References quoted in the ENSDF dataset: 192 REFERENCES
530 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 52, 375 (1937)
E.McMillan, M.Kamen, S.Ruben
Neutron Induced Radioactivity of the Noble Metals
Phys.Rev. 72, 352 (1947)
P.W.Levy
The Radiations from 60-Day Ir192 and 27-Day Pa233
Arkiv Mat.Astron.Fysik 36A, No.9 (1948)
N.Hole
Contribution to the Study of Nuclear Isomerism
Phys.Rev. 75, 1019 (1949)
G.Wilkinson
Radioactive Isotopes of Platinum and Gold
Phys.Rev. 78, 407 (1950)
R.L.Caldwell
The Internal Conversion Electrons of Several Short-Lived Neutron Induced Radioactivities
Can.J.Phys. 29, 480 (1951)
J.Kastner
The Half-Life of Iridium 192
doi: 10.1139/p51-051
Zhur.Eksptl.i Teoret.Fiz. 21, 1376 (1951)
V.S.Shpinel, N.V.Forafontov
An Investigation of the Radioactive Emissions of Ir192, Ag110 and In114
Izv.Akad.Nauk SSSR, Ser.Fiz. 16, 264 (1952)
A.A.Bashilov, N.M.Antoneva, B.S.Dzhelepov
β-Spectrum of Ir192
J.Am.Chem.Soc. 74, 2457 (1952)
R.W.Fink, E.O.Wiig
Neutron Deficient Mercury Isotopes
Proc.Phys.Soc.(London) 65A, 911 (1952)
J.H.Fremlin, M.C.Walters
An Experimental Investigation of the Stability of Nuclei Against Double Beta-Disintegration
doi: 10.1088/0370-1298/65/11/305
Phys.Rev. 90, 259 (1953)
T.C.Engelder
A Search for Short-Lived Nuclear Isomers
Proc.Roy.Soc.(Canada) 47, 126 (1953)
G.T.Ewan, A.L.Thompson
Conversion Electrons of Au193 and Au192
Z.Naturforsch., 8a, 580 (1953)
Von G.Weber, A.Flammersfeld
Zur Kernisomerie beim 192Ir
Phys.Rev. 93, 124 (1954)
L.P.Gillon, K.Gopalakrishnan, A.deShalit, J.W.Mihelich
Nuclear Spectroscopy of Neutron Deficient Hg Isotopes
Phys.Rev. 96, 1599 (1954)
M.W.Johns, S.V.Nablo
Disintegration of Ir192 and Ir194
Phys.Rev. 96, 444 (1954)
J.P.Mize, M.E.Bunker, J.W.Starner
Radiations from Ir192m
Z.Naturforsch. 9a, 115 (1954)
G.Weber
Kur Kernisomerie beim 52-Vanadium, 165-Dysprosium und 192-Iridium
Phys.Rev. 100, 1364 (1955)
L.L.Baggerly, P.Marmier, F.Boehm, J.W.M.DuMond
Decay of Ir192
Z.Naturforsch. 11a, 143 (1956)
W.Porschen, W.Riezler
Sehr langlebige naturliche α-Strahler
Compt.Rend.Acad.Sci. 245, 523 (1957)
R.Barloutaud, P.Lehmann, A.Leveque
Excitation Coulombienne de l'Osmium
Helv.Phys.Acta 30, 269 (1957)
J.Brunner, J.Halter, C.Perdrisat
Die Zerfallschemata von Hg-Au195 und Hg-Au193
Nuovo Cimento 5, 1456 (1957)
M.S.Huq
Radiation from 192Pt and Proposed Decay Scheme
Nucl.Phys. 4, 240 (1957)
V.M.Kelman, R.Ya.Metskhvarishvili, V.A.Romanov, V.V.Tuchkevich
Investigation of Conversion Lines in the β-Spectrum of Ir192
doi: 10.1016/0029-5582(87)90025-3
Zh.Eksp.Teoret.Fiz. 33, 588 (1957); Soviet Phys.JETP 6, 455 (1958)
V.M.Kelman, R.I.Metskhvarishvili, V.A.Romanov, V.V.Tuchkevich
An Investigation of Conversion Lines in the β Spectrum of Ir192
J.Phys.Radium 19, 60 (1958)
R.Barloutaud, A.Leveque, P.Lehmann, J.Quidort
Niveaux Collectifs dans les Noyaux Pair-Pair entre les Masses 182 et 206
Phys.Rev. 109, 901 (1958)
F.K.McGowan, P.H.Stelson
Yields, Angular Distributions, and Polarization of Gamma Rays from Coulomb Excitation
Nuclear Phys. 7, 296 (1958)
M.V.Mihailovic, B.Povh
The Half-Lives of Some Short-Lived Isotopes
doi: 10.1016/0029-5582(58)90263-3
Arkiv Fysik 13, 549 (1958)
P.A.Tove
Alpha-Emitters with Short Half-Life Induced by Protons on Heavy Elements
Nuovo Cimento 11, 609 (1959)
R.Balzer, H.Knoepfel, J.Lang, R.Muller, P.Stoll
Neutron Capture Gamma-Rays of Iodine, Iridium and Cerium
Z.Physik 156, 293 (1959)
H.Knoepfel, P.Scherrer, P.Stoll
Messung einiger (n, γ)-Spectren mit einem Paarspektrometer hoher Empfindlichkeit
Phys.Rev.Letters 3, 47 (1959)
G.Scharff-Goldhaber, M.McKeown
Triple Isomerism in Ir192
Brit.J.Appl.Phys. 11, 302 (1960)
J.W.Allison
Half-Life of Iridium 192
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
Zhur.Eksptl.i Teoret.Fiz. 38, 379 (1960); Soviet Phys.JETP 11, 276 (1960)
S.F.Antonova, S.S.Vasilenko, M.G.Kagansky, D.L.Kaminsky
Positron Decay of Ir192
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
Phys.Rev. 120, 1406 (1960)
W.B.Ewbank, L.L.Marino, W.A.Nierenberg, H.A.Shugart, H.B.Silsbee
Nuclear Spins of Six Neutron-Deficient Gold Isotopes
NUCLEAR STRUCTURE 194Au, 195Au, 192Au, 193Au, 191Au, 196Au; measured not abstracted; deduced nuclear properties.
Z.Physik 159, 158 (1960); See Also 60He01
H.H.Hennies
Kern-Isomerie bei Ir192 und Ir194
NUCLEAR STRUCTURE 194Ir, 192Ir; measured not abstracted; deduced nuclear properties.
Bull.Inst.Nuclear Sci.Boris Kidrich 10, 7 (1960)
L.Marinkov, M.Mladjenovic, M.Zupancic, R.Stepic
Internal Conversion Spectrum of Pt-192 and Os-192
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
J.Inorg.Nuclear Chem. 17, 15 (1961)
G.Andersson, I.B.Haller, R.Ringh
Thallium Isotopes 192 and 193
NUCLEAR STRUCTURE 193Tl, 192Tl; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(61)80180-2
Arkiv Fysik 19, 369 (1961)
W.Forsling
Alpha Radioactivities from Nuclides in the Atomic Number Region 80-83
NUCLEAR STRUCTURE 199Pb, 198Pb, 197Pb, 197Bi, 196Bi, 196Pb, 191Tl, 190Tl, 191Hg, 194Tl, 195Hg, 194Bi, 195Bi, 194Hg, 192Tl, 193Hg, 193Tl, 192Hg, 193Bi; measured not abstracted; deduced nuclear properties.
Naturwissenschaften 48, 97 (1961)
H.H.Hennies, A.Flammersfeld
Uber das 47 sec-Kern-Isomer beim Iridium
NUCLEAR STRUCTURE 192Ir, 194Ir, 104Rh; measured not abstracted; deduced nuclear properties.
Compt.Rend.Acad.Sci. 252, 2220 (1961); AEC-tr-4658 (1961)
J.Jastrzebski, P.Kilcher
Etude de la Desintegration du Mercure 192
NUCLEAR STRUCTURE 192Hg; measured not abstracted; deduced nuclear properties.
J.Phys.Radium 22, 672 (1961)
J.Jastrzebski, P.Kilcher
Transitions dans les Noyaux Impair-Impair 190Au et 192Au
NUCLEAR STRUCTURE 190Au, 192Au; 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.
Zhur.Eksptl.i Teoret.Fiz. 41, 1780 (1961); Soviet Phys.JETP 14, 1265 (1962)
K.A.Petrzhak, M.I.Yakunin
Investigation of the Alpha Radioactivity of Natural Platinum
NUCLEAR STRUCTURE 190Pt, 192Pt; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 22, 104 (1961)
D.H.Rester, M.S.Moore, F.E.Durham, C.M.Class
Internal Conversion Electrons from Coulomb Excitation of Heavy Elements
NUCLEAR STRUCTURE 232Th, 236U, 234U, 230Th, 192Os, 188Os, 189Os, 190Os, 186Os, 197Au, 238U; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90367-4
Naturwissenschaften 48, 96 (1961)
G.Scharff-Goldhaber, M.McKeown
Activities Observed in Iridium after Neutron Bombardment. Remarks on a Paper by H.H.Hennies and A.Flammersfeld
NUCLEAR STRUCTURE 194Ir, 192Ir, 104Rh; measured not abstracted; deduced nuclear properties.
Nucl.Sci.Eng. 11, 74 (1961)
E.I.Wyatt, S.A.Reynolds, T.H.Handley, W.S.Lyon, H.A.Parker
Half-Lives of Radionuclides. II
NUCLEAR STRUCTURE 153Sm, 147Pm, 142Pr, 22Na, 115Cd, 133Ba, 134Cs, 125Sb, 204Tl, 192Ir, 88Y, 82Br, 72Ga, 91Y, 24Na, 106Ru, 95Nb, 54Mn, 47Ca, 45Ca, 35S; measured not abstracted; deduced nuclear properties.
Physica 28, 417 (1962)
T.J.De Boer, H.Voorthuis, J.Blok
The Half-Lives of the First Excited States of 203Tl and 192Pt
NUCLEAR STRUCTURE 203Hg, 192Ir; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-8914(62)90020-4
Compt.Rend.Acad.Sci. 254, 1411 (1962)
J.Jastrzebski, P.Kilcher
Vie Moyenne des Premiers Etats Excites des Noyaux des Ors 192, 193, 195 et du Mercure 195
NUCLEAR STRUCTURE 195Hg, 192Hg, 193Hg; measured not abstracted; deduced nuclear properties.
