References quoted in the ENSDF dataset: 196 REFERENCES
446 references found.
Clicking on a keynumber will list datasets that reference the given article.
Naturwissenschaften 23, 372 (1935)
B.Fuchs, H.Kopfermann
Uber die Isotopen des Platins
Phys.Rev. 83, 390 (1951)
D.G.Karraker, A.Ghiorso, D.H.Templeton
Alpha-Decay Energies of Polonium Isotopes
RADIOACTIVITY 200,201Po(α), (EC), 206,207,208,209Po(α), 226Ra(α) [from 209Bi(p, X), E=100 MeV]; measured decay products, Eα, Iα; deduced α-particles energies, T1/2. Comparison with available data. Berkeley 184-inch and 60-inch cyclotrons.
Phys.Rev. 87, 374 (1952)
P.Stahelin
Lowest Excitation Level of Hg196
Phys.Rev. 89, 665 (1953)
R.M.Steffen
The Angular Momenta of the Excited States of Pt196
Phil.Mag. 45, 31 (1954)
F.D.S.Butement, A.J.Poe
Radioactivity of Neutron Excess Iridium Isotopes
Phil.Mag. 45, 1090 (1954)
F.D.S.Butement, A.J.Poe
A 7-Second Iridium Isomer
Phys.Rev. 100, 943 (1955)
E.L.Church, J.Weneser
Electric-Monopole Transitions in Atomic Nuclei
Phys.Rev. 99, 112 (1955)
P.H.Stelson, F.K.McGowan
Gamma-Ray Yields from Coulomb Excitation
Phys.Rev. 103, 1035 (1956)
E.L.Church, J.Weneser
Electric-Monopole Transitions in Atomic Nuclei
Phys.Rev. 101, 1031 (1956)
M.T.Thieme, E.Bleuler
Conversion of the Pt196 Gamma Rays
Phys.Rev. 108, 812 (1957)
D.E.Alburger
Radioactive Decays of Au194, Au196, and Au198
Arkiv Fysik 11, 297 (1957)
G.Andersson, E.Arbman, B.Jung
Lead and Thallium Isotopes in the Mass Range 195-199
Phil.Mag. 3, 105 (1958); Priv.Comm.
G.Andersson, J.O.Burgman, B.Jung
The Half-Life of Thallium 196 and the Multipolarity of the 426 keV Transition in Mercury 196
Phys.Rev. 109, 1299 (1958)
E.L.Church, M.E.Rose, J.Weneser
Electric-Monopole Directional-Correlation Experiments
Phys.Rev. 110, 1119 (1958)
T.R.Gerholm, B.G.Pettersson
Evidence for the Presence of E0 in Direct Competition with M1 and E2
Phys.Rev. 114, 822 (1959)
D.G.Gardner, W.W.Meinke
Search for the Isotope Ir196
Physica 25, 703 (1959)
R.van Lieshout, R.K.Girgis, R.A.Ricci, A.H.Wapstra, C.Ythier
Characterization of the 10 Hour 196Au Isomer
doi: 10.1016/S0031-8914(59)97325-2
Nuovo Cimento 16A, 378 (1960)
M.Ademollo, M.Bocciolini, G.Di Caporiacco, M.Mando
On the 196Au-m Isomeric State
NUCLEAR STRUCTURE 196Au; measured not abstracted; deduced nuclear properties.
Izvest.Akad.Nauk SSSR, Ser.Fiz. 24, 818 (1960); Columbia Tech.Transl. 24, 820 (1961)
M.A.Bak, K.A.Petrzhak, Chin Tya-Mei
The (n, 2n) and (γ, n) Reactions on Au197
Phys.Rev. 118, 1582 (1960)
B.L.Cohen, R.E.Price
Studies of Low-Lying Levels of Even-Even Nuclei with (d, p) and (d, t) Reactions
NUCLEAR STRUCTURE 118Sn, 113Sn, 116Sn, 114Cd, 120Sn, 124Te, 126Te, 66Zn, 196Pt, 194Pt, 112Cd, 110Cd, 76Se, 68Zn, 78Se, 92Zr, 90Zr, 94Mo, 98Mo, 96Mo; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 18, 446 (1960)
C.de Vries, J.H.Dijkstra
Precision Measurements of Energies of Gamma-Rays Following the Decay of Some Gold Isotopes
NUCLEAR STRUCTURE 198Au, 199Au, 196Au, 194Au; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90416-8
Nuclear Phys. 18, 454 (1960)
C.de Vries, E.J.Bleeker, N.Salomons-Grobben
Absolute and Relative Conversion Determinations of Pure E2 Transitions Occurring in 198Hg, 199Hg, 194Pt and 196Pt
NUCLEAR STRUCTURE 194Au, 196Au, 199Au, 198Au; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90417-X
Nuclear Phys. 15, 108 (1960)
B.Jung, G.Andersson
Low Mass Odd-Odd Isomers of Thallium
NUCLEAR STRUCTURE 198Tl, 196Tl, 194Tl, 194Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90288-1
Can.J.Phys. 38, 1436 (1960)
T.M.Kavanagh
Decay of Au196m
NUCLEAR STRUCTURE 196Au; measured not abstracted; deduced nuclear properties.
Ark.Fys. 18, 569 (1961)
O.Bergman
Some Features of the Decay of Au196 to Pt196
NUCLEAR STRUCTURE 196Au; measured not abstracted; deduced nuclear properties.
Phys.Rev. 122, 1274 (1961)
F.K.McGowan, P.H.Stelson
Coulomb Excitation of the Second 2+ States in W, Os, and Pt Nuclei
NUCLEAR STRUCTURE 190Os, 192Os, 194Pt, 188Os, 196Pt, 184W, 186W; measured not abstracted; deduced nuclear properties.
Ark.Fys. 19, 441 (1961)
J.Svedberg, B.Jung
The Internal Conversion Electron Spectrum of Pb196
NUCLEAR STRUCTURE 196Pb; measured not abstracted; deduced nuclear properties.
Phys.Rev. 127, 217 (1962)
N.A.Bonner, W.Goishi, W.H.Hutchin, G.M.Iddings, H.A.Tewes
Half-Lives of Tm167, Tm168, Tm170, Lu171, Lu172, Lu173, Lu174, Lu174m, Au195, Au196, and Au196m
NUCLEAR STRUCTURE 170,167,168Tm, 174m,174,173,172,171Lu, 195Au, 196m,196Au; measured not abstracted; deduced nuclear properties.
Phys.Rev. 127, 572 (1962)
Y.W.Chan, W.B.Ewbank, W.Nierenberg, H.A.Shugart
Nuclear Spin of 9.5-hr Au196m
NUCLEAR STRUCTURE 196Au; measured not abstracted; deduced nuclear properties.
Ark.Fys. 21, 241 (1962)
T.R.Gerholm, M.S.El-Nesr, E.Bashandy, B.-G.Pettersson
A Study of the E0 Admixture and M1 Penetration Matrix Element of the 333 keV 2+ → 2+ Transition in Pt196
NUCLEAR STRUCTURE 196Au; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 38, 121 (1962)
J.F.W.Jansen, S.Hultberg, P.F.A.Goudsmit, A.H.Wapstra
E2 Internal Conversion Coefficients of 2+ → 0+ Transitions from the Decay of 170Tm, 196Au, and 200Tl
NUCLEAR STRUCTURE 200Tl, 196Au, 170Tm; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)91022-2
Nucl.Phys. 31, 584 (1962)
E.W.A.Lingeman, K.E.G.Lobner, G.J.Nijgh, A.H.Wapstra
The Negaton Transition in 196Au
NUCLEAR STRUCTURE 196Au; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90778-2
Nucl.Phys. 31, 575 (1962)
A.H.Wapstra, J.F.W.Jansen, P.F.A.Goudsmit, J.Oberski
The Decay of 196Au
NUCLEAR STRUCTURE 196Au; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90777-0
Physica 29, 1013 (1963)
T.J.De Boer, E.W.Ten Napel, J.Blok
Half-Lifes of the First Excited States of Ru102, Xe126, Hg196, Dy160, Er164, Er166, and W180
NUCLEAR STRUCTURE 180Ta, 164Ho, 166Ho, 160Tb, 126I, 196Au, 102Rh; measured not abstracted; deduced nuclear properties.
Z.Phys. 173, 402 (1963)
A.Hofmann
γ-Strahlung bei Inelastischer Streuung von 14 MeV Neutronen an Calcium, Sauerstoff und Kohlenstoff
NUCLEAR STRUCTURE 12C, 16O, 40Ca; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 25, 1303 (1963)
R.W.Hoff, F.Asaro, I.Perlman
Alpha Decay of Neutron-Deficient Astatine Isotopes
NUCLEAR STRUCTURE 201At, 200At, 203At, 202At, 204At, 207At, 206At, 205At; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(63)80400-5
Nucl.Phys. 41, 130 (1963)
H.Ikegami, K.Sugiyama, T.Yamazaki, M.Sakai
Structure of Platinum Nuclei. (I) New Decay Scheme of Au196
NUCLEAR STRUCTURE 196Au, 192Ir; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90486-3
Arkiv Fysik 23, 57 (1963)
M.Karras, G.Andersson, M.Nurmia
Search for Alpha Activity in Neutron Deficient Isotopes of Pb, Tl, Hg, Pt, and Te
NUCLEAR STRUCTURE 119Te, 117Te, 116Te, 118Te, 198Bi, 198Tl, 198Pb, 197Pb, 196Bi, 196Pb, 194Tl, 195Tl, 193Hg, 193Au, 192Hg, 193Tl, 192Au, 190Hg, 191Hg, 191Au, 189Hg, 190Au, 189Au; measured not abstracted; deduced nuclear properties.
AD-402668 (1963)
R.A.Karam, T.F.Parkinson, W.H.Ellis
The Nuclear Properties of Rhenium
NUCLEAR STRUCTURE 184Re, 185Re, 186Re, 187Re, 188Re, 196Au; measured not abstracted; deduced nuclear properties.
Can.J.Chem. 41, 2634 (1963)
R.S.Tilbury, L.Yaffe
Nuclear Isomers Hg197m,197g, Hg195m,195g, and Au196m,196g Formed by Bombardment Of Gold with Protons of Energies from 8 to 60 MeV
NUCLEAR STRUCTURE 195Hg, 197Hg, 196Au; measured not abstracted; deduced nuclear properties.
doi: 10.1139/v63-384
Phys.Rev. 138, B514 (1965)
W.N.Bishop
Decay of Ir196
NUCLEAR STRUCTURE 196Ir; measured not abstracted; deduced nuclear properties.
J.Phys.Soc.Jpn. 20, 2118 (1965)
Y.Ishizaki, K.Kikuchi, K.Matsuda, T.Mikumo, Y.Nakajima, I.Nonaka, Y.Saji, A.Suzuki, H.Yamaguchi, R.Eisberg
An Experimental Survey of Nuclear Reactions Induced by 57 MeV Protons, Part II, (p, d) Reactions
NUCLEAR STRUCTURE 12C, 11C, 208Bi, 196Au, 57Ni, 26Al; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 64, 65 (1965)
P.Mukherjee
Nuclear Structure Studies in the Pt Region with (d, p), (d, t) and (d, d') Reactions
NUCLEAR REACTIONS 194,196,198Pt(d, p), Ed=15 MeV; measured σ(Ep, θ). 195Pt(d, p), Ed=15 MeV; measured σ(Ep). 194,195,196,198Pt(d, d'), Ed=15 MeV; measured σ(Ed'). 194,195,196,198Pt(d, t), Ed=15 MeV; measured σ(Et). 193,194,195,196,197,198,199Pt deduced levels, J, π. Enriched targets.
doi: 10.1016/0029-5582(65)90842-4
Nucl.Phys. 65, 466 (1965)
B.-G.Pettersson, L.Holmberg, T.R.Gerholm
Confirmation of the Presence of E0 in Direct Competition with M1 and E2
RADIOACTIVITY 196Au[from Pt(d, xn)]; measured γ ce(θ), γγ(θ). 196Pt deduced matrix elements, E0/E2. Natural target.
doi: 10.1016/0029-5582(65)90010-6
Nucl.Phys. 74, 81 (1965)
M.Sakai, T.Yamazaki, H.Ejiri
Measurement of Conversion Electrons from (p, 2n) Reactions on the Vibrational Nuclei
NUCLEAR REACTIONS 103Rh, 121,123Sb, 127I, 133Cs, 185,187Re, 191,193Ir, 197Au(p, 2nγ), E = 12, 13, 14 MeV. 114Cd(p, p'γ), E = 14 MeV; measured σ(E;E(ce)), ICC. 102Pd, 120,122Te, 126Xe, 132Ba, 184,186Os, 190,192Pt, 196Hg, 114Cd deduced levels, J, π. Natural targets.
doi: 10.1016/0029-5582(65)90248-8
Phys.Letters 17, 273 (1965)
E.Tielsch
Evidence for Isomeric States of 199Po and 201Po
NUCLEAR STRUCTURE 199Po, 202Po, 201Po, 200Po; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90528-7
Nucl.Phys. 88, 474 (1966)
L.Grodzins, R.R.Borchers, G.B.Hagemann
Coulomb Excitation in the Platinum Isotopes
NUCLEAR REACTIONS 190,192,194,195,196,198Pt(16O, 16O'γ), E = 36 MeV; measured Iγ. 190,192,194,196,198Pt deduced B(E2).
doi: 10.1016/0029-5582(66)90604-3
Program and Theses, Proc.16th All-Union Conf.Nucl.Spectroscopy and Struct.Of At.Nuclei, Moscow, p.41 (1966)
K.Y.Gromov, F.N.Mukhtasimov, G.Y.Umarov
New Data on Decay of 155Ho and 156Ho
RADIOACTIVITY 155,156Ho; measured Eγ, I(ce); deduced γ-multipolarity. 155Dy deduced levels, J, π.
Z.Phys. 195, 343 (1966)
H.Vonach, H.Munzer, P.Hille
Untersuchung der Bisher Ir198 Zugeschriebenen 50 sec-Aktivitat und Neuzuordnung Zum Zerfall von Ir196
NUCLEAR STRUCTURE 196Ir, 198Ir; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A94, 235 (1967)
J.F.W.Jansen, H.Pauw
Levels in 196Pt from the Decay of 6.2 d 196Au
RADIOACTIVITY 196Au [from 196Pt(d, 2n)]; 196Ir [from 198Pt(d, α)]; measured Eγ, Iγ, T1/2. 196Hg, 196Pt deduced levels. Enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(67)90821-4
Thesis, Univ.Amsterdam (1967)
J.F.W.Jansen
Internal Conversion Studies of E2 Transitions and the Level Structure of 196Pt
RADIOACTIVITY 196Au, 200Tl, 170Tm, 160Tb, 152,154Eu; measured ICC. 196Pt, 200Hg, 170Yb, 160Dy, 152Sm, 154Gd transitions deduced γ-multipolarity. 196Au; measured Eγ, Iγ, γγ-coin, deduced log ft. 196Ir; measured Eγ, Iγ, γγ-coin, γγ(t), Eβ, T1/2, γγ(θ). Deduced Q, log ft. 195m,195Pt measured Eγ, Iγ, Eβ, T1/2. Deduced log ft. 196Pt deduced levels, J, π, T1/2.
Phys.Rev. 161, 1196 (1967); R.R.Borchers - Priv.Comm. (May 1972)
R.Kalish, L.Grodzins, R.R.Borchers, J.D.Bronson, B.Herskind
Magnetic Moments of the First Excited 2+ States in the Even Pt Isotopes
NUCLEAR STRUCTURE 194Pt, 196Pt, 198Pt; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A99, 131 (1967)
Y.Le Beyec, M.Lefort
Reactions entre Protons de 30 a 155 MeV et Noyaux Lourds Complexes
RADIOACTIVITY 197,198,199,200,201,202,203,204Po; measured Eα, Iα. 202,204Bi; measured Iγ. 206Po; measured Iα. 209Bi(p, xn), (p, pxn) E=30-155 MeV; measured σ(E); deduced direct interaction model, evaporation parameters.
doi: 10.1016/0375-9474(67)90213-8
Arkiv Fysik 36, 183 (1967)
Y.Le Beyec, M.Lefort
Alpha Emission from Light Polonium Isotopes
NUCLEAR STRUCTURE 202Po, 201Po, 200Po, 199Po, 198Po, 197Po, 203Po, 204Po; measured not abstracted; deduced nuclear properties.
J.Phys.Soc.Japan 23, 919(1967)
M.Mishina, E.Tanaka, K.Kageyama, N.Mutsuro, A.Asami, Y.Kawarasaki, Y.Nakajima
Time-of-Flight Measurement of Photoneutrons from O16, Ca40, and P31
NUCLEAR REACTIONS 16O, 40Ca, 31P(γ, n), E < 20 MeV; measured σ(E;En).
Compt.Rend. 264B, 330 (1967)
E.Monnand, J.-A.Pinston, R.Henck
Decay of the 52-sec Isomer of 196Ir
NUCLEAR STRUCTURE 196Ir; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A101, 129 (1967)
A.Siivola
193-200Po Isotopes Produced Through Heavy Ion Bombardments
RADIOACTIVITY 193,194,195,196,197,198,199,200Po[from 185,187Re(19F, xn), 194Pt(12C, xn)]; measured Eα, T1/2. Enriched targets.
doi: 10.1016/0375-9474(67)90292-8
Nucl.Phys. A100, 425 (1967)
E.Tielsch-Cassel
Alpha-Decay Studies of Polonium Isotopes in the Mass Range 199 to 208
RADIOACTIVITY 199,208Po[from 209Bi(p, xn)]; measured Eα, T1/2.
doi: 10.1016/0375-9474(67)90419-8
Nucl.Phys. A97, 405 (1967)
W.Treytl, K.Valli
Alpha Decay of Neutron Deficient Astatine Isotopes
RADIOACTIVITY 196,197,198,199,200,201,202At, 190,191,192,194,195,196Bi; measured T1/2, Eα. 203,204At, 193,194,195,196,197,198,199,200,201,202Po; measured Eα. 185,187Re(20Ne, xn), E = 100-200 MeV; measured σ(E) for X = 4-11. Enriched targets.
doi: 10.1016/0375-9474(67)90495-2
Phys.Rev. 159, 1013 (1967)
K.Valli, M.J.Nurmia, E.K.Hyde
Alpha-Decay Properties of Neutron-Deficient Isotopes of Emanation
RADIOACTIVITY 201,202,203,204,205,206,207Rn, 203mRn; measured T1/2, Eα. 199mPo; measured Eα.
Yadern.Fiz. 6, 462 (1967); Sov.J.Nucl.Phys. 6, 337 (1968)
I.S.Vashakidze
A Calculation of Excited States of A = 18 Nuclei Using a Real Nucleon-Nucleon Interaction Potential
Proc.Intern.Conf.Atomic Masses, 3rd, Winnipeg, Canada, R.C.Barber, Ed., Univ.Manitoba Press, p.296 (1967)
K.Valli
Compilation of Experimental Eα Values in the Region Above Z = 81 and below N = 128
Nucl.Phys. A93, 527 (1967)
A.H.Wapstra, P.F.A.Goudsmit, J.F.W.Jansen, J.Konijn, K.E.G.Lobner, G.J.Nijgh, S.A.De Wit
The Isomer with Spin 12 in 196Au
RADIOACTIVITY 196mAu [from 196Pt(d, 2n), 197Au(n, 2n)]; measured Eγ, ce, Iγ, I(ce), γγ(θ, t), ceγ(t). 196Au deduced levels, T1/2, J, π, γ-multipolarities. Enriched 196Pt target.
doi: 10.1016/0375-9474(67)90305-3
Kgl.Danske Videnskab.Selskab., Mat.-Fys.Skrifter 3, No.5 (1967)
N.Zeldes, A.Grill, A.Simievic
Shell-Model Semi-Empirical Nuclear Masses (II)
Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.199 (1968)
R.Beraud, I.Berkes, J.Daniere, M.Levy, G.Marest, R.Rougny, H.Bernas, D.Spanjaard
The g-Factor of the First Excited State of 196Pt
RADIOACTIVITY 196Au; measured γγ(θ, H). 196Pt level deduced g.
Phys.Rev.Letters 20, 1298 (1968)
J.E.Glenn, J.X.Saladin
Determination of the Static Quadrupole Moments of the First 2+ States of 194Pt, 196Pt, and 198Pt
NUCLEAR STRUCTURE 194Pt, 196Pt, 198Pt; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.20.1298
Yadern.Fiz. 7, 937 (1968); Sov.J.Nucl.Phys. 7, 563 (1968)
L.V.Groshev, A.M.Demidov, A.S.Rakhimov
γ-Ray Spectrum from Capture of Thermal Neutrons in Pt
NUCLEAR REACTIONS 195Pt(n, γ), E=thermal; measured Eγ, Iγ. 196Pt deduced levels. Natural target.
Proc.Intern.Conf.Nucl.Struct., Tokyo (1967), J.Sanada, Ed., Suppl.J.Phys.Soc.Japan 24, 167 (1968)
H.Ikegami, T.Hirose, M.Sakai, T.Yamazaki, K.Sugiyama
E0, M1 and (22+ → 21+) Transitions in 188,190Os, 192,194,196Pt and 198Hg Nuclei (Values for 196Pt Read from Graph by Evaluator)
Nucl.Phys. A115, 321 (1968)
J.F.W.Jansen, H.Pauw, C.J.Toeset
The Radio-Active Decay of 52 s 196gIr and 1.40 h 196mIr
RADIOACTIVITY 196Ir [from 196Pt(n, p), 198Pt(d, α)]; measured T1/2, Eβ, Eγ, Iγ, I(ce), βγ-, γγ-, γce-coin, βγ-, γγ-delay, γγ(θ); deduced Iβ. 196Pt deduced levels, J, π, ICC, γ-multipolarities. 195Ir [from 198Pt(d, αn)]; measured T1/2, Eγ, Iγ. Enriched targets; Ge(Li), Si(Li) detectors.
doi: 10.1016/0375-9474(68)90007-9
Can.J.Phys. 46, 75 (1968)
J.Murray, T.A.McMath, J.A.Cameron
The Nuclear g Factor of the 356-keV Level in 196Pt and the Internal Field on Mercury in Iron
NUCLEAR STRUCTURE 196Pt, 196Au, 198Au; measured not abstracted; deduced nuclear properties.
Phys.Rev. 174, 1441 (1968)
R.F.Petry, R.A.Naumann, J.S.Evans
Levels in Even-Even Hg192, Hg194, Hg196, and Hg198
RADIOACTIVITY 192,194,196,198Tl; measured Eγ, Iγ, I(ce), ceγ-, γγ-coin, T1/2. 192,194,196,198Hg deduced levels, J, π, ICC, γ-multipolarity, γ-mixing.
Nucl.Phys. A121, 65 (1968)
C.Samour, H.E.Jackson, J.Julien, A.Bloch, C.Lopata, J.Morgenstern
Etude de la Capture Radiative des Neutrons de Resonance dans le Platine
RADIOACTIVITY 196Au; measured Eγ, Iγ. 196Pt deduced levels. Ge(Li) detector.
NUCLEAR REACTIONS 195Pt(n, γ), E=10-700 eV; measured σ(E; Eγ). 196Pt, deduced resonances, level-width γ. Pt(n, γ), E=th; measured Eγ, Iγ. 193,195,196,197,199Pt deduced levels, J. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(68)90497-1
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.
Phys.Rev. 188, 1905 (1969)
J.E.Glenn, R.J.Pryor, J.X.Saladin
Measurement of the Static Quadrupole Moments of the First 2+ States of 194Pt, 196Pt, and 198Pt
NUCLEAR REACTIONS 194,196,198Pt(16O, 16O'), E=42 MeV;(p, p') , E=6 MeV; measured σ(E(16O')), σ(Ep'). 194,196,198Pt levels deduced quadrupole moment, B(E2).
Nucl.Data Tables A5, 243 (1969)
L.V.Groshev, A.M.Demidov, V.I.Pelekhov, L.L.Sokolovskii, G.A.Bartholomew, A.Doveika, K.M.Eastwood, S.Monaro
Compendium of Thermal-Neutron-Capture γ-Ray Measurements. Pt.III. Z = 68 to Z = 94 (Er to Pu)
Nucl.Phys. A136, 257 (1969)
W.D.Hamilton
The Multipole Mixing Ratio of 2'+→2+ Transitions in 194Pt and 196Pt
RADIOACTIVITY 194,196Au [from Pt(p, n), 196Pt(p, n)]; measured γγ(θ), γ(linearly polarized γ)(θ). 194,196Pt levels deduced γ-ray mixing. Enriched target.
doi: 10.1016/0375-9474(69)90052-9
Nucl.Data Tables A6, 1 (1969)
R.S.Hager, E.C.Seltzer
Internal Conversion Tables. Part III: Coefficients for the Analysis of Penetration Effects in Internal Conversion and E0 Internal Conversion
Nucl.Phys. A138, 133 (1969)
K.Yagi, Y.Saji, Y.Ishizaki, T.Ishimatsu
Neutron Single-Hole States in 149Sm, 157Gd and 196Au Investigated by (p, d) Reactions
NUCLEAR REACTIONS 150Sm(p, d), 158Gd(p, d), 197Au(p, d), E = 55 MeV; measured σ(Ed, θ). 149Sm, 157Gd, 196Au deduced levels L(n), J, π, S. Enriched 150Sm, 158Gd targets.
doi: 10.1016/0375-9474(69)90387-X
Proc.Int.Conf.High Energy Phys.Nucl.Struct., 3rd, Columbia University, New York (1969), S.Devons, Ed., Plenum Press, New York, p.192 (1970)
H.Backe, R.Engfer, E.Kankeleit, W.U.Schroder, H.K.Walter, K.Wien
Measurements of Excitation Probabilities and Isomer Shifts of Nuclear Levels in μ-Atoms
NUCLEAR REACTIONS 182,184,186W, 188,190,192Os, 191,193Ir, 203,205Tl, 169Tm, 185,187Re, 194,196Pt(μ-, γ); measured excitation probability, isomer shift.
Nucl.Phys. A152, 495 (1970)
E.J.Bruton, J.A.Cameron, A.W.Gibb, D.B.Kenyon, L.Keszthelyi
Coulomb Excitation of Pt Nuclei
NUCLEAR REACTIONS 192,194,195,196,198Pt(α, α'γ), E=10, 15 MeV; 192,194,195,196,198Pt(16O, 16O'γ), E=35, 41 MeV; measured σ(Eγ, θ(γ)). 195Pt level deduced J, π. 192,194,195,196,198Pt levels deduced B(E2); recalculated T1/2, g.
doi: 10.1016/0375-9474(70)90927-9
Nucl.Phys. A151, 609 (1970)
C.L.Duke, P.G.Hansen, O.B.Nielsen, G.Rudstam
Strength-Function Phenomena in Electron-Capture Beta Decay
RADIOACTIVITY 182,183,184,185Ir, 182,183,184,185,186,187Pt, 183,184,185,186,187,188,189,190,191Au, 202,204Bi, 200,202,203,204,205,207Po, 204,205,206,207,208,209,210At, 205,206,207,208,209,210Rn; measured total-absorption γ spectra; deduced beta strength functions Sβ(E). Mass-separated samples.
doi: 10.1016/0375-9474(70)90400-8
IPCR Cyclotron Progr.Rep., Vol.4, p.67 (1970)
T.Inamura, S.Nagamiya, A.Hashizume, Y.Tendow, T.Katou
In-Beam Gamma-Ray Spectroscopy Utilizing Heavy Ions
NUCLEAR REACTIONS 185,187Re(14N, 5nγ), E=85 MeV; measured Eγ, Iγ, (14N)(γ)-delay. 194,196Pb levels deduced T1/2.
GA-10248 (1970)
V.J.Orphan, N.C.Rasmussen, T.L.Harper
Line and Continuum Gamma-Ray Yields from Thermal-Neutron Capture in 75 Elements
Acta Phys. 28, 263 (1970)
K.Raichev, L.Tron
Investigation of the Alpha Spectra of Po Isotopes
RADIOACTIVITY 200,201,202,203,204,206,208Po [from Bi(p, xn)]; measured T1/2, Eα.
Nucl.Phys. A144, 81 (1970)
V.C.Rogers, L.E.Beghian, F.M.Clikeman, F.S.Mahoney
The Level Structure of 181Ta from (n, n'γ) Experiments
NUCLEAR REACTIONS 181Ta(n, n'γ), E=0.24-1.8 MeV; measured Eγ, σ(E;En', Eγ). 181Ta deduced levels, J, π. Natural target.
doi: 10.1016/0375-9474(70)90493-8
Phys.Rev. C2, 225 (1970)
S.G.Schmelling, V.J.Ehlers, H.A.Shugart
Nuclear Magnetic Moment, Hyperfine Structure, and Hyperfine Structure Anomaly of 196Au
NUCLEAR MOMENTS 196Au; measured Δν; deduced μ, hfs anomaly. Atomic-beam magnetic resonance.
