-Shell Clusters and the Vibrational Field in 205Pb And 206Pb
NUCLEAR STRUCTURE 205,206Pb; calculated levels, S, B(E2).
Phys.Lett. 72B, 307 (1978)
A.M.R.Joye, A.M.Baxter, S.Hinds, D.C.Kean, R.H.Spear
Quadrupole Moments of the First Excited States of 204,206Pb
NUCLEAR REACTIONS 204,206Pb(α, α'), E=13.8-18.5 MeV; 204,206Pb(12C, 12C'), E=44-60 MeV; 204,206Pb(16O, 16O'), E=59-85 MeV; measured Coulomb excitation. 204,206Pb deduced quadrupole moment, B(E2).
doi: 10.1016/0370-2693(78)90125-9
Aust.J.Phys. 31, 377 (1978)
R.H.Spear, T.H.Zabel, A.M.Baxter, M.P.Fewell, S.Hinds, A.M.R.Joye, D.C.Kean
Determination of Maximum Safe Bombarding Energies and B(E3) Values in Reorientation Experiments with 204Pb, 206Pb and 208Pb
NUCLEAR REACTIONS 204,206Pb(α, α), (α, α'), E=13.8 MeV; 204,206Pb(12C, 12C), (12C, 12C'), E=52 MeV; 204,206,208Pb(16O, 16O), (16O, 16O'), E=60 MeV; measured σ(elastic), σ(inelastic); deduced optimum E-projectile for onset of Coulomb, nuclear interference. 204,206Pb deduced B(E3).
Phys.Lett. 88B, 48 (1979)
H.-E.Mahnke, T.K.Alexander, H.R.Andrews, O.Hausser, P.Taras, D.Ward, E.Dafni, G.D.Sprouse
Quadrupole Moments of the 12+ States in 206Pb and 200Pb
NUCLEAR REACTIONS 204,198Hg(α, 2n), E=33 MeV; measured γ(θ, H, t). 206,200Pb levels deduced quadrupole moments, T1/2, B(E2).
doi: 10.1016/0370-2693(79)90110-2
Nucl.Phys. A342, 485 (1980)
C.Bargholtz, S.Beshai, M.El-Khosht, B.Sundstrom, C.Wiktorsson
Gamma-Ray Multipolarities in 206Pb Studied by Gamma-Gamma Directional Correlations
RADIOACTIVITY 206Bi [from 206Pb(p, n)]; measured γγ(θ). 206Pb levels deduced δ, B(λ). Natural target.
doi: 10.1016/0375-9474(80)90557-6
Z.Phys. A296, 93 (1980)
A.Timmermann
High Resolution Two-Photon Spectroscopy of the 6p2 3P0 - 7p 3P0 Transition in Stable Lead Isotopes
NUCLEAR MOMENTS 204,206,207,208Pb; measured optical isotope shift. Doppler free two-photon, laser-induced transition.
JUL-Spez-99, p.46 (1981)
G.L.Borchert, P.G.Hansen, J.B.McGrory, B.Jonson, H.L.Ravn, O.W.B.Schult, J.Speth
Isotope Shifts of K X-Rays of Lead
NUCLEAR REACTIONS 204,206,207,208Pb(X, X), E not given; measured K X-ray isotope shifts. 208,207,206,204Pb deduced rms charge radii.
ORNL/TM-8137 (1982)
J.K.Dickens
206Pb Level Structure from 206Pb(n, n'γ) Measurements
NUCLEAR REACTIONS 206Pb(n, n'γ), E not given; measured γ-spectra. 206Pb deduced levels.
Phys.Rev. C25, 2614 (1982)
C.L.Hollas, C.R.Newsom, P.J.Riley, B.E.Bonner, G.Glass
Deuteron Spectrum in np → d(ππ)0 at 1.46 GeV/c
NUCLEAR REACTIONS 1H(n, d), E=795 MeV; measured σ(θ) vs deuteron momentum, missing mass spectra.