Arkiv Fysik 22, 289 (1962)
I.Marklund, E.Karlsson, K.Korkman
Decay Studies in the Neutron-Deficient Au-Isotopes Part A: Odd Isotopes
NUCLEAR STRUCTURE 193Au, 191Pt, 191Au; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 45, 632 (1963)
R.M.Diamond, F.S.Stephens
Isomeric Levels in the Light Thallium Isotopes
NUCLEAR STRUCTURE 199Tl, 198Tl, 200Tl, 201Tl, 202Tl, 203Tl, 196Tl, 197Tl, 193Tl, 192Tl, 195Tl, 194Tl, 205Tl, 207Tl, 204Tl; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90838-1
Nucl.Phys. 49, 449 (1963)
W.M.Doyle, R.Marrus
Atomic Beam Studies of Some Radioactive Isotopes of Refractory Group Elements
NUCLEAR STRUCTURE 192Ir, 194Ir, 188Re, 187W, 183Ta, 185W, 186Re; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90108-1
Ann.Acad.Sci.Fennicae, Ser. A VI, No.128 (1963); Priv.Comm. (1963)
G.Graeffe
On the Alpha Activity of Platinum Isotopes
NUCLEAR STRUCTURE 190Pt, 188Pt, 186Pt, 192Pt, 184Pt, 183Pt, 182Pt; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 41, 604 (1963)
G.Harbottle
The Half-Lives of Tl204, Au195, Ir192 and its Long-Lived Isomer Ir192m2
NUCLEAR STRUCTURE 204Tl, 192Ir, 195Au; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90539-X
Nucl.Phys. 45, 679 (1963)
J.Jastrzebski, P.Kilcher
La Desintegration du Mercure 192
NUCLEAR STRUCTURE 192Hg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90842-3
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.
J.Inorg.Nucl.Chem. 25, 220 (1963)
B.Keisch
Conversion Coefficient for the Ir192m Transition
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(63)80014-7
Phys.Rev. 134, B1032 (1964)
J.de Boer, G.Goldring, H.Winkler
Multiple Coulomb Excitation of Rotational Levels in Even-Even Nuclei
NUCLEAR STRUCTURE 192Os, 190Os, 188Os, 164Dy, 168Er, 170Er, 166Er, 150Sm, 152Sm, 154Sm, 182W, 180Hf, 184W, 186W, 158Gd, 156Gd, 160Gd, 162Dy, 178Hf, 176Yb, 172Yb, 174Yb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B1032
Nucl.Phys. 56, 1 (1964)
B.Harmatz, T.H.Handley
Properties of Nuclear Levels in a Number of Even-Mass Nuclei (184 < A < 192)
NUCLEAR STRUCTURE 188Ir, 190Ir, 186Ir, 192Ir, 184Re; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90451-1
Nucl.Phys. 58, 544 (1964)
C.J.Herrlander, R.L.Graham
Penetration Effects in the K and L Internal Conversion Coefficients of the 279 keV Transition in Tl203
RADIOACTIVITY 203Pb[from Tl(p, n)]; measured ce, ICC, γ-mixing. Natural Tl target. 188Re, 192Ir, 198,199Au; measured ICC.
doi: 10.1016/0029-5582(64)90566-8
Phys.Lett. 12, 29 (1964)
M.Sakai, T.Yamazaki, H.Ejiri
Dynamic Conversion-Electron Spectroscopy and New Doublets of the Two Phonon States in Neutron-Deficient Even Nuclei in the Vibrational Region
NUCLEAR STRUCTURE 196Hg, 190Pt, 192Pt, 126Xe, 122Te, 120Te, 132Ba, 102Pd, 108Cd, 106Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)91164-3
Compt.Rend. 261, 1835 (1965)
J.Blachot, E.Monnand, A.Moussa
Desintegration du Rhenium 192
NUCLEAR STRUCTURE 192Re; measured not abstracted; deduced nuclear properties.
Proc.Phys.Soc.(London) 86, 31 (1965)
D.K.Butt, D.A.Jackson
Measurement of the Lifetimes of Some Excited States of 192Pt
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
doi: 10.1088/0370-1328/86/1/305
Nucl.Phys. 61, 385 (1965)
M.W.Johns, M.Kawamura
The Decay of Ir192
RADIOACTIVITY 192Ir; measured β, βγ, γγ(θ). 192Pt deduced levels, J.
doi: 10.1016/0029-5582(65)90100-8
Nucl.Phys. 63, 466 (1965)
N.L.Lark, H.Morinaga
Collective Levels of W, Os and Pt Studied by Gamma-Ray Spectroscopy of (α, xn) Reactions
NUCLEAR REACTIONS 88Sr, 110Pd, 138Ba, 140Ce, 176,178,180Hf, 182,184,186W, 188,190,192Os(α, 4nγ), E=48 or 52 MeV; measured σ(except for 88Sr), Eγ; 178,180Hf, 186W, 192Os(α, 2nγ), E=27 MeV; measured σ, Eγ. 88Zr, 110Cd, 138Cs, 140Nd, 188,190,192,194Pt, 182,184,186,188Os, 176,178,180,182W deduced levels.
doi: 10.1016/0029-5582(65)90476-1
Ark.Fys. 29, 321 (1965)
B.Nyman, S.Antman, C.Bergman, G.Backstrom
Transitions in the Decay of Au192
NUCLEAR STRUCTURE 192Au; measured not abstracted; deduced nuclear properties.
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
Izv.Akad.Nauk SSSR, Ser.Fiz. 30, 2022 (1966); Bull.Acad.Sci.USSR, Phys.Ser. 30, 2107 (1967)
H.Daniel, P.Jahn, W.Todt
Precision Measurements of the Conversion Electron Spectrum of 192Ir by Means of the New Heidelberg (1/2)π Square Root 13 Focusing Beta Spectrometer
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 80, 33 (1966); G.Goldring - Priv.Comm. (April 1972)
G.Goldring, R.Kalish, H.Spehl
Gyromagnetic Ratios of the First Excited 2+ States in Even Os Isotopes
NUCLEAR REACTIONS 188,190,192Os(16O, 16O'), E = 35.6 MeV; measured 16O'γ-coin(θ, H). 188,190,192Os levels deduced g. Enriched targets.
doi: 10.1016/0029-5582(66)90823-6
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
Phys.Lett. 20, 395 (1966)
P.Jahn, W.Todt, H.Daniel
192Ir Conversion Lines and 192Pt X-Ray Levels
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90757-8
Forschungsber.Landes Nordrhein-Westfalen No.1640 (1966)
G.Kauw
Untersuchungen an angereicherten Isotopen auf naturliche alphastrahlung
RADIOACTIVITY 142Ce, 143,145Nd, 152Gd, 156Dy, 174Hf, 180,183W, 190,192Pt, 204Pb; measured Eα, T1/2. 204Pb deduced Q.
Nucl.Phys. 88, 63 (1966)
B.Nyman, A.Johansson, C.Bergman, G.Backstrom
The Decay of 192Au
RADIOACTIVITY 192Au [from Pt(p, xn)]; measured T1/2, Eγ, Eβ, I(ce), Iβ, Iγ; deduced Q. 192Pt deduced levels. Natural target.
doi: 10.1016/0029-5582(66)90453-6
Phys.Lett. 21, 541 (1966)
R.F.Petry, R.A.Neumann, J.S.Evans
Negative-Parity Levels in Even-Even Hg Isotopes
NUCLEAR STRUCTURE 192Tl, 194Tl, 198Tl, 196Tl; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91292-3
Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn. (1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.197 (1966)
M.Sakai, T.Yamazaki, H.Ejiri
Anomalous K/L Ratio of the Conversion Electrons from (p, 2n) Reactions
NUCLEAR STRUCTURE 190Pt, 192Pt, 196Hg, 120Te, 122Te, 126Xe, 132Ba, 102Pd, 108Cd, 106Cd; measured not abstracted; deduced nuclear properties.
Phys.Rev. 141, 1206 (1966)
A.Schwarzschild
Lifetimes of First 2+ and 4+ States of 192Pt and Some Systematics of E2 Transitions in Even-Even Nuclei
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
Helv.Phys.Acta 39, 420 (1966)
L.Schellenberg, J.Kern
Der Zerfall von 192Ir
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
Priv.Comm., quoted by 1967Tr06 (1967)
A.Siivola
Nucl.Phys. 78, 576 (1966)
O.A.Wasson, J.E.Draper
Thermal and Resonance Neutron Capture in Cl, Sc, V, Co and Ir
NUCLEAR REACTIONS Cl, Sc, V, Co, Ir(n, γ), E < 10 keV; measured γ-ray spectra. Natural targets.
doi: 10.1016/0029-5582(66)90896-0
Phys.Rev. 159, 1056 (1967)
S.K.Bhattacherjee, S.K.Mitra, H.C.Jain, H.C.Padhi
Beta-Gamma Correlation Measurements on Ir192
NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.
Phys.Rev.Lett. 18, 912 (1967)
R.F.Casten, J.S.Greenberg, G.A.Burginyon, D.A.Bromley
Experimental Tests of Recent Pairing-Plus-Quadrupole Model Calculations in the Osmium Nuclei
NUCLEAR STRUCTURE 186Os, 188Os, 190Os, 192Os; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.18.912
Nucl.Phys. 87, 657 (1967)
S.A.De Wit, G.Backenstoss, C.Daum, J.C.Sens, H.L.Acker
Measurement and Analysis of Muonic X-Ray Spectra in Deformed Nuclei
ATOMIC PHYSICS, Mesic-Atoms Sm, Eu, Tb, Ho, Hf, Ta, W, Os, Ir, Th, 233U, 235U, 238U, 239Pu; measured muonic X-rays; deduced nuclear charge distribution parameters, Q0.
doi: 10.1016/0029-5582(67)90003-X
Rev.Roum.Phys. 12, 561 (1967)
D.I.Dorcioman, M.S.Popa, M.I.Cristu
Gamma Rays from Thermal Neutron Capture in Manganese, Germanium and Iridium Nuclei
NUCLEAR STRUCTURE 73Ge, 56Mn, 192Ir, 194Ir; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A101, 305 (1967)
O.Dragoun, P.Jahn
M-Subshell Internal Conversion Coefficients. Comparison of Present Calculations with Experiments for E2 transitions
RADIOACTIVITY 192Ir, 75Se[from 191Ir, 74Se(n, γ)]; measured I(ce). 192Pt, 75As deduced M ICC. Enriched 74Se target.
doi: 10.1016/0375-9474(67)90189-3
Nucl.Phys. A91, 85 (1967); G.Goldring - Priv.Comm. (April 1972)
P.Gilad, G.Goldring, R.Herber, R.Kalish
Precession Measurements Following Coulomb Excitation with Oxygen Ions (II). Gyromagnetic Ratios of the 2+ States in Hf, W and Os Isotopes
NUCLEAR REACTIONS 178,180Hf, 186W, 186,190,192Os(16O, 16O'γ), E=35.4 MeV; measured σ(Eγ, θ(γ), H). 178,180Hf, 186W, 186,188,190,192Os levels deduced g. 186,192Os levels deduced B(E2).
doi: 10.1016/0375-9474(67)90452-6
Inst.Nucl.Study, Univ.Tokyo, Ann.Rept. 1966, p.43 (1967)
M.Ishihara, H.Ejiri, Y.Gono, M.Sakai, K.Katori
Measurement of Conversion Electrons from (p, 4n), (p, 6n) Reactions
NUCLEAR REACTIONS 197Au, 203Tl, 205Tl, 209Bi(p, 4nγ), (p, 6nγ), E=50, 55 MeV; measured E(ce), I(ce), I(ce)(θ). 192,194Hg, 198,200Pb deduced levels, J, π.