Nucl.Phys. A153, 129 (1970)
H.Ton, G.H.Dulfer, J.Brasz, R.Kroondijk, J.Blok
Lifetimes of High-Spin States in Doubly Even Pt and Hg Isotopes
RADIOACTIVITY 194,196Ir, 194,196,198Tl, 200Au; measured βγ-, γce, γγ-delay. 194,196Pt, 194,196,198,200Hg levels deduced T1/2, B(E2), B(E1).
doi: 10.1016/0375-9474(70)90761-X
Thesis, Univ.Amsterdam (1970)
H.Ton
Lifetimes of Excited States in Heavy Nuclei
RADIOACTIVITY 212Bi, 228Th, 232U, 238,240Pu, 242,244Cm, 243Am, 252Cf; measured αce-delay. 224Ra, 228Th, 234,236U, 238,240Pu, 239Np, 248Cm levels deduced T1/2, B(E2), quadrupole moment. 233U, 239Pu; measured αce-delay. 229Th, 235U levels deduced T1/2, gK, gR. 198mTl; measured ceγ-delay. 196mIr; measured ceγ-, βγ-delay. 194mIr; measured ceγ-, βγ-, γγ-delay. 200mAu; measured γγ-, ceγ-delay. 194,196Pt, 198,200Hg levels deduced T1/2, B(EL).
Phys.Lett. 37B, 181 (1971)
F.Bacon, G.Kaindl, H.-E.Mahnke, D.A.Shirley
Magnetic Moment of the 12- Isomer of 196Au
NUCLEAR MOMENTS 196mAu; measured μ.
doi: 10.1016/0370-2693(71)90045-1
Program and Theses, Proc.21st Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Moscow, Pt.1, p.132 (1971)
R.Broda, E.Golchevski, T.Kempisti, T.Morek, S.Khoinatskii, L.K.Peker, K.Petrozolin
On the Decay Schemes of 196Bi and 194Bi
RADIOACTIVITY 194,196Bi; measured T1/2, Eγ, Iγ. 194,196Pb deduced levels, J, π.
JINR-P6-5879 (1971)
S.Chojnacki, T.Morek, L.K.Peker, T.Kempisty, K.Petrozolin
Investigation of Excited Levels of 196Pb and 194Pb Nuclei
RADIOACTIVITY 194,196Bi; measured T1/2, Eγ, Iγ, γγ-coin. 194,196Bi deduced levels, J, π.
Nucl.Phys. A177, 418 (1971); Erratum Nucl.Phys. A196, 633 (1972)
H.A.Doubt, W.D.Hamilton
Monopole Admixtures in the 2'+-2+ Transitions in 192,194,196Pt Nuclei
RADIOACTIVITY 192Ir, 194,196Au[from 191Ir(n, γ), Pt(p, n)]; measured ceγ(θ). 192,194,196Pt levels deduced E0:E2 mixing ratio.
doi: 10.1016/0375-9474(71)90301-0
Nucl.Phys. A163, 277 (1971)
P.Hornshoj, K.Wilsky, P.G.Hansen, A.Lindahl, O.B.Nielsen
Alpha Decay of Neutron-Deficient Radon and Polonium Isotopes
RADIOACTIVITY 200,201,202,203,204,205,206,207,208Rn[from Th(p, spall)]; 196,197,198,199,200,201,202Po from(Rn decay); measured T1/2, Eα; deduced α-branching ratios. Mass-separated samples.
doi: 10.1016/0375-9474(71)90536-7
Phys.Rev. C3, 240 (1971)
K.S.Krane, R.M.Steffen
Experimental Test of the Kumar-Baranger Pairing-Plus-Quadrupole Force Model in the A = 190 Region Through E2-M1 Mixing Amplitudes
RADIOACTIVITY 186,188,190Ir, 194,196Au; measured γγ(θ). 186,188,190Os, 194,196Pt transitions deduced γ-mixing ratios.
Nucl.Phys. A177, 1 (1971)
W.T.Milner, F.K.McGowan, R.L.Robinson, P.H.Stelson, R.O.Sayer
Coulomb Excitation of 182,184,186W, 186,188,190,192Os and 192,194,196,198Pt with Protons, 4He and 16O Ions
NUCLEAR REACTIONS 182,184,186W(p, p'γ), E=5 MeV;182,184,186W(α, α'γ), E=14, 15 MeV; 182,184,186W(16O, 16O'γ), E=45.5 MeV; 188,190,192Os(p, p'γ), E=4.56-5.08 MeV; 186Os(α, α'γ), E=3-5 MeV; 188,190,192Os(α, α'γ), E=15 MeV; 186,188,190,192Os(16O, 16O'γ), E=42, 45.1, 45.5 MeV; 192,194,196,198Pt(p, p'γ), E=4.5 MeV; 192,194,196,198Pt(16O, 16O'γ), E=43.75 MeV; measured Iγ, Eγ, (16O)(γ)-coin, 182,184,186W, 186,188,190,192Os, 192,196,194,198Pt deduced B(E2), B(M1), J. Enriched, natural targets.
doi: 10.1016/0375-9474(71)90161-8
Thesis, Univ.Wisconsin (1971); Diss.Abstr. 32B, No.6, 3572 (1971)
R.H.Nord
Measurement of Mean Lifetimes of Coulomb-Excited Nuclear States Using the Plunger Recoil-Distance Technique
NUCLEAR REACTIONS reaction not specified; measured recoil distance. 109Ag, 112Cd, 194,195,196Pt levels deduced T1/2.
Nucl.Phys. A172, 643 (1971)
B.Rosner, J.Felsteiner, H.Lindeman, D.Zellermayer
Lifetime and Decay Modes of the 84.6 keV Isomer of 196Au
RADIOACTIVITY 196mAu[from 197Au(n, 2n)]; measured XX-delay, Iγ; deduced T1/2, γ-multipolarity, ICC.
doi: 10.1016/0375-9474(71)90051-0
Z.Phys. 247, 153 (1971)
M.Waldschmidt, P.Osterman
Das Konversionselektronenspektrum von 196Pt nach Neutroneneinfang
NUCLEAR REACTIONS 195Pt(n, γ), E=thermal; measured E(ce), I(ce). 196Pt transitions deduced ICC, γ-multipolarity.
J.Phys.(Paris) 33, 835 (1972)
G.Albouy, J.M.Lagrange, M.Pautrat, J.N.Rimbert, C.Roulet, H.Sergolle, J.Vanhorenbeeck, H.Abou-Leila
Probabilities de Transition E1 dans les Isotopes de Plomb de Masse 200, 198, 196 et 194
RADIOACTIVITY 200Bi, 198Bi; measured γγ-, Xγ-delay. 198,200Pb levels deduced T1/2.
NUCLEAR REACTIONS 188Os(12C, 4nγ), 182W(16O, 4nγ), E not given; measured γγ-delay. 194,196Pb levels deduced T1/2.
Phys.Scr. 6, 219 (1972)
G.Albouy, J.M.Lagrange, M.Pautrat, C.Roulet, H.Sergolle, J.Vanhorenbeeck
Low-Lying High Spin States in the Neutron Deficient Lead Isotopes
NUCLEAR REACTIONS 188,190,192Os(12C, 4nγ); 182,184,186W(16O, 4nγ); measured Eγ, γγ, γγ(t). 194,196,198,200Pb deduced levels, J, π, T1/2.
Contrib.European Conf.Nucl.Phys., Aix-En-Provence, Vol.2, p.106 (1972)
G.Albouy, J.M.Lagrange, M.Pautrat, N.Poffe, C.Roulet, H.Sergolle, J.Vanhorenbeeck
Isotopes du Plomb formes par Reaction (Ions Lourds, xn)
NUCLEAR REACTIONS 188,190,192Os(12C, 4nγ), 182,184,186W(16O, 4nγ), 185,187Re(14N, 5nγ); measured delays, γγ-coin. 194,196,198,200Pb deduced levels, T1/2, B(λ).
Phys.Rev. C6, 1098 (1972)
I.Berkes, R.Rougny, M.Meyer-Levy, R.Chery, J.Daniere, G.Lhersonneau, A.Troncy
Electromagnetic Properties of Even-Even Platinum Nuclei
RADIOACTIVITY 194Ir, 196Au; measured ceγ-, ceX-delay. 192,194,196Pt levels deduced T1/2, B(λ), g. Other data Input.
BMBW-FBK 72-07, p.20 (1972)
J.Glatz, K.E.G.Lobner
Messung eines 7.4-Sekunden-Isomers in 196Au
RADIOACTIVITY 196mAu; measured T1/2.
FRNC-TH-253 (1972)
M.Pautrat
Neutron-Deficient Even Pb Isotopes
RADIOACTIVITY 198,200,202Bi; 198,200,202Pb deduced levels.
NUCLEAR REACTIONS Re, W, Os(HI, xnγ); 194,196,198,200Pb deduced levels.
Nucl.Phys. A185, 403 (1972)
K.-H.Speidel, H.A.Doubt, J.B.Fechner, K.Hagemeyer, A.M.Kleinfeld
Hyperfine Interactions of Pt Nuclei Recoiling into Helium and Vacuum
NUCLEAR REACTIONS 194,195,196,198Pt(16O, 16O'γ), E=36 MeV; measured σ(θ(γ), pressure) for recoil into He, vacuum. 195,198Pt levels deduced g. Natural, enriched targets.
doi: 10.1016/0375-9474(72)90021-8
Nucl.Instrum.Methods 113, 509 (1973)
G.Albouy, J.C.David, J.M.Lagrange, M.Pautrat, C.Roulet, H.Sergolle, J.Vanhorenbeeck
Mesures de Vies Moyennes en Ligne sur Faisceau d'Ions Lourds dans la Gamme de la Microseconde
NUCLEAR REACTIONS 182,184,186W(16O, 4nγ), 188,190,192Os(12C, 4nγ); measured Eγ, γ(t). 194,196,198,200Pb deduced levels, T1/2.
Phys.Rev. C7, 1654 (1973)
F.Bacon, G.Kaindl, H.-E.Mahnke, D.A.Shirley
Nuclear Magnetic Resonance of Oriented 196Au, 198Au, and 200m-Au
RADIOACTIVITY 200mAu; measured γ(θ, H, t), NMR. 200mAu deduced J, μ. 200Hg deduced γ-mixing. 196,198Au measured NMR, deduced hyperfine field in Ni, hyperfine anomaly. 197,198Au deduced hyperfine anomaly.
Thesis, Univ.Lyon (1973)
R.Beraud
Etude Spectroscopie des Isotopes 202Hg, 200Hg, 198Hg et 196Hg
RADIOACTIVITY 202,200,198,196Tl; measured Eγ, Iγ, E(ce), I(ce), γγ(θ). Deduced ICC. 196,198,200,202Hg deduced levels, J, π, γ-mixing.
Phys.Rev. C8, 323 (1973)
F.Djadali, K.Krien, R.A.Naumann, E.H.Spejewski
Isomeric States in Light Even Pb Isotopes
NUCLEAR REACTIONS 198Hg(α, xnγ), E=40 MeV; 198,200,202Hg(3He, xnγ), E=65 MeV; measured Eγ, Iγ, αγ(t), 3Heγ(t), γγ(t). 194,196,198,200Pb levels deduced T1/2.
Nucl.Phys. A207, 379 (1973)
H.J.Evans
Gamma-Rays Following Muon Capture
NUCLEAR REACTIONS Si, Ti, Mn, Fe, Co, Ni, Y, Ag, Au(μ-, xnyp), E approx 0; measured Eγ, Iγ, 27Al, 45,46,47,48Sc, 53,54Cr, 53,55,56Mn, 56,57,58Fe, 57,59Co, 87,88Sr, 104,106,108Pd, 194,196Pt deduced transitions.
doi: 10.1016/0375-9474(73)90354-0
Program and Theses, Proc.23rd Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Tbilisi, p.115 (1973)
S.Khoinatsky, T.Kempisty, A.Korman, T.Morek, L.K.Peker, Z.Kharatym
The Search for Isomeric States in 194Bi and 196Bi
RADIOACTIVITY 194,196Bi; measured Eγ; deduced isomeric states, configurations. 194,196Pb deduced transitions.
Nucl.Phys. A201, 449 (1973)
M.Pautrat, G.Albouy, J.C.David, J.M.Lagrange, N.Poffe, C.Roulet, H.Sergolle, J.Vanhorenbeeck, H.Abou-Leila
Etude des Isotopes du Plomb de Masse 200, 198, 196 et 194 Formes par Reaction (Ions Lourds, xn)
NUCLEAR REACTIONS Os(12C, 4n), W(16O, 4n), Re(14N, 5n), E=60-100 MeV;measured Eγ, Iγ, σ(E, Eγ), Iγ(θ), γγ-coin, γγ-delay. 194,196,198,200Pb deduced levels, J, π, T1/2. Enriched, natural targets.
doi: 10.1016/0375-9474(73)90314-X
At.Data Nucl.Data Tables 12, 101 (1973)
K.Takahashi, M.Yamada, T.Kondoh
Beta-Decay Half-Lives Calculated on the Gross Theory
COMPILATION Z=3-100; calculated β T1/2.
doi: 10.1016/0092-640X(73)90015-6
UCD-CNL-172, p.13 (1973)
W.G.Wyckoff, J.E.Draper
In-Beam Studies of Lead Isotopes
NUCLEAR REACTIONS 198,202,204Hg(α, γ); measured Iγ, I(ce), γ(t), γγ-coin. 64Zn(p, nγ); measured Eγ, Iγ, E(ce), nγ-, γγ-coin. 194,196,198,200,202,204,206Pb levels deduced transitions, T1/2, ICC. 64Ga deduced levels.
Nucl.Phys. A234, 469 (1974)
H.Backe, R.Engfer, E.Kankeleit, R.Link, R.Michaelsen, C.Petitjean, L.Schellenberg, H.Schneuwly, W.U.Schroder, J.L.Vuilleumier, H.K.Walter, A.Zehnder
Nuclear Excitation and Isomer Shifts in Muonic Atoms (I). Experiment and Evaluation
ATOMIC PHYSICS, Mesic-Atoms 152Sm, 156,158,160Gd, 153Eu, 169Tm, 170Yb, 181Ta, 182,184,186W, 185,187Re, 188,190,192Os, 191,193Ir, 194,196Pt, 198,199,200,202Hg, 203,205Tl, 209Bi; measured Eγ, Iγ of muonic isotopes; deduced muonic isomer shifts.
doi: 10.1016/0375-9474(74)90576-4
Nucl.Instrum.Methods 122, 547 (1974)
M.J.Canty, P.H.Debenham, D.A.Dohan, M.Skalsey, J.W.Watson
Nuclear Lifetime Measurements with an on-Line Electron Spectrometer
NUCLEAR REACTIONS 197Au(p, 4n), (p, 2n), E=36 MeV; measured γγ(t). 194m,196mHg deduced T1/2.
Proc.Nucl.Phys.Solid State Phys. Symp., Bombay, Vol.17B, p.29 (1974)
R.K.Chattopadhyay, P.Bhattacharyya, B.Sethi, V.K.Tikku
Decay Schemes of the 9.7 H and 6.2 D Isomers of 196Au
RADIOACTIVITY 196,196mAu; measured Eγ, Iγ. 196Hg, 196Pt deduced levels, transitions.
Z.Phys. 270, 163 (1974)
D.A.Garber, M.Behar, Z.W.Grabowski, W.C.King
Nuclear g-Factors of the 328 keV State in 194Pt, the 240 keV State in 195Pt, and the 356 keV State in 196Pt Determined by Recoil-Implantation Into Iron and Cobalt Hosts
NUCLEAR REACTIONS 194,195,196Pt(16O, 16O'γ), E=36 MeV; measured 16O'γ(θ, H, t). 194,195,196Pt levels deduced g.
Nucl.Phys. A230, 380 (1974)
P.Hornshoj, P.G.Hansen, B.Jonson
Alpha-Decay Widths of Neutron-Deficient Francium and Astatine Isotopes
RADIOACTIVITY 204,205,206,207,208,209,213,220Fr, 201,202At; measured Eα, Iα, T1/2. 212Fr, 200,203,204,205At; measured Eα, Iα; deduced α-branching ratios, α-width. 212,214Ra; measured Eα, Iα, T1/2. Mass separated samples.
doi: 10.1016/0375-9474(74)90144-4
Nucl.Phys. A231, 301 (1974)
D.Proetel, R.M.Diamond, F.S.Stephens
High-Spin Excitation Modes in Even Hg Nuclei
RADIOACTIVITY 188Tl; measured Eγ, Iγ, γγ-coin. 188Hg deduced levels, J, π.
NUCLEAR REACTIONS 194,195,196,198Pt(α, xnγ), E=34-50 MeV; measured σ(E, Eγ, θ), γγ-coin, γγ(t); 172Yb(20Ne, 4nγ), E=104 MeV; measured Eγ, Iγ, γ(θ), γ(t); 164Dy(28Si, 4nγ), E=128, 135, 144 MeV; measured Eγ, Iγ. 188,194,196,198Hg deduced levels, J, π, T1/2. Enriched, natural targets.
doi: 10.1016/0375-9474(74)90523-5
Nucl.Phys. A234, 504 (1974)
H.K.Walter
Nuclear Excitation and Isomer Shifts in Muonic Atoms (II). Model-Independent Parametrization and Discussion
NUCLEAR STRUCTURE A=150-202; calculated muonic isomer shifts.
doi: 10.1016/0375-9474(74)90577-6
Nucl.Phys. A222, 301 (1974)
S.W.Yates, J.C.Cunnane, R.Hochel, P.J.Daly
High-Spin Negative Parity States in Doubly Even Hg, Pt and Os Nuclei
NUCLEAR REACTIONS 194,196,198Pt, 188,190,192Os, 182,184,186W(α, 2nγ), E=24 MeV; 197Au, 191,193Ir(p, 2nγ), E=14 MeV; measured Eγ, Iγ, γγ-coin. 196,198,200Hg, 190,192,194Pt, 184,186,188Os deduced levels, J, π.
doi: 10.1016/0375-9474(74)90394-7
CSNSM-1973-1975 Prog.Rept., p.35 (1975)
G.Bastin, C.F.Liang
Spectres α d'Isotopes d'Astate Deficients en Neutrons Produits et Separes en Ligne
RADIOACTIVITY 199,200,201,202,203,204,200mAt; measured Eα, Iα, T1/2. 198At; measured Eα, Iα.
BARC-831, p.25 (1975)
R.K.Chattopadhyay, P.Bhattacharya, B.Sethi, V.K.Tikku
Decay Schemes of the 9.7 H and 6.2 D Isomers of 196Au
RADIOACTIVITY 196,196mAu; measured Eγ, Iγ. 196Pt, 196Au, 196Hg deduced transitions, levels.
Nucl.Phys. A266, 337 (1976)
F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin
Nuclear Shapes of the Transitional Nuclei 194,196,198Pt
NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14-24 MeV, θlab=127.5°; measured σ(E, e'). 194,196,198Pt deduced β2, β4 charge, mass deformations. 194Pt deduced sign of interference term.
doi: 10.1016/0375-9474(76)90362-6
Acta Phys.Pol. B7, 823 (1976)
S.Chojnacki, T.Morek, A.Korman, Z.Haratym, T.Kempisty
Levels in 194Pb and 196Pb Populated in the Decay of 194Bi and 196Bi
RADIOACTIVITY 194,196Bi; measured Eγ, Iγ, γγ-coin, T1/2. 194,196Pb deduced levels.
Helv.Phys.Acta 49, 778 (1976)
W.Dey, H.P.Isaak, H.K.Walter, R.Engfer, H.Guyer, R.Hartmann, E.A.Hermes, H.Muller, H.S.Pruys, W.Reichart, J.Morgenstern
Measurement of Neutrons and Charged Particles Following π- Absorption in Nuclei
NUCLEAR REACTIONS 12C, 181Ta, 197Au(π-, p), (π-, d), (π-, t), (π-, n), (π-,3He), (π-, α), E=0 MeV; measured spectra.
Bull.Am.Phys.Soc. 21, No.8, 976, BC10 (1976)
P.T.Deason, C.H.King, F.M.Bernthal, T.L.Khoo, J.A.Nolen, Jr.
An Examination of the Structure of 192,194,196,198Pt with the (p, t) and (p, p') Reactions
NUCLEAR REACTIONS 194,196,198Pt(p, t), (p, p'); measured σ.
Hyperfine Interactions 1, 437 (1976)
C.Ekstrom, G.Wannberg, Y.S.Shishodia
Hyperfine Structure and Nuclear Magnetic Moments of Some Neutron-Deficient Thallium Isotopes
NUCLEAR MOMENTS 193,194,196Tl; measured nuclear spin I. 194,196,198,198m,200,202Tl; measured hfs. 194,195,196,197,198,198m,199,200,201,202Tl; measured μ. ABMR method.
J.Phys.Chem.Ref.Data 5, 835 (1976)
G.H.Fuller
Nuclear Spins and Moments
COMPILATION A=1-253; compiled μ, quadrupole moment, I.
ERDA/NDC-3/U, p.2 (1976)
R.G.Helmer
Evaluated Decay Scheme Data for Use in the ILRR Program
COMPILATION 24Na, 27Mg, 46,47,48Sc, 51Cr, 54Mn, 58,60Co, 59Fe, 64Cu, 95,97Zr, 103,106,106mRu, 115m,116mIn, 132Te, 137Cs, 140Ba, 140La, 141,143,144Ce, 144Pr, 196,198Au, 239Np; compiled, evaluated T1/2, Eγ, absolute Iγ.
Bull.Amer.Phys.Soc. 21, No.4, 558, DG7 (1976)
C.H.King, P.T.Deason, F.M.Bernthal, T.L.Khoo, J.A.Nolen, Jr.
A Study of the Even Platinum Nuclides Using the (p, t) Reaction
NUCLEAR REACTIONS 194,196,198Pt(p, t), E=35 MeV; measured σ(Et, θ).
Proc.Int.Conf.Nucl.Structure, Tokyo, Japan, Int.Academic Printing Co., Ltd.Japan, Vol.1, p.443 (1977)
A.Bockisch, K.Bharuth-Ram, A.M.Kleinfeld, K.P.Lieb
Quadrupole Moment Measurements for Even Hg Isotopes
NUCLEAR REACTIONS Hg(α, α'γ), E=11, 13 MeV; Hg(16O, 16O'γ), E=47, 56 MeV; measured Coulomb excitation, reorientation effect. 196Hg deduced B(E2). 198,200,202,204Hg deduced B(E2), quadrupole moment.
Mich.State Univ.Cyclotron Lab. Ann.Rept., 1976-1977, p.29 (1977)
P.T.deason, C.H.King, T.L.Khoo, F.M.Bernthal, J.A.Nolen
An Inelastic Proton Scattering Study of 194Pt, 196Pt and 198Pt at 35 MeV
NUCLEAR REACTIONS 194,196,198Pt(p, p'), E=35 MeV; measured σ(Ep').
Phys.Rev. C15, 1298 (1977)
C.Gunther, H.Hubel, A.Kleinrahm, D.Mertin, B.Richter, W.D.Schneider, R.Tischler
High-Spin States in Even Hg Nuclei and Rotation Alignment in 198Hg
NUCLEAR REACTIONS 194,196,198Pt(α, xnγ), E=28, 31, 34, 48 MeV; measured Eγ, Iγ, γγ-coin, γ(θ, t), ce(t). 194,196,198,200Hg deduced levels, J, π, T1/2, ICC, λ, B(λ). Rotation-alignment model.
Phys.Rev. C16, 1559 (1977)
P.E.Haustein, E.-M.Franz, R.F.Petry, J.C.Hill
New Neutron-Rich Isotope: 196Os
RADIOACTIVITY 196Os [from 198Pt(n, n2p)]; measured T1/2, Eγ, Iγ, Eβ, βγ-coin; deduced log ft limits, Q. 196Ir; measured Eγ, Iγ, Eβ; deduced levels, J, π, Q. 196Pt deduced transitions. Enriched targets, Ge(Li), Si(Li), plastic detectors.
Phys.Rev.Lett. 39, 684 (1977)
I.Y.Lee, D.Cline, P.A.Butler, R.M.Diamond, J.O.Newton, R.S.Simon, F.S.Stephens
Determination of γ Softness in 192,194,196Pt from Coulomb Excitation with 136Xe Projectiles
NUCLEAR REACTIONS 192,194,196Pt(136Xe, 136Xe), E=595, 620, 680 MeV; measured Coulomb excitation. 194Pt deduced levels, J, π.
doi: 10.1103/PhysRevLett.39.684
Phys.Lett. 68B, 113 (1977)
F.R.May, V.V.Pashkevich, S.Frauendorf
A Prediction on the Shape Transitions in Very Neutron-Deficient Even-Mass Isotopes in the Lead Region
NUCLEAR STRUCTURE 184,186,188,190,192Pb, 188,190,192,194,196,198Pt, 188,190,192,194,196Po; calculated equilibrium shapes of yrast states.
doi: 10.1016/0370-2693(77)90179-4
Nucl.Phys. A283, 269 (1977)
N.I.Molla, S.M.Qaim
A Systematic Study of (n, p) Reactions at 14.7 MeV
NUCLEAR REACTIONS 44Ca, 46,47,48,49,50Ti, 51V, 52,53,54Cr, 56,57,58Fe, 60,61,62Ni, 63,65Cu, 64,66,68Zn, 69,71Ga, 72,73Ge, 75As, 74,76,77,78Se, 81Br, 85,87Rb, 84,86,88Sr, 127I, 187Re, 186,188,189Os, 191,193Ir, 194,195,196Pt, 203,205Tl(n, p), E=14.7 MeV; measured σ, isomeric σ ratios. Natural, enriched targets; Ge(Li) detector. Investigated (n, p) σ systematics, competition between major reactions.
doi: 10.1016/0375-9474(77)90431-6
Nucl.Phys. A285, 156 (1977)
C.Roulet, G.Albouy, G.Auger, J.M.Lagrange, M.Pautrat, K.G.Rensfelt, H.Richel, H.Sergolle, J.Vanhorenbeeck
Magnetic Moments of the 12+ Isomeric States in 194,196,198Pb
NUCLEAR REACTIONS W(16O, 4nγ), E=97 MeV; measured γ(θ, H, t). 194m,196m,198mPb deduced T1/2, g. Natural metallic target.
doi: 10.1016/0375-9474(77)90152-X
Z.Phys. A286, 215 (1978)
R.Beetz, F.W.N.de Boer, J.K.Panman, J.Konijn, P.Pavlopoulos, G.Tibell, K.Zioutas, I.Bergstrom, K.Fransson, L.Tauscher, P.Blum, R.Guigas, H.Koch, H.Poth, L.M.Simons
High Spin States and Neutron Multiplicities after Pion Capture in 181Ta and 209Bi
NUCLEAR REACTIONS 181Ta, 209Bi(π-, xnγ), E=0 MeV; measured prompt, delayed γ; deduced σ. 194,196,198,200,202,204,206,203,205,207Pb, 202,206,207Tl, 166,168,170,172,174,176,178Hf deduced transitions.
NUCLEAR MOMENTS, Mesic-Atoms 181Ta, 209Bi; measured hyperfine splitting; deduced quadrupole moment.
Proc.Intern.Symp.Neutron Capture Gamma Ray Spectroscopy and Related Topics, 3rd, BNL, Upton, NY (1978), R.E.Chrien, W.R.Kane, Eds., Plenum Press, New York, p.561 (1978)
Z.Berant, Y.Birenbaum, R.Moreh
Study of the Energy Levels of 196Au Using the (γ, n) Reaction
NUCLEAR REACTIONS 197Au(γ, n), E not given; measured σ(En); deduced Q. 196Au deduced levels.
Phys.Rev.Lett. 40, 167 (1978)
J.A.Cizewski, R.F.Casten, G.J.Smith, M.L.Stelts, W.R.Kane, H.G.Borner, W.F.Davidson
Evidence for a New Symmetry in Nuclei: The Structure of 196Pt and the 0(6) Limit
NUCLEAR REACTIONS 195Pt(n, γ), E=2 keV; measured Eγ, Iγ. 196Pt deduced levels, J, π.
doi: 10.1103/PhysRevLett.40.167
Helv.Phys.Acta 51, 87 (1978)
W.Dey, H.J.Pfeiffer, U.Sennhauser, H.K.Walter, R.Engfer, R.Hartmann, E.A.Hermes, H.P.Isaak, H.S.Pruys, F.W.Schleputz
Charged Particle Emission Following Negative Pion Absorption in Nuclei
NUCLEAR REACTIONS 12C, 59Co, 197Au(π-, p), 12C, 59Co, 197Au(π-, d), 12C, 59Co, 197Au(π-, t), 12C, 59Co, 197Au(π-,3He), 12C, 59Co, 197Au(π-, α), 12C(π-,6Li), E=0; measured σ.