KFK-3344 (1982)
H.Rebel, G.Schatz
Laser Induced Flourescence Spectroscopy in Atomic Beams of Radioactive Nuclides
NUCLEAR MOMENTS 40,41,42,44,45,46,47,48Ca, 204,206,207,208Pb, 130,132,134,136,137,138Ba; analyzed hfs, isotope shift data; deduced rms charge radius variation with mass.
Z.Phys. A311, 185 (1983)
J.Rikovska, D.Novakova, J.Ferencei, M.Finger
Gamma-Ray Polarization and Nuclear Orientation Measurements on 182Ta(Fe)
RADIOACTIVITY 182Ta(β-); measured linear polarization, γγ(θ), oriented nuclei. 182W deduced transition γ-multipolarity, δ, B(λ) ratios, hindrance factors.
Nucl.Phys. A411, 248 (1983)
Ch.Stenzel, H.Grawe, H.Haas, H.-E.Mahnke, K.H.Maier
Magnetic Moments of (νi13/2)(-n) Isomers in Neutron-Deficient Lead Isotopes
NUCLEAR REACTIONS 156Gd(40Ar, 4n), E=185 MeV; 196,198,204Hg(α, xn), E=45, 60 MeV; measured Iγ(θ, H, t). 192,196,198,200,205,206Pb level deduced g, T1/2. Ge(Li) detectors, enriched liquid metallic Hg targets.
doi: 10.1016/0375-9474(83)90391-3
J.Phys.(London) G9, 443 (1983)
R.C.Thompson, M.Anselment, K.Bekk, S.Goring, A.Hanser, G.Meisel, H.Rebel, G.Schatz, B.A.Brown
High-Resolution Measurements of Isotope Shifts and Hyperfine Structure in Stable and Radioactive Lead Isotopes
RADIOACTIVITY 210Pb; 212Pb [from 232Th decay]; 205Pb [from 204Pb(n, γ)]; 209Pb [from 208Pb(d, p)]; 198,199,200,202Pb [from Hg(α, xn), E=104 MeV]; 201,202m,203Pb [from Tl(d, xn), E=38, 48 MeV]; measured hfs, isotope shifts. 201,202m,205,209Pb deduced μ, quadrupole moment, rms charge radii. 199Pb level deduced J, π, μ, quadrupole moment, rms charge radius. 198,210,212Pb deduced rms charge radius. Droplet model, Skyrme interactions.
NUCLEAR MOMENTS 204,206,207Pb; measured hfs, isotope shifts; deduced rms charge radii. Droplet model, Skyrme interactions.
doi: 10.1088/0305-4616/9/4/010
Phys.Rev. C30, 704 (1984)
M.V.Hoehn, E.B.Shera
Energies of the Muonic L and M Transitions of the Even-A Pb Isotopes
NUCLEAR MOMENTS 204,206,208Pb; measured muonic E X-ray, I X-ray. 204,206,208Pb deduced isotope shifts.
ATOMIC PHYSICS, Mesic-Atoms 204,206,208Pb; measured muonic X-rays; deduced transition energy differences.
Phys.Rev.Lett. 52, 247 (1984)
C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, J.S.McCarthy, D.Goutte, J.M.Cavedon, B.Frois, M.Huet, P.Leconte, Phan Xuan Ho, S.Platchkov, I.Sick
Effective Charge of Neutron Quasiparticle Pairs in 206Pb and 204Pb
NUCLEAR REACTIONS 204,206,208Pb(e, e'), E=52-502 MeV; measured σ. 204,206,208Pb levels deduced transition charge densities, B(λ).
doi: 10.1103/PhysRevLett.52.247
Nucl.Phys. A451, 471 (1986)
M.Anselment, W.Faubel, S.Goring, A.Hanser, G.Meisel, H.Rebel, G.Schatz
The Odd-Even Staggering of the Nuclear Charge Radii of Pb Isotopes
RADIOACTIVITY 196,197,197m,211,214Pb; measured hfs, isotope shift; deduced hyperfine constants. 196,197,197m,198,199,200,201,202,202m,203,204,205,206,207,208,209,210,211,212,214Pb deduced nuclear charge radii, nuclear, odd-even staggering parameters, μ, quadrupole moment. Laser spectroscopic techniques, other data input.