Phys.Lett. 24B, 148 (1967)
S.E.Karlsson, S.Hogberg, O.Nilsson
Precision Measurements on the 296 keV and 316 keV Transition in 192Pt
doi: 10.1016/0370-2693(67)90507-2
Ark.Fys. 36, 177 (1967)
R.A.Naumann, R.F.Petry, J.S.Evans
Nuclear Spectroscopy of Light Platinum and Mercury Isotopes
NUCLEAR STRUCTURE 196Tl, 198Tl, 194Tl, 188Au, 192Tl; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A95, 673 (1967)
T.J.Palaska, V.R.Potnis, C.E.Mandeville
Gamma Rays Emitted in Disintegration of 192Ir and 194Ir
RADIOACTIVITY 192Ir, 194Ir [from 191Ir (n, γ), 193Ir (n, γ)]; measured Eγ, Iγ. 192Pt, 192Os, 194Pt deduced levels. Natural targets.
doi: 10.1016/0375-9474(67)90860-3
Helv.Phys.Acta 40, 639 (1967)
L.Schellenberg, O.Huber, P.Siffert, J.M.Kuchly
Energiereiche Gammastrahlung des 192Ir
NUCLEAR STRUCTURE 192Ir; 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
Izv.Akad.Nauk SSSR, Ser.Fiz. 31, 269 (1967); Bull.Acad.Sci.USSR, Phys.Ser. 31, 253 (1968)
G.I.Sychikov, V.R.Burmistrov, I.S.Vodolazhskaya, O.D.Kovrigin, A.F.Novgorodov
Investigation of the Radiation from the Iridium Fraction from Proton-Bombarded Gold
NUCLEAR STRUCTURE 190Ir, 189Ir, 192Ir; measured not abstracted; deduced nuclear properties.
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.Letters 27B, 425 (1968)
R.Baader, H.Backe, R.Engfer, K.Hesse, E.Kankeleit, U.Schroder, H.K.Walter, K.Wien
Muonic Isomer Shift Measurements in Sm, W and Os Isotopes and Their Interpretation in Terms of Changes in Nuclear Charge Distribution
ATOMIC PHYSICS, Mesic-Atoms Sm, W, Os(μ-, γ), E=0; measured Eγ. 152Sm, 182,184,186W, 188,190,192Os levels deduced muonic isomer shift.
doi: 10.1016/0370-2693(68)90226-8
Nucl.Phys. A106, 209 (1968)
M.Bogdanovic, M.Mladjenovic, R.Stepic
Internal Conversion M/L and (N+O)/M Ratios for E2 Transitions
RADIOACTIVITY 134Cs, 152Eu, 160Tb, 166Ho, 170Tm, 182Ta, 186Re, 188Re, 192Ir [all (n, γ) produced ]; measured ICC.
doi: 10.1016/0375-9474(67)90839-1
Z.Physik 216, 267 (1968)
M.Bogdanovic, M.Mladjenovic, R.Stepic
Measurement of Internal Conversion K/L3 and K/L Ratios for E2 Transitions
RADIOACTIVITY 152Eu, 160Tb, 166Ho, 182Ta, 186,188Re, 192Ir, 198Au; measured I(ce). 152Sm, 160Dy, 166Er, 182W, 186,188Os, 192Os, 192Pt, 198Hg E2 transitions deduced K/L, K/L3 conversion ratios.
Nucl.Instr.Methods 59, 1 (1968)
K.E.Davies, W.D.Hamilton
Gamma-Gamma Linear Polarization Measurements
RADIOACTIVITY 46Sc, 192Ir; measured γ-linear polarization correlations, γγγ-triple coin.
Nucl.Phys. A122, 165 (1968)
W.D.Hamilton, K.E.Davies
Angular Correlation Measurements in 192Pt
RADIOACTIVITY 192Ir [from 191Ir(n, γ)]; measured γγ(θ), γ-polarization. 192Pt levels deduced J, γ-ray mixing.
doi: 10.1016/0375-9474(68)90710-0
Nucl.Phys. A118, 628 (1968)
P.Kilcher
Les Niveaux Excites des Noyaux Impairs 190Au et 192Au
RADIOACTIVITY 190Hg, 192Hg [from 197Au (p, 8n), 197Au(p, 6n)]; measured Eγ, Iγ, γ ce-coin. 190Au, 192Au deduced levels J, π, ICC. Ge(Li) detectors.
doi: 10.1016/0375-9474(68)90445-4
Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 52(1968); Bull.Acad.Sci.USSR, Phys.Ser. 32, 53(1969)
O.Nilsson, S.-E.Karlsson, I.Andersson, G.Malmsten, S.Hogberg, C.-H.Norberg, A.H.El-Farrash, C.Nordling, K.Siegbahn
Some Recent Work Performed at the 50-cm Iron-Free Spectrometer at Uppsala
RADIOACTIVITY 160Tb, 166Ho, 170Tm, 182Ta, 192Ir, 166Dy, 212Pb; measured I(ce), subshell conversion ratios. 160Dy, 166Er, 170Yb, 182W, 192Pt, 166Ho, 212Bi deduced γ-multipolarities.
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.
Z.Phys. 213, 56 (1968)
B.Wilken
Konversionskoeffizienten und Fluoreszenzausbeuten beim Zerfall des Ir192m und Co58m
RADIOACTIVITY 58Co, 192Ir; measured I(ce), ICC.
Indian J.Pure Appl.Phys. 7, 316 (1969)
K.B.Appalacharyulu, D.L.Sastry, S.Jnanananda
Beta-Gamma Directional Correlation Studies in 192Ir
RADIOACTIVITY 192Ir; measured βγ(θ); deduced matrix element parameters.
Phys.Rev. 187, 1532 (1969)
R.F.Casten, J.S.Greenberg, S.H.Sie, G.A.Burginyon, D.A.Bromley
Transition Matrix Elements in the Even-Even Osmium Isotopes: A Comparison with Pairing-Plus-Quadrupole Model Calculations
NUCLEAR REACTIONS 186,188,190,192Os(16O, 16O'γ), E=42-80 MeV; measured σ(E(16O'), Eγ, θ(γ), θ(16O'γ)), γγ-coin. 186,188,190,192Os deduced levels, B(E2), branching ratios, quadrupole moment, J, π.
Phys.Rev. 183, 1019 (1969)
Z.W.Grabowski
Mixing Ratios of Transitions in the Decay of Ir192
RADIOACTIVITY 192Ir [from 191Ir(n, γ)]; measured Eγ, γγ(θ). 192Os, 192Pt deduced γ-mixing. Ge(Li) detector.
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
Can.J.Phys. 47, 2395 (1969)
D.B.Kenyon, L.Keszthelyi, J.A.Cameron
Nuclear g Factors of Three Levels of 192Pt
RADIOACTIVITY 192Ir; measured γγ(θ, H). 192Pt levels deduced g, γ-mixing ratios.
Phys.Rev. 182, 1259 (1969)
M.Y.Khan, L.D.Wyly, C.H.Braden, E.T.Patronis, Jr.
γ-γ Directional Correlations in the Decay of 192Ir
RADIOACTIVITY 192Ir [from 191Ir(n, γ)]; measured γγ(θ). 192Os, 192Pt levels deduced J, γ-mixing. Ge(Li) detector.
Thesis, Univ.Michigan (1969); TID-25592 (1969)
S.L.Lee
The Decay Schemes of 131Ba and 192Ir Nucleus
RADIOACTIVITY 131Ba; measured Eγ, Iγ, γγ-coin; deduced log ft. 192Ir; measured Eγ, Iγ, T1/2, γγ-coin; deduced log ft. 131Cs, 192Pt, 192Os deduced levels, J, π, ICC, γ-multipolarity.
Nucl.Phys. A131, 601 (1969)
L.Marinkov, I.Anicin, I.Bikit, R.Stepic
On the Existence of the Electric Monopole Component in the 2+'→2+ Transition in 192Pt
RADIOACTIVITY 192Ir [from 191Ir(n, γ)]; measured γce(θ), I(ce), K/L3. 192Pt deduced matrix element, E0/E2. Enriched target.
doi: 10.1016/0375-9474(69)90597-1
Nucl.Phys. A129, 273 (1969)
P.G.E.Reid, M.Sott, N.J.Stone
A Study of the Magnetic Dipole Moments of 192Ir and 194Ir and the Decay Scheme of 192Ir by Nuclear Orientation
RADIOACTIVITY 192,194Ir[from Ir(n, γ)]; measured Eγ, Iγ(θ, T) in Fe. 192,194Ir deduced μ. 192,194Pt deduced levels, γ-mixing.
doi: 10.1016/0375-9474(69)90667-8
Nucl.Phys. A123, 193 (1969)
R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer
Gamma-Gamma Angular Correlations Following Coulomb Excitation
NUCLEAR REACTIONS 107,109Ag, 110Pd, 117Sn(α, α'γ), E=9.5-10 MeV; 190,192Os(p, p'γ), E=4.5 MeV; measured γγ(θ). 107,109Ag, 110Pd, 117Sn, 190,192Os deduced levels, J, γ-mixing ratio. Enriched target.
doi: 10.1016/0375-9474(69)90899-9
Phys.Rev. C1, 303 (1970)
R.Beraud, I.Berkes, R.Chery, R.Haroutunian, M.Levy, G.Marguier, G.Marest, R.Rougny
Lifetimes and Nuclear Moments in Os192 and Pt192
RADIOACTIVITY 192Ir; measured ceγ-delay, γγ(θ, H). 192Os, 192Pt levels deduced T1/2, g, γ-mixing, B(λ).
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
Izv.Akad.Nauk SSSR, Ser.Fiz. 34, 1635 (1970); Bull.Acad.Sci.USSR, Phys.Ser. 34, 1452 (1971)
B.R.Erdal, M.Finger, R.Foucher, J.P.Husson, J.Jastrzebski, A.Johnson, R.Henck, P.Siffert, G.Astner, A.Kjelberg, P.Patzelt
Properties of Low-Lying Levels of Even Isotopes of Pt
RADIOACTIVITY 184,186,188,190,192Au; measured Eγ, Iγ. 184,186,188,190,192Pt deduced levels, J, π, γ-branching. Isolde on-line mass separator.
Radiochim.Acta 13, 132 (1970)
G.Harbottle
The Half-Lives of Two Long-Lived Nuclear Isomers, 108mAg and 192m2Ir, and of 137Cs and 204Tl
RADIOACTIVITY 108mAg, 137Cs, 192mIr, 204Tl; measured T1/2.