Nucl.Phys. A308, 147 (1978)
A.J.Kreiner, M.Fenzl, W.Kutschera
Rotational Structures in Doubly Odd Transitional Tl Nuclei
NUCLEAR REACTIONS 197Au(α, 5nγ), E ≈ 55-65 MeV; 194Pt(6Li, 4nγ), E ≈ 44 MeV; measured Eγ, Iγ, σ(Eα, Eγ, θ(γ), t), γγ-coin, γX-coin. 196Tl deduced levels, J, π, T1/2, δ. Enriched target. Ge(Li) detectors.
doi: 10.1016/0375-9474(78)90447-5
Table of Isotopes, 7th Ed., John Wiley and Sons, Inc., New York (1978)
C.M.Lederer, V.S.Shirley, E.Browne, J.M.Dairiki, R.E.Doebler, A.A.Shihab-Eldin, L.J.Jardine, J.K.Tuli, A.B.Buyrn
COMPILATION A=1-263; compiled, evaluated structure data.
Univ.Rochester, 1977 Ann.Rept., p.82 (1978)
J.Sprinkle, D.Cline, P.Russo, R.Scharenberg, P.Vold
Static Quadrupole Moment Measurements and the Shape Transitions in Platinum Nuclei
NUCLEAR REACTIONS 192,194,196,198Pt(58Ni, 58Ni'), E=80-130 MeV; measured γ(particle)-coin following Coulomb excitation. 192,194,196,198Pt levels deduced static quadrupole moments.
Z.Phys. A287, 121 (1978)
H.L.Yadav, H.Toki, A.Faessler
Staggering of Even and Odd Spin States in 196,198Tl Nuclei
NUCLEAR STRUCTURE 196,198Tl; calculated band structure.
Phys.Rev. C19, 2138 (1979)
R.E.Anderson, P.A.Batay-Csorba, R.A.Emigh, E.R.Flynn, D.A.Lind, P.A.Smith, C.D.Zafiratos, R.M.DeVries
(3He, n) Reaction Near and Above Z = 82
NUCLEAR REACTIONS 204,206,208Pb, 204Hg, 194,196Pt(3He, n), E=33.3 MeV; measured σ(E, θ). Enriched targets, DWBA analysis.
Z.Phys. A289, 231 (1979)
A.Bockisch, K.Bharuth-Ram, A.M.Kleinfeld, K.P.Lieb
Oblate Shapes of 200,202,204Hg
NUCLEAR REACTIONS Hg(16O, 16O'), E=56-64 MeV; measured relative γ-yield following Coulomb excitation. 200,202,204Hg deduced quadrupole moment, oblate shapes. 196,198,200,202,204Hg levels deduced B(E2). Natural target.
J.Phys.Soc.Jpn. 47, 1397 (1979)
H.H.Bolotin, I.Katayama, H.Sakai, Y.Fujita, M.Fujiwara, K.Hosono, T.Itahashi, T.Saito, S.H.Sie, D.Conley, D.L.Kennedy, A.E.Stuchbery
Lifetime Measurements of Excited States in 196Pt
NUCLEAR REACTIONS 196Pt(20Ne, 20Ne'), E=90 MeV; 196Pt(58Ni, 58Ni'), E=220 MeV; measured Eγ, particle γ-coin, RDM, DSA. 196Pt levels deduced T1/2, γ-branching ratios, B(E2). Enriched target.
Nucl.Phys. A323, 349 (1979)
J.A.Cizewski, R.F.Casten, G.J.Smith, M.R.Macphail, M.L.Stelts, W.R.Kane, H.G.Borner, W.F.Davidson
The Level Structure of 196Pt
NUCLEAR REACTIONS 195Pt(n, γ), E=thermal, 11.9 eV, 19.6 eV, 2 keV; measured Eγ, Iγ, γγ-coin. 196Pt deduced levels, transitions, J, π. Ge(Li) detectors, curved-crystal spectrometers. Enriched targets. Interacting boson approximation model in O(6) limit, negative parity decoupled bands.
doi: 10.1016/0375-9474(79)90115-5
Phys.Lett. 88B, 207 (1979)
J.A.Cizewski, E.R.Flynn, R.E.Brown, J.W.Sunier
Two-Particle Transfer in O(6) Nuclei
NUCLEAR REACTIONS 192,194,196,198Pt, 186,188,190,192Os(t, p), E=17 MeV; measured σ(θ). 194,196,198,200Pt, 188,190,192,194Os deduced 2n transfer strengths. Natural, enriched target. DWBA analysis, O(6) limit interacting boson approximation model.
doi: 10.1016/0370-2693(79)90449-0
Bull.Am.Phys.Soc. 24, No.4, 685, JL7 (1979)
J.A.Cizewski, E.R.Flynn, R.E.Brown, D.L.Hanson, J.W.Sunier
Two-Neutron Transfer Studies in the Pt Nuclei
NUCLEAR REACTIONS 194,196,198Pt(t, p), E not given; measured σ(Ep, θ). 196,198,200Pt deduced levels. Interpretation in terms of O(6) limit of interacting boson model.
Phys.Rev. C20, 927 (1979)
P.T.Deason, C.H.King, T.L.Khoo, J.A.Nolen, Jr., F.M.Bernthal
194,196,198Pt(p, t) Reactions at 35 MeV
NUCLEAR REACTIONS 194,196,198Pt(p, t), E=35 MeV; measured σ(Et, θ). 192,194,196Pt deduced levels, L, J, π, enhancement factor. DWBA analysis. Interacting boson approximation model. Enriched targets.
Nucl.Phys. A314, 161 (1979)
O.Hausser, B.Haas, D.Ward, H.R.Andrews
The g-Factors of Excited States in 205,203Tl Measured by Transient Field Interaction at High Recoil Velocities
NUCLEAR REACTIONS 194,196,198Pt(40Ca, 40Ca'γ), E=120 MeV; 194,196,198Pt(81Br, 81Br'γ), E=190 MeV; 203,205Tl(40Ca, 40Ca'γ), E=120 MeV; measured γ-precession. 203,205Tl deduced g. 194,196,198Pt deduced g-ratios for 2+ levels. Enhanced transient field, IMPAC technique.
doi: 10.1016/0375-9474(79)90560-8
Nucl.Data Sheets 28, 485 (1979)
J.Halperin
Nuclear Data Sheets for A = 196
COMPILATION 196Os, 196Ir, 196Pt, 196Au, 196Hg, 196Tl, 196Pb, 196Bi, 196Po, 196At; compiled, evaluated structure data.
Nucl.Phys. A331, 16 (1979)
V.Paar
A Parabolic Rule for the Energy Dependence on x = I(I + 1) for Proton-Neutron Multiplets in Odd-Odd Nuclei
NUCLEAR STRUCTURE 48Sc, 94Tc, 122Sb, 116In, 196Tl; calculated energies of pn-multiplet states. Parabolic rule, exchange of quadrupole, spin-vibrational phonon.
doi: 10.1016/0375-9474(79)90297-5
J.Phys.(Paris), Lett. 40, L-465 (1979)
D.N.Poenaru, M.Ivascu, A.Sandulescu
La Radioactivite Alpha Etudiee par les Methodes de la Fission
RADIOACTIVITY, Fission 222,224,226Ra, 224,226,228,230,232Th, 226,228,230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 194,196,198,200,202,204,206,208,210,212,214,216,218Po; calculated α-decay T1/2, Q; deduced plausible SF. Liquid drop model, phenomenological shell correction.
Z.Phys. A292, 79 (1979)
H.Toki, H.L.Yadav, A.Faessler
Study of Transitional Odd-Odd Mass Nuclei
NUCLEAR STRUCTURE 190,192,194Au, 196,198Tl; calculated energy levels, electromagnetic transitions, moments γ-deformed rotor model.
Diss.Abst.Int. 40B, 5666 (1980)
P.T.Deason, Jr.
A Study of 192,194,196,198Pt using the (p, t) and (p, p') Reactions and the Interacting Boson Approximation Model
NUCLEAR REACTIONS 194,196,198Pt(p, t), (p, p'), E=35 MeV; measured σ(θ). 192,194,196,198Pt deduced levels, J, π. Interacting boson model, coupled-channels analysis, deformed optical potential.
Nucl.Instrum.Methods 171, 361 (1980)
D.L.Kennedy, A.E.Stuchbery, H.H.Bolotin
The Extraction of Lifetimes of Weakly-Populated Nuclear Levels in Recoil Distance Method Experiments
NUCLEAR REACTIONS 196,198Pt(58Ni, 58Ni'), E=220 MeV; measured Eγ, Iγ, Coulomb excitation, recoil, DSA. 196,198Pt levels deduced T1/2. Enriched target, analytic extension of recoil distance method data.
J.Phys.(London) G6, L13 (1980)
A.J.Kreiner, M.A.J.Mariscotti
Evidence for a Predicted Change of Phase in the Level Staggering of Bands in Doubly-Odd Nuclei
NUCLEAR STRUCTURE 76Br, 104,106Ag, 108In, 132,134La, 134,136Pr, 150,152Eu, 196,198Tl, 196Au; analyzed data on odd-p, odd-n nuclei; deduced change of phase in level staggering of bands.
doi: 10.1088/0305-4616/6/1/004
Phys.Rev. C22, 2570 (1980)
A.J.Kreiner
πh9/2 x νi13/2 Bands in Doubly Odd Tl Isotopes Including a Proton-Neutron Residual Interaction
NUCLEAR STRUCTURE 191,192,193,194,195,196,197,198,199,200,201Tl; calculated levels, band structure. Two-quasiparticle and rotor model, neutron-proton residual interaction.
Phys.Lett. B97, 197 (1980)
R.Kroth, S.K.Bhattacherjee, C.Gunther, M.Guttormsen, K.Hardt, H.Hubel, A.Kleinrahm
g-Factors of High-Spin Isomers in 194Hg and 196Hg
RADIOACTIVITY 194,196Hg [from 194,196Pt(γ, 4n), E=48 MeV]; measured Eγ, Iγ, γ(θ), γ(θ, H). 194,196Hg levels deduced g, configuration. Cranking model calculations.
doi: 10.1016/0370-2693(80)90581-X
Phys.Rev. C22, 2135 (1980)
M.Lifshitz, P.Singer
Nuclear Excitation Function and Particle Emission from Complex Nuclei Following Muon Capture
NUCLEAR REACTIONS 27Al, 28Si, 31P, 39,41K, 51V, 55Mn, 56Fe, 60Ni, 63,65Cu, 75As, 94Zr, 115In, 121Sb, 165Ho, 79Br, 107Ag, 127I, 133Cs, 181Ta, 197Au, 208Pb, 209Bi(μ-, xnp), (μ-, α), (μ-, p), (μ-, d), E at rest; calculated σ(Ep), σ(En), σ(Eα), σ(Ed), neutron multiplicities. Preequilibrium, compound nucleus emission models.
Yad.Fiz. 31, 88 (1980); Sov.J.Nucl.Phys. 31, 46 (1980)
V.M.Strutinsky, F.A.Ivanyuk, V.V.Pashkevich
Accuracy of Calculations of Shell Corrections
NUCLEAR STRUCTURE 208Pb, 204Hg, 196Os; calculated shell correction energies for protons, neutrons; deduced accuracy conditions. Woods-Saxon potential, harmonic oscillator basis.
Phys.Rev. C22, 1323 (1980)
K.J.Weeks, T.Tamura
Boson Expansion Description of Collective States in Osmium and Platinum Isotopes
NUCLEAR STRUCTURE 186,188,190,192,194Os, 188,190,192,194,196,198Pt; calculated levels, B(E2), magnetic, static quadrupole moments. Boson expansion theory.
Nucl.Phys. A356, 401 (1981)
V.M.Abazov, V.S.Butsev, D.Chultem, Yu.K.Gavrilov, A.B.Kurepin
The Probability of the Reaction (π-, p) and the Problem of Δ++ Isobars in the Atomic Nucleus
NUCLEAR REACTIONS 45Sc, 59Co, 89Y, 133Cs, 141Pr, 197Au(π-, p), E at rest; measured yields for 44K, 58Mn, 88Rb, 132I, 140La, 196mIr; deduced single proton emission upper limit, Δ-isobar admixture in initial nuclear state.
doi: 10.1016/0375-9474(81)90197-4
Nucl.Phys. A370, 146 (1981)
H.H.Bolotin, A.E.Stuchbery, I.Morrison, D.L.Kennedy, C.G.Ryan, S.H.Sie
Lifetimes of Excited States in 196,198Pt; Application of interacting boson approximation model to even Pt isotopes systematics
NUCLEAR REACTIONS 196,198Pt(58Ni, 58Ni'), E=220 MeV; measured Coulomb excitation, recoil, (particle)γ-coin; 198Pt(58Ni, 58Ni'), E=220 MeV; measured γ(θ). 196,198Pt levels deduced T1/2, B(E2). Interacting boson approximation calculations, systematics of even Pt isotopes.
doi: 10.1016/0375-9474(81)90759-4
Phys.Rev. C23, 1453 (1981)
J.A.Cizewski, E.R.Flynn, R.E.Brown, D.L.Hanson, S.D.Orbesen, J.W.Sunier
Two-Neutron Transfer in Pt Nuclei and the Structure of 200Pt
NUCLEAR STRUCTURE 186,188,190,192,194,196,198,200Pt; calculated L=4 transition systematics. Interacting boson, schematic, pairing vibration, boson expansion models.
NUCLEAR REACTIONS 194,196,198Pt(t, p), E=17 MeV; measured σ(Ep, θ). 196,198,200Pt deduced levels, J, π, L, two-nucleon transfer strengths. DWBA analysis.
Phys.Rev. C23, 1414 (1981)
P.T.Deason, C.H.King, R.M.Ronningen, T.L.Khoo, F.M.Bernthal, J.A.Nolen, Jr.
194,196,198Pt(p, p') Reactions at 35 MeV
NUCLEAR REACTIONS 194,196,198Pt(p, p'), E=35 MeV; measured σ(Ep, θ); deduced optical model parameters. 194,196,198Pt deduced levels, J, π, quadrupole, hexadecapole moments, β2, β4, B(E4), band structure. Magnetic spectrograph, enriched targets. Interacting boson model, coupled-channels calculation.
Yad.Fiz. 33, 591 (1981)
L.Z.Djilavyan, L.E.Lazareva, V.N.Ponomarev, A.A.Sorokin
Isomeric Yield Ratios of the Reactions 197Au(γ, n)196m,gAu and 197Au(e, e'n)196m,gAu at Energies of 10-90 MeV
NUCLEAR REACTIONS 197Au(γ, n), (e, e'n), E=10-90 MeV; measured Eγ, Iγ. 196Au deduced levels, J, π, isomeric yield ratios. Activation technique.
Phys.Lett. B97, 183 (1980); see 1980Ha56
F.Hachenberg, H.C.Chiang, J.Hufner
Pickup in the Surface - The Origin of Deuterons in Nuclear Precompound Reactions
doi: 10.1016/0370-2693(80)90577-8
RCNP (Osaka), Ann.Rept., 1980, p.83 (1981)
M.Hyakutake, I.Kumabe, N.Koori, K.Yuasa, T.Yamagata, S.Kishimoto, T.Komatuzaki, Y.Ishizaki, T.Tohei, T.Nakagawa
Excitation of High Spin States by the (p, t) Reaction on Even-Even Pt and Cd Isotopes
NUCLEAR REACTIONS 196,198Pt, 112Cd(p, t), E=54.6 MeV; measured σ(θ), triton momentum spectra. 110Cd deduced 8+ level population. Zero-range DWBA.
J.Phys.Soc.Jpn. 50, 1832 (1981)
M.Kawamura, T.Tomiyama, H.Kato
The g-Factor of the First Excited Level of 196Pt
RADIOACTIVITY 196Au; measured γγ(θ, H) in Fe. 196Pt level deduced g.
Bull.Am.Phys.Soc. 26, No.8, 1117, AD8 (1981)
W.R.Kane, R.F.Casten, D.D.Warner, K.Schreckenbach, H.Faust, S.Blakeway
E0 Transitions in 188Os and 196Pt: Structure of IBA model wave functions
NUCLEAR REACTIONS 187Os, 195Pt(n, e), (n, γ), E=thermal; measured σ(E(e), Eγ, Iγ). 188Os, 196Pt deduced 0+ states, E0 transitions. Interacting boson model.
Phys.Lett. 99B, 209 (1981)
R.Kroth, K.Hardt, M.Guttormsen, G.Mikus, J.Recht, W.Vilter, H.Hubel, C.Gunther
Identification of the Missing Rotation-Aligned (νi-213/2) 12+ State in 196Hg
NUCLEAR REACTIONS 194Pt(α, 2n), E=30 MeV; 196Pt(α, 4n), E=48 MeV; 197Au(α, 3n), E=22 MeV; measured γγ-coin, I(ce), ce(t). 196Hg deduced levels, T1/2, J, π, B(E2), γ-branching, configuration, rotation-aligned structure.
doi: 10.1016/0370-2693(81)91109-6
Phys.Rev. C23, 1394 (1981)
C.M.McCullagh, M.L.Stelts, R.E.Chrien
Dipole Radiative Strength Functions from Resonance Neutron Capture
NUCLEAR REACTIONS 56Fe(n, γ), E=1167 eV; 105Pd(n, γ), E=11.8 eV; 127I(n, γ), E=20.5 eV; 143Nd(n, γ), E=55 eV; 175Lu(n, γ), E=thermal; 27Al, 35Cl, 125Te, 181Ta, 182,183W, 195Pt, 236U(n, γ), E not given; measured σ; deduced E1, M1 strength function vs mass. 57Fe, 106Pd, 128I, 144Nd, 176Lu resonances deduced Γγ, J, π.
Nucl.Phys. A352, 388 (1981)
H.S.Pruys, R.Engfer, R.Hartmann, E.A.Hermes, H.P.Isaak, F.W.Schlepuetz, U.Sennhauser, W.Dey, K.Hess, H.-J.Pfeiffer, H.K.Walter, W.Hesselink
Charged Particle Emission following the Absorption of Stopped π- in 12C, 59Co and 197Au
NUCLEAR REACTIONS 12C, 59Co, 197Au(π-, p), (π-, d), (π-, t), (π-,3He), (π-, α), E at rest; measured σ(Ep), σ(Ed), σ(Et), σ(E(3He)), σ(Eα). Quasideuteron pion absorption model.
doi: 10.1016/0375-9474(81)90418-8
Nucl.Phys. A370, 231 (1981)
J.Sauvage-Letessier, P.Quentin, H.Flocard
Deformation Properties of Osmium, Platinum, Mercury Isotopes from Self-Consistent Calculations: Influence of the pairing treatment
NUCLEAR STRUCTURE 184,188,192,196Os, 182,184,186,188,190,192,196Pt, 180,184,186,188,190,192,200Hg; calculated binding energies, deformation parameters β2, β4, rms charge radii, neutron, proton pairing gaps; 184,188,192Os, 196Pt, 200Hg; calculated quadrupole moment. Hartree-Fock, BCS, Skyrme interaction.
doi: 10.1016/0375-9474(81)90074-9
Nucl.Phys. A365, 317 (1981)
A.E.Stuchbery, C.G.Ryan, H.H.Bolotin, I.Morrison, S.H.Sie
Gyromagnetic Ratios of Excited States in 198Pt; Measurements and Interacting Boson Approximation Model Calculations
NUCLEAR REACTIONS 196,198Pt(58Ni, 58Ni'), E=220 MeV; measured γ(θ, H) in polarized Fe, (particle)γ-coin, Coulomb excitation. 198Pt levels deduced g, δ. Enriched target, thin foil technique.
NUCLEAR STRUCTURE 198Pt; calculated levels, g, static dipole moments; deduced M1 selection rules. Interacting boson approximation, O(6) limit.
doi: 10.1016/0375-9474(81)90299-2
Phys.Rev. C24, 1480 (1981)
A.E.Stuchbery, C.G.Ryan, H.H.Bolotin
Velocity Dependence of Transient Hyperfine Field at Pt Ions Rapidly Recoiling through Magnetized Fe
NUCLEAR REACTIONS 196Pt(32S, 32S'), E=80, 120 MeV; 196Pt(58Ni, 58Ni'), E=150, 220 MeV; measured γ(θ, H) in polarized Fe, Coulomb excitation; deduced transient field, velocity dependence for Pt ions in Fe.
Phys.Rev. C24, 2106 (1981)
A.E.Stuchbery, C.G.Ryan, I.Morrison, H.H.Bolotin
Gyromagnetic Ratios of Low-Lying Excited States in 196Pt
NUCLEAR REACTIONS 196Pt(58Ni, 58Ni'), E=220 MeV; measured γ(θ, H) in polarized Fe, Coulomb excitation, 58Niγ-coin. 196Pt levels deduced g. Enriched targets, thin foil technique.
NUCLEAR STRUCTURE 192,194,196,198Pt; calculated g. Interacting boson approximation.
Phys.Lett. 100B, 383 (1981)
J.Vervier
Dynamical Supersymmetry in 196Pt and 197Au
NUCLEAR STRUCTURE 196Pt, 197Au; calculated levels, B(E2); 198Hg; calculated B(E2); deduced supersymmetry model validation. Interacting boson model.
NUCLEAR REACTIONS 196Pt(3He, d), E not given; calculated one-nucleon transfer C2S; deduced supersymmetry model validation. Interacting boson model.
doi: 10.1016/0370-2693(81)90142-8
Phys.Lett. 107B, 349 (1981)
M.Vergnes, G.Berrier-Ronsin, G.Rotbard, J.Vernotte, H.Langevin-Joliot, E.Gerlic, J.Van de Wiele, J.Guillot, S.Y.van der Werf
The 197Au(d, 3He)196Pt Reaction and the Supersymmetry Scheme
NUCLEAR REACTIONS 197Au(d, 3He), E=108 MeV; measured σ(θ), σ(E(3He)). 196Pt levels deduced spectroscopic factors. Supersymmetry scheme validity tested.
doi: 10.1016/0370-2693(81)90339-7
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., p.N33 (1981)
M.Vergnes, G.Berrier-Ronsin, G.Rotbard, J.Vernotte, H.Langevin-Joliot, E.Gerlic, J.van de Wiele, J.Guillot, S.Y.van der Werf
Reaction 197Au(d, 3He)196Pt et Supersymetrie
NUCLEAR REACTIONS 197Au(d, 3He), E=108 MeV; measured σ(E(3He)). 196Pt levels deduced C2S, supersymmetry selection rule validity.
Hyperfine Interactions 9, 109 (1981)
S.Zywietz, H.Grawe, H.Haas, M.Menningen
Nuclear Quadrupole Moments of 12+-Isomers in 196,198Pb
RADIOACTIVITY 196,198Pb [from 196,198Hg(α, 4n), E=55 MeV]; measured Eγ, γ(t), γ(θ, H, t) in Hg. 196,198Pb deduced isomer quadrupole moment. Enriched Hg target.
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., p.E77 (1982)
G.Berrier-Ronsin, M.Vergnes, G.Rotbard, J.Vernotte, S.Fortier, J.M.Maison, R.Tamisier
Etude des Isotopes Lourds du Hg en Reaction (p, t)
NUCLEAR REACTIONS Hg, 204,202,200,198Hg(p, t), E=25 MeV; measured not abstracted. 202,200,198,196Hg deduced ground state population strength, symmetry characteristics. 198Hg(p, d), E=25 MeV; measured Q. 197Hg deduced mass excess.
NIKHEF-K Ann.Rept., 1981-82, p.11 (1982)
W.T.A.Borghols, C.W.de Jager, H.de Vries, N.Blasi, M.N.Harakeh, S.Y.van der Werf
Electron Scattering of 196Pt
NUCLEAR REACTIONS 196Pt(e, e'), E=70, 107, 133 MeV; measured σ(θ=154°); 196Pt(e, e), E=70-280 MeV; measured σ(θ). 196Pt deduced possible collective band splitting.
Nucl.Phys. A373, 256 (1982)
E.Hagn, E.Zech
Nuclear Magnetic Moment of the 9.7 h 12- Isomer 196mAu
RADIOACTIVITY 196mAu [from 198Pt(d, 4n)]; measured Iγ(θ, T), NMR on oriented nuclei. 196mAu deduced g, μ, configuration of isomeric state. Recoil implantation into Ni.
doi: 10.1016/0375-9474(82)90150-6
Phys.Rev. C25, 2710 (1982)
K.H.Hicks, T.E.Ward, J.Wiggins, C.A.Fields, F.W.N.de Boer
Decays of 194,195,196Pb
RADIOACTIVITY 194,195,196Pb [from 197Au(6Li, xn), E=95 MeV]; measured Eγ, Iγ, γγ-coin; deduced log ft. 194,195,196mPb deduced T1/2. 194,195,196Tl deduced levels, J, π, Nilsson configurations. Ge(Li) detectors.
Z.Phys. A309, 27 (1982)
R.Hingmann, H.-G.Clerc, C.-C.Sahm, D.Vermeulen, K.-H.Schmidt, J.G.Keller
Alpha Decay Properties of 199Rn and 199mRn
NUCLEAR REACTIONS 86Kr(116Sn, X), (116Sn, 2n), (116Sn, 3n), E=345-385 MeV; measured residual production σ vs E, (evaporation residue)(α)(t), αα(t). 199m,199Rn levels deduced α-decay T1/2, decay characteristics, possible J, π. Correlation analysis, shell model.
Z.Phys. A305, 111 (1982)
S.Hofmann, W.Reisdorf, G.Munzenberg, F.P.Hessberger, J.R.H.Schneider, P.Armbruster
Proton Radioactivity of 151Lu
NUCLEAR REACTIONS 96Ru(58Ni, xnyp), E=261-302 MeV; 99,100Ru(58Ni, xnyp), E=97.4, 98.1 MeV; 92Mo(58Ni, xnyp), E=249, 261, 277 MeV; 102Pd(58Ni, xnyp), E=240-302 MeV; measured cumulative yields vs E for 151Ho, 152Er, 157,158Ta, 156,157,158Hf, 155,156Lu, 155Yb. Activation, concidence techniques, enriched Ru targets, mass separated Pd, Mo targets.
RADIOACTIVITY 151Lu [from 96Ru(58Ni, 2np), E=261 MeV]; measured Ep, Ip, direct proton decay T1/2, Q(p). Coincidence techniques, enriched Ru target.
Phys.Lett. 117B, 15 (1982)
W.R.Kane, R.F.Casten, D.D.Warner, K.Schreckenbach, H.R.Faust, S.Blakeway
Strengths of E0 Transitions in 188Os and 196Pt and the Structure of IBA Wavefunctions in the Os-Pt Transition Region
NUCLEAR REACTIONS 187Os, 195Pt(n, γ), E=thermal; measured I(ce), Eγ, Iγ. 188Os, 196Pt deduced levels, B(E0)/B(E2), E0 transition strength. Interacting boson model, O(6) limit.
doi: 10.1016/0370-2693(82)90864-4
Phys.Rev. C25, 293 (1982)
R.Levy, N.Tsoupas, N.K.B.Shu, A.Lopez-Garcia, W.Andrejtscheff, N.Benczer-Koller
Magnetic Moment Measurements in Osmium and Platinum Nuclei
NUCLEAR REACTIONS 186,188Os, 194,196Pt(32S, 32S'), E ≈ 80 MeV; measured γ(θ, H) in polarized Fe, Coulomb excitation, γ32S-coin, γ(θ). 188,186Os, 194,196Pt level deduced g.
LBL-13366, p.44 (1982)
M.Leino, S.Yashita, A.Ghiorso
Alpha Decay of Neutron Deficient Polonium and Bismuth Isotopes
RADIOACTIVITY 192,193,193m,194,195,195m,196Po, 191,192,193,193mBi(α) [from Ce(56Fe, xn), (56Fe, xnp), 141Pr(56Fe, xnp), (56Fe, xnα), E=240-280 MeV]; measured Eα, Iα. 194,193,193m,192Po, 191mBi; measured α-decay T1/2.
NUCLEAR REACTIONS Ce(56Fe, xn), (56Fe, xnp), 141Pr(56Fe, xnp), (56Fe, xnα)192Po/193Po/193mPo/194Po/195Po/195mPo/196Po/191Bi/192Bi/193Bi/193mBi, E=240-280 MeV; measured residuals production σ vs E. Activation technique.
Z.Phys. A307, 141 (1982)
M.H.Simbel
Is Neutron Evaporation from Highly Excited Nuclei a Poisson Random Process ( Question )
NUCLEAR REACTIONS 164Dy(40Ar, 4n), (40Ar, 5n), (40Ar, 6n), (40Ar, 7n), (40Ar, 8n), (40Ar, 9n), (40Ar, 10n), 197Au(12C, 4n), (12C, 5n), (12C, 6n), (12C, 7n), (12C, 8n), 197Au(α, n), (α, 2n), (α, 3n), (α, 4n), (α, 5n), (α, 6n), (α, 7n), (α, 8n), (α, 9n), (α, 10n), (α, 11n), (α, 3np), (α, 5np), (α, 7np), E not given; calculated residual production σ(E). Poisson distribution function, post, preequilibrium components.
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., p.E76 (1982)
M.Vergnes, G.Berrier-Ronsin, G.Rotbard, J.Vernotte, J.Kalifa, R.Tamisier
Sections Efficaces Pour la Reaction (p, t) dans la Region Os, Ir, Pt, Au, Hg
NUCLEAR REACTIONS 194,196Pt, 193Ir, 192Os, 198Hg, 197Au(p, t), E=25 MeV; measured σ. 192Os, 193Ir, 196Pt, 197Au, 198Hg deduced supersymmetry validity.