doi: 10.1016/0375-9474(86)90071-0
Hyperfine Interactions 30, 265 (1986)
J.Billowes
Nuclear Deorientation of W, Os and Pt Recoiling in Vacuum at 0.02c
NUCLEAR REACTIONS 182,184,186W, 192,190Os, 194,196Pt(32S, 32S'), E=100 MeV; measured γ yields, γγ-coin following Coulomb excitation, γ(particle)(θ) vs t, recoil distance; deduced nuclear deorientation parameters. 204,206Pb levels deduced g factor upper limit. Other data input, recoil in vacuum.
J.Phys.(London) B19, 1881 (1986)
S.Bouazza, Y.Guern, J.Bauche
Isotope Shift and Hyperfine Structure in Low-Lying Levels of Pb II
NUCLEAR MOMENTS 206,208Pb; measured hfs, isotope shifts; deduced hyperfine components. Fabry-Perot interferometer.
doi: 10.1088/0022-3700/19/13/002
Z.Phys. A328, 253 (1987)
U.Dinger, J.Eberz, G.Huber, R.Menges, S.Schroder, R.Kirchner, O.Klepper, T.Kuhl, D.Marx, G.D.Sprouse
Nuclear Moments and Change in the Charge-Radii of Neutron Deficient Lead Isotopes
RADIOACTIVITY 192,194,195,196Pb [from W(16O, xn)]; measured hfs, isotope shifts; deduced hyperfine constants. 195Pb deduced μ, spectroscopic quadrupole moments, rms charge radius. 192,194,196Pb deduced rms charge radii. Collinear laser spectroscopy.
NUCLEAR MOMENTS Pb; measured isotope shifts, hfs. 204,206,207,208Pb deduced rms charge radii. Collinear laser spectroscopy.
Phys.Rev. C36, 555 (1987)
M.Schanz, A.Richter, E.Lipparini
Mixing of Isoscalar and Isovector Magnetic Dipole Excitation Modes in 206Pb and 208Pb: Case of electron scattering form factors
NUCLEAR REACTIONS 206,208Pb(e, e'), E=70 MeV; measured σ(E(e'), θ). 206,208Pb deduced levels, J, π, B(M1), form factors, transition density. Enriched 206Pb target. Isoscalar-isovector mixing model.
Phys.Scr. 38, 664 (1988)
P.Buch, J.Nellessen, W.Ertmer
Laser Spectroscopic Studies of 6pns, 6pnd, and 6png Rydberg States of Lead
ATOMIC PHYSICS Pb; measured Rydberg transitions, hfs, isotope shift.
NUCLEAR MOMENTS 206,204,208,207Pb; measured hfs, isotope shift; deduced 207Pb hyperfine parameter.
Nucl.Phys. A490, 348 (1988)
F.Garcias, M.Casas, J.Martorell
A Comparison between Different Models for the Isotopic Differences in Lead
NUCLEAR STRUCTURE 204,206,207,208Pb; calculated isotopic shifts, charge differences. Density-dependent Hartree-Fock approach.
doi: 10.1016/0375-9474(88)90510-6
Program and Thesis, Proc.39th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Tashkent, p.125 (1989)
S.A.Berendakov, A.M.Demidov, I.V.Mikhailov
Multipole Mixing of 206Pb γ-Transitions from (n, n'γ) Reaction
NUCLEAR REACTIONS 206Pb(n, n'γ), E=fast; measured Eγ, Iγ, γ(t), linear polarization. 206Pb transitions deduced δ.
Hyperfine Interactions 59, 77 (1990)
U.Dinger, S.Dutta, J.Eberz, G.Huber, R.Kirchner, O.Klepper, T.Kuhl, D.Marx, R.Menges, S.Schroder, G.Sprouse
Laser Spectroscopy of Radioactive Lead and Thallium Isotopes
NUCLEAR MOMENTS 204,206,207,208Pb; measured hfs, isotope shifts; deduced μ, electric quadrupole moments, rms charge radii. Collinear fast beam laser spectroscopy.