Proc.Int.Conf.Prop.Nuclei Far from Region of Beta-Stability, Leysin, Switzerland, Vol.2, p.985 (1970); CERN 70-30 (1970)
G.Herrmann, N.Kaffrell, N.Trautmann, R.Denig, W.Herzog, D.Hubscher, K.L.Kratz
Some Studies on Neutron-Rich Nuclei
RADIOACTIVITY 90,91,92Br, 139,140,141I; measured T1/2. 106Tc; measured Eγ, Iγ, γγ-coin. 106Ru deduced levels, J, π, γ-branching. 192mOs, 192Re; measured Eγ, Iγ, γγ-coin. 192Os deduced levels, J, π, γ-branching. 164Tb; measured Eγ, Iγ; deduced log ft. 164Dy deduced levels, J, π. 238Pa; measured Eγ, Iγ, γγ-coin. 238U deduced levels, J, π, γ-branching.
Nucl.Phys. A146, 220 (1970)
T.Hirose, S.Morinobu, H.Ikegami
Structure of Pt Nuclei (II). Structure of 192Pt Investigated by Electron-Gamma and Gamma-Gamma Directional Correlations
RADIOACTIVITY 192Ir; measured Eγ, Iγ, βγ(θ), ceγ(θ), γγ(θ); deduced log ft. 192Pt deduced levels, J, π, M1 penetration factor, ICC, γ-mixing, B(EL) ratios.
doi: 10.1016/0375-9474(70)91100-0
Phys.Rev. C2, 2341 (1970)
A.T.Hirshfeld, D.D.Hoppes
Transition Mixing Ratios Determined from a Study of the Electron and Gamma-Ray Distributions from Oriented 192Ir
RADIOACTIVITY 192Ir;(oriented) measured Iγ(θ), Iβ(θ). 192Os, 192Pt transitions deduced γ-mixing ratios.
Nucl.Phys. A142, 63 (1970)
J.Legrand, J.Morel, C.Clement
Schemas de Desintegration du 59Fe et de l'192Ir
RADIOACTIVITY 59Fe, 192Ir; measured Iγ, branching ratios. Ge(Li) detectors.
doi: 10.1016/0375-9474(70)90474-4
Nucl.Phys. A144, 369 (1970)
M.Levanoni, F.C.Zawislak, D.D.Cook
Magnetic Moments of Excited States in 190Os, 192Os and 192Pt
RADIOACTIVITY 190Ir[from 190Os(p, n)]; 192Ir[from 191Ir(p, n)]; measured γγ(θ, H) in Fe lattice. 190Os, 192Os, 192Pt levels deduced μ.
doi: 10.1016/0375-9474(70)90366-0
Atompraxis 16, 313 (1970)
M.Ninkovic, M.Mladjenovic
Specific Gamma-Ray Constant and Gamma Spectrum of 192Ir
RADIOACTIVITY 192Ir; measured Eγ, Iγ; deduced γ-ray constant.
Czech.J.Phys. 20B, 840 (1970)
Z.Plajner, J.Frana, A.Spalek, M.Vobecky, M.Fiser
Gamma-Ray Spectrum of 192Au
RADIOACTIVITY 192Au; measured Eγ, Iγ; deduced ICC, log ft. 192Pt deduced levels, J, π, λ.
Phys.Rev. C1, 1573 (1970)
R.J.Pryor, J.X.Saladin
Determination of the Electric Quadrupole Moment of the First 2+ States of Os188,190,192
NUCLEAR REACTIONS 188,190,192Os(α, α'), E=10, 11, 12 MeV; 188,190,192Os(16O, 16O'), E=42, 47, 52, 53 MeV; measured σ(Eα'), σ(E(16O')). 188,190,192Os levels deduced quadrupole moment.
Phys.Rev. C2, 721 (1970)
J.W.Seubert, R.G.Wilkinson
Angular Correlations in the Decay of Ir192
RADIOACTIVITY 192Ir; measured βγ(θ), γce(θ). 192Pt transition deduced γ-mixing.
Nucl.Phys. A156, 19 (1970)
J.R.Sites, W.A.Steyert
Angular Distribution of Gamma Rays Resulting from Polarized 124Sb, 192Ir and 194Ir
RADIOACTIVITY 124Sb, 192,194Ir[from sb, ir(n, γ)]; measured Iγ(θ) from polarized nuclei. 124Sb deduced μ, Lβ. 192,194Ir deduced Lβ. 124Te deduced γ-mixing.
doi: 10.1016/0375-9474(70)91109-7
Yad.Fiz. 12, 455 (1970); Sov.J.Nucl.Phys. 12, 248 (1971)
N.I.Tarantin, A.P.Kabachenko, A.V.Demyanov
Identification and Study of the Radioactive Properties of Bismuth Isotopes with an Electromagnetic Mass Separator in a Heavy-Ion Beam
RADIOACTIVITY 192,193,194,195,196,197Bi, 193mBi, 195mBi, 197mBi; measured T1/2, Eα.
Nucl.Instrum.Methods 84, 157 (1970)
J.B.Willett
A Method for the High Precision Measurement of Relative Intensities and Internal Conversion Coefficients
RADIOACTIVITY 137Cs, 192Ir, 207Bi; measured Iγ, ICC.
Z.Phys. 241, 435 (1971)
H.Backe
Intensitatsmessung von Rontgen- und Kerngammastrahlung an einigen schweren Myonenatomen
ATOMIC PHYSICS, Mesic-Atoms W, Os, 209Bi(μ-, X), E not given; measured absolute, relative I X-rays.
NUCLEAR STRUCTURE 182,184,186W; 190,192,188Os, 191,193Ir, 203,205Tl, 209Bi; analyzed muonic X-ray, Iγ data. 188Os, 203,205Tl levels deduced excitation probability.
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.Instrum.Methods 97, 219 (1971)
R.J.Gehrke, R.A.Lokken
Calibration of the Efficiency of a Si(Li) Photon Spectrometer in the Energy Region 5 to 125 keV
RADIOACTIVITY 145Pm, 155Eu, 241Am; measured Iγ, I(X-ray). 60m-Co, 94mNb, 176mLu, 192mIr, 210Pb; measured I(X-ray)/Iγ. 60mCo, 94mNb, 176mLu transitions deduced α(K). 192mIr, 210Bi transitions deduced α(L). Detector - Si(Li).
ANCR-1016, p.77 (1971)
R.G.Helmer, R.A.Lokken
Limits on the Precision of Measured Relative Internal-Conversion Coefficients - 192Ir
RADIOACTIVITY 192Ir; measured I(ce) ratios. 192Pt, 192Os transitions deduced ICC.
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
Nucl.Phys. A163, 311 (1971)
A.Hoglund, S.G.Malmskog, A.Backlin, B.Fogelberg, B.Jonson
Transition Rates in 192Au
RADIOACTIVITY 192Hg[from Pb(p, 3pxn)]; measured E(ce), I(ce), cece-delay. 192Au levels deduced T1/2, γ-mixing, B(M1), B(E1), B(E2). Isotope separated sources.
doi: 10.1016/0375-9474(71)90539-2
Phys.Lett. 37B, 170 (1971)
M.J.Holmes, W.D.Hamilton, R.A.Fox
An Angular Correlation Test of Time Reversal Invariance
RADIOACTIVITY 192Ir; measured γγ(θ); deduced no T-invariance violation.
doi: 10.1016/0370-2693(71)90042-6
Phys.Rev. C4, 1382 (1971); R.P.Scharenberg - Priv.Comm. (April 1972)
W.C.King, Z.W.Grabowski, R.P.Scharenberg
Magnetic Dipole Moments of the First 2+ States in Os192 and Pt192; Room-Temperature Nuclear-Magnetic-Resonance Measurement of the Os Hyperfine Field in Fe and Ni Hosts
RADIOACTIVITY 192Ir; measured γγ(θ, H) in Fe, Ni. 192Os, 192Pt levels deduced μ.
Nucl.Phys. A169, 363 (1971)
H.Kruger, H.Hanle, M.Koriath, K.Stelzer
Neutron Capture γ-Rays from 192Ir and 194Ir
NUCLEAR REACTIONS 191,193Ir(n, γ), E=thermal, epithermal; measured Eγ, Iγ, γγ-coin; deduced Q. 192,194Ir deduced levels, γ-branching. Enriched targets;Ge(Li) detectors, Ge(Li)-NaI(Tl) pair spectrometer.
doi: 10.1016/0375-9474(71)90890-6
Nucl.Phys. A169, 177 (1971)
T.Kruse, W.Makofske, H.Ogata, W.Savin, M.Slagowitz, M.Williams, P.Stoler
Elastic and Inelastic Proton Scattering from Heavy Collective Nuclei
NUCLEAR REACTIONS 148,150,152,154Sm, 165Ho, 172,174,176Yb, 182,184,186W, 188,190,192Os, 194,198Pt(p, p), (p, p'), Ep=16 MeV; measured σ(θ); deduced optical model parameters. 148,150,152,154Sm, 165Ho, 172,174,174,176Yb, 182,184,186W, 188,190,192Os, 194,198Pt deduced β2 . Enriched target.
doi: 10.1016/0375-9474(71)90570-7
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
Indian J.Phys. 45, 499 (1971)
S.Sen, B.K.Sinha, R.Bhattacharyya
High Resolution Gamma-Spectrum in the Decay of Ir-192
RADIOACTIVITY 192Ir; measured Eγ, Iγ. 192Os, 192Pt deduced levels, ICC, J, π, γ-mixing.
Nucl.Phys. A188, 369 (1972)
M.Finger, R.Foucher, J.P.Husson, J.Jastrzebski, A.Johnson, G.Astner, B.R.Erdal, A.Kjelberg, P.Patzelt, A.Hoglund, S.G.Malmskog, R.Henck
Properties of Low-Lying Levels in the Even Platinum Nuclei (182 < A < 192)
RADIOACTIVITY 192Au, 190Au, 188Au, 186Au, 184Au, 182Au[from pb(p, 3pxn)Hg-Au, mass separated]; measured Eγ, Iγ, E(ce), I(ce), γγ-, ceγ-coin, cece-delay, ceγ--delay. 182,184,186,188,190,192Pt deduced levels, J, π, ICC, T1/2. Au chemical purification. Magnetic spectrometers, Ge(Li), Si(Li).
doi: 10.1016/0375-9474(72)90064-4
Phys.Rev.Lett. 29, 958 (1972)
H.Gauvin, Y.Le Beyec, M.Lefort, N.T.Porile
α Decay of Neutron-Deficient Isotopes of Bismuth and Lead Produced in (Ar, xn) and (Kr, xn) Reactions
RADIOACTIVITY 186,187,188,189,190Pb, 190,191Bi, 191mBi, 192,193Bi, 193mBi, 194,195Bi, 195mBi, 197mBi; measured Eα, T1/2; deduced α-branching ratios.
doi: 10.1103/PhysRevLett.29.958
Progr.Theor.Phys. 48, 1569 (1972)
T.Konishi
On the Nuclear Excitation by the Bound Muon and the Muonic Hyperfine Structure
ATOMIC PHYSICS, Mesic-Atoms 192Os; calculated μ-mesic E(X-ray), I(X-ray); analyzed nuclear excitation.