KVI Ann.Rept., 1982, p.25 (1983)
N.Blasi, M.N.Harakeh, W.A.Sterrenburg, S.Y.van der Werf
The 197Au(d, 3He)196Pt Reaction at E(d) = 50 MeV
NUCLEAR REACTIONS 197Au(d, 3He), E=50 MeV; measured σ(E(3He)). 196Pt levels deduced spectroscopic strength, configurational characteristics.
Phys.Lett. 130B, 167 (1983)
P.D.Bond, R.F.Casten, D.D.Warner, D.Horn
Excited States in 196Os and the Structure of the Pt-Os Transition Region
NUCLEAR REACTIONS 198Pt(14C, 16O), E=100 MeV; measured σ(E(16O)); deduced Q, Pt to Os transition region. 196Os deduced ground state mass, levels, possible J, π.
doi: 10.1016/0370-2693(83)91034-1
Program and Theses, Proc.33rd Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Moscow, p.147 (1983)
B.I.Gorbachev, A.I.Levon, O.F.Nemets, O.B.Sevastyuk
Nuclear g-Factors and the Structure of Isomeric States in the Isotopes 186,188Os and 196,198Hg
NUCLEAR REACTIONS 184,186W, 194,196Pt(α, 2nγ), E not given; measured γ(θ, H, t). 186,188Os, 196,198Hg levels deduced T1/2, g, configurations.
Nucl.Phys. A398, 119 (1983)
M.Guttormsen, A.V.Grumbkow, Y.K.Agarwal, K.P.Blume, K.Hardt, H.Hubel, J.Recht, P.Schuler, H.Kluge, K.H.Maier, A.Maj, N.Roy
The (νi213/2)(8+, 10+, 12+) Triplets in 190-196Hg
NUCLEAR REACTIONS 181Ta(14N, 5n), E=100 MeV; 192,194,196Pt(α, 4n), E=50 MeV; measured (ce)(ce)(t). 190,192,194,196Hg deduced levels, J, π, M1/E2 mixing, γ-multipolarity, B(E2). Superconducting solenoid, Si(Li) detectors.
doi: 10.1016/0375-9474(83)90651-6
Phys.Rev. C28, 1382 (1983)
H.Helppi, S.K.Saha, P.J.Daly, S.R.Faber, T.L.Khoo
Rotation-Aligned Bands in 196Hg
NUCLEAR REACTIONS 196Pt(α, 4n), E=48.6 MeV; measured Eγ, Iγ(θ), γγ(t), γγ-coin. 196Hg deduced high-spin levels, J, π, backbending, γ-branching. Cranked shell model.
Z.Phys. A313, 69 (1983)
A.A.Raduta, C.Lima, A.Faessler
Coupling of Two Quasiparticles to Coherent Cores in the Pt Isotopes
NUCLEAR STRUCTURE 190,192Pt; calculated levels, B(E2) ratios, yrast level g. 180,194Pt; calculated levels, B(E2) ratios. Quadrupole collective core-particle motion coupling, angular momentum projected coherent states.
Phys.Rev. C27, 434 (1983)
A.E.Stuchbery, C.G.Ryan, H.Ohnuma, G.B.Beard, H.H.Bolotin
Transient Hyperfine Field Measurements of Gyromagnetic Ratios in Os and Pt Nuclei
NUCLEAR REACTIONS 192Os, 198Pt(32S, 32S'), E=80 MeV; 192Os, 198Pt(58Ni, 58Ni'), E=220 MeV; measured γ(θ, H, T); deduced transient fields on Pt, Os in Fe, Co. 194,196,198Pt level deduced g. Ion recoil in polarized Co foils.
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
Phys.Rev. C27, 1342 (1983)
P.van Nes, Z.Sujkowski, W.Hesselink, J.van Ruyven, H.Verheul, M.J.A.de Voigt
Search for Collective Bands in 194,196Pb Nuclei above the Jπ = 12+ Isomers
NUCLEAR REACTIONS 188Os(12C, 4n), (12C, 6n), E=101 MeV; measured Eγ, Iγ, γ(θ), I(ce), γγ(t), X-ray(γ(t)); deduced K X-ray multiplicities. 194,196Pb deduced levels, J, π, γ-branching. Miniorange spectrometer, Ge, Ge(Li) detectors, NaI(Tl) sum spectrometer.
IPNO-DRE-83-24 (1983)
M.Vergnes, G.Berrier-Ronsin, G.Rotbard, J.Vernotte, S.Fortier, J.M.Maison, R.Tamisier, S.Grafeuille, P.D.Duval, E.R.Flynn
Anomalies in Heavy Hg Isotopes
NUCLEAR REACTIONS Hg, 204,202,200,198,196Hg(p, t), E=25 MeV; measured σ(θ). 194,196,198,200,202,204Hg deduced levels, ground state transition enhancement factors. 200Hg deduced intruder state. Interacting boson model.
Phys.Lett. 123B, 173 (1983)
H.W.Wilschut, R.K.Bhowmik, P.B.Goldhoorn, J.F.W.Jansen, R.H.Siemssen, K.Siwek-Wilczynska, Z.Sujkowski, J.Wilczynski
Selection of Heavy Ion Reaction Channels via Particle K X-Ray Coincidences
NUCLEAR REACTIONS 197Au(14N, α), (14N, 7Li), (14N, 9Be), (14N, 10Be), (14N, 10B), (14N, 11B), (14N, 12B), (14N, 13C), (14N, 15N), E=140 MeV; measured E(X-ray), I(X-ray), (particle)(X-ray)-, (particle)(X-ray)(X-ray)-coin; deduced inclusive, exclusive σ(θ).
doi: 10.1016/0370-2693(83)90416-1
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., p.E20 (1984)
G.Albouy, J.M.Lagrange, M.Pautrat, J.Dionisio Santana, J.Vanhorenbeeck, Ch.Vieu
Etats de Haut Spin des Isotopes 197Pb, 198Pb et 196Pb
NUCLEAR REACTIONS 186W(16O, 4n), (16O, 5n), (16O, 6n), E=95 MeV; measured I(ce), Iγ, Eγ. 197,198,196Pb deduced levels, J, π.
Phys.Lett. 141B, 309 (1984)
I.Anthony, D.Branford, A.G.Flowers, J.C.McGeorge, M.R.Sene, A.C.Shotter, P.J.Thorley, C.H.Zimmerman, J.Friedrich, N.Voegler, K.Bangert, U.E.P.Berg
Determination of the Total Photo-Absorption Cross Section of 197Au from (γ, xn) Reaction Cross Sections
NUCLEAR REACTIONS 197Au(γ, n), (γ, 3n), (γ, 5n), (γ, 7n), E=60-340 MeV bremsstrahlung; measured yield per electron; deduced photon absorption σ, E1 sum rule enhancement factor.
doi: 10.1016/0370-2693(84)90251-X
Phys.Scr. 30, 164 (1984)
C.Bengtsson, C.Ekstrom, L.Robertsson, J.Heinemeier, and the ISOLDE Collaboration
Nuclear Spins of Some Indium and Thallium Isotopes
NUCLEAR MOMENTS 194,195,196,197,198,198m,199,200,201,202Tl; analyzed data; deduced dipole constant a, μ.
RADIOACTIVITY 121,119,118mIn(β-); 121m,119m,118mIn(β-), (IT); 191mTl(EC), (β+) [from U(p, F), E=600 MeV]; measured J. ABMR technique.
Phys.Rev. C30, 1671 (1984)
F.Calaprice, G.T.Ewan, R.-D.von Dincklage, B.Jonson, O.C.Jonsson, H.L.Ravn
Alpha Decay of 198Rn
NUCLEAR REACTIONS Th(p, X)198Rn/199Rn/199mRn/200Rn, E=600 MeV; measured Rn isotope production yields, Eα; deduced evidence for 198Rn. Activation technique.
RADIOACTIVITY 198,199,199m,200Rn(α) [from Th(p, X), E=600 MeV]; measured α-decay rate, Eα, Iα, T1/2. High temperature target, mass separation.
Phys.Rev. C30, 236 (1984)
J.M.D'Auria, M.Dombsky, G.Sheffer, T.E.Ward, H.J.Karwowski, A.I.Yavin, J.L.Clark
Inclusive Measurement of Quasifree (p, xn) Charge Exchange Reactions on Bismuth from 62 to 800 MeV
NUCLEAR REACTIONS, ICPND 209Bi(p, n), (p, 2n), (p, 4n), (p, 6n), E=62-800 MeV; measured residuals production σ(E), production σ relative to 208Po vs E. 209Bi(p, X), E=210-480 MeV; measured residuals production σ relative to 202o. Radiochemical activation techniques. Intranuclear cascade calculation.
Nucl.Instrum.Methods 223, 1 (1984)
C.De Vries, C.W.De Jager, L.Lapikas, G.Luijckx, R.Maas, H.De Vries, P.K.A.De Witt Huberts
The 500 MeV Electron-Scattering Facility at NIKHEF-K
NUCLEAR REACTIONS 196Pt(e, e'), E=370.9 MeV; measured σ(E(e')). 12C(e, e'p), E at 295 MeV/c; 1H(e, e'p), E at 277 MeV/c; measured missing energy, momentum spectra. QDD, QDQ spectrometers.
Yad.Fiz. 39, 518 (1984); Sov.J.Nucl.Phys. 39, 326 (1984)
B.I.Gorbachev, A.I.Levon, O.F.Nemets, E.P.Saenko, N.M.Tkach
Nuclear g Factors and the Structure of Isomer 7- States in Isotopes 186,188Os and 196,198Hg
NUCLEAR REACTIONS 184,186W, 194,196Pt(α, 2n), E=27 MeV; measured γ(θ, H), γ(θ, H, t). 186,188Os, 196,198Hg deduced 7- isomer g, configuration.
Phys.Lett. 137B, 323 (1984)
R.Guigas, P.Blum, H.Koch, M.Meyer, H.Poth, U.Raich, B.Richter, G.Backenstoss, P.Pavlopoulos, L.Tauscher, L.Adiels, K.Fransson, A.Nilsson, M.Suffert, K.Zioutas
Strong Interaction Effects in Antiprotonic 6Li/7Li Atoms
ATOMIC PHYSICS 6,7Li(p-bar, X), E at 600 MeV/c; measured E X-ray, I X-ray; deduced strong interaction shifts, widths.
NUCLEAR REACTIONS 6,7Li(p-bar, X), E at 600 MeV/c; measured E X-ray, I X-ray; deduced strong interaction effects. Optical model comparison.
doi: 10.1016/0370-2693(84)91725-8
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., p.E29 (1984)
H.Langevin-Joliot, E.Gerlic, J.Guillot, J.van de Wiele, S.Y.van der Werf
Etats de Trous de Proton dans les Couches Interne et de Valence Observes par la Reaction 197Au(d, 3He)196Pt a 108 MeV
NUCLEAR REACTIONS 197Au(d, 3He), E=108 MeV; measured σ(θ), σ(E(3He)). 198Pt deduced levels, L, configuration.
ATOMKI Kozlem. 26, 87 (1984)
R.J.Liotta, C.Pomar
Multistep Shell-Model Method
NUCLEAR STRUCTURE 202,200,198,196,192,190Pb; calculated single particle energies. Multi-step shell model.
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
KVI Ann.Rept., 1983, p.23 (1984)
J.Penninga, W.H.A.Hesselink, A.Stolk, Z.Sujkowski, H.Verheul, M.J.A.de Voigt, A.Zemel
Level Structure Above the 12+ Isomers in 194,196Pb
RADIOACTIVITY 196Pb(EC) [from 198Hg(α, 6n), E=75 MeV]; measured γ(θ), γ(t). 196Pb deduced levels, isomer, J, π decay characteristics. Ge detectors.
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
Z.Phys. A317, 313 (1984)
P.Schuler, J.Recht, H.Wilzek, K.Hardt, C.Gunther, K.P.Blume, K.Euler, V.Kolschbach
Investigation of 196,198Pt and 202,204Hg with the (d, pnγ) Reaction
NUCLEAR REACTIONS 174Yb, 196,198Pt, 232Th(d, xnp), 174Yb, 196,198Pt, 232Th, 202,204Hg(d, np), E=25 MeV; measured Eγ, Iγ, I(ce), pγ-, γγ-coin. 196,198Pt, 202,204Hg deduced levels, J, π, yrast sequence, γ-branching, B(λ). Interacting boson model.
RCNP (Osaka), Ann.Rept., 1983, p.124 (1984)
T.Shibata
The Escape Probabilities Estimated Using an Exciton Model for the First Doorway States Produced by Various Reactions
NUCLEAR REACTIONS, ICPND 197Au(α, n), (α, 2n), (α, 3n), (α, 4n), (α, 5n), (α, 6n), (α, 7n), (α, 8n), (α, 9n), E=20-120 MeV; measured σ(E). 92Zr(α, α'n), E=109 MeV; measured σ(θα, Eα, En).
Phys.Rev.Lett. 52, 1974 (1984)
P.Van Duppen, E.Coenen, K.Deneffe, M.Huyse, K.Heyde, P.Van Isacker
Observation of Low-Lying J(π) = 0+ States in the Single-Closed-Shell Nuclei 192-198Pb
RADIOACTIVITY 192,194,196,198Bi(β+), (EC) [from Re(16O, X), E=110-180 MeV]; measured Eγ, Iγ, I(ce), E(X-ray), I(X-ray), γγ-, γX-ray-, (ce)γ-coin. 192,194,196,198Pb deduced evidence for low lying 0+ state, configuration.
doi: 10.1103/PhysRevLett.52.1974
ATOMKI Kozlem. 26, 54 (1984)
P.Van Duppen, E.Coenen, K.Deneffe, M.Huyse
Anomalous Low Lying 0+ State in the 198-192Pb Isotopes
RADIOACTIVITY 192Bi(α); 194Bi(α), (β+), (EC); 196,198Bi(β+), (EC) [from Re(16O, xn)]; measured Eγ, Iγ, I(ce), E(X-ray), I(X-ray), γγ-, γ(X-ray)-, (ce)γ-coin. 192,194,196,198Pb deduced levels, γ-branching, B(E2) ratios.
Phys.Rev. C30, 517 (1984)
M.Vergnes, G.Berrier-Ronsin, G.Rotbard, J.Vernotte, J.M.Maison, R.Bijker
Breaking of the Multi-j Supersymmetry Schemes in the 195Pt(d, p)196Pt Reaction
NUCLEAR REACTIONS 195Pt(d, p), E=25.2 MeV; measured σ(θ), σ(Ep); deduced supersymmetry breaking evidence. 196Pt levels deduced spectroscopic strengths. DWBA analysis.
Phys.Rev. C31, 653 (1985)
N.Blasi, M.N.Harakeh, W.A.Sterrenburg, S.Y.van der Werf
Two-Step Processes in the Population of the 2+2 State via the 197Au(d, 3He)196Pt Reaction
NUCLEAR REACTIONS 197Au(d, 3He), E=50 MeV; measured σ(E), σ(θ); deduced reaction mechanism. 196Pt levels deduced spectroscopic factors. DWBA, CCBA analyses.
Phys.Lett. 152B, 330 (1985)
W.T.A.Borghols, N.Blasi, R.Bijker, M.N.Harakeh, C.W.De Jager, J.B.van der Laan, H.de Vries, S.Y.van der Werf
Excitation of Hexadecapole Transitions in 196Pt via Electron Scattering and Their Interpretation in the Interacting Boson Approximation
NUCLEAR REACTIONS 196Pt(e, e'), E not given; measured form factors. 196Pt levels deduced transition densities, neutron, proton structure functions. Interacting boson approximations.
doi: 10.1016/0370-2693(85)90505-2
Phys.Lett. 157B, 353 (1985)
M.P.Fewell, G.J.Gyapong, R.H.Spear, M.T.Esat, A.M.Baxter, S.M.Burnett
The Quadrupole Moment of 196Pt - A Crucial Test of Nuclear Models
NUCLEAR REACTIONS 196Pt(16O, 16O'), E=55-61 MeV; 196Pt(12C, 12C'), E=41-56 MeV; measured Coulomb excitation, particle spectra. 196Pt level deduced B(E2), quadrupole moment. Bohr-Mottelson, O(6) interacting boson model limits.
doi: 10.1016/0370-2693(85)90379-X
Phys.Lett. 155B, 303 (1985)
K.Heyde, P.Van Isacker, R.F.Casten, J.L.Wood
A Shell-Model Interpretation of Intruder States and the Onset of Deformation in Even-Even Nuclei
NUCLEAR STRUCTURE 164,168,172,176,180,184,188,192,196,200,204,208Pb, 102,106,110,114,118,122,126,130Sn, 98,102,106,110,114,118Zr, 154,158,162,166,170,174,178,182,186,190Gd; calculated monople binding, intruder 0+ state energies; deduced intruder state mass dependence. Shell model.
doi: 10.1016/0370-2693(85)91575-8
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.
Hyperfine Interactions 22, 439 (1985)
M.Huyse, G.Brijs, P.De Bisschop, J.Gentens, E.Coenen, K.Deneffe, P.Van Duppen
Recent Developments at the Leuven Isotope Separator On Line
RADIOACTIVITY 104,105Sn(β+), (EC) [from 92Mo(20Ne, X), E=210 MeV]; measured Eγ, Iγ, E X-ray, I X-ray, γγ(t), γ(X-ray)(t). 104,105In deduced levels, γ-branching.
NUCLEAR REACTIONS Ni(32S, X)84Sr/83Sr/81Sr/84Rb/81Rb/80Rb/79Rb/78Rb/78mRb/77Rb/76Rb/75Rb/81Kr/81mKr/78Kr/75Kr/73Kr/77Br/77mBr/75Br/74mBr/74Br/73Br/72Br, E=280 MeV; 92Mo(20Ne, X)107In/106In/105In/104In/103In/102In/103Cd/102Cd/103Ag/102Ag, E=180 MeV; Re(16O, X)196Bi/195Bi/194Bi/193Bi/192Bi/195Pb/194Pb/193Pb/192Pb/191Pb/194Tl/193Tl/192Tl/191Tl, E=210 MeV; measured residual yields. Activation technique.
Nucl.Phys. A439, 189 (1985)
V.Kolschbach, P.Schuler, K.Hardt, D.Rosendaal, C.Gunther, K.Euler, R.Tolle, M.Marten-Tolle, P.Zeyen
On the Rotation-Aligned Coupling of the h11/2 Proton-Hole States in 191,193Au
NUCLEAR REACTIONS 191,193Ir, 194,196,198Pt(α, 4n), E=50 MeV; measured Eγ, Iγ, γ(θ, H), I(ce), (ce)γ-coin. 191Au deduced levels, J, π. 191,193Au deduced levels, T1/2, B(λ), g. 194,196,198Hg deduced levels T1/2, B(λ).
doi: 10.1016/0375-9474(85)90427-0
Nucl.Phys. A436, 221 (1985)
K.Miura, Y.Hiratate, T.Shoji, T.Suehiro, H.Yamaguchi, Y.Ishizaki
Ground-State Transition Strengths of the (p, t) Reactions for Nuclei with A=23-238
NUCLEAR REACTIONS 23Na, 24,26Mg, 27Al, 28,30Si, 35,37Cl, 40,44Ca, 46,48,50Ti, 51V, 54,56Fe, 58,60,62Ni, 63,65Cu, 64,66,68Zn, 76,78,80,82Se, 90,92,94,96Zr, 92,96,98,100Mo, 102,104Ru, 104,106,108,110Pd, 112,114,116Cd, 115In, 118,120,122,124Sn, 122,124,126,128,130Te, 136,138Ba, 140,142Ce, 144,146,148,150Nd, 158,160Gd, 165Ho, 168,170Er, 172,174,176Yb, 181Ta, 184,186W, 188,190,192Os, 191,193Ir, 194,196,198Pt, 197Au, 202,204Hg, 208Pb, 209Bi, 232Th, 238U(p, t), E=51.9 MeV, measured σ(θ). 21Na, 22,24Mg, 25Al, 26,28Si, 33,35Cl, 38,42Ca, 44,46,48Ti, 49V, 52,54Fe, 56,58,60Ni, 61,63Cu, 62,64,66Zn, 74,76,78,80Se, 88,90,92,94Zr, 90,94,96,98Mo, 100,102Ru, 102,104,106,108Pd, 110,112,114Cd, 113In, 116,118,120,122Sn, 120,122,124,126,128Te, 134,136Ba, 138,140Ce, 142,144,146,148Nd, 156,158Gd, 163Ho, 166,168Er, 170,172,174Yb, 179Ta, 182,184W, 186,188,190Os, 189,191Ir, 192,194,196Pt, 195Au, 200,202Hg, 206Pb, 207Bi, 230Th, 236U deduced systematic g.s. transition strength. Natural, enriched targets.
doi: 10.1016/0375-9474(85)90197-6
KVI Ann.Rept., 1984, p.33 (1985)
J.Pennings, W.H.A.Hesselink, H.Ho, J.van Klinken, H.J.Riezebos, A.Stolk, H.Verheul, M.J.A.de Voigt, A.Zemel
Shape Coexistence in Neutron Deficient Pb Isotopes
NUCLEAR REACTIONS 198Hg(α, 6n), E=75 MeV; measured γ-spectra, γ(θ), γ(K X-ray)-, γ(L X-ray)-coin. 196Pb deduced levels, J, π, γ-branching, T1/2, g. Ge, Si-Li detectors.
Z.Phys. A322, 83 (1985)
C.Stenzel, H.Grawe, H.Haas, H.-E.Mahnke, K.H.Maier
E2 Moments and g-Factors in Neutron Deficient Lead Isotopes
NUCLEAR REACTIONS 158,160Gd(36Ar, 4n), E=175 MeV; 156Gd(40Ar, 4n), E=185 MeV; measured Eγ, Iγ(t). 182W(16O, 4n), E=85 MeV; measured γ(θ, H, t). 190,192Pb deduced isomer T1/2, B(E2), quadrupole moment. 194Pb deduced isomer T1/2, quadrupole moment, g, B(E2). 196,198Hg(α, xn), E=60 MeV; analyzed data. 195,196,197,198,199,200Pb levels deduced g, T1/2, configuration. Two-quasiparticle Tamm-Dancoff calculation, surface delta interaction.
Phys.Lett. 154B, 354 (1985)
P.Van Duppen, E.Coenen, K.Deneffe, M.Huyse, J.L.Wood
Low-Lying J(π) = 0+ States in 190,192Pb Populated in the α-Decay of 194,196Po
RADIOACTIVITY 194,196Po(α) [from W(20Ne, X), E=225 MeV]; measured Eγ, Iγ. 192,194Pb deduced 0+ state.
doi: 10.1016/0370-2693(85)90408-3
JYFL Ann.Rept., 1984-85, p.70 (1985)
E.Verho, R.Julin, J.Kantele, J.Kumpulainen, M.Luontama, A.Passoja
Decay of 0+ in 196Hg
NUCLEAR REACTIONS 197Au(p, 2n), E=12 MeV; measured Eγ, Iγ, I(ce), γγ-coin. 196Hg deduced levels, γ-multipolarity.
Yad.Fiz. 42, 1082 (1985)
M.V.Zverev, E.E.Sapershtein
Some Questions of the Self-Consistent Theory of Pairing in Atomic Nuclei. The Lead Region and the ' Magic ± 2 Particles ' Nuclei
NUCLEAR STRUCTURE 208,204,207Pb, 209Bi; calculated charge radii differences. 201,197,193,211,205Pb; calculated single particle level energies. 188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated neutron separation energies; deduced nucleon stability boundaries. Self-consistent theory of pairing.
Phys.Rev. C33, 321 (1986)
A.Ansari
Shape Transition in Os and Pt Isotopes
NUCLEAR STRUCTURE 186,188,190,192,194,196Os, 186,188,190,192,194,196Pt; calculated pairing gaps, β2, β4; deduced shape transition behavior. Self-consistent HFB method.
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
Phys.Rev. C33, 1785 (1986)
D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi-Alvarez, R.Zannoni, M.de Poli
g Factors of the Lowest (5/2)+ and (7/2)+ States in 197Au and Calibration of the Transient Magnetic Field in Gd
NUCLEAR REACTIONS 197Au, 194,196Pt(63Cu, 63Cu'), E=180 MeV; 194,196Pt, 184,186W(58Ni, 58Ni'), E=150 MeV; measured γ(θ, H) in thin polarized Gd, Coulomb excitation; deduced transition field strengths. 197Au levels deduced g.
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.
Phys.Lett. 167B, 6 (1986)
M.P.Fewell
Plantinum-196 as a U(5) Nucleus
NUCLEAR STRUCTURE 196Pt; calculated levels, B(E2); deduced U(5) limit validity. Interacting boson model.
doi: 10.1016/0370-2693(86)90534-4
Nucl.Phys. A458, 165 (1986)
G.J.Gyapong, R.H.Spear, M.T.Esat, M.P.Fewell, A.M.Baxter, S.M.Burnett
Electric Quadrupole Moments of the First Excited States of 194Pt, 196Pt and 198Pt
NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14-15.6 MeV; 196Pt(α, α'), E=16.8-18.6 MeV; 194,196,198Pt(12C, 12C'), E=41-45 MeV; 194,196,198Pt(16O, 16O'), E=55-63 MeV; measured Coulomb excitation probabilities. 194,196,198Pt levels deduced B(E2), quadrupole moments. Enriched targets.
doi: 10.1016/0375-9474(86)90289-7
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., p.E26 (1986)
J.M.Lagrange, M.Pautrat, J.Vanhorenbeeck, J.S.Dionisio, Ch.Vieu
Probabilites de Transition B(E2;12+ → 10+) et B(E2;(33/2)+ → (29/2)+) dans les Isotopes de Plomb Deficients en Neutrons
NUCLEAR REACTIONS 184W(16O, 4n), (16O, 5n), (16O, 6n), E=98 MeV; measured γ(ce)-coin. 196,195,194Pb deduced isomers, γ-branching, configuration, B(E2).
KVI Ann.Rept., 1985, p.14 (1986)
G.W.R.Leibbrandt, S.Brandenburg, R.De Leo, L.P.Ekstrom, S.Grafeuille, P.Grasdijk, M.N.Harakeh, J.Janecke, H.J.Hofmann, M.Pignanelli, T.Poelhekken, H.J.Riezebos, J.M.Schippers, S.Y.van der Werf
Total-, Escape- and Spreading Widths of the IAS in Even Au Isotopes and 181W
NUCLEAR REACTIONS 190,192,194,196,198Pt, 181Ta(3He, t), E=60 MeV; measured σ(Et, θ=0°), Eγ, Iγ. 192,194,196,198Au, 181W deduced IAS, escape, spreading widths.
J.Phys.(London) G12, 1285 (1986)
M.Pautrat, J.M.Lagrange, J.S.Dionisio, Ch.Vieu, J.Vanhorenbeeck
Direct Measurement of the Isomeric 12+ → 10+ and (33/2)+ → (29/2)+ Transition Energies in the Isotopes 194Pb to 197Pb
NUCLEAR REACTIONS 184W(16O, 4n), (16O, 5n), (16O, 6n), E=98 MeV; measured Eγ, Iγ, I(ce), γγ(t), γ(ce)-coin. 197,194,195,196Pb deduced isomer decay, T1/2, ICC transition energies, B(λ). Ge(Li), Si-Li detectors, enriched target. Tamm-Dancoff approximation, other data input.
doi: 10.1088/0305-4616/12/11/016
Phys.Scr. 34, 378 (1986)
M.Pautrat, J.M.Lagrange, A.Virdis, J.S.Dionisio, Ch.Vieu, J.Vanhorenbeeck
Electron Measurements in the 194,195,196Pb Isotopes
NUCLEAR REACTIONS 184W(16O, 4n), (16O, 5n), (16O, 6n), E=100 MeV; measured Eγ, Iγ, I(ce), σ(θ), σ(E), γγ-, γ(ce)-coin, γ(θ). 194,195,196Pb deduced levels, γ-multipolarity, T1/2, ICC. Ge(Li) detector. TDA calculations.
Amer.Chem.Soc.Symposium Ser.324 on Nuclei Off the Line of Stability, Chicago, p.252 (1985), R.A.Meyer, D.S.Brenner Eds., Washington, p.252 (1986)
J.Penninga, W.H.A.Hesselink, A.Stolk, H.Verheul, J.K.Ho, J.van Klinken, H.J.Riezebos, M.J.A.de Voigt, A.Zemel
Shape Coexistence in Neutron-Deficient Pb Isotopes
NUCLEAR REACTIONS 188Hg(α, 6n), (α, 8n), E=75 MeV; measured γγ-, γ(ce)-coin, γ(θ). 188Os(12C, 4n), E not given; measured γγ-coin, γγ(t). 196Pb deduced levels, J, π, T1/2, isomer g, configuration, shape features. 194Pb deduced transitions.