RADIOACTIVITY 190,191,192,193,194,195,196,197Pb, 188,190,191,192,194,196Tl; measured hfs, isotope shifts; deduced μ, electric quadrupole moments, rms charge radii. Collinear fast beam laser spectroscopy.
Z.Phys. A335, 475 (1990)
W.H.Trzaska, J.Kantele, R.Julin, J.Kumpulainen, P.Van Duppen, M.Huyse, J.Wauters
Comparison of Experimental and Calculated K/L Ratios of E0 Transitions in Some Heavy Nuclei
RADIOACTIVITY 154Gd, 192,194,196,198,202,204,206,208Pb, 208Po; compiled measured, calculated I(ce) ratios; deduced no major differences.
Phys.Rev. C44, 128 (1991)
D.J.Horen, R.L.Auble, J.R.Beene, F.E.Bertrand, M.L.Halbert, G.R.Satchler, M.Thoennessen, R.L.Varner, V.R.Brown, P.L.Anthony, V.A.Madsen
Isospin Character of Transitions to Bound States in 204,206,208Pb using Inelastic Scattering of 17O Ions
NUCLEAR REACTIONS 204,206,208Pb(17O, 17O'), E=375 MeV; measured σ(θ); deduced optical model parameters. 204,206,208Pb levels deduced B(λ), neutron, proton matrix element ratio. Enriched targets. DWBA analysis.
NUCLEAR STRUCTURE 204,206,208Pb; calculated B(λ), neutron, proton matrix element ratio. RPA method.
Phys.Rev. A44, R1439 (1991)
J.M.Reeves, E.N.Fortson
Isotope Shifts at 1.28 μm in Pb
NUCLEAR MOMENTS 206,207,208Pb; measured isotope shifts. 207Pb deduced hfs constants. Parity nonconservation in Pb relevance.
doi: 10.1103/PhysRevA.44.R1439
Phys.Rev. C46, 499 (1992)
D.J.Horen, C.L.Morris, S.J.Seestrom, F.W.Hersman, J.R.Calarco, M.Holtrop, M.Leuschner, M.Rawool-Sullivan, R.W.Garnett, S.J.Greene, M.A.Plum, J.D.Zumbro
Isospin Character of the Transition to the 0.803-MeV State in 206Pb from π± Scattering at 180 MeV
NUCLEAR REACTIONS 206Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured missing mass spectra, σ(θ). 206Pb deduced neutron, proton matrix elements ratio for quadrupole, octupole transitions. Deformed optical model, DWIA analyses.
Phys.Rev. C48, 1431 (1993)
R.Alarcon, S.Choi, R.M.Laszewski, D.S.Dale
Isoscalar M1 Strength in Lead
NUCLEAR REACTIONS 206Pb(γ, γ), E=5.5-7 MeV; measured σ(Eγ). 206Pb deduced B(M1). Polarized photons.
Nucl.Phys. A554, 45 (1993)
J.Blomqvist, R.Liotta, L.O.Norlin, U.Rosengard, B.Fant, T.Weckstrom, H.C.Jain, T.Lonnroth
High-Spin States in 206Pb
NUCLEAR REACTIONS 204Hg(α, 2n), E=35 MeV; measured Eγ, Iγ, γ(t), γ(θ), γγ-coin. 206Pb deduced levels, decay features, J, π. Metallic 204Hg target, Ge detectors. Shell-model calculations.
doi: 10.1016/0375-9474(93)90356-3
Nucl.Phys. A580, 43 (1994)
A.R.Poletti, G.D.Dracoulis, A.P.Byrne, A.E.Stuchbery, B.Fabricius, T.Kibedi, P.M.Davidson
Structure of High-Spin Yrast States in 205Pb and 206Pb
NUCLEAR REACTIONS 204Hg(9Be, 4nα), (9Be, 3nα), E=55-65 MeV; measured γγ(t), Eγ, Iγ(θ), Iγ(E, t), linear polarization. 205,206Pb deduced high-spin levels J, π, T1/2. Enriched target, pulsed beam, Ge hyperpure Compton suppressed detectors, Ge hyperpure detectors in linear polarimeter.