Int.J.Appl.Radiat.Isotop. 23, 219 (1972)
F.Lagoutine, J.Legrand, C.Perrot, J.P.Brethon, J.Morel
Periodes de Quelques Radionucleides
RADIOACTIVITY 33P, 57Co, 67Cu, 85,89Sr, 113Sn, 134Cs, 192Ir; measured T1/2.
doi: 10.1016/0020-708X(72)90058-0
Phys.Rev. C6, 613 (1972)
S.A.Lane, J.X.Saladin
Static Quadrupole Moments of the First 2+ States of the Even-Even Osmium Nuclei
NUCLEAR REACTIONS 184,186,188,190,192Os(α, α'γ), E=10, 12, 14 MeV; 184,186,188,190,192Os(16O, 16O'γ), E=36, 42, 48 MeV; 184,186,188,190,192Os(32S, 32S'γ), E=48, 52, 56 MeV; measured σ(Eγ, θ(γ)). 184,186,188,190,192Os deduced B(E2), quadrupole moment.
Phys.Lett. 42B, 57 (1972)
R.Link, L.Schellenberg, H.Backe, R.Engfer, E.Kankeleit, R.Michaelsen, H.Schneuwly, W.U.Schroder, J.L.Vuilleumier, H.K.Walter, A.Zehnder
Magnetic Hyperfine Interaction of the 2+ Rotational States in Muonic 190,192Os
NUCLEAR REACTIONS Os(μ-, Xγ), E approx 0; measured I(X-ray), Iγ. 190,192Os nuclear transitions deduced magnetic hfs splitting.
doi: 10.1016/0370-2693(72)90715-0
Phys.Lett. 39B, 343 (1972)
P.Sioshansi, D.A.Garber, W.C.King, R.P.Scharenberg, R.M.Steffen, R.M.Wheeler
Comparison of Impact and Radioactivity Techniques and the Magnetic Dipole Moments of the First 2+ States in 188Os, 190Os, and 192Os
NUCLEAR REACTIONS Os(16O, 16O'γ), E=36 MeV; measured (16O')(γ)(θ, H) in Fe, Ni; deduced internal magnetic fields. 188,190,192Os levels deduced g.
doi: 10.1016/0370-2693(72)90134-7
Phys.Rev. C6, 2245 (1972)
P.Sioshansi, D.A.Garber, Z.W.Grabowski, R.P.Scharenberg, R.M.Steffen, R.M.Wheeler
Magnetic Dipole Moments of First 2+ States in Even Osmium Nuclei Recoil-Implanted in Nickel
NUCLEAR REACTIONS 186,188,190,192Os(16O, 16O'γ), E=36 MeV; measured σ(E(16O'), Eγ, θ(γ)) in Ni; deduced omegatau. 186,188,190,192Os levels deduced g.
Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1652 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 77 (1974)
A.B.Aldushchenkov, I.M.Band, N.A.Voinova, D.M.Kaminker, M.A.Listengarten
Angular Correlation of K and L Conversion Electrons in 192Pt
RADIOACTIVITY 192Ir; measured ceγ(θ). 192Pt deduced transitions, λ, γ-mixing.
Proc.Intern.Conf. on Nuclear Moments and Nuclear Structure, Osaka, Japan, p.586 (1972); J.Phys.Soc.Jpn. 34, p.586 Supplement (1973)
H.Backe, F.Boehm, 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
Magnetization Distribution of Single-Particle States and 2+ Rotational States from Muonic Atoms
NUCLEAR MOMENTS 115In, 203,205Tl, 190,192Os; measured muonic atom hyperfine splitting; deduced magnetization distribution. 190,192Os deduced μ.
ATOMIC PHYSICS, Mesic-Atoms 115In, 203,205Tl, 190,192Os; measured muonic atom hyperfine splitting; deduced magnetization distribution. 190,192Os deduced μ.
Nucl.Phys. A209, 461 (1973)
R.C.Chopra, P.N.Tandon, S.H.Devare, H.G.Devare
Half-Lives of Excited States in 77As, 97Tc and 192Os
RADIOACTIVITY 77Ge [from 76Ge(n, γ)], 97Ru [from 96Ru(n, γ)], 192Ir [from 191Ir(n, γ)]; measured βγ-, γγ-, γ-X delay. Levels in 77As, 97Tc, 192Os; deduced T1/2, B(M1), B(E2).
doi: 10.1016/0375-9474(73)90839-7
Nucl.Phys. A204, 26 (1973)
R.J.Gehrke
The Decay of 192Ir
RADIOACTIVITY 192Ir; measured Eγ, Iγ; deduced log ft. 192Os, 192Pt deduced levels. α(K), γ-branching. Ge(Li) detectors.
doi: 10.1016/0375-9474(73)90003-1
Nucl.Phys. A199, 401 (1973)
M.J.Holmes, W.D.Hamilton, R.A.Fox
An Angular Correlation Test of Time Reversal Invariance
RADIOACTIVITY 192Pt[from 191Ir(n, γ)]; measured γγ(θ) from cryogenically polarized nucleus; deduced limit on T-violation in E.M. Interaction.
doi: 10.1016/0375-9474(73)90557-5
Phys.Lett. 45B, 187 (1973)
M.Ikeda, A.Ikeda, R.K.Sheline
The Effects of γ-Instability on the Muonic X-Rays of 192Os
NUCLEAR STRUCTURE, Mesic-Atoms 192Os; calculated muonic X-ray spectra.
doi: 10.1016/0370-2693(73)90178-0
Nucl.Phys. A203, 17 (1973)
J.Meyer, J.Speth
Change of Nuclear Radii Due to Rotation; Calculation of Mossbauer and Muonic Isomer Shifts
NUCLEAR STRUCTURE 150Nd, 152,154Sm, 154,156,158,160Gd, 156,158,160,162,164Dy, 158,160,162,164,166,168,170Er, 164,166,168,170,172,174,176,178Yb, 172,174,176,178,180Hf, 180,182,184,186W, 188,190,192Os; calculated Mossbauer, muonic isomer shifts of 2+-70+ transitions.
doi: 10.1016/0375-9474(73)90421-1
Phys.Fenn. 8, 345 (1973)
A.Pakkanen, D.W.Heikkinen
A 6.1 s Isomer and Rotational Bands in 192Os
RADIOACTIVITY 192mOs; measured T1/2, Eγ, Iγ, Iβ, βγ-coin, γγ-coin. 192Os deduced levels, J, π, λ.
NUCLEAR REACTIONS 192Os(n, n'γ), E=14.5 MeV; measured 192mOs yield.
Curr.Sci.(India) 42, 16 (1973)
R.Prasad, S.P.Ram, L.Chaturvedi, S.N.Chaturvedi, A.K.Nigam
On the Levels of 192Pt and 192Os
RADIOACTIVITY 192Ir; measured Eγ; 192Os, 192Pt deduced levels.
Spectra of Electromagnetic Transitions and Level Schemes Following Thermal Neutron Capture by Nuclides with A 143-193, P.Prokofev, J.Berzins, G.Rezvaya, Eds., Publishing House 'Zinatne', Riga (1973)
P.Prokofev, M.Balodis, M.Beitins, Y.Berzin, V.Bondarenko, N.Kramer, A.Krumina, G.Rezvaya, L.Simonova
NUCLEAR REACTIONS 143,145Nd, 149Sm, 167Er, 174Yb, 175,176Lu, 177,178Hf, 181Ta, 186W(n, γ), E=thermal; measured Eγ, Iγ, I(ce). Deduced ICC. 151Eu, 155Gd(n, γ), E=thermal; measured Eγ, I(ce). Deduced ICC. 157Gd, 162,164Dy, 165Ho, 168Yb, 169Tm(n, γ), E=thermal; measured I(ce). Deduced ICC. 191,193Ir(n, γ), E=thermal; measured Eγ, Iγ. 144Nd, 150Sm, 156,158Gd, 163,165Dy, 166Ho, 168Er, 169,175,177Yb, 170Tm, 176Lu, 178Hf, 182Ta deduced levels, J, π, γ-multipolarities. 146Nd, 185W, 194Ir deduced levels, J, π. 152Eu deduced transitions, γ-multipolarities. 187W, 192Ir deduced transitions.
Nucl.Phys. A202, 409 (1973)
G.J.Smith, P.C.Simms
Centroid-Shift Measurement of the Mean Lifetimes of the 316 and 612 keV States of 192Pt
RADIOACTIVITY 192Ir; measured βγγ-coin. 192Pt levels deduced T1/2.
doi: 10.1016/0375-9474(73)90234-0
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
Ann.Phys.(New York) 78, 496 (1973)
J.B.Willett, G.T.Emery
Relative intensity and internal conversion coefficient measurements in the decays of 51Cr, 137Cs, 192Ir, and 207Bi
RADIOACTIVITY 51Cr, 207Bi(EC), 137Cs, 192Ir(β-); measured decay products, Eγ, Iγ, Eβ, Iβ; deduced γ-ray energies and intensities, ICC, B(E2). Comparison with available data.
doi: 10.1016/0003-4916(73)90269-8
Z.Naturforsch. 29a, 1125 (1974)
E.Bashandy, M.S.El-Nesr
Possible Nuclear Structure Effects in Even-Even Osmium Nuclei
RADIOACTIVITY 186,188Re; measured βce-, (ce)(ce)-coin, I(ce), Iγ. 192Ir; measured (ce)(ce)-coin, I(ce), Iγ. 186,188,192Os levels deduced B(M1), B(E2), γ-mixing.
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.Phys. A235, 428 (1974)
F.T.Baker, T.H.Kruse, M.E.Williams, W.Savin
Coulomb-Nuclear Interference for Inelastic Deuteron Scattering
NUCLEAR REACTIONS 54,56Fe, 60Ni, 114Cd, 152Sm, 192Os(d, d'), E=3-16 MeV; measured σ(E, Ed'). 54,56Fe, 60Ni, 114Cd, 152Sm, 192Os levels deduced deformation lengths βL R. Enriched targets.
doi: 10.1016/0375-9474(74)90203-6
Phys.Rev.Lett. 32, 843 (1974)
H.Beuscher, W.F.Davidson, R.M.Lieder, A.Neskakis, C.Mayer-Boricke
High-Spin States and Coriolis-Decoupled Bands in 190-194Hg
NUCLEAR REACTIONS 194,196Pt(α, xnγ), E=65-108 MeV; measured σ(E;Eγ, θ, t), γγ-coin. 181Ta(14N, 5n), E=93 MeV; measured σ(Eγ, θ). 190,191,192,193,194Hg deduced levels, J, π.
doi: 10.1103/PhysRevLett.32.843
Fiz.Elem.Chastits At.Yadra 5, 382 (1974); Sov.J.Particles Nucl. 5, 152 (1974)
R.Engfer, H.-K.Walter, H.Schneuwly
Study of the Properties of Atomic Nuclei with the Aid of Muonic Atoms
NUCLEAR STRUCTURE, Mesic-Atoms 93Nb, 115In, 127I, 133Cs, 139La, 141Pr, 151Eu, 190,192Os, 199,200Hg, 203,205Tl, 209Bi; calculated hyperfine splitting constants. 150Nd, 152Sm, 154,156,158,160Gd, 166Er, 170Yb, 182,184,186W, 188,190,192Os, 194,196Pt, 198,199,200,202Hg, 153Eu, 169Tm, 181Ta, 185,187Re, 191,193Ir, 203,205Tl; calculated muonic excitation probabilities.