KVI Ann.Rept., 1985, p.33 (1986)
J.Penninga, A.Balanda, W.H.A.Hesselink, J.van Klinken, H.J.Riezebos, A.Stolk, H.Verheul, M.J.A.de Voigt
Shape Coexistence and Collective Excitations in 194,196Pb
NUCLEAR REACTIONS 198Hg(α, 6n), 188Os(12C, 4n), E not given; analyzed γγ-coin data. 196Pb deduced isomer, T1/2, decay intruder characteristics, rotational band. 194Pb deduced isomer, J, π, associated rotational band. Data input from γγ-, (ce)γ-coin.
Nucl.Phys. A449, 579 (1986)
J.J.Van Ruyven, J.Penninga, W.H.A.Hesselink, P.Van Nes, K.Allaart, E.J.Hengveld, H.Verheul, M.J.A.De Voigt, Z.Sujkowski, J.Blomqvist
High-Spin Neutron Excitations in Neutron-Deficient Even-Mass Pb Isotopes
NUCLEAR REACTIONS, ICPND 188Os(12C, 3n), (12C, 4n), (12C, 5n), (12C, 6n), (12C, 7n), E=70-110 MeV; measured σ(E), Eγ, Iγ(t), γγ(t), sum spectra, I(ce), σ(Eγ, θ); 198Hg(α, 6n), E=75 MeV; measured Eγ, Iγ(t), γγ(t), sum spectra, I(ce), σ(Eγ, θ). 194,196Pb deduced levels, J, π, γ-branching, T1/2, B(λ). Enriched targets, Ge(Li), Ge, Si(Li) detectors, sum spectrometer, mini-orange filter.
NUCLEAR STRUCTURE 194,196Pb; calculated levels, B(λ). 190,192,194,196,198,200,202,204,206Pb; calculated levels, energy differences. One-, two-broken-pair models.
doi: 10.1016/0375-9474(86)90235-6
JYFL Ann.Rept., 1986, p.59 (1986)
E.Verho, R.Julin, J.Kantele, J.Kumpulainen, A.Passoja
Low-Lying Levels in 196Hg
NUCLEAR REACTIONS 197Au(p, 2n), E=12 MeV; measured I(ce), γγ-coin. 196Hg deduced levels, J, π, γ-branching.
Chin.J.Nucl.Phys. 8, 120 (1986)
Zhang Weimin
Microscopic Study of Nuclear Collective States (II) The Microscopic Calculation of Single Boson Energy Spectrum and Structure of Fermion Pairs Cluster Operators
NUCLEAR STRUCTURE 196,198,200,202,204,206Pb; calculated levels. Shell model, Boson expansion method.
At.Energ. 62, 59 (1987); Sov.At.Energy 62, 81 (1987)
S.V.Bakhmutkin, A.I.Bogdanov, V.G.Bogdanov, N.P.Kocherov, V.I.Kucheryuk, A.A.Nosov, A.A.Rimsky-Korsakov
Energy Spectra of Neutrons on the Surface of a Cylindrical Lead Target Irradiated with 1-GeV Protons
NUCLEAR REACTIONS, ICPND Pb(p, xn), E=1 GeV; measured neutron spectra. Activation technique. 197Au(n, γ), E=0.1-1 MeV; 197Au(n, 2n), E=9.50 MeV; 197Au(n, 3n), E=15-50 MeV; 197Au(n, 4n), E=25-50 MeV; measured σ(E). 59Co(n, 2n), E ≤ 50 MeV; 59Co(p, np), E ≈ 12.5-50 MeV; 59Co(n, 3n), E ≈ 25-50 MeV; 59Co(p, 2np), E ≈ 25-50 MeV; measured residual production σ(E). Activation technique.
Phys.Rev. C36, 1286 (1987)
B.L.Berman, R.E.Pywell, S.S.Dietrich, M.N.Thompson, K.G.McNeill, J.W.Jury
Absolute Photoneutron Cross Sections for Zr, I, Pr, Au, and Pb
NUCLEAR REACTIONS Zr, 127I, 141Pr, 197Au, Pb(γ, n), E ≈ 12-17 MeV; Zr, 127I, 141Pr, 197Au, Pb(γ, 2n), E=threshold-17 MeV; measured absolute photonucleon σ(E).
Phys.Lett. 186B, 285 (1987)
W.Boeglin, P.Egelhof, I.Sick, J.M.Cavedon, B.Frois, D.Goutte, X.H.Phan, S.K.Platchkov, S.Williamson, M.Girod
Electron Scattering from Transitional Nuclei
NUCLEAR REACTIONS 188,190,192Os, 194,196Pt(e, e), (e, e'), E=200, 500 MeV; measured σ(θ), transition charge densities. HFB calculations.
doi: 10.1016/0370-2693(87)90296-6
At.Energ. 62, 236 (1987); Sov.At.Energy 62, 277 (1987)
M.G.Davydov, V.G.Magera, A.V.Trukhov
Isomeric Ratios of the Yields (Cross Sections) of Photonuclear Reactions
NUCLEAR REACTIONS 27Al, 45Sc, 46Ti, 55Mn, 54Fe, 59Co, 60Ni, 71Ga, 76Ge, 74,82Se, 81Br, 85Rb, 86,88Sr, 89Y, 90Zr, 92,94,96,98,100Mo, 102Ru, 103Rh, 108,110Pd, 107Ag, 116Cd, 113,115In, 112,118,120,124Sn, 121Sb, 120Te, 136Xe, 138Ba, 138,140Ce, 142,144Nd, 167,168Er, 179,180Hf, 181Ta, 182,183,184W, 198Pt, 197Au, 198Hg, 208Pb(γ, n), (γ, p), E=12.5-150 MeV; analyzed photonuclear reaction product isomeric yield ratios.
Phys.Rev. C35, 942 (1987)
J.P.Delaroche, F.S.Dietrich
Coupled-Channel Description of Inelastic Scattering from Soft Nuclei
NUCLEAR REACTIONS 196Pt(polarized p, p), (polarized p, p'), E=35 MeV; calculated σ(θ), analyzing power vs θ. Many-body collective wave functions, coupled-channels description.
Hyperfine Interactions 34, 443 (1987)
G.de Doncker, J.van Cauteren, M.Rots
Hyperfine Interaction in Ni79Mn21 and Ni76Mn24
RADIOACTIVITY 111In(EC); measured γγ(θ, H); deduced 111Cd hyperfine field vs temperature in NiMn alloys.
Nucl.Phys. A466, 189 (1987)
K.Heyde, J.Jolie, J.Moreau, J.Ryckebusch, M.Waroquier, P.van Duppen, M.Huyse, J.L.Wood
A Shell-Model Description of 0+ Intruder States in Even-Even Nuclei
NUCLEAR STRUCTURE 106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated 0+ intruder state energies. 190,192,194,196,198,200,202,204,206,208Pb; calculated intruder state energies, monopole, quadupole binding energy corrections. 90,92,94,96,98,100Zr; calculated 2p-2h intruder state energies, pairing energy contributions. 96,98,100,102,104Mo; calculated monopole energy correction term. 146,148,150,152,154,156,158,160Gd; calculated intruder state energies. Shell model.
doi: 10.1016/0375-9474(87)90439-8
Nucl.Phys. A462, 221 (1987)
H.Langevin-Joliot, E.Gerlic, J.Guillot, J.Van De Wiele, S.Y.Van Der Werf, N.Blasi
Proton Hole Response Function on 196Pt and 197Au Transitional Target Nuclei up to High Excitation Energy
NUCLEAR REACTIONS 196Pt, 197Au(d, 3He), E=108.4 MeV; 197Au(d, 3He), E=50 MeV; measured σ(E(x), θ). 195Pt deduced levels, valence, inner-proton hole strength functions, spectroscopic factors, hole-state Γ, L. Core quasiparticle coupling model, DWBA analysis.
doi: 10.1016/0375-9474(87)90546-X
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., pE60 (1987)
H.Langevin-Joliot, E.Gerlic, J.Guillot, J.van de Wiele, S.Y.van der Werf
Fonctions de Response a un Trou de Proton dans les Noyaux Cibles 208Pb, 197Au et 120Sn
NUCLEAR REACTIONS 208Pb, 197Au, 120Sn(d, 3He), E=108 MeV; analyzed data. 196Pt, 207Tl deduced hole strength distribution.
Contrib.Proc. 5th Int.Conf.Nuclei Far from Stability, Rosseau Lake, Canada, C12 (1987)
J.K.P.Lee, G.Savard, J.E.Crawford, G.Thekkadath, H.T.Duong, J.Pinard, S.Liberman, F.Le Blanc, P.Kilcher, J.Obert, J.Oms, J.C.Putaux, B.Roussiere, J.Sauvage, and the ISOCELE Collaboration
Resonant Ionization Spectroscopy of Laser-Desorbed Gold Isotopes
RADIOACTIVITY 186,187,190,192,194,196Au; measured hfs, isotope shifts; deduced μ, rms charge radii.
Z.Phys. D7, 193 (1987)
W.Neu, G.Passler, G.Sawatzky, R.Winkler, H.-J.Kluge
Isotope Shift and Hyperfine Structure of Stable Platinum Isotopes
NUCLEAR MOMENTS 190,192,194,195,196,198Pt; measured hfs, isotope shifts; deduced hyperfine, other parameters, King plot. 190,192,194,195,196,198Pt deduced relative nuclear charge radius parameter. Laser fluorescence spectroscopy.
Phys.Rev. C36, 2072 (1987)
S.Ohya, S.Ohtake, K.Nishimura, N.Mutsuro
Nuclear Orientation and Nuclear Magnetic Resonance of 196Au in Fe
RADIOACTIVITY 196Au(EC), (β+), (β-) [from 196Pt(α, 3np), E=65 MeV]; measured I(γ)(θ, T, H), NMR, oriented nuclei in Fe; deduced μ, spectroscopic quadrupole moment.
Nucl.Phys. A471, 535 (1987)
J.Penninga, W.H.A.Hesselink, A.Balanda, A.Stolk, H.Verheul, J.van Klinken, H.J.Riezebos, M.J.A. de Voigt
Proton Particle-Hole States and Collective Excitations in 196Pb
NUCLEAR REACTIONS 198Hg(α, 6n), E=75 MeV; measured E(γ), I(γ)(t), γγ(θ), I(ce), γ(ce)-coin. 196Pb deduced levels, isomer J, π, T1/2, γ-branching, g. Enriched target, Ge, Si-Li detectors, mini-orange filter.
doi: 10.1016/0375-9474(87)90098-4
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), T1/2, β2, β2/β2(sp), EWSR, intrinsic quadrupole moments.
doi: 10.1016/0092-640X(87)90016-7
Nucl.Phys. A474, 155 (1987)
H.Sagawa, A.Arima, O.Scholten
Nuclear Compression Modulus and Isotope Shifts of Pb Nuclei
NUCLEAR STRUCTURE 196,197,198,199,200,201,202,203,204,205,206,207,209,210,211,212,213,214,215Pb; calculated isotope shifts, B(E2) sum values. Perturbative method, giant resonance effects.
doi: 10.1016/0375-9474(87)90198-9
Phys.Rev. C35, 1861 (1987)
P.Van Duppen, E.Coenen, K.Deneffe, M.Huyse, J.L.Wood
β+/Electron-Capture Decay of 192,194,196,198,200Bi: Experimental evidence for low lying O+ states
NUCLEAR STRUCTURE 192,194,196,198,200Pb; calculated levels, B(λ) ratios, intruder states, mixing. One broken pair model.
RADIOACTIVITY 192,194,196,198,200Bi(β+), (EC) [from Re(16O, xn), E < 210 MeV; 181Ta(20Ne, xn), E < 190 MeV]; measured E X-ray, I X-ray, Eγ, Iγ, γγ-, γ(ce)-coin, I(ce), γγ(t), γ(ce)(t); deduced T1/2. 192,194,196,198,200Pb deduced levels, J, π, ICC, configuration, B(E0)/B(E2), γ-branching. Ge, Si-Li detectors.
Contrib.Proc. 5th Int.Conf.Nuclei Far from Stability, Rosseau Lake, Canada, C11 (1987)
K.Wallmeroth, G.Bollen, M.J.G.Borge, J.Campos, A.Dohn, P.Egelhof, H.-J.Kluge, U.Kronert, R.B.Moore, A.Rodriguez, A.Venugopalan, J.Wood, and the ISOLDE Collaboration
Nuclear Shape-Transition in Neutron-Deficient Gold Isotopes
RADIOACTIVITY 185,186,187,188,189,190,191,192,193,194,195,196Au; measured hfs; deduced μ, rms charge radii, shape transitions. On-line resonance ionization mass spectroscopy.
Phys.Lett. 185B, 299 (1987)
D.Zawischa, U.Regge, R.Stapel
Effective Interaction and the Staggering of Nuclear Charge Radii
NUCLEAR MOMENTS 112,114,115,116,117,118,119,122,124Sn, 198,199,200,201,202,204Hg, 206,207,208Pb; calculated isotope shifts; deduced charge radii odd-even staggering. HFB approximation, separable four-body, three-body contact forces.
RADIOACTIVITY 110,111,113,117m,121,121m,123,125Sn, 203,205,206Hg, 196,197,198,199,200,201,202,203,205,209,210,211,212,213Pb; calculated isotope shifts; deduced charge radii odd-even staggering. HFB approximation, separable four-body, three-body contact forces.
doi: 10.1016/0370-2693(87)91003-3
Phys.Rev. C37, 1667 (1988)
B.Al-Bataina, J.Janecke
Reduced Alpha Widths for Nuclei with N ≥ 84, Z ≤ 84
NUCLEAR STRUCTURE Z=60-84; analyzed α-decay width data. 142Ce, 149Sm, 156Dy, 162,164Er, 168Yb, 176,174Hf, 180W, 184,186,188Os, 192Pt, 196Hg, 204Pb; calculated α-decay T1/2.
Phys.Rev. C38, 493 (1988)
G.E.Arenas Peris, P.Federman
Weak-Coupling Description of Intruder States
NUCLEAR STRUCTURE 185,187,189,191,193,195,197,199,201,203Au, 185,187,189,191,193,195,197,199,201Tl, 199,201,203,205,207,209Bi, 209,211At, 184,186,188,196,198Hg, 190,192,194,196,198,200,202,204,206,208Pb, 198,200,202,204,206,208Po; calculated levels. Weak coupling, intruder states.
Phys.Rev. C38, 1392 (1988)
A.B.Balantekin, B.R.Barrett, P.Halse
β Vibrations in the O(6) Limit of the Proton-Neutron Interacting Boson Model
NUCLEAR STRUCTURE 196Pt, 134Ba; calculated (β)-vibrational state energy. Proton-neutron interacting boson model, O(6) limit.
Univ.Paris, Inst.Phys.Nucl., 1987 Ann.Rept., p.E11 (1988)
G.Berrier-Ronsin, G.Rotbard, M.Vergnes, J.Vernotte, J.M.Maison, S.Fortier
Structure of Hg Isotopes via the (p, t) Reaction
NUCLEAR REACTIONS 196,197,198,199,200,202,204Hg(p, t), E=25 MeV; measured σ(θ). 198,199,200,202,201,204,206Hg deduced levels, J, π.
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, 152,154,156,158,160Gd, 156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 160,162,164,166,168,170,172,174,176Yb, 166,168,170,172,174,176,178,180Hf, 180,182,184,186W, 182,184,186,188,190,192Os, 190,192,194,196Pt, 230,232,234Th, 232,234,236,238U, 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
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
Nucl.Phys. A477, 399 (1988)
W.Boeglin, P.Egelhof, I.Sick, J.M.Cavedon, B.Frois, D.Goutte, V.Meot, P.Leconte, X.H.Phan, S.K.Platchkov, S.Williamson, M.Girod
Electron Scattering from Transitional Nuclei
NUCLEAR REACTIONS 188,190,192Os, 194,196Pt(e, e'), E=200, 500 MeV; measured σ(E(e')), σ(θ). 190,188,192Os, 194,196Pt levels deduced transition charge densities.
doi: 10.1016/0375-9474(88)90349-1
Z.Phys. D10, 1 (1988)
S.Bouazza, J.Bauche
Hyperfine Structure in Low-Lying Levels of PtII, AuII and BiII
NUCLEAR MOMENTS 190,192,194,195,196,198Pt, 197Au, 209Bi; measured hfs, isotope shifts for Pt; deduced hyperfine constants, parameters. Fabry-Perot spectrometry.
J.Phys.(London) G14, 1139 (1988)
M.C.A.Campos, E.Wolynec, M.N.Martins
M1 Strength in 197Au
NUCLEAR REACTIONS 197Au(e, n), E=9-23 MeV; measured σ(E). 197Au deduced E2 and M1 transition strengths. Virtual photon analysis.
doi: 10.1088/0305-4616/14/8/016
Phys.Rev. C38, 1619 (1988)
P.D.Cottle, V.Hnizdo, R.J.Philpott, K.A.Stuckey, K.W.Kemper, J.A.Carr
Negative Parity States of Even-A Pt Isotopes from Proton Inelastic Scattering
NUCLEAR REACTIONS 194,196,198Pt(p, p'), E=35 MeV; analyzed σ(θ); deduced 3- state systematics in Os, Pt, Hg region. 194,196,198Pt level deduced β3, B(E3).
Phys.Rev. C38, 2843 (1988)
P.D.Cottle, K.A.Stuckey, K.W.Kemper
Fragmentation of Octupole Strength in Even-A Pt Isotopes
NUCLEAR REACTIONS 198Pt(p, p'γ), E=12 MeV; 194,198,196Pt(p, p'), E=35 MeV; analyzed σ(θ). 194,196,198Pt deduced octupole strength fragmentation.
Aust.J.Phys. 41, 37 (1988)
M.P.Fewell, G.J.Gyapong, R.H.Spear
Coulomb Excitation of the 41+ States of 194,196,198Pt
NUCLEAR REACTIONS 194,196Pt(α, α'), E=14.199-15.599; 198Pt(α, α'), E=15.599 MeV; 194,198Pt(12C, 12C'), E=40.998-49.998 MeV; 196Pt(12C, 12C'), E=40.985-55.996 MeV; 194Pt(16O, 16O'), E=54.998-62.998 MeV; 196Pt(16O, 16O'), E=54.993-60.994 MeV; 198Pt(16O, 16O'), E=56.997-62.998 MeV; measured Coulomb excitation probability. 194,196,198Pt levels deduced E2, E4 transition matrix elements, deformation parameters.
Phys.Rev.Lett. 61, 2424 (1988)
M.Gai
Local Deviations from the Grodzins Systematics: Enhanced Collectivity in the Transitional Ra-Th Nuclei
NUCLEAR STRUCTURE 192,194,196Pt, 196,198,200,202,204Hg, 204,206,210Pb, 218,222,224,226,228Ra, 222,226,228,230,232,234Th, 230,232,234,236,238U, 238,240,242,244Pu, 244,246,250Cm; analyzed isoscalar quadrupole transition EWSR, two-neutron separation energy systematics; deduced ground, deformed state mixing.
doi: 10.1103/PhysRevLett.61.2424
Nucl.Phys. A484, 275 (1988)
K.Heyde, J.Ryckebusch, M.Waroquier, J.L.Wood
Intruder States in Odd-Mass and Odd-Odd Nuclei
NUCLEAR STRUCTURE 190,192,194,196,198,200,202,204,206,208Pb, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated pairing energies; 111,113,115,117,119,121In, 113,115,117,119,121,123,125,127Sb; calculated intruder state energies. N=49, 50, 51, 81, 82, 83; calculated 1particle-2 hole state energies. Shell model.
doi: 10.1016/0375-9474(88)90073-5
Phys.Rev. C37, 1787 (1988)
S.E.Hicks, M.T.McEllistrem
Energy Dependence of the Mean-Field Potential for Neutron Scattering from 190,192Os and 194,196Pt
NUCLEAR REACTIONS 190,192Os, 194,196Pt(n, n'), E ≤ 10 MeV; analyzed σ(E, θ), σ; deduced model parameter energy dependence. Coupled-channels method plus dispersion relation.
Phys.Lett. 201B, 293 (1988)
M.Huyse, E.Coenen, K.Deneffe, P.van Duppen, K.Heyde, J.van Maldeghem
Intruder States in Odd-Odd Tl Nuclei: The completion of a unique set of intruder systematics
RADIOACTIVITY 190,192,194Bi(α) [from Re(16O, xn), E<180 MeV; 181Ta(20Ne, xn), E<230 MeV]; measured Eα, Iα, T1/2. 186,188,190Tl deduced levels, possible J, π, intruder state systematics.
doi: 10.1016/0370-2693(88)91142-2
Phys.Rev. C38, 2985 (1988)
J.K.P.Lee, G.Savard, J.E.Crawford, G.Thekkadath, H.T.Duong, J.Pinard, S.Liberman, F.Le Blanc, P.Kilcher, J.Obert, J.Oms, J.C.Putaux, B.Roussiere, J.Sauvage
Charge-Radius Changes in Even-A Platinum Nuclei
NUCLEAR MOMENTS 190,192,194,196,198Pt; measured isotopic shifts, atomic transition; deduced rms charge radii.
RADIOACTIVITY 186,188Pt; measured isotopic shifts, atomic transition; deduced rms charge radii.
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.
J.Phys.(London) G14, 931 (1988)
N.L.Singh, A.V.Mohan Rao, S.Mukherjee, R.Upadhyay, R.K.Jain, S.K.Bose, L.Chaturvedi, J.Rama Rao
Alpha-Induced Reactions on Gold
NUCLEAR REACTIONS, ICPND 197Au(α, n), (α, 2n), (α, 3n), (α, n2p), (α, nα), (α, 3nα), E=threshold-75 MeV; measured σ(E). Hybrid model.
doi: 10.1088/0305-4616/14/7/011
Nucl.Instrum.Methods Phys.Res. A271, 546 (1988)
Y.Uwamino, T.Ohkubo, A.Torii, T.Nakamura
Semi-Monoenergetic Neutron Field for Activation Experiments up to 40 MeV
NUCLEAR REACTIONS 27Al(n, α), 197Au(n, 2n), (n, 4n), E=threshold-40 MeV; measured σ(E), σ(En); deduced reaction rates. Activation technique.
doi: 10.1016/0168-9002(88)90318-X
Phys.Rev. C38, 414 (1988)
J.Vanthournout, H.De Meyer, G.Vanden Berghe
Symmetry-Preserving Higher-Order Terms in the O(6) Limit of the Interacting Boson Model
NUCLEAR STRUCTURE 196Pt; calculated levels, B(λ). Interacting boson model, O(6) limit.
At.Data Nucl.Data Tables 39, 281 (1988)
A.H.Wapstra, G.Audi, R.Hoekstra
Atomic Masses from (Mainly) Experimental Data
NUCLEAR STRUCTURE A=72-212; analyzed data; deduced masses.
ATOMIC MASSES A=72-212; analyzed data; deduced masses.
doi: 10.1016/0092-640X(88)90030-7
Hyperfine Interactions 43, 321 (1988)
E.F.Zganjar, J.L.Wood
Shape Coexistence and Intruder States: The Z = 82 region
NUCLEAR STRUCTURE 185,187,189,191,193,195Au, 182,184,186,188,190,192,194,196,198Hg, 176,178,180,182,184,186,188,190,192,194,196Pt; analyzed level systematics; deduced intruder state, shape coexistence phenomena.
Z.Phys. A334, 269 (1989)
R.Bengtsson, W.Nazarewicz
Shape Coexistence in the Neutron Deficient Pb Isotopes and the Configuration-Constrained Shell Correction Approach
NUCLEAR STRUCTURE 185,187,189,191,193,195,197,199,201Tl, 186,188,190,192,194,196,198,200,202,204,206Pb; calculated level relative excitation energy. 186,196,202Pb; calculated potential energy surfaces. 196Pb; calculated intruder states. Configuration-constrained shell correction method.
Nucl.Phys. A500, 308 (1989)
P.Bonche, S.J.Krieger, P.Quentin, M.S.Weiss, J.Meyer, M.Meyer, N.Redon, H.Flocard, P.-H.Heenen
Superdeformation and Shape Isomerism at Zero Spin
NUCLEAR STRUCTURE 186,196,194,192,190,188,186,202,210Os, 200,198,196,194,192,190,188,186Pt, 194,202,210,218Hg; calculated Hartree-Fock energies, energy surfaces. 192,194,196,198,200,202,204,206,208,210,212,214,216,218Hg; calculated secondary minima deformations. 194,196,198Pt; calculated axial deformation energies. 66,68Ni, 190,192Pt, 206,208,210Os, 194,196,214Hg; deduced possible superdeformation effects. Microscopic Hartree-Fock plus BCS.
doi: 10.1016/0375-9474(89)90426-0
JINR-E1-89-481 (1989)
C.Damdinsuren, V.I.Ilyushchenko, P.Kozma, D.Chultem
Yields of Radionuclides Formed in the Interaction of 3.65 AGeV 12C-Ions and Protons with (nat)Pb
NUCLEAR REACTIONS Pb(p, X), (12C, X)24Na/28Mg/41Ar/43K/44mSc/46Sc/48Sc/54Mn/59Fe/57Ni/72As/73Se/76Br/77Br/81Rb/82mRb/84Rb/92Sr/86Y/87mY/86Zr/90Nb/96Nb/93mMo/99Mo/93Tc/94Tc/95Tc/96Tc/103Ru/112Pd/111In/122Sb/124Sb/119Te/119mTe/121Te/121mTe/123mTe/131mTe/121I/123I/125Xe/127Xe/127Cs/128Ba/131Ba/132La/132Ce/135Ce/139mNd/145Eu/147Gd/149Gd/149Tb/151Tb/152Tb/155Dy/157Dy/158Er/161Er/171Er/166Yb/169Yb/170Hf/171Hf/173Hf/175Hf/175Ta/176Ta/177W/181Re/182Re/184Re/190mRe/182Os/183mOs/184Ir/186Ir/186mIr/186Pt/192Au/198Au/200mAu/192Hg/193mHg/197mHg/203Hg/196Tl/196mTl/198Tl/198mTl/199Tl/200Tl/201Tl/202Tl/198Pb/200Pb/201Pb/202mPb/203Pb/202Bi/203Bi/204Bi/206Bi/207Bi/204Po/206Po, E=3.65 GeV/nucleon; measured residual independent, cumulative yields, 119,121Te, 196,198Tl isomeric σ ratios. Activation technique.
Phys.Lett. 226B, 27 (1989)
P.Dendooven, P.Decrock, M.Huyse, G.Reusen, P.Van Duppen, J.Wauters
Life Time Measurements of 0+ Intruder States in 190,192,194Pb
RADIOACTIVITY 194,196,198Po(α) [from 182W(20Ne, xn), E=240 MeV]; measured Eα, Iα, α(ce)-coin, α(ce)(t). 190,192,194Pb deduced intruder state T1/2, level mixing.
doi: 10.1016/0370-2693(89)90282-7
Phys.Scr. 39, 50 (1989)
J.B.Gupta, S.Sharma
Interband B(E2) Ratios in the Rigid Triaxial Model, a Review
NUCLEAR STRUCTURE 146,148,150Nd, 148,150,152,154,156Sm, 150,152,154,156,158,160Gd, 154,156,158,160,162,164Dy, 156,158,160,164,166,168,170Er, 158,164,166,168,170,172,174,176,178Yb, 166,168,170,172,174,176,178,180Hf, 170Er, 178,180,182,184,186W, 178,180,182,184,186,188,190,192,194Os, 180,182,184,186,188,190,192,194,196Pt; analyzed B(E2); deduced asymmetry parameter (γ0). Rigid triaxial model.
Nucl.Instrum.Methods Phys.Res. B40/41, 429 (1989)
J.H.Hamilton
Shapes and Structures of Exotic Nuclei
NUCLEAR STRUCTURE A=80-100; 182,184,186,188,190,192,196,198Hg; analyzed band systematics; deduced shape features.
doi: 10.1016/0168-583X(89)91013-6
Ann.Phys.(New York) 192, 133 (1989)
F.Iachello
The Role of Dynamic Symmetries and Supersymmetries in Nuclear Physics
NUCLEAR STRUCTURE 110Cd, 156Gd, 196Pt; calculated levels; deduced dynamical symmetry role. 190Os, 191Ir; calculated levels; deduced dynamical supersymmetry role. Dynamic symmetries, supersymmetries.
doi: 10.1016/0003-4916(89)90122-X
Phys.Rev. C39, 1142 (1989)
C.S.Lim, R.H.Spear, W.J.Vermeer, M.P.Fewell
Possible Discontinuity in Octupole Behavior in the Pt-Hg Region
NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14.6 MeV; 194,196,198Pt(12C, 12C'), E=43 MeV; 194,196,198Pt(7Li, 7Li'), E not given; measured particle spectra following Coulomb excitation. 194,196,198Pt levels deduced B(λ).
GSI-89-1, p.33 (1989)
R.Menges, U.Dinger, G.Huber, S.Schroder, S.Dutta, R.Kirchner, O.Klepper, T.Kuhl, D.Marx, G.Sprouse
Collinear Laser Spectroscopy of Neutron Deficient Thallium Isotopes
RADIOACTIVITY 188,190,192,194,196,198,200,202,204Tl [from W(16O, xnp)]; measured hfs, isotope shifts; deduced μ, rms charge radii. Collinear laser spectroscopy.