NUCLEAR STRUCTURE 205,206Pb; calculated levels. Semi-empirical shell model.
doi: 10.1016/0375-9474(94)90814-1
Nucl.Instrum.Methods Phys.Res. B99, 513 (1995)
B.Antonot, S.Cluzeau, P.Le Tourneur, F.Bergamo
Application of a Sealed Tube Neutron Generator to the Characterization of Very Short Half-Life Isomeric States
NUCLEAR REACTIONS 115In, 182W, 207,208,206Pb, 209Bi(n, 2n), 181Ta, 206,207Pb(n, n'γ), E=14 MeV; measured residuals production σ. SODERN sealed tube neutron generator, hyperpure Ge detector, activation technique.
RADIOACTIVITY 114mIn, 181mW, 181mTa, 205m,206m,207mPb, 208mBi [from 115In, 180W, 206,207,208Pb(n, 2n), 181Ta, 206,207Pb(n, n'γ), E=14 MeV]; measured T1/2. SODERN sealed tube neutron generator, hyperpure Ge detector, activation technique.
doi: 10.1016/0168-583X(94)00661-X
Phys.Rev. C53, 2732 (1996); Erratum Phys.Rev. C54, 2786 (1996)
S.Raman, J.B.McGrory, E.T.Jurney, J.W.Starner
Gamma-Ray Transitions in 206Pb Studied in the 205Pb(n, γ) Reaction
NUCLEAR REACTIONS 205Pb(n, γ), E=thermal; measured Eγ, Iγ; deduced capture σ(E). 206Pb deduced levels, neutron binding energy, γ-branching ratio. Model comparison.
Nuovo Cim. 111A, 691 (1998)
H.J.Wollersheim, and the EBGSI-Collaboration
Octupole Vibrational States in the Lead Region
NUCLEAR REACTIONS 206,207,208Pb, 209Bi(208Pb, 208Pb'), E=5 MeV/nucleon; measured Eγ, Iγ following Coulomb excitation. 206,207,208Pb, 209Bi deduced one-phonon octupole-vibrational states, B(E3). 206Pb deduced levels excitation probabilities. 208Pb deduced no two-phonon octupole vibration.
Phys.Rev. C57, R2794 (1998)
A.H.Wuosmaa, C.M.Conner, I.Ahmad, B.B.Back, R.R.Betts, R.W.Dunford, S.M.Fischer, R.Ganz, J.P.Greene, N.I.Kaloskamis, L.Lamm, C.J.Lister, V.Nanal, D.E.Roa, J.P.Schiffer
Positron-Electron Angular Correlations in Internal Pair Conversion
RADIOACTIVITY 90Y(β-); 206,207Bi(EC); measured e+e--coin, sum energy spectra, opening angle correlations from internal pair conversion in daughter nuclei. 90Zr, 206,207Pb deduced transitions internal pair conversion coefficients.
doi: 10.1103/PhysRevC.57.R2794
J.Radioanal.Nucl.Chem. 239, 123 (1999)
T.Ohtsuki, J.Kasagi, N.Kasajima, H.Yamazaki, H.Yuki, M.Yukishima
Bremmsstrahlung Emission in α-Decay of 210Po
RADIOACTIVITY 210Po(α); measured Eα, Eγ, αγ-coin; deduced bremsstrahlung yields, emission mechanism.