Nucl.Phys. A223, 13 (1974)
H.Helppi, A.Pakkanen, J.Hattula
The E2/M1 Mixing of the Transitions from the Kπ = 2+ Bands in 190,192Os and 192Pt
RADIOACTIVITY 190Ir [from 192Os(p, 3n)], 192Ir [from 191Ir(n, γ)]; measured γγ, γγ(θ). 190,192Os, 192Pt deduced γ-multipole mixing. Natural targets.
doi: 10.1016/0375-9474(74)90276-0
Nucl.Phys. A230, 365 (1974)
P.Hornshoj, P.G.Hansen, B.Jonson, H.L.Ravn, L.Westgaard, O.B.Nielsen
Widths for s- and d-Wave α-Decay of Neutron-Deficient Isotopes with Z ≤ 82
RADIOACTIVITY 188,189,190,191,192Pb [from 232Th(p, spall)]; measured K X/α; deduced α-branching ratios. 180Hg [from Pb(p, spall)]; 176Pt [from 180Hg α-decay]; measured Eα, Iα, αγ-coin; deduced α fine-structure intensities. Mass-separated samples, natural target. Si surface barrier detector Ge(Li) detector.
doi: 10.1016/0375-9474(74)90143-2
Nucl.Instrum.Methods 116, 457 (1974)
N.Lavi
160Tb, 182Ta, and 192Ir as Efficiency Calibration Standards for Ge(Li) Detectors
RADIOACTIVITY 160Tb, 182Ta, 192Ir; measured Eγ, Iγ.
Phys.Rev. C9, 1091 (1974)
Y.Le Beyec, M.Lefort, J.Livet, N.T.Porile, A.Siivola
New Neutron-Deficient Pb and Bi Nuclides Produced in Cross Bombardments with Heavy Ions
RADIOACTIVITY 189,190,191,191m,192,193,193m,194,195,195m,197mBi, 186,187,188,189,190,191,192Pb; measured T1/2, Eα, Iα.
COO-1265-154, p.119 (1974)
H.L.Sharma, N.M.Hintz
A Search for Collective Vibrational Excitations in 187Os, 189Os and 192Os by the (d, d') Reactions
NUCLEAR REACTIONS 187,189,192Os(d, d'), E=17 MeV; measured σ(Ed', θ). 187,189,192Os deduced levels, S.
BARC-777, p.61 (1974)
N.Singh, S.S.Bhati, P.C.Mangal, P.N.Trehan
Level Structure Studies in 192Pt and 192Os and Experimental Test of Pairing-Plus Quadrupole Model
RADIOACTIVITY 192Pt, 192Ir; measured Eγ, Iγ, γγ(θ). 192Ir, 192Os levels deduced J, γ-mixing.
Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 778 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.4, 102 (1974)
M.Subotowicz, Y.Sarzhinski
On the Parity of the 192Ir Ground State
RADIOACTIVITY 192Ir; measured βγ(θ); deduced ground state π.
Nucl.Phys. A235, 123 (1974)
N.A.Voinova, D.M.Kaminker, Y.V.Sergeenkov
Electric Monopole Component in the 2+' → 2+ Transition in 192Pt
RADIOACTIVITY 192Ir; measured ceγ(θ), ICC. 192Pt transition deduced E0/E2 mixing, γ-mixing, λ, nature of 2+' level.
doi: 10.1016/0375-9474(74)90181-X
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
Ann.Rep.Res.Reactor Inst., Kyoto Univ. 7, 1 (1974)
S.Yamada, K.Aoki, T.Hayashi
Gamma-Gamma Angular Correlations in the Decay of 192Ir
RADIOACTIVITY 192Ir; measured γγ(θ). 192Os, 192Pt levels deduced γ-mixing, J, δ.
ATOMKI Kozlem. 17, 171 (1975)
Z.Awwad, M.R.El-Aasser
Half-Life of the 4+ Excited State in 192Pt
RADIOACTIVITY 192Ir; measured ce ce(t). 192Pt level deduced T1/2.
Z.Phys. A273, 43 (1975)
J.Becker, S.Beshai, L.Eriksson, L.Gidefeldt
Gamma-Gamma Directional Correlation Measurements in 192Os
RADIOACTIVITY 192Ir; measured γγ(θ). 192Os levels deduced γ-mixing.
Z.Naturforsch. 30a, 274 (1975)
G.L.Borchert, W.Scheck, K.P.Wieder
Precision Measurement of the γ-Ray Energies from the Radioactive Decay of 51Cr, 169Yb, 170Tm, 192Ir and 203Hg
RADIOACTIVITY 51Cr, 169Yb, 170Tm, 192Ir, 203Hg; measured precision Eγ.
Phys.Rev. C12, 702 (1975)
B.K.Dasmahapatra
K-Capture Probability (p(K)) in the Decay of 152Eu (12.4 yr) and 192Ir (74 Day)
RADIOACTIVITY 152Eu, 192Ir; measured K X-ray, γ-ray sum peak areas; deduced K-capture probability.
Phys.Lett. 55B, 436 (1975)
L.Funke, P.Kemnitz, G.Winter, S.A.Hjorth, A.Johnson, T.Lindblad
Rotation Alignment in 190Pt and 192Pt
NUCLEAR REACTIONS 190Os(α, 4n), E=46 MeV; 192Os(α, 4n), E=48 MeV; measured Eγ, Iγ, γ(t), I(ce), γγ-coin, γ(θ). 190,192Pt deduced levels, J, π, T1/2, λ, ICC.
doi: 10.1016/0370-2693(75)90549-3
Hyperfine Interactions 1, 113 (1975)
I.Katayama, S.Morinobu, H.Ikegami
Nuclear g Factors of the First and Second 2+ States in 192,194Pt
RADIOACTIVITY 192,194Ir; measured γγ(θ, H, t). 192,194Pt levels deduced g. IPAC.
Z.Phys. A274, 223 (1975)
V.Lakshminarayana, R.Brock, H.Hubel
Level Structure of 192Au and 194Au
NUCLEAR REACTIONS Ir(α, 3nγ), E=34-43 MeV; measured σ(E, Eγ, θ), γγ-coin. 192,194Au deduced levels.
Nucl.Phys. A248, 317 (1975)
R.M.Lieder, H.Beuscher, W.F.Davidson, A.Neskakis, C.Mayer-Boricke
Excitation of High-Spin States in 190,191,192,193,194Hg Through (α, xn) Reactions
NUCLEAR REACTIONS 194,195,196Pt(α, xnγ), E=65-108 MeV; 181Ta(14N, 5nγ), E=93 MeV; measured Eγ, Iγ, γ(t), γ(θ), γγ(t). 190,191,192,193,194,195Hg deduced levels, J, π, δ, γ-branching. 190,192,194Hg levels deduced T1/2. 191,193Hg transitions deduced B(E2). Enriched targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(75)90168-2
Ann.Rep.Res.Reactor Inst., Kyoto Univ. 8, 72 (1975)
Y.Miyatake, S.Yamada, T.Hayashi
Measurements of Coincidence Spectra on Weak γ-Transitions in 192Pt
RADIOACTIVITY 192Ir; measured γγ(θ), γγ-coin; deduced log ft. 192Pt deduced levels, J, π, δ.
Indian J.Phys. 49, 350 (1975)
U.S.Pande, B.P.Singh
Gamma-Gamma-Gamma Angular Correlation Method for the Study of the Cascade 589-296-316 keV in Pt192
RADIOACTIVITY 192Ir; measured γγ(θ). 192Pt level deduced λ, δ.
Phys.Rev.Lett. 34, 1110 (1975)
M.Piiparinen, J.C.Cunnane, P.J.Daly, C.L.Dors, F.M.Bernthal, T.L.Khoo
High-Spin Level Systematics in 186-194Pt and Rotation-Alignment Coupling
NUCLEAR REACTIONS 186,188,190,192Os(α, xnγ), E=28-50 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 186,187,188,189,190,191,192,193,194Pt deduced levels, K, J, π. Systematics.
doi: 10.1103/PhysRevLett.34.1110
Nucl.Phys. A243, 317 (1975)
R.Prasad, L.Chaturvedi, S.N.Chaturvedi, A.K.Nigam
The Decay of 192Ir
RADIOACTIVITY 192Ir; measured Eγ, Iγ, γ(t), γγ-coin. 192Os, 192Pt deduced levels, transitions. Sum-coin spectrometer.
doi: 10.1016/0375-9474(75)90251-1
Yad.Fiz. 21, 1145 (1975); Sov.J.Nucl.Phys. 21, 589 (1976)
P.T.Prokofev, L.I.Simonova
Double Internal Conversion in 150Sm, 179Hf and 192Ir
RADIOACTIVITY 150Sm, 179Hf, 192Ir; measured double internal conversion, ICC.
Program and Theses, Proc.25th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Leningrad, p.148 (1975)
P.T.Prokofev, L.I.Simonova, Zh.Kern
Lower Excited States of 192Ir
NUCLEAR REACTIONS 191Ir(n, γ), E not given; measured γ-spectra, ce-spectra. 192Ir deduced levels, J, π, γ-multipolarity, δ, B(n).
BARC-831, p.62 (1975)
N.Singh, S.S.Bhati, P.Das, P.N.Trehan
Conversion Coefficient Measurements in 144Pr, 192Pt and 192Os
RADIOACTIVITY 144Pr, 192Ir; measured I(ce), Eγ, Iγ; deduced ICC. 192Pt deduced levels, J, π, λ, δ. 192Os transitions deduced δ, λ.
Yad.Fiz. 22, 873 (1975); Sov.J.Nucl.Phys. 22, 455 (1976)
T.B.Vandlik, J.Vandlik, N.G.Zaitseva, Z.Mate, I.Mahunka, M.Mahunka, H.Tyrroff, T.Fenyes
Decay of the Isotopes 192Tl and 190Tl
RADIOACTIVITY 190,192Tl; measured Eγ, Iγ, I(ce), T1/2; deduced log ft, ICC. 190,192Hg deduced levels, J, π, λ.