GSI-89-06 (1989)
R.Menges
Kollineare Laserspektroskopie an Radioaktiven Neutronenarmen Blei-und Thalliumisotopen
RADIOACTIVITY 190,191,192,193,194,195,196,197Pb [from W(16O, xn)]; 186,187,188,190,191,192,193,194,195,196,197Tl; measured hfs, isotope shift; deduced rms radii, staggering parameter. Collinear laser spectroscopy.
At.Data Nucl.Data Tables 42, 189 (1989)
P.Raghavan
Table of Nuclear Moments
COMPILATION Z=1-99; compiled μ, electric quadrupole moments.
doi: 10.1016/0092-640X(89)90008-9
Nucl.Data Sheets 56, 75 (1989)
B.Singh
Nuclear Data Sheets for A = 194
COMPILATION 194Os, 194Ir, 194Pt, 194Au, 194Hg, 194Tl, 194Pb, 194Bi, 194Po, 194At; compiled, evaluated structure data.
Z.Phys. A333, 281 (1989)
X.Sun, U.Rosengard, H.Grawe, H.Haas, H.Kluge, A.Kuhnert, K.H.Maier
Conversion Electron Measurement of Isomeric Primary Transitions in 196,198,199,200,201Pb
NUCLEAR REACTIONS 182,184,186W(18O, xn), E=85 MeV; 192Os(13C, xn), E=70 MeV; measured (ce)(ce)-, γ(ce)-coin. 196,198,199,200,201Pb deduced isomer, J, π, T1/2, decay, B(λ).
Z.Phys. A332, 61 (1989)
A.Yokoyama, T.Saito, M.Shoji, H.Baba, S.Baba, K.Hata, T.Sekine, S.Ichikawa
Nuclear Transfer in Highly Mass-Asymmetric Reaction Systems between 197Au and Relatively Light Projectiles in the Energy Region below 10 MeV/u I. Target-Like Products
NUCLEAR REACTIONS, ICPND 197Au(12C, X), (16O, X), (37Cl, X), (14N, X)199Au/198Au/198mAu/196Au/196mAu/195Au/194Au/193Au/192Au, E ≈ threshold-130 MeV; measured residual production σ(E); deduced reaction mechanism. Activation technique.
Chin.J.Nucl.Phys. 11, No.2, 83 (1989)
W.Zhao, H.Lu
Measurements of Cross Sections for 197Au(d, X) Reaction
NUCLEAR REACTIONS, ICPND 197Au(d, p), (d, 2n), (d, 2np), E ≈ threshold-12.8 MeV; measured reaction σ(E).
Nucl.Phys. A520, 187c (1990)
J.A.Becker, N.Roy, E.A.Henry, S.W.Yates, A.Kuhnert, J.E.Draper, W.Korten, C.W.Beausang, M.A.Deleplanque, R.M.Diamond, F.S.Stephens, W.H.Kelly, F.Azaiez, J.A.Cizewski, M.J.Brinkman
Level Spin and Moments of Inertia in Superdeformed Nuclei Near A = 194
NUCLEAR STRUCTURE 190,191,192,193,194Hg, 194,196Pb, 193,194Tl; analyzed data; deduced levels, J, superdeformed band parameters. Least-squares fit to rotational formulas.
doi: 10.1016/0375-9474(90)91146-I
Phys.Rev. C42, R2271 (1990)
H.G.Borner, J.Jolie, S.Robinson, R.F.Casten, J.A.Cizewski
First Measurement of B(E2) Values from σ < N States of an O(6) Nucleus: Gamma-ray-induced Doppler broadening studies in 196Pt
NUCLEAR REACTIONS Pt(n, γ), E=thermal; measured γ-spectra, Doppler profile. 196Pt levels deduced T1/2, B(λ). GRID technique.
doi: 10.1103/PhysRevC.42.R2271
Nucl.Phys. A519, 509 (1990)
P.Bonche, J.Dobaczewski, H.Flocard, P.H.Heenen, S.J.Krieger, J.Meyer, M.S.Weiss
Quadrupole Collective Correlations and the Depopulation of the Superdeformed Bands in Mercury
NUCLEAR STRUCTURE 190,192,194,196,198Hg; calculated deformation energy, wave functions, proton quadrupole moments, superdeformed band decay Iγ. Self-consistent generator coordinate method, Hartree-Fock plus BCS wave functions.
doi: 10.1016/0375-9474(90)90443-P
Z.Phys. A336, 115 (1990)
M.J.Brinkman, A.Kuhnert, E.A.Henry, J.A.Becker, S.W.Yates, R.M.Diamond, M.A.Deleplanque, F.S.Stephens, W.Korten, F.Azaiez, W.H.Kelly, J.E.Draper, C.W.Beausang, E.Rubel, J.A.Cizewski
Superdeformation in Lead Nuclei
NUCLEAR REACTIONS 176Yb(24Mg, xn), E=122-132 MeV; measured γγ-coin. 194,196Pb deduced levels, J, π, superdeformed band structure.
Europhys.Lett. 13, 37 (1990)
A.A.Cowley, S.V.Fortsch, J.J.Lawrie, J.V.Pilcher, F.D.Smit, D.M.Whittal
Importance of Nucleon-Nucleon Scattering in the Interaction of Protons with 197Au at 200 MeV
NUCLEAR REACTIONS 197Au(p, 2p), E=200 MeV; measured σ(θ1, θ2, E1); deduced reaction mechanism. DWIA analysis.
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.
Phys.Lett. 248B, 235 (1990)
J.Dudek, T.R.Werner, Z.Szymanski
Prediction of Octupole-Deformation Effects in Superdeformed Nuclei of A ≈ 150 and A ≈ 190 Mass Regions and Possible Interrelation with Pseudo-Spin Symmetry
NUCLEAR STRUCTURE 146Nd, 148Sm, 150Gd, 152Dy, 154Er, 156Yb, 186,188,190,192,194,196,198,200,202Hg; calculated potential energy vs deformation parameter; deduced pronounced octupole effects, superdeformed nuclei.
doi: 10.1016/0370-2693(90)90284-D
Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 1006 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.5, 190 (1990)
V.I.Gavrilyuk, V.A.Zheltonozhsky, S.V.Reshitko, V.B.Kharlanov
Measurement of the Isomeric Ratios for Nuclei with A > 150
NUCLEAR REACTIONS, ICPND 151Eu(n, γ), E=reactor; 151Eu(α, n), E=15.6-26.3 MeV; 184W(p, n), E=3.8-6.7 MeV; 193Ir(α, n), E=16.4-23.5 MeV; measured residuals isomeric production σ ratios. Activation technique. Cascade-evaporation model.
Chin.J.Nucl.Phys. 12, No.2, 151 (1990)
Y.Ha, D.Fu
IBM-II Continuous Representation and Its Application to Pt and Gd Potential Surface Analysis
NUCLEAR STRUCTURE 186,188,190,192,194,196Pt, 150,152,154,156Gd, 148,154Sm, 78Se; analyzed data; deduced model parameters. 186Pt, 150,156Gd; calculated potential surfaces. Interacting boson model, continuous representation.
Proc.Inter.Conf.Nuclear Structure of the Nineties, Oak Ridge, Tennessee, Vol.1, p.19 (1990)
E.A.Henry, J.A.Becker, A.Kuhnert, S.W.Yates, R.A.Meyer, T.F.Wang, Y.A.Akovali, M.J.Brinkman, H.K.Carter, W.D.Schmidt-Ott, C.R.Bingham, H.V.Carmichael, J.Kormicki, Y.Xu
Search for Shape Isomers in Mercury Nuclei via Light-Ion Reactions and Beta Decay
NUCLEAR REACTIONS 197Au(p, 2n), (t, 2n), E not given; measured I(ce). 196,198Hg deduced preliminary level scheme.
RADIOACTIVITY 194Tl(β+); measured not given. 194Hg deduced preliminary level scheme.
Hyperfine Interactions 59, 97 (1990)
Th.Hilberath, St.Becker, G.Bollen, M.Gerber, H.-J.Kluge, U.Kronert, G.Passler
Charge Radii and Shape Transitions in Short- Lived Hg, Au and Pt Isotopes
RADIOACTIVITY 183,184Au, 197,193,191,189,188,187,186,185,184,183Pt; measured hfs, isotope shift; deduced rms charge radii changes. 183Pt deduced μ.
NUCLEAR MOMENTS 198,196,195,195,192,190Pt; measured hfs, isotope shift; deduced rms charge radii changes.
Z.Phys. A336, 363 (1990)
J.Holler, S.Aberg
Octupole Instability of Super- and Hyperdeformed Nuclei
NUCLEAR STRUCTURE 152Dy, 190,194Hg, 200Rn; calculated potential energy surfaces; deduced possible superdeformation, hyperdeformation. 146Gd, 152Dy, 194,190Hg, 196Pb, 198Po, 200Rn; calculated octupole softness; deduced possible superdeformation. Cranked Nilsson-Strutinsky model.
KVI 1989 Ann.Rept., p.1 (1990)
M.A.Hofstee, S.Y.van der Werf, J.A.Bordewijk, A.M.van den Berg, N.Blasi, M.Pignanelli, S.Micheletti, R.De Leo, S.Fortier, M.Morlet, H.Langevin-Joliot, A.Willis, G.T.Emery
Stretched Spin Configurations Studied with the (p, p') Reaction at 200 MeV
NUCLEAR REACTIONS 90Zr, 116Sn, 196Pt, 208Pb(p, p'), E=200 MeV; measured σ(θ). 90Zr, 116Sn, 196Pt, 208Pb deduced stretched spin configurations.
Nucl.Phys. A509, 195 (1990)
B.Jakobsson, G.Jonsson, L.Karlsson, V.Kopljar, B.Noren, K.Soderstrom, F.Schussler, E.Monnand, H.Nifenecker, G.Fai, J.P.Bondorf, K.Sneppen
On the Observation of a Transition from Fusion to Multifragmentation in High Multiplicity 16O Induced Reactions
NUCLEAR REACTIONS Br, Ag(16O, X), E=94 MeV/nucleon; measured high multiplicity collision charge distribution; deduced charge distribution moments.
doi: 10.1016/0375-9474(90)90381-U
Nucl.Phys. A520, 75c (1990)
R.V.F.Janssens, M.P.Carpenter, M.W.Drigert, P.B.Fernandez, E.F.Moore, D.Ye, I.Ahmad, K.B.Beard, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, Z.W.Grabowski, T.L.Khoo, W.Reviol, F.L.H.Wolfs
Superdeformation in the Mercury Nuclei
NUCLEAR STRUCTURE 194,196Pb, 193,194Tl, 189,190,191,192,193,194Hg; compiled, analyzed superdeformed band data.
doi: 10.1016/0375-9474(90)91135-E
J.Phys.(London) G16, 813 (1990)
G.L.Long, Y.X.Liu, H.Z.Sun
Staggering in Nuclear Spectra and the Proton-Neutron Interacting Boson Model
NUCLEAR STRUCTURE 98,100,102,104Ru, 196Pt; calculated levels, B(λ), quadrupole moment. Proton-neutron interacting boson model.
doi: 10.1088/0954-3899/16/6/006
Z.Phys. A336, 263 (1990)
A.Mauthofer, K.Stelzer, J.Idzko, Th.W.Elze, H.J.Wollersheim, H.Emling, P.Fuchs, E.Grosse, D.Schwalm
Triaxiality and γ-Softness in 196Pt
NUCLEAR REACTIONS 196Pt(208Pb, 208Pb'), E=4.8 MeV/nucleon; measured Eγ, Iγ, γγ-coin following Coulomb excitation; deduced γ yield ratios. 196Pt deduced levels, J, π, T1/2, B(λ), band structure. Models comparison.
Phys.Rev. C42, 988 (1990)
G.Maino, A.Mengoni, A.Ventura
Collective Enhancement of Nuclear Level Density in the Interacting Boson Model
NUCLEAR STRUCTURE 110Cd, 196Pt, 238U; calculated excitation energy, boson number, partition function vs temperature.
GSI-90-06 (1990)
A.Mauthofer, K.Stelzer, J.Idzko, Th.W.Elze, H.J.Wollersheim, H.Emling, P.Fuchs, E.Grosse, D.Schwalm
Triaxiality and γ-Softness in 196Pt
NUCLEAR REACTIONS 196Pt(208Pb, 208Pb'), E=4.8 MeV/nucleon; measured γ(particle)-, γγ(particle)-coin following multiple Coulomb excitation. 196Pt deduced E2-transition moments, static quadrupole moments, B(λ). Different theoretical models.
Phys.Lett. 251B, 229 (1990)
M.Mukerjee
Compact to Noncompact Transition with Application to Nuclear Collective Levels
NUCLEAR STRUCTURE 196Pt; calculated B(λ). Transition from interacting boson model to noncompact algebra.
doi: 10.1016/0370-2693(90)90927-X
Phys.Rev. C41, 889 (1990)
Y.Nagame, K.Sueki, S.Baba, H.Nakahara
Isomeric Yield Ratios in Proton-, 3He-, and α-Particle-Induced Reactions on 197Au
NUCLEAR REACTIONS, ICPND 197Au(p, np), (p, 3n), E=threshold-50 MeV; 197Au(3He, 2p), (3He, α), E=threshold-40 MeV; 197Au(α, nα), (α, 3n), E=threshold-40 MeV; measured σ(E), residual isomeric yield ratio; deduced reaction mechanism, systematics of isomeric yield ratio. Compound nuclear reaction, direct reaction, pre-equilibrium reaction mechanisms, analyzed other data.
Fiz.Elem.Chastits At.Yadra 21, 467 (1990); Sov.J.Part.Nucl 21, 199 (1990)
E.G.Nadzhakov
Models of Dynamical Symmetries of the Nucleus
NUCLEAR STRUCTURE 218Ra, 220Th, 198,197Au, 196,197Pt; analyzed calculated level schemes; deduced dynamical symmetries role.
Nucl.Instrum.Methods Phys.Res. A286, 601 (1990)
Zs.Nemeth, A.Veres
Comparison of Experimental and Theoretical High Multipole-Order Internal Conversion Coefficients
NUCLEAR STRUCTURE A=85-197; analyzed ICC for high multipole transitions; deduced discrepancies. Different model calculations.
doi: 10.1016/0168-9002(90)90923-T
Nucl.Phys. A512, 241 (1990)
G.Savard, J.E.Crawford, J.K.P.Lee, G.Thekkadath, H.T.Duong, J.Pinard, S.Liberman, F.Le Blanc, P.Kilcher, J.Obert, J.Oms, J.C.Putaux, B.Roussiere, J.Sauvage, and the ISOCELE Collaboration
Laser Spectroscopy of Laser-Desorbed Gold Isotopes
RADIOACTIVITY 186,187,190,192,194,195,196Au [from Pt(p, xn)Au, on-line mass separation]; 198,199Au [from Au(n, γ)Au, Pt(n, γ)Pt, mass-separation]; measured hfs, isotope shifts; deduced μ, rms charge radii, deformation parameters β. Laser desorption, laser resonant ionization spectroscopy.
doi: 10.1016/0375-9474(90)93192-9
Ann.Phys.(New York) 199, 227 (1990)
D.K.Sunko
Phase Transition Induced by Particle Number in a Model Finite System
NUCLEAR STRUCTURE 124Sn, 196Pt, 198Au, 237,238,239U, 210Bi; calculated cumulative level numbers, level density. Model finite system, particle number induced phase transition.
doi: 10.1016/0003-4916(90)90379-3
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.
JYFL Ann.Rept., 1989-1990, p.110 (1990)
W.H.Trzaska, R.Julin, J.Kantele, J.Kumpulainen, P.Van Duppen, M.Huyse, J.Wauters
Comparison of Experimental and Calculated K/L Ratios of E0 Transitions in Heavy Nuclei
NUCLEAR STRUCTURE 154Gd, 192,194,196,198,202,204,206,208Pb; calculated E0 transition K/L ratios.
Fizika(Zagreb) 22, 233 (1990)
J.Van Maldeghem, K.Heyde
Proton-Neutron Multiplets in Odd-Odd Tl Nuclei
NUCLEAR STRUCTURE 186,188,190,192,194,196,198,200Tl; calculated levels. 192Tl; calculated level g-factor, quadrupole moments, B(λ). Particle-core coupling model.
Nucl.Phys. A514, 381 (1990)
M.Vergnes, G.Berrier-Ronsin, G.Rotbard, J.Skalski, W.Nazarewicz
Evidence for a Change of Structure in the Heavy Mercury Isotopes Around 200Hg
NUCLEAR REACTIONS Hg, 196,198,200,202,204Hg(p, t), E=25 MeV; measured σ(θ). 194,196,198,200,202Hg deduced levels, J, π, enhancement factors. DWBA analysis.
doi: 10.1016/0375-9474(90)90149-G
Z.Phys. A339, 225 (1991)
D.Alber, R.Alfier, C.E.Bach, D.B.Fossan, H.Grawe, H.Kluge, M.Lach, K.H.Maier, M.Schramm, R.Schubart, M.P.Waring, L.Wood, H.Hubel, J.-Y.Zhang
Quadrupole and Octupole Collectivity in Light Po Isotopes
NUCLEAR REACTIONS 160Dy(40Ar, 4n), E=182 MeV; measured γ(X-ray)-, γγ-energy coincidence spectra. 183W(20Ne, 5n), E=115 MeV; measured γγ-coin. 198,196Po deduced levels, J, π, T1/2, γ-multipolarity, collectivity features.
Phys.Lett. 266B, 243 (1991)
R.R.Chasman
Superdeformed and Hyperdeformed Banana Shaped Nuclides Near A = 190
NUCLEAR STRUCTURE 190Pt, 189,190,191,192Au, 188,189,190,191,192,193,194,195Hg, 189,190,191,192,193,194,195Tl, 190,191,192,193Pb, 193,194,195,196Bi, 194Po; calculated level energy relative to prolate mininum, barrier heights, reflection symmetric shapes; deduced superdeformed, hyperdeformed minima, deformation features.
doi: 10.1016/0370-2693(91)91033-R
Ann.Nucl.Energy 18, 503 (1991)
F.C.Difilippo
Correlation between Fission Neutrons and the Calculation of Stochastics Descriptors Application to the 252Cf Ratio Method
doi: 10.1016/0306-4549(91)90095-F
Nucl.Sci.Eng. 109, 319 (1991)
C.L.Hartmann, P.M.DeLuca, Jr.
Measurement of the 19F(n, 2n)18F Cross Section from 18 to 27 MeV
NUCLEAR REACTIONS Zr, 197Au, 19F(n, 2n), E=18-27 MeV; measured σ. Nearly monoenergetic beam, Teflon target.
Phys.Rev. C43, R16 (1991)
J.Jolie, U.Mayerhofer, T.von Egidy, H.Hiller, J.Klora, H.Lindner, H.Trieb
Predictive Power of Supersymmetry in Nuclear Structure Tested by Pickup Transfer Reactions to 196Au
NUCLEAR REACTIONS 197Au(d, t), E=22 MeV; 197Au(3He, α), E=33 MeV; measured σ(θ). 196Au deduced levels, L, deduced supersymmetry model applicability. Model calculations, supersymmetry.
Phys.Lett. 263B, 347 (1991)
S.Kuyucak, V.-S.Lac, I.Morrison, B.R.Barrett
γ-Unstable Nuclei in the sdg Boson Model
NUCLEAR STRUCTURE 194,196,198Pt; calculated levels, E4 matrix elements. 126Xe; calculated levels. sdg boson model, O(6) limit.
doi: 10.1016/0370-2693(91)90471-2
J.Phys.(London) G17, 877 (1991)
Y.X.Liu, G.L.Long, H.Z.Sun
An IBM2 Description of the Staggering Phenomenon in the Platinum Isotopes
NUCLEAR STRUCTURE 188,190,192,194,196,198Pt; calculated levels, E2, M1 transition features, electric quadrupole moments. Interacting boson model.
doi: 10.1088/0954-3899/17/6/010
Z.Phys. A339, 317 (1991)
D.Mehta, Y.K.Agarwal, K.P.Blume, S.Heppner, H.Hubel, M.Murzel, K.Theine, W.Gast, G.Hebbinghaus, R.M.Lieder, W.Urban
Spectroscopy of 195Hg and 196Hg
NUCLEAR REACTIONS 198Pt(α, xn), E=78 MeV; measured γγ-coin, Eγ, Iγ, DCO ratios. 195,196Hg deduced levels, J, π, band structure.
Nucl.Phys. A533, 223 (1991)
P.Navratil, J.Dobes
Similarity-Transformed Dyson Mapping and SDG-Interacting Boson Hamiltonian
NUCLEAR STRUCTURE 144,145,146,148,149,150,151,152,153,154Sm, 150Nd, 196Pt; calculated levels, B(λ). sdg-interacting boson hamiltonian.
doi: 10.1016/0375-9474(91)90488-R
At.Data Nucl.Data Tables 47, 205 (1991)
A.Rytz
Recommended Energy and Intensity Values of Alpha Particles from Radioactive Decay
RADIOACTIVITY A=146-257; compiled Eα, Iα; deduced recommended values.
doi: 10.1016/0092-640X(91)90002-L
Nucl.Phys. A529, 289 (1991)
W.Satula, S.Cwiok, W.Nazarewicz, R.Wyss, A.Johnson
Structure of Superdeformed States in Au-Ra Nuclei
NUCLEAR STRUCTURE 190,192,194,196Hg, 192,194,196,198Pb, 194,196,198,200,202Po, 198,200,202,204,206Rn, 204,206,208,210,212Ra; calculated superdeformed state energies, equilibrium deformations, band head energies, barrier heights, potential energy surfaces. 189,191,193,195,190,192,194,196Tl, 187,189,191,193,195Au; calculated equilibrium deformations. Strutinsky shell correction method.
doi: 10.1016/0375-9474(91)90797-A
Phys.Rev. C44, 700 (1991)
A.Sethi, N.M.Hintz, D.N.Mihailidis, A.M.Mack, M.Gazzaly, K.W.Jones, G.Pauletta, L.Santi, D.Goutte
Inelastic Proton Scattering from Pt Isotopes and the Interacting Boson Model
NUCLEAR REACTIONS 194,196Pt(polarized p, p), (polarized p, p'), E=647 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 194,196Pt levels deduced deformation parameters, E2, E4 matrix elements, B(λ). Coupled-channels analysis, interacting boson model.
Nucl.Phys. A528, 447 (1991)
A.E.Stuchbery, G.J.Lampard, H.H.Bolotin
Transient Field Measurements of g-Factors in 194,196,198Pt; g(21+) Systematics in transitional W, Os, Pt Nuclei
NUCLEAR REACTIONS 194,196,198Pt, 182,184,186W(37Cl, 37Cl'), E=115 MeV; 182,184,186W, 194,196,198Pt(58Ni, 58Ni'), E=160 MeV; measured γ(θ, H, T) in polarized Gd, (particle)γ-coin, Coulomb excitation, transient-field precession W(Gd), Pt(Gd). 186W, 194,196,198Pt levels deduced g. Natural targets, thin foil transient field IMPAC technique.
NUCLEAR STRUCTURE 180,182,184,186W, 186,188,190,192Os, 192,194,196,198Pt; calculated g. Interacting boson model.
doi: 10.1016/0375-9474(91)90098-Q
Z.Phys. A338, 261 (1991)
D.Troltenier, J.A.Maruhn, W.Greiner, V.V.Aguilar, P.O.Hess, J.H.Hamilton
Shape Transitions and Shape Coexistence in the Ru and Hg Chains
NUCLEAR STRUCTURE 182,184,186,188,190,192,194,196Hg, 96,98,100,102,104,106,108Ru; calculated levels, B(λ), potential energy surfaces, quadrupole moments.
Nucl.Phys. A529, 268 (1991)
P.Van Duppen, P.Decrock, P.Dendooven, M.Huyse, G.Reusen, J.Wauters
Intruder States in Odd-Odd Tl Nuclei Populated in the α-Decay of Odd-Odd Bi Isotopes
RADIOACTIVITY 190,192,194,196Bi [from Re(16O, xn), E < 180 MeV; 182W(20Ne, xnp), E < 240 MeV]; measured Eα, Iα, T1/2, Eγ, Iγ, αγ(t), α(X-ray)(t), α(ce)(t); deduced isomer, ground state T1/2, α-branching ratios. 186,188,190,192Tl deduced levels, J, π, ICC, γ multipolarity, T1/2. Hyperpure Ge, Ge(Li), plastic, BaF2, Si(PIPS) detectors, mass separated samples.
doi: 10.1016/0375-9474(91)90796-9
Phys.Rev. C43, R2465 (1991)
T.F.Wang, A.Kuhnert, J.A.Becker, E.A.Henry, S.W.Yates, M.J.Brinkman, J.A.Cizewski, F.A.Azaiez, M.A.Deleplanque, R.M.Diamond, J.E.Draper, W.H.Kelly, W.Korten, A.O.Macchiavelli, E.Rubel, F.S.Stephens
Superdeformation in 198,196Pb
NUCLEAR REACTIONS 154Sm(48Ca, xn), E=205 MeV; 176Yb(26Mg, xn), E=135 MeV; measured γγ-coin. 198,196Pb deduced levels, superdeformed band features. Other isotopes discussed.
doi: 10.1103/PhysRevC.43.R2465
J.Phys.(London) G17, S243 (1991)
Yu.Zdesenko
Double Beta Decay Experiments at Kiev
RADIOACTIVITY 116Cd, 196Hg(2β); measured γ-spectra; deduced 0ν-, 2ν-accompanied 2β-decay T1/2 limits. CdWo4 scintillator enriched by 116Cd, hyperpure Ge detectors.
doi: 10.1088/0954-3899/17/S/026
Phys.Lett. 295B, 5 (1992)
B.R.Barrett, E.D.Davis, A.F.Diallo
g-Boson Panacea for Magnetic Properties of the Nuclear Groundstate Band ( Questiion )
NUCLEAR STRUCTURE 198,196,194,192Pt, 188,190,192Os; analyzed ground state band g-factor data; deduced g-boson degree of freedom does not resolve discrepancies. Other nuclei included, sdg-version of the interacting boson model, variation-after-angular momentum projection Hartree-Bose approximation.
doi: 10.1016/0370-2693(92)90079-J
Nucl.Phys. A536, 366 (1992)
F.Brandolini, M.Ionescu-Bujor, P.Pavan, D.Bazzacco, C.Rossi-Alvarez, M.De Poli, A.M.I.Haque, R.V.Ribas
Gyromagnetic Ratios of Low-Lying States in 192,194,196Pt
NUCLEAR REACTIONS 192,194,196Pt(58Ni, 58Ni'), E=180-210 MeV; measured γ(θ, H, T) in polarized Gd, Fe, (particle)-γ coin, Coulomb excitation. 192,194,196Pt levels deduced g-factors. Enriched targets, thin foil transient-field IMPAC technique.
NUCLEAR STRUCTURE 192,194,198Pt; calculated g-factors. Pairing-plus-quadrupole, dynamical deformation, interacting bosons models.
doi: 10.1016/0375-9474(92)90388-Z
Nucl.Phys. A536, 179 (1992)
C.H.Dasso, A.Vitturi
Excitation Patterns of γ-Unstable Nuclei
NUCLEAR REACTIONS 196Pt(208Pb, 208Pb'), E=650, 900 MeV; calculated γ-unstable band Coulomb excitation probabilities. Sudden limit supplemented by coupled-channels approach.
doi: 10.1016/0375-9474(92)90253-G
Z.Phys. A342, 1 (1992)
Th.Hilberath, St.Becker, G.Bollen, H.-J.Kluge, U.Kronert, G.Passler, J.Rikovska, R.Wyss, and the ISOLDE Collaboration
Ground-State Properties of Neutron-Deficient Platinum Isotopes
NUCLEAR MOMENTS 198,196,195,194,193,192,190Pt; measured hfs, isotope shift; deduced μ, quadrupole moments, rms charge radii, quadrupole moments. Particle-triaxial rotor model, mean field calculations. Other isotopes studied. Resonance ionization mass spectroscopy, pulser-laser induced desorption techniques, Pt isotopes produced as daughters of Hg-isotopes obtained from on-line isotope separator.
RADIOACTIVITY 183,184,185,185m,186,187,188,189,190,191Pt; measured hfs, isotope shift; deduced μ, quadrupole moments, rms charge radii, quadrupole moments. Particle-triaxial rotor model, mean field calculations. Other isotopes studied. Resonance ionization mass spectroscopy, pulser-laser induced desorption techniques, Pt isotopes produced as daughters of Hg-isotopes obtained from on-line isotope separator.
Phys.Rev. C46, 1682 (1992)
S.T.Hsieh, H.C.Chiang, M.M.King Yen
Spectral Anomalies of Even-Mass Hg Isotopes
NUCLEAR STRUCTURE 184,186,188,190,192,194,196,198,200Hg; calculated levels, B(λ) ratios. Interacting boson approximation plus fermion pair model.