Eur.Phys.J. D 36, 249 (2005)
T.J.Wasowicz, R.Drozdowski, J.Kwela
Hyperfine structure and isotope shift study in a singly ionized lead
NUCLEAR MOMENTS 204,206,207,208Pb; measured hfs, isotope shifts.
doi: 10.1140/epjd/s2005-00215-5
Phys.Rev. C 75, 045501 (2007)
D.F.Measday, T.J.Stocki, H.Tam
γ rays from muon capture in I, Au, and Bi
NUCLEAR REACTIONS 127I(μ-, ν), (μ-, nν), (μ-, 2nν), (μ-, 3nν), (μ-, 4nν), (μ-, 5nν), (μ-, 6nν), E at rest; 197Au(μ-, nν), (μ-, 3nν), E at rest; 209Bi(μ-, nν), (μ-, 2nν), (μ-, 3nν), (μ-, 4nν), (μ-, 5nν), E at rest; measured Eγ, Iγ, X-ray spectra.
doi: 10.1103/PhysRevC.75.045501
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
Eur.Phys.J. A 49, 50 (2013)
J.W.Beeman, F.Bellini, L.Cardani, N.Casali, S.Di Domizio, E.Fiorini, L.Gironi, S.S.Nagorny, S.Nisi, F.Orio, L.Pattavina, G.Pessina, G.Piperno, S.Pirro, E.Previtali, C.Rusconi, C.Tomei, M.Vignati
New experimental limits on the α decays of lead isotopes
RADIOACTIVITY 204,206,207,208Pb(α); measured energy, heat, light yield using PbWO4 as cryogenic particle detector (bolometer); deduced T1/2 limits. Compared with published theoretical calculations.
doi: 10.1140/epja/i2013-13050-7
J.Phys.(London) G45, 035105 (2018)
N.Lalovic, for the AGATA Collaboration
Study of isomeric states in 198, 200, 202, 206Pb and 206Hg populated in fragmentation reactions
NUCLEAR REACTIONS 9Be(208Pb, X)198Pb/200Pb/202Pb/206Pb, 206Hg, E=1 GeV/nucleon; measured reaction products, Eγ, Iγ; deduced isomeric state T1/2, level energies, J, π. Comparison with available data.
Phys.Lett. B 797, 134797 (2019)
D.Ralet, E.Clement, G.Georgiev, A.E.Stuchbery, M.Rejmund, P.Van Isacker, G.de France, A.Lemasson, J.Ljungvall, C.Michelagnoli, A.Navin, D.L.Balabanski, L.Atanasova, A.Blazhev, G.Bocchi, R.Carroll, J.Dudouet, E.Dupont, B.Fornal, S.Franchoo, C.Fransen, C.Muller-Gatermann, A.Goasduff, A.Gadea, P.R.John, D.Kocheva, T.Konstantinopoulos, A.Korichi, A.Kusoglu, S.M.Lenzi, S.Leoni, R.Lozeva, A.Maj, R.Perez, N.Pietralla, C.Shand, O.Stezowski, D.Wilmsen, D.Yordanov, D.Barrientos, P.Bednarczyk, B.Birkenbach, A.J.Boston, H.C.Boston, I.Burrows, B.Cederwall, M.Ciemala, J.Collado, F.Crespi, D.Cullen, H.J.Eberth, J.Goupil, L.Harkness, H.Hess, A.Jungclaus, W.Korten, M.Labiche, R.Menegazzo, D.Mengoni, B.Million, J.Nyberg, Zs.Podolyak, A.Pullia, B.Quintana Arnes, F.Recchia, P.Reiter, F.Saillant, M.D.Salsac, E.Sanchis, C.Theisen, J.J.Valiente Dobon, O.Wieland
Evidence of octupole-phonons at high spin in 207Pb
NUCLEAR REACTIONS 100Mo(208Pb, 207Pb), E=6.25 MeV/nucleon; measured reaction products, Eγ, Iγ. 207Pb; deduced γ-ray energies, T1/2, B(E3) for 19/2- state. Recoil Distance Doppler-Shift (RDDS) method.
doi: 10.1016/j.physletb.2019.134797
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.
INDC(NDS)-0833 (2021)
N.J.Stone
Table of Nuclear Electric Quadrupole Moments
COMPILATION Z=1-102; compiled experimental measurements of static electric quadrupole moments of ground states and excited states of atomic nuclei throughout the periodic table.
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.