CSNSM 1973-1975 Prog.Rept., p.32 (1975)
C.Vieu, J.S.Dionisio, V.Berg, C.Bourgeois
Les Spectres de Positons Emis par 191,192,193Hg et 191,192,193Au
RADIOACTIVITY 191,192,193Hg, 191,192,193Au; measured positron spectra; deduced Q(EC). Gerholm spectrometer.
Nucl.Phys. A258, 43 (1976)
F.T.Baker, T.H.Kruse, W.Hartwig, I.Y.Lee, J.X.Saladin
Nuclear Shapes of the Transitional Nuclei 186,188,190,192Os
NUCLEAR REACTIONS 186,188,190,192Os(α, α'), E=13-24 MeV, θlab=130°; measured σ(E, Eα'). 186,188,190,192Os deduced β2 charge, mass deformations, 186,188,192Os deduced β4 charge, mass deformations. 192Os(α, α'), E=24 MeV; measured σ(Eα', θ). 192Os deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(76)90526-1
Phys.Rev.Lett. 37, 193 (1976)
F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin
Experimental Determination of the Signs of E2 Interference Terms for 192Os and 194Pt
NUCLEAR REACTIONS 192Os, 194Pt(α, α'), E=12-24 MeV; analyzed data. 192Os, 194Pt deduced sign of interference term.
doi: 10.1103/PhysRevLett.37.193
J.Phys.(London) G2, 823 (1976)
D.K.Butt, M.A.Raoof, S.A.Raoof
The Measurement of the Electromagnetic Lifetimes of the First Four Excited States of 192Pt
RADIOACTIVITY 192Ir; measured (ce)(ce)t. 192Pt levels deduced T1/2, B(λ).
doi: 10.1088/0305-4616/2/11/007
Phys.Rev. C13, 2197 (1976)
J.C.Cunnane, M.Piiparinen, P.J.Daly, C.L.Dors, T.L.Khoo, F.M.Bernthal
High-Spin Level Structure of 190Pt and 192Pt
NUCLEAR REACTIONS 190,192Os(α, 4nγ), 188,190Os(α, 2nγ), E=28-50 MeV; measured σ(E, Eγ, θ), γγ(t). 190,192Pt deduced levels, J, π, T1/2, backbending.
Nucl.Phys. A262, 328 (1976)
S.A.Hjorth, A.Johnson, T.Lindblad, L.Funke, P.Kemnitz, G.Winter
Two-Quasiparticle and Rotation-Aligned Structures in 190Pt, 192Pt and 194Pt
NUCLEAR REACTIONS 190,192Os(α, 4nγ), E=43-51 MeV; 188,190,192Os(α, 2nγ), E=23-27 MeV; measured σ(Eα, Eγ, θ), Eγ, Iγ, γγ-coin, γγ-delay, Ee, Ie. 190,192,194Pt deduced levels, J, π, T1/2, ICC. Calculations within the rotation-alignment model.
doi: 10.1016/0375-9474(76)90625-4
J.Phys.(Paris) 37, 1383 (1976)
J.Jastrzebski, R.Kaczarowski, J.Lukasiak, S.Andre, J.Treherne
Levels in 192Os Excited by the (p, p') and (d, d') Reactions
NUCLEAR REACTIONS 192Os(p, p'γ), E=16 MeV; 192Os(d, d'γ), E=23.2 MeV; measured Eγ, Iγ, γγ-coin. 192Os deduced levels, K, J, π.
Helv.Phys.Acta 49, 645 (1976)
A.Raemy, W.Beer, J.-C.Dousse, R.Eichler, J.Kern, T.von Ledebur, W.Schwitz
Dispositif pour la Mesure de Reactions (n, γ) a l'Aide d'un Spectrometre a Cristal Incurve
NUCLEAR REACTIONS 191,193Ir(n, γ); measured Eγ. 192,194Ir deduced transitions.
Proc.Int.Conf.Selected Topics in Nucl.Struct., Dubna, Vol.1, p.63 (1976); JINR-D-9682 (1976)
I.A.Romany, A.P.Kliucharev, V.A.Lutsik, Y.N.Rakivnenko
Decay Schemes of Isomers 192mAu and 194mAu
NUCLEAR REACTIONS 191,193Ir(α, 3n), E=38 MeV; measured Eγ, I(ce), (ce)(ce)-coin, isomer ic production ratio. 192,194Au levels deduced J, π, γ-branching.
Univ.Paris, Inst.Phys.Nucl., Ann.Rept., p.N38 (1976)
M.Vergnes, G.Rotbard, G.Berrier, J.Kalifa, J.Vernotte, R.Seltz, H.L.Sharma, N.M.Hintz
Etudes des Pt au moyens des Reactions (p, t) et (p, d)
NUCLEAR REACTIONS 192,194,196Pt(p, d), (p, t), E=26 MeV; measured σ(θ). 190,191,192,193,194,195Pt deduced levels.
Phys.Lett. 66B, 129 (1977)
R.D.Bagnell, Y.Tanaka, R.K.Sheline, D.G.Burke, J.D.Sherman
Possible Hexadecapole Vibrations in 190,192Os
NUCLEAR REACTIONS 191,193Ir(t, α), E=15 MeV; measured σ(Eα). 190,192Os levels deduced possible hexadecapole character.
doi: 10.1016/0370-2693(77)90157-5
J.Phys.(Paris), Lett. 38, L-393 (1977)
S.Della Negra, B.Lagarde, Y.Le Beyec
Very Neutron-Deficient Polonium Isotopes Produced Through 20Ne Induced Reactions
RADIOACTIVITY 194,193,193mPo; measured Eα, T1/2. 192Po; measured Eα.
Phys.Rev. C16, 902 (1977)
D.L.Hanson, K.A.Erb, J.S.Vaagen, R.J.Ascuitto, D.A.Bromley, J.J.Kolata
Quadrupole Transfer Strength Studied Through Heavy-Ion Induced Two-Neutron Transfer between the Shape Transitional Nuclei 190,192Os
NUCLEAR REACTIONS 192Os(12C, 12C), (12C, 14C), E=70 MeV; measured σ(θ); deduced effect of shape transitions on quadrupole transfer strength. CCBA analysis.
Phys.Rev.Lett. 39, 1313 (1977)
M.V.Hoehn, E.B.Shera, Y.Yamazaki, R.M.Steffen
Electromagnetic Moments of the Even Os Nuclei from Muonic X Rays
NUCLEAR REACTIONS 186,188,190,192Os(μ-, X-ray), E ≈ 0 MeV; measured muonic X-ray spectra. 186,188,190,192Os levels deduced B(E2), quadrupole moment.
doi: 10.1103/PhysRevLett.39.1313
Phys.Rev. C15, 1325 (1977)
N.R.Johnson, P.P.Hubert, E.Eichler, D.G.Sarantites, J.Urbon, S.W.Yates, T.Lindblad
Lifetimes of Ground-Band States in 192Pt and 194Pt
NUCLEAR REACTIONS 192,194Pt(40Ar, 40Ar'γ), E=149 MeV; measured Coulomb excitation, Doppler shift recoil distance. 192,194Pt levels deduced T1/2, B(E2).
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
J.Phys.(London), G3, 637 (1977)
K.V.Ramaniah, G.K.Raju, K.V.Reddy
Spectral Shape Studies in the Beta Decay of 192Ir
RADIOACTIVITY 192Ir; measured β-spectrum shape, βγ-coin. 192Pt levels deduced J, π.
Phys.Rev. C16, 571 (1977)
R.M.Ronningen, R.B.Piercey, A.V.Ramayya, J.H.Hamilton, S.Raman, P.H.Stelson, W.K.Dagenhart
Coulomb Excitation of 2+ and 3- States in 192Pt and 194Pt
NUCLEAR REACTIONS 192,194Pt(α, α'), E=14.9 MeV; measured Coulomb excitation. 192,194Pt levels deduced B(E2), B(E3). Enriched targets.
Bull.Am.Phys.Soc. 22, No.4, 545, BG1 (1977)
G.Scharff-Goldhaber
Multipole Order and Enhancement Factor of Long-Lived Isomeric Transition in 192Ir
NUCLEAR STRUCTURE 192Ir transition calculated enhancement.
Nukleonika 22, 31 (1977)
R.Seltz
Is the (p, t) Reaction a Useful Tool for the Investigation of Shape Transition and Core-Excitation in Nuclei < question >
NUCLEAR REACTIONS 192,194,196Pt(p, t), E=26 MeV; 205,203Tl(p, t), E=19 MeV; measured σ(θ). 201,203Tl levels deduced J, π, L. 190,192,194Pt level deduced β-vibrational character. Davydov, Kumer-Baranger models. Intermediate coupling calculations, DWBA analysis.
Proc.Intern.Conf.Nucl.Structure, Tokyo, Vol.1, p.438 (1977)
T.Tohei, N.Sekine, T.Nakagawa, T.Suehiro, K.Miura, Y.Ishizaki
High Spin States in Even Pt Isotopes
NUCLEAR REACTIONS 194,196Pt(p, t), E=52 MeV; measured σ(Et, θ). 192,194Pt deduced levels.
JINR-P6-10417 (1977)
T.Vylov
Precision Spectrometry of Gamma-Rays of Radioactive Nuclides using Semiconductor Detectors
RADIOACTIVITY 22,24Na, 65Zn, 75Se, 95mTc, 88Y, 56,57,60Co, 113Sn, 109Cd, 133Ba, 134Cs, 110mAg, 139,144Ce, 140La, 160Tb, 169Yb, 152Eu, 182Ta, 198Au, 192Ir, 203Hg, 171,173Lu, 209Bi, 241Am; measured Eγ, Iγ.
JINR-P6-10414 (1977)
T.Vylov, V.S.Aleksandrov, L.A.Vydova, V.M.Gorozhankin, A.F.Novgorodov, S.Omanov, B.P.Osipenko, M.I.Fominykh, V.G.Chumin, Y.Yurkovski
Spectrometry of Radioactive Nuclide Radiation using Semiconductor Detectors. 4. Standard Gamma-Ray Energies and Relative Intensities
RADIOACTIVITY 23Na, 65Zn, 75Se, 95mTc, 88Y, 56,57,60Co, 113Sn, 109Cd, 133Ba, 134Cs, 110mAg, 139,144Ce, 140La, 160Tb, 169Yb, 152Eu, 182Ta, 198Au, 192Ir, 203Hg, 171,173Lu, 207Bi, 241Am; measured Eγ, Iγ.
JINR-P6-10416 (1977)
Ts.Vylov, V.S.Aleksandrov, Yu.A.Andreev, V.N.Gorozhankin, A.I.Ivanov, Sh.Omanov, B.P.Osipenko, E.K.Stepanov, V.G.Chumin
Spectrometry of Radioactive Nuclide Radiation using Semiconductor Detectors. 6. Gamma-Rays of Radioactive Nuclides used in Spectrometer Calibration
RADIOACTIVITY 171Lu, 75Se, 169Yb, 133Ba, 156Gd, 173Lu, 207Bi, 192Ir, 134Cs, 182Ta, 152Eu, 144Ce, 160Tb, 110mAg, 56Co; measured Eγ, Iγ.