Phys.Rev. C46, 1209 (1992)
M.Huyse, P.Decrock, P.Dendooven, G.Reusen, P.Van Duppen, J.Wauters
Isomers in Three Doubly Odd Fr-At-Bi α-Decay Chains
RADIOACTIVITY 206,204,202Fr(α), 202,200At(α), (β+); 198At(α); measured Eα, Iα, T1/2, γγ-coin, Eγ, Iγ, electron spectra. 206,204,202Fr, 202,200,198At, 198,196,194Bi deduced levels, J, π, α-reduced widths, α-branching ratios, Q(α), B(E3), γ-multipolarity, configuration, isomer transitions.
Nucl.Phys. A542, 43 (1992)
S.J.Krieger, P.Bonche, M.S.Weiss, J.Meyer, H.Flocard, P.-H.Heenen
Super-Deformation and Shape Isomerism: Mapping the isthmus
NUCLEAR STRUCTURE Z=108-152; calculated excitation energy, rigid moment of inertia. 190,192,194,196,198,200,202,204,206,210,212,214,216,218,220,222,224,226,228,230Pb calculated rigid moment of inertia, quadrupole moment, superdeformed isomers; deduced shape isomerism isthmus superdeformation region. Microscopic Hartree-Fock-BCS formalism.
doi: 10.1016/0375-9474(92)90395-Z
Nucl.Phys. A539, 418 (1992)
V.-S.Lac, S.Kuyucak
Description of Transitional Nuclei in the sdg Boson Model
NUCLEAR STRUCTURE 192,194,196,198Pt, 192,190,188Os; calculated levels, E2 transitions reduced matrix elements, quadrupole moments. sdg boson model.
doi: 10.1016/0375-9474(92)90285-R
Nucl.Phys. A548, 308 (1992)
C.S.Lim, R.H.Spear, M.P.Fewell, G.J.Gyapong
Measurements of Static Electric Quadrupole Moments of the 2+1, 2+2, 4+1 and 6+1 States of 196Pt
NUCLEAR REACTIONS 196Pt(α, α), E=14.2-15.8 MeV; 196Pt(7Li, 7Li), E=22, 22.5 MeV; 196Pt(12C, 12C), E=42-46 MeV; 196Pt(58Ni, 58Ni), E=214-226 MeV; measured (particle)γ-coin, Eγ, Iγ, γγ(θ), Coulomb excitation probabilities. 196Pt levels deduced B(E2), B(E4), static quadrupole moments.
doi: 10.1016/0375-9474(92)90013-A
Phys.Rev. C45, 233 (1992)
M.Meyer, N.Redon, P.Quentin, J.Libert
Superdeformed Single-Particle Orbitals in the A = 190 Region from Hartree-Fock Plus BCS Calculations
NUCLEAR STRUCTURE 192,194,196,198,200Pb, 194,192,190Hg; calculated superdeformed nucleon state components, spectra; deduced particle number symmetry restoration role. Self-consistent axial Hartree-Fock plus BCS.
Z.Phys. A341, 475 (1992)
R.Menges, U.Dinger, N.Boos, G.Huber, S.Schroder, S.Dutta, R.Kirchner, O.Klepper, T.Kuhl, D.Marx, G.D.Sprouse
Nuclear Moments and the Change in the Mean Square Charge Radius of Neutron Deficient Thallium Isotopes
RADIOACTIVITY 190,192,194,196,191,188Tl [from Pb isotopes decay following W(16O, xn) reaction]; measured hfs, isomeric shifts; deduced μ, quadrupole moments, rms charge radii.
Nucl.Phys. A549, 180 (1992)
V.Yu.Ponomarev, W.T.A.Borghols, S.A.Fayans, M.N.Harakeh, C.W.de Jager, J.B.van der Laan, A.P.Platonov, H.de Vries, S.Y.van der Werf
Transition Charge Densities of Low-Lying Collective States in 196Pt from Inelastic Electron Scattering
NUCLEAR REACTIONS 196Pt(e, e'), E=90-334 MeV; measured spectra, longitudinal form factors. 196Pt levels deduced transition charge densities, J, π, B(λ). Fourier-Bessel analysis. Compared to microscopic quasiparticle phonon model.
doi: 10.1016/0375-9474(92)90039-M
Phys.Rev. C46, 1715 (1992)
M.M.Sharma, P.Ring
Relativistic Mean-Field Description of Neutron-Deficient Platinum Isotopes
NUCLEAR STRUCTURE 184,186,188,190,192,194,196,198Pt; calculated binding energy per nucleon, deformation parameters, rms charge radii changes, neutron skin thickness. Relativistic mean field approach.
Phys.Lett. 274B, 1 (1992)
J.Skalski
Octupole Correlations at Superdeformed Shape in the Hg-Pb Region - Including Nonaxial Components
NUCLEAR STRUCTURE 192,194Hg, 192,194,196,198Pb; calculated routhian stiffness vs octupole deformation components; deduced octupole vibration frequencies at superdeformed minima.
doi: 10.1016/0370-2693(92)90294-E
Phys.Rev. C45, 261 (1992)
C.S.Wu, J.Y.Zeng, Z.Xing, X.Q.Chen, J.Meng
Spin Determination and Calculation of Nuclear Superdeformed Bands in A ≈ 190 Region
NUCLEAR STRUCTURE 190,191,192,193,194Hg, 193,194Tl, 194,196Pb; calculated superdeformed bands, transition energies. Two-parameter approach.
Phys.Rev. C45, 2507 (1992)
C.S.Wu, L.Cheng, C.Z.Lin, J.Y.Zeng
Relation between the Kinematic and Dynamic Moments of Inertia in Superdeformed Nuclei
NUCLEAR STRUCTURE 164,166Er, 168,170,172,174,176Yb, 170,172,174,176,178Hf, 238U, 242Pu, 248Cm; analyzed ground state bands data. 191,192,193,194Hg, 193,194Tl, 194,196Pb, 151,152Dy, 150Tb, 150Gd; analyzed superdeformed band level data; deduced R-parameter remains independent of spin.
Phys.Rev. C47, R2443 (1993)
B.Cederwall, M.-A.Deleplanque, F.Azaiez, R.M.Diamond, P.Fallon, W.Korten, I.-Y.Lee, A.O.Macchiavelli, J.R.B.Oliveira, F.S.Stephens, W.H.Kelly, D.T.Vo, J.A.Becker, M.J.Brinkman, E.A.Henry, J.R.Hughes, A.Kuhnert, M.A.Stoyer, T.F.Wang, J.E.Draper, C.Duyar, E.Rubel, J.deBoer
New Oblate Band in 196Hg with Quenched M1 Strength
NUCLEAR REACTIONS 192Os(9Be, 5n), E=65 MeV; measured γγ-coin. 196Hg deduced levels, J, π, band structure, B(λ) ratio, shape features, configurations.
doi: 10.1103/PhysRevC.47.R2443
J.Phys.(London) G19, 465 (1993)
P.J.Dagnall, C.W.Beausang, P.Fallon, P.D.Forsyth, E.S.Paul, J.F.Sharpey-Schafer, P.J.Twin, I.Ali, D.M.Cullen, M.J.Joyce, G.Smith, R.Wadsworth, R.M.Clark, P.H.Regan, A.Astier, M.Meyer, N.Redon
Coexistence of Collective Oblate and Superdeformed Prolate Shapes in 196Pb
NUCLEAR REACTIONS 184W(16O, 4n), E=98 MeV; 186W(16O, 6n), E=120 MeV; measured γγ-coin. 196Pb deduced levels, J, π, collective oblate, superdeformed prolate band coexistence.
doi: 10.1088/0954-3899/19/3/014
Phys.Rev. C47, 2492 (1993)
R.M.Davidson
One-Loop Corrections to Threshold γp → pπ0 Production in the Linear Sigma Model
NUCLEAR REACTIONS 1H(γ, π0), E ≈ threshold; calculated pion production one-loop coprrections. Linear sigma model.
Phys.Rev. C48, 2603 (1993)
D.P.DiPrete, T.Belgya, E.M.Baum, E.L.Johnson, S.W.Yates, P.D.Cottle, M.A.Kennedy, K.A.Stuckey
Search for High-Lying Octupole States and Octupole Fragmentation in 196Pt with the (n, n'γ) Reaction
NUCLEAR REACTIONS 196Pt(n, n'γ), E=2-3.5 MeV; measured Eγ, Iγ(θ), DSA. 196Pt deduced levels, J, π, branching ratios, T1/2, B(λ), octupole features. Enriched target, hyperpure Ge detectors.
Phys.Rev. C48, R1488 (1993)
D.H.Feng, M.W.Guidry, X.-W.Pan, C.-L.Wu, I.Zlatev
Effective Fermion SO(6) Dynamical Symmetry in the Platinum Nuclei
NUCLEAR STRUCTURE 196Pt; calculated levels; deduced fermion SO(6) dynamical symmetry evidence.
doi: 10.1103/PhysRevC.48.R1488
Phys.Rev. C48, 1739 (1993)
M.W.Guidry, M.R.Strayer, C.-L.Wu, D.H.Feng
Some General Constraints on Identical Band Symmetries
NUCLEAR STRUCTURE 192,194,196Hg, 234,236,238U, 238,240,242,244Pu, 246,248Cm, 248,250Cf; analyzed band structure; deduced normal, superdeformed identical bands related features.
Phys.Rev. C47, R1337 (1993)
J.R.Hughes, Y.Liang, R.V.F.Janssens, A.Kuhnert, J.A.Becker, I.Ahmad, I.G.Bearden, M.J.Brinkman, J.Burde, M.P.Carpenter, J.A.Cizewski, P.J.Daly, M.A.Deleplanque, R.M.Diamond, J.E.Draper, C.Duyar, B.Fornal, U.Garg, Z.W.Grabowski, E.A.Henry, R.G.Henry, W.Hesselink, N.Kalantar-Nayestanaki, W.H.Kelly, T.L.Khoo, T.Lauritsen, R.H.Mayer, D.Nissius, J.R.B.Oliveira, A.J.M.Plompen, W.Reviol, E.Rubel, F.Soramel, F.S.Stephens, M.A.Stoyer, D.Vo, T.F.Wang
Collective Oblate Bands in 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4n), E=142-151 MeV; 176Yb(26Mg, 6n), E=138 MeV; measured γγ-coin. 196Pb deduced levels, J, π, band structure, B(λ) ratio, shape features.
doi: 10.1103/PhysRevC.47.R1337
Nucl.Phys. A557, 125c (1993)
S.Mizutori, T.Nakatsukasa, K.Arita, Y.R.Shimizu, K.Matsuyanagi
Octupole Correlations in Superdeformed High-Spin States
NUCLEAR STRUCTURE 158,156,154,152,150,148,146,144,142Gd, 184,186,188,190,192,194,196,198,200Hg; calculated curvature against octupole deformation, stretched octupole strengths; deduced octupole instability, superdeformed shape relationship.
doi: 10.1016/0375-9474(93)90536-7
Phys.Rev. C48, 2261 (1993)
E.F.Moore, Y.Liang, R.V.F.Janssens, M.P.Carpenter, I.Ahmad, I.G.Bearden, P.J.Daly, M.W.Drigert, B.Fornal, U.Garg, Z.W.Grabowski, H.L.Harrington, R.G.Henry, T.L.Khoo, T.Lauritsen, R.H.Mayer, D.Nisius, W.Reviol, M.Sferrazza
Spectroscopy of the Superdeformed Band in 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4n), E=142-151 MeV; measured Eγ, Iγ, γγ-coin, DSA. 196Pb deduced superdeformed band transitions, intrinsic quadrupole moment, dynamic moment of inertia. Model comparison.
Phys.Lett. 305B, 195 (1993)
W.Nazarewicz
Variety of Shapes in the Mercury and Lead Isotopes
NUCLEAR STRUCTURE 166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200Hg, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210Pb; calculated shape coexistence configurations excitation energies; deduced prolate, oblate shapes competition. Axial reflection-asymmetric Woods-Saxon model. Other nuclei, intruder states discussed.
doi: 10.1016/0370-2693(93)90107-S
Phys.Rev. C47, 1921 (1993)
G.Rotbard, G.Berrier, M.Vergnes, S.Fortier, J.Kalifa, J.M.Maison, L.Rosier, J.Vernotte, P.Van Isacker, J.Jolie
Transfer Results for Odd-Odd 196Au and the Extended Supersymmetry
NUCLEAR REACTIONS 197Au(p, d), E=25 MeV; measured σ(θ), σ(Ed). 196Au deduced levels, L, possible J, π, spectroscopic factors.
Phys.Rev. C48, 140 (1993)
R.Tanczyn, G.Kumbartzki, A.Pique, T.Vass, A.Pakou, N.Benczer-Koller
Calibration of the Transient Field for Pt Ions in Gadolinium and Magnetic Moments of the 2+1 States in 196,198Pt
NUCLEAR REACTIONS 148Nd, 194,196Pt(32S, 32S'), E=77 MeV; 198Pt(32S, 32S'), E=80 MeV; 194,196,198Pt(58Ni, 58Ni'), E=150 MeV; measured γ(particle)-coin, Iγ(θ) precession following Coulomb excitation; deduced average transient field, Pt and Nd ions recoiling through Gd. 194,196,198Pt levels deduced relative g.
Phys.Rev. C47, 1447 (1993)
J.Wauters, P.Dendooven, M.Huyse, G.Reusen, P.Van Duppen, P.Lievens, and the ISOLDE Collaboration
α-Decay Properties of Neutron-Deficient Polonium and Radon Nuclei
RADIOACTIVITY 192,193m,193,194,195,195m,196,197,197m,198,199,199m,200,201,201m,202,204,206,208,210,212,214,216,218Po, 198,199,199m,200,201,202,203,204,205,206,207,208,209Rn(α); measured Eα, T1/2, α-branching ratios, reduced widths; deduced intruder configuration role. Data on 170-188Pt, 176-188Hg, 182-210Pb isotopes also discussed.
Phys.Lett. 312B, 372 (1993)
A.Wolf, O.Scholten, R.F.Casten
F-Spin Purity of 2+1 States in Even-Even Nuclei
NUCLEAR STRUCTURE 110Pd, 152Sm, 154Gd, 168Er, 184W, 130,132Ba, 186,192Os, 146,148Ce, 150Nd, 192,194,196Pt, 170Yb, 180Hf; analyzed g factor data; deduced F-spin purity upper limits.
doi: 10.1016/0370-2693(93)90969-O
Phys.Rev. C48, 1745 (1993)
N.V.Zamfir, P.D.Cottle, J.L.Johnson, R.F.Casten
Octupole Fragmentation and O(6) Symmetry in Even-A Pt Isotopes
NUCLEAR STRUCTURE 194Pt, 146Nd, 168Er, 192Os; calculated B(λ). 194,196,198Pt; calculated octupole fragmentation; deduced O(6) dynamical symmetry role.
Phys.Rev. C50, 1222 (1994)
R.M.Clark, R.Wadsworth, K.Hauschild, I.M.Hibbert, E.Dragulescu, C.W.Beausang, M.H.Bergstrom, S.Clarke, P.J.Dagnall, P.M.Jones, E.S.Paul, A.T.Semple, J.F.Sharpey-Schafer, J.Simpson, W.Satula, R.Wyss
Superdeformation in the Pb Nuclei and the Evolution of the Dynamic Moments of Inertia
NUCLEAR REACTIONS 186W(18O, xn), E=113 MeV; measured Eγ, Iγ, γγ-coin. 194,196,198Pb deduced superdeformed band features, dynamic moments of inertia. Comparison with cranked Woods-Saxon calculations. Enriched targets, hyperpure Ge detectors, BGO suppression shields.
Phys.Rev. C52, 621 (1995)
L.A.Bernstein, J.A.Cizewski, H.-Q.Jin, W.Younes, R.G.Henry, L.P.Farris, A.Charos, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, I.G.Bearden, D.Ye, J.A.Becker, E.A.Henry, M.J.Brinkman, J.R.Hughes, A.Kuhnert, T.F.Wang, M.A.Stoyer, R.M.Diamond, F.S.Stephens, M.A.Deleplanque, A.O.Macchiavelli, I.Y.Lee, B.Cederwall, J.R.B.Oliveira, J.Burde, P.Fallon, C.Duyar, J.E.Draper, E.Rubel, D.T.Vo
Onset of Collectivity in Neutron Deficient 196,198Po
NUCLEAR REACTIONS 172Yb(28Si, 4n), E=141, 142, 145 MeV; 174Yb(29Si, 5n), E=141, 146 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, DCO ratios. 196,198Po deduced levels, J, π, γ-multipolarity, B(λ) ratios, γ-ray branching ratios. Single-particle, vibrational phonon models, systematics of the Po isotopes studied.
Phys.Rev.Lett. 75, 4571 (1995)
N.Bijnens, P.Decrock, S.Franchoo, M.Gaelens, M.Huyse, H.-Y.Hwang, G.Reusen, J.Szerypo, J.von Schwarzenberg, J.Wauters, J.G.Correia, A.Jokinen, P.Van Duppen, and the ISOLDE Collaboration
Intruder States and the Onset of Deformation in the Neutron-Deficient Even-Even Polonium Isotopes
RADIOACTIVITY 200,198Rn(α) [from Th(p, X), E=1 GeV]; measured Iα, (αe)-, α(X-ray)-coin. 200,202At(EC), (β+) [from Re(20Ne, X), E=200 MeV]; measured γγ(t), γe(t), γ(X-ray)(t), I(ce). 198Rn deduced T1/2. 196,194,198Po deduced level, J, π, configuration. 202,200Po deduced levels, J, π, configuration, ICC, γ multipolarity. Other data input.
doi: 10.1103/PhysRevLett.75.4571
Phys.Rev. C51, R1052 (1995)
R.M.Clark, S.Bouneau, F.Azaiez, S.Asztalos, J.A.Becker, B.Cederwall, M.A.Deleplanque, R.M.Diamond, J.Duprat, P.Fallon, L.P.Farris, E.A.Henry, J.R.Hughes, W.H.Kelly, I.Y.Lee, A.O.Macchiavelli, M.G.Porquet, J.F.Sharpey-Schafer, F.S.Stephens, M.A.Stoyer, D.T.Vo, A.N.Wilson
Superdeformation in the Bismuth Nuclei
NUCLEAR REACTIONS 183W(19F, xn), E=108 MeV; measured γγ-coin. 196,197Bi deduced tentative high-spin levels, J, π, evidence for superdeformation.
doi: 10.1103/PhysRevC.51.R1052
Phys.Rev. C51, 115 (1995)
E.F.Moore, M.P.Carpenter, Y.Liang, R.V.F.Janssens, I.Ahmad, I.G.Bearden, P.J.Daly, M.W.Drigert, B.Fornal, U.Garg, Z.W.Grabowski, H.L.Harrington, R.G.Henry, T.L.Khoo, T.Lauritsen, R.H.Mayer, D.Nisius, W.Reviol, M.Sferrazza
Collectivity of Dipole Bands in 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4nγ), E=142 MeV; measured Eγ, Iγ, γγ(θ), oriented nuclei, DSA. 196Pb deduced high-spin levels J, π, T1/2, B(λ). Cranked shell model.
Z.Phys. A352, 7 (1995)
K.Morita, Y.H.Pu, J.Feng, M.G.Hies, K.O.Lee, A.Yoshida, S.C.Jeong, S.Kubono, T.Nomura, Y.Tagaya, M.Wada, M.Kurokawa, T.Motobayashi, H.Ogawa, T.Uchibori, K.Sueki, T.Ishizuka, K.Uchiyama, Y.Fujita, H.Miyatake, T.Shimoda, T.Shinozuka, H.Kudo, Y.Nagai, S.A.Shin
New α-Decaying Neutron Deficient Isotopes 197Rn and 200Fr
NUCLEAR REACTIONS 166Er(36Ar, 5n), E=186, 200 MeV; 169Tm(36Ar, 5n), E=186 MeV; measured Eα, Iα; deduced evidence for 197,197mRn, 200Fr. Evaporation residues obtained from gas-filled recoil separator, implanted onto position sensitive solid state detector.
RADIOACTIVITY 197,197mRn(α) [from 166Er(36Ar, 5n), E=186, 200 MeV]; 200Fr(α) [from 169Tm(36Ar, 5n), E=186 MeV]; 193,193mPo(α) [from 197,197mRn(α-decay)]; 196Rn(α) [from 166Er(36Ar, 6n)]; 192Po(α) [from 196Rn(α-decay)]; 200Fr(α) [from 169Tm(36Ar, 5n), E=186 MeV]; 196At(α) [from 200Fr(α-decay)]; measured Eα, Iα, T1/2, αα-energy correlations. Evaporation residues obtained from gas-filled recoil separator, implanted onto position sensitive solid state detector.
Nucl.Phys. A587, 747 (1995)
U.Moor, G.Rasche, W.S.Woolcock
Electromagnetic Corrections to the Threshold Pion-Pion Charge Exchange Amplitude and the Lifetime of Pionium
doi: 10.1016/0375-9474(95)00050-B
Z.Phys. A353, 15 (1995)
U.J.van Severen, W.Korten, H.Hubel, D.Bazzacco, G.LoBianco, N.H.Medina, C.Rossi Alvarez, S.Signorelli, K.Strahle, P.Willsau
A Pair of Excited Superdeformed Bands in 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4n), E=143 MeV; measured γγ-coin. 196Pb deduced levels, J, π, excited superdeformed bands.
Z.Phys. A355, 337 (1996)
G.Baldsiefen, H.Hubel, W.Korten, U.J.van Severen, J.A.Cizewski, N.H.Medina, D.R.Napoli, C.Rossi Alvarez, G.Lo Bianco, S.Signorelli
Crossing of Shears Bands in 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4n), E=143 MeV; measured γγ-coin. 196Pb deduced high-spin levels, J, π, band structure.
Phys.Rev. C53, 117 (1996)
R.M.Clark, S.Bouneau, A.N.Wilson, B.Cederwall, F.Azaiez, S.Asztalos, J.A.Becker, L.Bernstein, M.J.Brinkman, M.A.Deleplanque, I.Deloncle, R.M.Diamond, J.Duprat, P.Fallon, L.P.Farris, E.A.Henry, J.R.Hughes, W.H.Kelly, I.Y.Lee, A.O.Macchiavelli, M.G.Porquet, J.F.Sharpey-Schafer, F.S.Stephens, M.A.Stoyer, D.T.Vo
Superdeformation in Bismuth
NUCLEAR REACTIONS 183W(19F, 5n), (19F, 6n), (19F, 7n), E=108 MeV; 181Ta(20Ne, 4n), (20Ne, 5n), (20Ne, 6n), E=123 MeV; measured γγ-coin. 195,196,197Bi deduced superdeformed bands.
Z.Phys. A354, 1 (1996)
T.Enqvist, K.Eskola, A.Jokinen, M.Leino, W.H.Trzaska, J.Uusitalo, V.Ninov, P.Armbruster
Alpha Decay Properties of 200-202Fr
NUCLEAR REACTIONS 170Yb(35Cl, 5n), E=5.3 MeV/nucleon; measured production σ.
RADIOACTIVITY 200,201,202Fr, 196,197,198At(α) [from 170Yb(35Cl, xn), E=4.9-5.3 MeV/nucleon and subsequent decay]; measured Eα, Iα, T1/2.
Phys.Rev. C54, 2926 (1996)
R.B.E.Taylor, S.J.Freeman, J.L.Durell, M.J.Leddy, A.G.Smith, D.J.Blumenthal, M.P.Carpenter, C.N.Davids, C.J.Lister, R.V.F.Janssens, D.Seweryniak
γ Decay from States at Low Excitation Energy in the Neutron-Deficient Isotope, 200Rn, Identified by Correlated Radioactive Decay
NUCLEAR REACTIONS 176Hf(28Si, xn), E=142 MeV; measured Eγ, Iγ, γ(recoil)-coin, Eα, Iα following residuals radioactive decays, (mass)α-correlations. 200,202Rn deduced levels.
RADIOACTIVITY 200,201,202,203,204Rn [from 176Hf(28Si, xn), E=142 MeV]; 196,197,198,199,200Po(α) [from 200,201,202,203,204Rn(α-decay)]; 199,200,201,202,203At(α); measured αα-correlations, Eα, γα-coin, T1/2.
Phys.Rev.Lett. 76, 2029 (1996)
P.von Brentano, J.Eberth, J.Enders, L.Esser, R.-D.Herzberg, N.Huxel, H.Meise, P.von Neumann-Cosel, N.Nicolay, N.Pietralla, H.Prade, J.Reif, A.Richter, C.Schlegel, R.Schwengner, S.Skoda, H.G.Thomas, I.Wiedenhover, G.Winter, A.Zilges
First Observation of the Scissiors Mode in a γ-Soft Nucleus: The case of 196Pt
NUCLEAR REACTIONS 196Pt(γ, γ'), E ≤ 4.7 MeV bremsstrahlung; measured γ spectra. 196Pt deduced levels, J, π, Γ0/Γ, B(λ).
doi: 10.1103/PhysRevLett.76.2029
Acta Phys.Hung.N.S. 6, 289 (1997)
F.Azaiez, S.Bouneau, J.Duprat, I.Deloncle, M.-G.Porquet, U.J.van Severen, T.Nakatsukasa, M.M.Aleonard, A.Astier, G.Baldsiefen, C.W.Beausang, F.A.Beck, C.Bourgeois, D.Curien, N.Dozie, L.Ducroux, B.Gall, H.Hubel, M.Kaci, W.Korten, M.Meyer, N.Redon, H.Sergolle, J.F.Sharpey-Schafer
Octupole Vibrations of the Superdeformed 196Pb Nucleus
NUCLEAR REACTIONS 186W(16O, 6n), E=110 MeV; measured Eγ, Iγ, γγ-coin. 196Pb deduced superdeformed bands, possible octupole vibrations.
Z.Phys. A358, 179 (1997)
S.Bouneau, F.Azaiez, J.Duprat, I.Deloncle, M.-G.Porquet, U.J.van Severen, T.Nakatsukasa, M.-M.Aleonard, A.Astier, G.Baldsiefen, C.W.Beausang, F.A.Beck, C.Bourgeois, D.Curien, N.Dozie, L.Ducroux, B.J.P.Gall, H.Hubel, M.Kaci, W.Korten, M.Meyer, N.Redon, H.Sergolle, J.F.Sharpey-Schafer
New Results on the Superdeformed 196Pb Nucleus: Decay of the excited bands to the yrast band
NUCLEAR REACTIONS 186W(16O, 6n), E=110 MeV; measured Eγ, Iγ, γγγ-coin. 196Pb deduced superdeformed bands, dynamical moments of inertia. RPA model comparisons.
Z.Phys. A358, 133 (1997)
J.A.Cizewski, W.Younes
Onset of Deformation in Polonium Nuclei
NUCLEAR STRUCTURE 194,196,198,200,202,204,206,208Po; calculated levels, wavefunctions; deduced proton-neutron interaction role in collective motion increase. Particle-core model, QRPA.
Yad.Fiz. 60, No 4, 581 (1997); Phys.Atomic Nuclei 60, 503 (1997)
A.M.Demidov, L.I.Govor, V.A.Kurkin, I.V.Mikhailov
Signs of the Multipole-Mixing Ratios for 2+(2, 3)-2+1 and 3+1-2+1 Transitions in Even-Even Nuclei
NUCLEAR STRUCTURE 52Cr, 54,56,58Fe, 62,64,68,70Zn, 70,72,74,76Ge, 74,76,78Se, 80,82Kr, 84Sr, 96Mo, 100,102,104,106,108Ru, 104,106Pd, 106,108,110,112,114,116Cd, 116,120,122,124Sn, 122,126,128,130Te, 124,126,128,132,134Xe, 130,132,134,136,138,140Ba, 140,142Ce, 142,144,146,148,150Nd, 146,148,150,152Sm, 152,154,156Gd, 160,164Dy, 166,168,170Er, 182,184,186W, 174,176,178,180,182,184,186,188,190,192Os, 192,196Pt, 204,206Pb; analyzed, reviewed δ data for certain transitions; deduced model parameters dependence. Interacting boson model.
Nucl.Phys. A621, 802 (1997)
C.De Coster, B.Decroix, K.Heyde, J.L.Wood, J.Jolie, H.Lehmann
Particle-Hole Excitations in the Interacting Boson Model (III): The O(6)-SU(3) coupling
NUCLEAR STRUCTURE 180,182,184,186Os, 184,186,188,190Po, 180,178W, 190,192,182,184Pt, 196,194,188,186Pb, 192,190Rn, 196Th; calculated levels. 182,184,186,188,190,192,194,196,198Pt; calculated g factors. Extended interacting boson model.
doi: 10.1016/S0375-9474(97)00195-4
Z.Phys. A358, 181 (1997)
I.Deloncle, M.Kaci, M.G.Porquet, J.Duprat, F.Azaiez, S.Bouneau, C.Bourgeois, H.Sergolle
Highest Spin Reached in the Superdeformed Well in the A ≈ 190 Mass Region
NUCLEAR STRUCTURE 190,192,194Hg, 193,195Tl, 192,194,196,198Pb, 190Po; analyzed superdeformed bands maximum spin vs fissility parameter; deduced linear relationship.
Phys.Lett. 405B, 25 (1997)
M.K.Harder, K.T.Tang, P.Van Isacker
An IBM Description of Coexistence in the Platinum Isotopes
NUCLEAR STRUCTURE A=172-192; calculated levels for Pt isotopes. 184,186,188,190,192,194,196,198Pt; analyzed g for 2+ states, isotope shifts. Configuration mixing, interacting boson model approach.
doi: 10.1016/S0370-2693(97)00612-6
Phys.Rev. C56, 2440 (1997)
J.K.Jewell, P.D.Cottle, K.W.Kemper, L.A.Riley
Octupole States in 196Pt(p, p'γ)
NUCLEAR REACTIONS 196Pt(p, p'γ), E=12.7 MeV; measured Eγ, Iγ, Ep, Ip, pγ-coin. 196Pt deduced levels, J, π, possible octupole, mixed symmetry states.
At.Data Nucl.Data Tables 66, 131 (1997)
P.Moller, J.R.Nix, K.-L.Kratz
Nuclear Properties for Astrophysical and Radioactive-Ion-Beam Applications
NUCLEAR STRUCTURE Z=8-136; A=16-339; calculated, compiled total binding energy, one-, two-neutron, proton separation energies, pairing gaps, odd-nucleon parity, spin projection. Folded-Yukawa single particle potential, Lipkin-Nogami approximation.
RADIOACTIVITY Z=8-136; A=16-339; calculated, compiled β-, α-decay Q, T1/2. Folded-Yukawa single particle potential, Lipkin-Nogami approximation.
Z.Phys. A357, 1 (1997)
Y.H.Pu, K.Morita, M.G.Hies, K.O.Lee, A.Yoshida, T.Nomura, Y.Tagaya, T.Motobayashi, M.Kurokawa, H.Minemura, T.Uchibori, T.Ariga, K.Sueki, S.A.Shin
New α-Decaying Neutron-Deficient Isotope 196Rn
NUCLEAR REACTIONS 166Er(36Ar, 6n), (36Ar, xnypzα), E=208 MeV; measured Eα, αα-correlations; deduced 196Rn production σ. 196Rn deduced α-decay T1/2.
RADIOACTIVITY 197,197m,196Rn(α) [from 166Er(36Ar, xn), E=208 MeV]; 192Po(α) [from 196Rn(α-decay)]; measured Eα, α-correlation. 196Rn deduced T1/2.
Proc.Conf on Exotic Nuclei and Atomic Masses, Bellaire, Michigan, June 23-27, 1998, p.486 (1998); AIP Conf.Proc. 455 (1998)
J.A.Cizewski, K.Y.Ding, N.Fotiades, D.P.McNabb, W.Younes, R.Julin, M.Leino, J.Cocks, P.Greenlees, K.Helariutta, P.Jones, S.Juutinen, H.Kankaanpaa, H.Kettunen, P.Kuusiniemi, M.Muikku, P.Rahkila, A.Savelius, C.N.Davids, R.V.F.Janssens, D.Seweryniak, M.P.Carpenter, H.Amro, P.Decrock, P.Reiter, D.Nisius, L.T.Brown, S.Fischer, T.Lauritsen, J.Wauters, C.R.Bingham, M.Huyse, A.Andreyev
Evolution of Collective Motion in Light Polonium Nuclei
NUCLEAR REACTIONS 172Yb(28Si, 4n), E=143 MeV; measured Eγ, Iγ, (recoil)γ-coin. 196Po deduced levels, J, π, B(E2), branching ratios. Jurosphere array. Level systematics in neighboring isotopes discussed. Recoil-decay tagging technique.
Phys.Lett. 440B, 251 (1998)
R.M.Clark, R.Krucken, S.J.Asztalos, J.A.Becker, B.Busse, S.Chmel, M.A.Deleplanque, R.M.Diamond, P.Fallon, D.Jenkins, K.Hauschild, I.M.Hibbert, H.Hubel, I.Y.Lee, A.O.Macchiavelli, R.W.MacLeod, G.Schmid, F.S.Stephens, U.J.van Severen, K.Vetter, R.Wadsworth, S.Wan
The Shears Mechanism in the Lead Isotopes
NUCLEAR REACTIONS 172,174,176Yb(26Mg, xn), E=135, 137, 139 MeV; measured Eγ, Iγ, γγ-coin, DSA. 193,194,195,196,197Pb deduced rotational bands transitions T1/2, B(M1), shears mechanism. Magnetic rotation, tilted axis cranking.
doi: 10.1016/S0370-2693(98)01179-4
Acta Phys.Pol. B29, 2999 (1998)
H.Clement, R.Bilger, A.Denig, K.Fohl, J.Grater, W.Kluge, R.Meier, J.Patzold, M.G.Schepkin, G.J.Wagner, for the LEPS Collaboration
Pionic Double Charge Exchange
Phys.Lett. 434B, 14 (1998)
U.J.van Severen, R.M.Clark, R.Krucken, H.Hubel, S.J.Asztalos, J.A.Becker, B.C.Busse, M.A.Deleplanque, R.M.Diamond, P.Fallon, K.Hauschild, I.M.Hibbert, I.Y.Lee, A.O.Macchiavelli, R.W.MacLeod, G.Schmid, F.S.Stephens, K.Vetter, R.Wadsworth, S.Wan
Comparative Quadrupole Moments of Superdeformed Bands in 193-196Pb
NUCLEAR REACTIONS 172,174,176Yb(26Mg, xn)192Pb/193Pb/194Pb/195Pb/196Pb/197Pb, E=135-139 MeV; measured Eγ, Iγ, γγ-coin, DSA. 193,194,195,196Pb deduced superdeformed bands T1/2, quadrupole moments, configurations.
doi: 10.1016/S0370-2693(98)00819-3
Phys.Rev.Lett. 83, 1542 (1999)
A.Metz, J.Jolie, G.Graw, R.Hertenberger, J.Groger, C.Gunther, N.Warr, Y.Eisermann
Evidence for the Existence of Supersymmetry in Atomic Nuclei
NUCLEAR REACTIONS 196Pt, 197Au(p, d), E=26 MeV; 196Pt, 197Au(polarized d, t), E=25 MeV; 198Hg(polarized d, α), E=18 MeV; measured particle spectra, σ(θ), analyzing powers; deduced absolute transfer strengths. 195Pt, 196Au deduced levels, J, π, configurations, supersymmetry related features. Interacting boson model.
doi: 10.1103/PhysRevLett.83.1542
Phys.Rev. C59, 673 (1999)
R.B.E.Taylor, S.J.Freeman, J.L.Durell, M.J.Leddy, S.D.Robinson, B.J.Varley, J.F.C.Cocks, K.Helariutta, P.Jones, R.Julin, S.Juutinen, H.Kankaanpaa, A.Kanto, H.Kettunen, P.Kuusiniemi, M.Leino, M.Muikku, P.Rahkila, A.Savelius, P.T.Greenlees
γ Decay of Excited States in 198Rn Identified using Correlated Radioactive Decay
NUCLEAR REACTIONS 166Er(36Ar, X), (36Ar, 4n), E=175 MeV; measured Eγ, Iγ, (recoil)γ-coin. 198Rn deduced levels, J, π, deformed intruder states. 195,196Po, 198,199At deduced transitions, intensities. Recoil decay tagging, Jurosphere array, recoil separator.
RADIOACTIVITY 195,196Po, 198,199At, 198Rn(α); measured Eα(t).
Phys.Rev. C62, 064304 (2000)
J.Groger, J.Jolie, R.Krucken, C.W.Beausang, M.Caprio, R.F.Casten, J.Cederkall, J.R.Cooper, F.Corminboeuf, L.Genilloud, G.Graw, C.Gunther, M.de Huu, A.I.Levon, A.Metz, J.R.Novak, N.Warr, T.Wendel
Nuclear Structure of 196Au: More evidence for its supersymmetric description
NUCLEAR REACTIONS 196Pt(p, n), (p, 2n), E=9.1-11.7 MeV; measured Eγ, Iγ, γ-ray excitation functions. 196Pt(p, n), E=9.1 MeV; measured Eγ, Iγ, E(Ce), I(ce), (X-ray)γ-, (ce)γ-, γγ-coin. 196Au deduced levels, J, π. Comparison with extended supersymmetry model predictions.
doi: 10.1103/PhysRevC.62.064304
J.Phys.(London) G26, 787 (2000)
M.B.Smith, R.Chapman, J.F.C.Cocks, K.-M.Spohr, O.Dorvaux, K.Helariutta, P.M.Jones, R.Julin, S.Juutinen, H.Kankaanpaa, H.Kettunen, P.Kuusiniemi, Y.Le Coz, M.Leino, D.J.Middleton, M.Muikku, P.Nieminen, P.Rahkila, A.Savelius
Isomeric State in the Doubly Odd 196At Nucleus
NUCLEAR REACTIONS 165Ho(36Ar, 5n), E=178 MeV; measured Eα, Eγ, αγ-coin, T1/2, conversion coefficient. 196At deduced isomer energy, spin, T1/2, γ decay multipolarity. Recoil decay tagging method.
doi: 10.1088/0954-3899/26/6/303
Acta Phys.Pol. B32, 2655 (2001)
D.L.Balabanski, K.Vyvey, G.Neyens, D.Almehed, P.Blaha, D.Borremans, S.Chmel, N.Coulier, R.Coussement, W.De Clercq, S.Frauendorf, G.Georgiev, H.Hubel, A.Lepine-Szily, M.Mineva, N.Nenoff, S.Pancholi, D.Rossbach, R.Schwengner, S.Teughels, P.M.Walker
Quadrupole Moments of High-Spin Isomers: Test of the tilted-axis cranking model
NUCLEAR REACTIONS 170Er(13C, 4n), E=63 MeV; Re(14N, xn)196Pb, E not given; measured Eγ, Iγ(θ, H, t). 179W, 196Pb deduced quadrupole moments for high-spin isomers. Level-mixing spectroscopy technique. Comparison with tilted-axis cranking predictions.
Acta Phys.Pol. B32, 2673 (2001)
H.Hubel
Spectroscopy of Superdeformed Pb Isotopes
NUCLEAR REACTIONS 168Er(30Si, 5n), E=160 MeV; measured Eγ, Iγ, γγ-coin. 170Er(30Si, 4n), E=144 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 193,196Pb deduced superdeformed bands, J, π, configurations. 196Pb deduced octupole vibrational excitation. Gammasphere, Euroball arrays.
Phys.Rev. C63, 044315 (2001)
H.Kettunen, J.Uusitalo, M.Leino, P.Jones, K.Eskola, P.T.Greenlees, K.Helariutta, R.Julin, S.Juutinen, H.Kankaanpaa, P.Kuusiniemi, M.Muikku, P.Nieminen, P.Rahkila
α Decay Studies of the Nuclides 195Rn and 196Rn
RADIOACTIVITY 191,191m,192Po, 195,195m,196Rn(α) [from 142Nd(56Fe, xn) and subsequent decay]; measured Eα, T1/2; deduced possible deformation features. Mass-separated sources.
doi: 10.1103/PhysRevC.63.044315
Eur.Phys.J. A 11, 121 (2001)
G.Kemper, A.Dewald, I.Wiedenhover, R.Peusquens, S.Kasemann, K.O.Zell, P.von Brentano, H.Hubel, S.Chmel, A.Gorgen, D.Bazzacco, R.Venturelli, S.Lunardi, D.R.Napoli, F.Hannachi, A.Lopez-Martens, R.Krucken, J.R.Cooper, R.M.Clark, M.A.Deleplanque, I.Y.Lee, A.O.Machiavelli, F.S.Stephens
Investigation of the Magnetic Rotation in 196Pb
NUCLEAR REACTIONS 164Dy(36S, 4n), E=168 MeV; measured Doppler-shifted Eγ, γγ-coin. 196Pb deduced high-spin levels, J, π, magnetic rotational band, T1/2, B(M1), role of shears mechanism. Euroball array, coincidence recoil distance technique.
Phys.Rev. C63, 047307 (2001)
K.Lindenberg, F.Neumann, D.Galaviz, T.Hartmann, P.Mohr, K.Vogt, S.Volz, A.Zilges
Half-Lives of Au, Hg, and Pb Isotopes from Photoactivation
RADIOACTIVITY 196Au(β-), (EC); 195,197Hg, 203Pb(EC); 203Hg(β-); 199mHg, 204mPb(IT); measured T1/2. Photoactivation technique.
doi: 10.1103/PhysRevC.63.047307
Phys.Lett. 513B, 9 (2001)
D.Rossbach, A.Gorgen, H.Hubel, E.Mergel, G.Schonwasser, A.N.Wilson, F.Azaiez, A.Astier, D.Bazzacco, M.Bergstrom, C.Bourgeois, N.Buforn, F.Hannachi, K.Hauschild, A.Korichi, W.Korten, T.Kroll, A.Lopez-Martens, R.Lucas, H.J.Maier, N.Redon, P.Reiter, C.Rossi-Alvarez, O.Stezowski, P.Thirolf
Evidence for Octupole Vibration in Superdeformed 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4n), E=144 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 196Pb deduced high-spin levels, superdeformed bands, octupole vibration. Euroball IV array.
doi: 10.1016/S0370-2693(01)00749-3
Phys.Rev. C64, 054614 (2001)
E.Tavukcu, L.A.Bernstein, K.Hauschild, J.A.Becker, P.E.Garrett, C.A.McGrath, D.P.McNabb, W.Younes, M.B.Chadwick, R.O.Nelson, G.D.Johns, G.E.Mitchell
196Pt(n, xnypγ) Reactions using Spallation Neutrons from En = 1 to 250 MeV
NUCLEAR REACTIONS 196Pt(n, xnyp)184Pt/186Pt/188Pt/190Pt/191Pt/192Pt/193Pt/194Pt/194Pt/196Pt/189Ir/191Ir/193Ir, E=1-250 MeV; measured prompt Eγ, Iγ, γγ-coin; deduced γ-ray excitation functions. Comparison with model predictions.
doi: 10.1103/PhysRevC.64.054614
Phys.Rev. C66, 024316 (2002)
D.Rossbach, A.Gorgen, H.Hubel, E.Mergel, G.Schonwasser, F.Azaiez, C.Bourgeois, F.Hannachi, A.Korichi, A.Lopez-Martens, A.Astier, N.Buforn, N.Redon, O.Stezowski, D.Bazzacco, T.Kroll, C.Rossi-Alvarez, K.Hauschild, W.Korten, R.Lucas, H.J.Maier, P.Reiter, P.G.Thirolf
Lifetimes in the yrast and an octupole-vibrational superdeformed band in 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4n), E=144 MeV; measured Eγ, Iγ, γγ-coin, DSA. 196Pb deduced superdeformed band transitions T1/2, B(E2), transition quadrupole moments, configuration. Euroball array.
doi: 10.1103/PhysRevC.66.024316
Nucl.Phys. A707, 3 (2002)
A.K.Singh, N.Nenoff, D.Rossbach, A.Gorgen, S.Chmel, F.Azaiez, A.Astier, D.Bazzacco, M.Belleguic, S.Bouneau, C.Bourgeois, N.Buforn, B.Cederwall, I.Deloncle, J.Domscheit, F.Hannachi, K.Hauschild, H.Hubel, A.Korichi, W.Korten, T.Kroll, Y.LeCoz, A.Lopez-Martens, R.Lucas, S.Lunardi, H.J.Maier, E.Mergel, M.Meyer, C.M.Petrache, N.Redon, P.Reiter, C.Rossi-Alvarez, G.Schonwasser, O.Stezowski, P.G.Thirolf, A.N.Wilson
Detailed Study of Magnetic Rotation in 196Pb
NUCLEAR REACTIONS 186W(16O, 6n), E=110 MeV; 170Er(30Si, 4n), E=144 MeV; measured γγ-coin, Eγ, Iγ, DCO ratios, linear polarization. 196Pb deduced levels, magnetic dipole bands. Shears bands, magnetic rotation, tilted-axis cranking calculations.
doi: 10.1016/S0375-9474(02)00966-1
Phys.Rev. C 66, 064314 (2002)
A.K.Singh, H.Hubel, D.Rossbach, S.Chmel, A.Gorgen, E.Mergel, G.Schonwasser, F.Azaiez, C.Bourgeois, F.Hannachi, A.Korichi, A.Lopez-Martens, A.Astier, N.Buforn, N.Redon, O.Stezowski, D.Bazzacco, T.Kroll, C.Rossi-Alvarez, K.Hauschild, W.Korten, R.Lucas, H.J.Maier, P.Reiter, P.G.Thirolf, A.N.Wilson
Lifetimes of magnetic-rotational bands in 196Pb
NUCLEAR REACTIONS 170Er(30Si, 4n), E=144 MeV; measured Eγ, Iγ, γγ-coin, DSA. 196Pb deduced rotational bands transitions T1/2, B(M1). Euroball array. Comparison with model predictions.
doi: 10.1103/PhysRevC.66.064314
Phys.Rev. C65, 064309 (2002)
E.Tavukcu, L.A.Bernstein, K.Hauschild, J.A.Becker, P.E.Garrett, C.A.McGrath, D.P.McNabb, W.Younes, P.Navratil, R.O.Nelson, G.D.Johns, G.E.Mitchell, J.A.Cizewski
State in 196Pt Observed with the (n, n'γ) Reaction
NUCLEAR REACTIONS 196Pt(n, n'γ), E=1-8 MeV; measured Eγ, Iγ, γγ-coin; deduced γ-ray excitation functions. 196Pt deduced levels, J, π. Geanie array, interacting boson model calculations.
doi: 10.1103/PhysRevC.65.064309
Phys.Rev.Lett. 88, 102502 (2002)
K.Vyvey, S.Chmel, G.Neyens, H.Hubel, D.L.Balabanski, D.Borremans, N.Coulier, R.Coussement, G.Georgiev, N.Nenoff, S.Pancholi, D.Rossbach, R.Schwengner, S.Teughels, S.Frauendorf
Quadrupole Moment of the 11- Intruder Isomer in 196Pb and Its Implications for the 16- Shears Band Head
NUCLEAR REACTIONS 187Re(14N, 5n), E=87 MeV; measured Eγ, Iγ(0°)/Iγ(90°) vs magnetic field strength following implantation on Re host. 196Pb deduced high-spin magnetic moment, absolute value of quadrupole moment, shears bandhead quadrupole moment, deformation parameters. Level mixing spectroscopy technique, comparison with Tilted Axis Cranking model.
doi: 10.1103/PhysRevLett.88.102502
Nucl.Phys. A729, 337 (2003)
G.Audi, A.H.Wapstra, C.Thibault
The AME2003 atomic mass Evaluation (II). Tables, graphs, and references
COMPILATION A=1-293; compiled, evaluated atomic mass data.
doi: 10.1016/j.nuclphysa.2003.11.003
Acta Phys.Pol. B34, 2395 (2003)
K.A.Gladnishki, Zs.Podolyak, J.Gerl, M.Hellstrom, Y.Kopatch, S.Mandal, M.Gorska, P.H.Regan, H.J.Wollersheim, A.Banu, G.Benzoni, H.Boardman, M.La Commara, J.Ekman, C.Fahlander, H.Geissel, H.Grawe, E.Kaza, A.Korgul, M.Matos, M.N.Mineva, R.D.Page, C.J.Pearson, C.Plettner, D.Rudolph, Ch.Scheidenberger, V.Shishkin, D.Sohler, K.Summerer, J.J.Valiente-Dobon, H.Weick, M.Winkler
Isomer spectroscopy in the neutron-deficient lead region following projectile fragmentation
RADIOACTIVITY 188Hg, 192Tl, 192,193,194,195,196Pb, 195,197,199Bi, 198,200Po(IT) [from Be(238U, X)]; measured Eγ, Iγ, T1/2.
Phys.Rev. C 69, 024617 (2004)
K.A.Gladnishki, Zs.Podolyak, P.H.Regan, J.Gerl, M.Hellstrom, Y.Kopatch, S.Mandal, M.Gorska, R.D.Page, H.J.Wollersheim, A.Banu, G.Benzoni, H.Boardman, M.La Commara, J.Ekman, C.Fahlander, H.Geissel, H.Grawe, E.Kaza, A.Korgul, M.Matos, M.N.Mineva, C.J.Pearson, C.Plettner, D.Rudolph, Ch.Scheidenberger, K.-H.Schmidt, V.Shishkin, D.Sohler, K.Summerer, J.J.Valiente-Dobon, P.M.Walker, H.Weick, M.Winkler, O.Yordanov
Angular momentum population in the projectile fragmentation of 238U at 750 MeV/nucleon
NUCLEAR REACTIONS Be(238U, X)188Hg/192Tl/192Pb/193Pb/194Pb/195Pb/196Pb/195Bi/197Bi/198Po/200Po/202Po, E=750 MeV/nucleon; measured delayed Eγ, Iγ, (fragment)γ-coin; deduced isomer yield ratios, angular momentum population. 188Hg, 192Tl, 192,193,194,195,196Pb, 195,197Bi, 198,200,202Po deduced isomeric levels T1/2. Mass separator, comparison with model predictions.
doi: 10.1103/PhysRevC.69.024617
Eur.Phys.J. A 20, 47 (2004)
E.Gueorguieva, J.J.Lawrie, P.Mutshena, M.Benatar, W.Damon, P.Kwinana, G.K.Mabala, S.Mukherjee, S.M.Mullins, N.J.Ncapayi, R.T.Newman, D.G.Roux, F.D.Smit, J.F.Sharpey-Schafer, Z.Vilakazi, P.Vymers
New nanosecond isomers identified with the AFRODITE array
NUCLEAR REACTIONS 198Pt(α, 6n), E=65 MeV; 142Nd(27Al, 5n), E=150 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 196Hg, 164Ta deduced isomeric states features. Afrodite array, recoil shadow anisotropy method.
doi: 10.1140/epja/i2002-10320-5
nucl-ex/0410023, 10/18/2004 (2004)
A.Prevost, B.Rosse, M.Meyer, N.Redon, C.Schmitt, O.Stezowski, P.Lautesse, A.Astier, I.Deloncle, M.-G.Porquet, T.Duguet, H.Hubel, E.Mergel, D.Rossbach, N.Nenoff, G.Schonwasser, D.Curien, G.Duchene, B.J.P.Gall, J.Robin, J.P.Vivien
Observation of the lowest energy γ-ray in any superdeformed nucleus : 196Bi
NUCLEAR REACTIONS 184W(19F, 7n), E=114 MeV; measured Eγ, Iγ, γγ-coin. 196Bi deduced superdeformed band transitions, configuration. Euroball IV array.
Phys.Rev. C 69, 054605 (2004)
N.Takigawa, S.Ayik, K.Washiyama, S.Kimura
Quantum effect in the diffusion along a potential barrier: Comments on the synthesis of superheavy elements
doi: 10.1103/PhysRevC.69.054605
Phys.Rev. C 69, 064318 (2004)
K.Vyvey, G.D.Dracoulis, A.N.Wilson, P.M.Davidson, A.E.Stuchbery, G.J.Lane, A.P.Byrne, T.Kibedi
g factors of the 9- and 11- isomers in 194Pb and 196Pb: Configuration mixing and deformation
NUCLEAR REACTIONS 170Er(30Si, 4n), E=136 MeV; 170Er(29Si, 5n), E=143 MeV; measured Eγ, Iγ(θ, H, t). 194,196Pb deduced isomeric states g factors, configurations, deformation. Time-dependent perturbed angular distribution technique.
doi: 10.1103/PhysRevC.69.064318
Phys.Rev. C 70, 014610 (2004)
H.-F.Wirth, G.Graw, S.Christen, Y.Eisermann, A.Gollwitzer, R.Hertenberger, J.Jolie, A.Metz, O.Moller, D.Tonev, B.D.Valnion
One- and two-nucleon transfer reactions to 196Au
NUCLEAR REACTIONS 197Au(p, d), E=26 MeV; 194Pt(α, d), E=36 MeV; 195Pt(3He, d), E=36 MeV; measured deuteron spectra, σ(θ). 197Au(polarized d, t), E=25 MeV; 198Hg(polarized d, α), E=18 MeV; measured σ(E, θ), Ay(E, θ). 196Au deduced levels, J, π. Comparison with model predictions, previous results.
doi: 10.1103/PhysRevC.70.014610
Eur.Phys.J. A 23, 243 (2005)
H.De Witte, A.N.Andreyev, S.Dean, S.Franchoo, M.Huyse, O.Ivanov, U.Koster, W.Kurcewicz, J.Kurpeta, A.Plochocki, K.Van de Vel, J.Van de Walle, P.Van Duppen
Alpha-decay of neutron-deficient 200Fr and heavier neighbours
RADIOACTIVITY 200,201,203,205Fr, 196,197,199,201At, 193Bi(α) [from Th(p, X) and subsequent decay]; measured Eα, T1/2. 201Fr, 197At, 193Bi, 189Tl deduced levels, J, π.
doi: 10.1140/epja/i2004-10077-9
Phys.Rev. C 72, 064319 (2005)
G.D.Dracoulis, G.J.Lane, T.M.Peaty, A.P.Byrne, A.M.Baxter, P.M.Davidson, A.N.Wilson, T.Kibedi, F.R.Xu
E3 strength of the 11- to 8+ isomeric decays in 194Pb and 196Pb and oblate deformation
NUCLEAR REACTIONS 170Er(29Si, 5n), E=147 MeV; 170Er(30Si, 4n), E=138 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 194,196Pb deduced levels, J, π, B(E1), B(E2), B(E3), isomer decay features. Caesar array, potential energy surface calculations.
doi: 10.1103/PhysRevC.72.064319
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
Phys.Rev. C 71, 024306 (2005)
J.Uusitalo, M.Leino, T.Enqvist, K.Eskola, T.Grahn, P.T.Greenlees, P.Jones, R.Julin, S.Juutinen, A.Keenan, H.Kettunen, H.Koivisto, P.Kuusiniemi, A.-P.Leppanen, P.Nieminen, J.Pakarinen, P.Rahkila, C.Scholey
α decay studies of very neutron-deficient francium and radium isotopes
NUCLEAR REACTIONS 141Pr(65Cu, xnypzα), E=283-293 MeV; measured delayed Eα, Iα, αα-, (recoil)α-coin; deduced evidence for 199,200,201Rn, 202,203,204Fr, 203,204Ra. 141Pr(63Cu, xnypzα), E=278-288 MeV; measured delayed Eα, Iα, αα-, (recoil)α-coin; deduced evidence for 198,199,200,201,202Rn, 201,202Fr, 201,202Ra. 170Yb(36Ar, xnypzα), E=180-185 MeV; measured delayed Eα, Iα, αα-, (recoil)α-coin; deduced evidence for 201Fr, 203Ra. Gas-filled recoil separator.
RADIOACTIVITY 201,202,203,204Ra, 197,198,199,200Rn, 193,194,195,196Po, 201,202,203,204Fr, 197,198,199,200At(α) [from 141Pr(63,65Cu, xnypzα), 170Yb(36Ar, xnypzα), and subsequent decay]; measured Eα, T1/2, αα-coin for ground and metastable state decay. 193,195Bi, 197,199At, 201,203Fr deduced levels, J, π. Comparisons with previous results.
doi: 10.1103/PhysRevC.71.024306
Phys.Rev.Lett. 95, 182501 (2005)
A.N.Wilson, A.K.Singh, H.Hubel, P.M.Davidson, A.Gorgen, D.Rossbach, A.Korichi, A.Astier, F.Azaiez, D.Bazzacco, C.Bourgeois, N.Buforn, A.P.Byrne, G.D.Dracoulis, F.Hannachi, K.Hauschild, W.Korten, T.Kroll, G.J.Lane, A.Lopez-Martens, N.Redon, P.Reiter, C.Rossi-Alvarez, G.Schonwasser, O.Stezowski, P.G.Thirolf
Excitation Energies of Superdeformed States in 196Pb: Towards a Systematic Study of the Second Well in Pb Isotopes
NUCLEAR REACTIONS 170Er(30Si, 4n), E=144 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 196Pb deduced superdeformed band excitation energy, J, π. Euroball IV array, time-correlated spectroscopy.
NUCLEAR STRUCTURE 192,194,196Pb; analyzed superdeformed bands level energies, binding energies. Several models compared with data.
doi: 10.1103/PhysRevLett.95.182501
Nucl.Phys. A764, 24 (2006)
A.I.Levon, Yu.V.Nosenko, V.A.Onischuk, A.A.Shevchuk, A.E.Stuchbery
Nuclear g factors and structure of high-spin isomers in 190, 192, 194Pt and 196, 198Hg
NUCLEAR REACTIONS 188,190,192Os, 194,196Pt(α, 2n), E=27 MeV; measured Eγ, Iγ(θ, H, t). 190,192,194Pt, 196,198Hg deduced isometric states g factors. Enriched targets, integral perturbed angular distribution technique. Anomalous orbital g factor for neutrons discussed.
doi: 10.1016/j.nuclphysa.2005.09.016