Phys.Rev. C16, 1549 (1977)
L.K.Wagner, E.B.Shera, G.A.Rinker, R.K.Sheline
Model-Independent Interpretation of the Dynamic Hyperfine Effect in Muonic Atoms with an Application to 192Os
NUCLEAR MOMENTS, Mesic-Atoms 192Os; measured muonic X-ray spectra; deduced charge parameters, static quadrupole charge density, electric moments.
Phys.Rev. C17, 1559 (1978)
F.T.Baker, A.Scott, R.M.Ronningen, T.H.Kruse, R.Suchannek, W.Savin
192Pt(α, α') Reaction at E = 24 MeV
NUCLEAR REACTIONS 192Pt(α, α'), E=24 MeV; measured σ(Eα', θ). 192Pt levels deduced β, relative signs of matrix elements. Coupled channels analysis. Enriched target.
Nucl.Phys. A294, 66 (1978)
J.Burde, V.Richter
Lifetime Measurements of the 3+ and 41+ States in 192Pt
RADIOACTIVITY 192Ir [from 191Ir(n, γ)]; measured βce(t). 192Pt levels deduced T1/2, B(E2). Natural target.
doi: 10.1016/0375-9474(78)90395-0
Phys.Lett. 78B, 48 (1978)
D.G.Burke, M.A.M.Shahabuddin, R.N.Boyd
Hexadecapole Vibrations in Osmium Isotopes
NUCLEAR REACTIONS 188,190,192Os(α, α'), E=24 MeV; measured σ(θ). 188,190,192Os deduced β(L).
doi: 10.1016/0370-2693(78)90344-1
Nucl.Phys. A309, 206 (1978)
R.F.Casten, H.G.Borner, J.A.Pinston, W.F.Davidson
Level Structure of 192Os and the IBA Model
NUCLEAR REACTIONS 191Os(n, γ), E=th; measured σ(Eγ), Eγ, Iγ. 192Os deduced levels, K, J, π. Two-neutron capture on enriched 190Os target, bent-crystal spectrometer.
doi: 10.1016/0375-9474(78)90543-2
Contrib.Int.Symp.Neutron Capture Gamma-Ray Spectrosc. and Related Topics, 3rd, BNL, Upton, NY, No.20 (1978)
C.Coceva, P.Giacobbe
Low Energy γ Rays from Resonance Neutron Capture in 191Ir
NUCLEAR REACTIONS 191Ir(n, γ), E not given; measured Eγ, Iγ. 192Ir deduced J of parent states contributing to γ-decay.
Phys.Rev. C17, 501 (1978)
E.R.Flynn, D.G.Burke
188,190,192Os(t, p) Reaction at 15 MeV
NUCLEAR REACTIONS 188,190,192Os(t, p), E=15 MeV; measured σ(Ep, θ). 190,192,194Os deduced levels, J, π.
Nucl.Instrum.Methods 155, 189 (1978)
R.G.Helmer, R.C.Greenwood, R.J.Gehrke
Reevaluation of Precise γ-Ray Energies for Calibration of Ge(Li) Spectrometers
COMPILATION 51Cr, 57,60Co, 109Cd, 137Cs, 139,141Ce, 145Eu, 153Sm, 160Tb, 169Yb, 170Tm, 183Ta, 198,199Au, 203Hg, 241Am, 192Ir, 182Ta, 152Eu, 153Gd, 169Yb, 7Be, 22Na, 46Sc, 54Mn, 58Co, 59Fe, 65Zn, 75Se, 85Sr, 88Y, 94,95Nb, 95Zr, 95mTc, 113Sn, 133Ba, 185Os, 203Pb, 207Bi, 228Th; compiled, reevaluated Eγ, measurement relative to 411-keV γ-ray from 198Au. Curved-crystal diffraction spectrum.
Phys.Rev.Lett. 40, 171 (1978)
E.G.Kessler, Jr., R.D.Deslattes, A.Henins, W.C.Sauder
Redetermination of 198Au and 192Ir γ-Ray Standards between 0.1 and 1.0 MeV
RADIOACTIVITY 198Au, 192Ir; measured absolute Eγ.
doi: 10.1103/PhysRevLett.40.171
Nucl.Phys. A301, 365 (1978)
D.Mertin, R.Tischler, A.Kleinrahm, R.Kroth, H.Hubel, C.Gunther
Investigation of Level Energies and B(E2) Values for Rotation-Aligned Bands in Hg Isotopes
NUCLEAR REACTIONS 192,194,198Pt(α, xn), E=31-57 MeV; 192Pt(3He, 4n), E=35 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, I(ce), ce(t). 197Hg deduced levels, J, π. 197,199Hg deduced ICC. 191,192,193,195,197Hg deduced T1/2, B(λ).
doi: 10.1016/0375-9474(78)90055-6
Phys.Scr. 17, 487 (1978)
C.Roulet, H.Sergolle, P.P.Hubert, T.Lindblad
Study of Transition Probabilities in 192Pt
NUCLEAR REACTIONS 192Pt(84Kr, 84Kr'γ), E=370 MeV; measured Coulomb excitation. 192Pt deduced levels, J, π, B(E2).
Z.Phys. A288, 67 (1978)
R.Tischler, D.Mertin, A.H.El Farrash, B.V.T.Rao, R.Kroth, A.Kleinrahm, C.Gunther, H.Hubel
Lifetimes of Rotation-Aligned States in 190-193Pt
NUCLEAR REACTIONS Os, 190Os(α, 3n), E=40 MeV; Os, 190Os(α, 4n), E=49 MeV; measured Eγ, Iγ, I(ce), ce(t). 188,190,191,192,193Pt levels deduced T1/2, B(E2).
Phys.Rev. C20, 42 (1979)
R.D.Bagnell, Y.Tanaka, R.K.Sheline, D.G.Burke, J.D.Sherman
Two-Quasiproton States in 190Os and 192Os Studied with the (t, α) Reaction
NUCLEAR REACTIONS 191,193Ir(t, α), E=15 MeV; measured σ(Eα, θ). 190,192Os deduced levels, J, π, K assignments. DWBA, strong coupling model, RPA.
Phys.Rev. C19, 1205 (1979)
B.L.Berman, D.D.Faul, R.A.Alvarez, P.Meyer, D.L.Olson
Giant Resonance in Transitional Nuclei: Photoneutron Cross Sections for Osmium Isotopes
NUCLEAR REACTIONS 186,188,189,190,192Os(γ, xn), E=7-30 MeV; measured 4π-neutron yield, multiplicities, average energies for X=1-3. 186,188,190,192Os deduced GDR parameters, nuclear shape parameters, integral σ(γ, nx), B(E2).
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
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.
ZFK-385, p.52 (1979)
L.Funke, P.Kemnitz, G.Winter, F.Donau
Zur Dreiaxialitat der Pt-Isotope
NUCLEAR REACTIONS 188,190,192Os(α, 2n), E=27 MeV; measured Eγ, Iγ, γ(θ). 190,192,194Pt levels deduced δ, B(E2) ratios.
Phys.Rev. C20, 2293 (1979)
S.B.Kaufman, E.P.Steinberg, G.W.Butler
Spallation of Gold by 100-300 MeV Pions
NUCLEAR REACTIONS 197Au(π-, X), (π+, X), E=100-300 MeV; measured Eγ, Iγ. 196,196mAu, 194Au, 192,193mHg, 192Au, 190,188Ir deduced independent yields, σ ratio. 191,193Au, 191,188,186Pt, 189,188m,185,184Ir, 182,183,183m,185Os, 181Re, 173,174,175,177Ta, 176W, 171Lu, 167Tm deduced cumulative yields, σ ratio.
Priv.Comm. (September 1979)
N.Kaffrell
Phys.Lett. 80B, 194 (1979)
A.Neskakis, R.M.Lieder, H.Beuscher, Y.Gono, D.R.Haenni, M.Muller-Veggian, C.Mayer-Boricke
Observation of Rotation-Aligned Bands in the Odd-Odd Nuclei 190,192,194Au
NUCLEAR REACTIONS 191,193Ir(α, xn), E=40, 61.5, 63 MeV; measured Eγ, Iγ, γ-branching for X=3, 5. 190,192,194Au deduced levels, δ, rotational-aligned bands based on (11-), (12-) isomers. Configurations in agreement with triaxial-rotor-plus-particle model.
doi: 10.1016/0370-2693(79)90196-5
Nucl.Phys. A323, 495 (1979)
C.Roulet, G.Albouy, G.Auger, J.M.Lagrange, M.Pautrat, K.G.Rensfelt, H.Richel, H.Sergolle, J.Vanhorenbeeck
Properties of 192,190Pb: Behaviour of the Very Neutron-Deficient Even Lead Isotopes
NUCLEAR REACTIONS 156Gd(40Ar, 4nγ), E=190 MeV; 154Gd(40Ar, 4nγ), E=195 MeV; 156Gd(40Ar, 6nγ), E=225 MeV; 182W(16O, 6nγ), E=132 MeV; measured Eγ, Iγ, γγ(E, t), γX-coin. 192,190Pb deduced levels, γ-branching. 192Pb level deduced T1/2.
doi: 10.1016/0375-9474(79)90122-2
LAFI-10 (1979)
L.I.Simonova, N.D.Kramer, P.T.Prokofev
Internal Conversion Electron Spectra of 192,194Ir Emitted by (n, γ) Reaction
RADIOACTIVITY 192,194Ir [from thermal n-irradiation of 191,193Ir]; measured I(ce). 192,194Ir transitions deduced γ-multipolarity.
Phys.Rev. C19, 2399 (1979)
K.S.Toth, M.A.Ijaz, C.R.Bingham, L.L.Riedinger, H.K.Carter, D.C.Sousa
Anomalous α-Decay Rate of 192Pb
RADIOACTIVITY 192Pb [from 180W(16O, 4n), E not given]; measured T1/2, Eγ, Iγ, I(ce), Eα, Iα, γγ-coin; deduced α-reduced widths. 192Tl deduced levels.
Phys.Rev. C22, 2383 (1980)
C.Baktash, J.X.Saladin, J.J.O'Brien, J.G.Alessi
Electromagnetic Properties of the Low-Lying States in Heavy (A≈190)Transitional Nuclei
NUCLEAR REACTIONS 188,190,192Os(α, α'), E=14.5 MeV; 188,190,192Os(16O, 16O'), E=48 MeV; 188,190,192Os(32S, 32S'), E=62 MeV; measured(particle)γ-coin, Coulomb excitation. 188,190,192Os levels deduced quadrupole moment, γbranching ratio. Thick natural target. 188Os(16O, 16O'), E=45 MeV; measured σ(E(16O), θ). 188Os levels deduced quadrupole moment. Thin enriched target. Coupled-channel analysis, semiclassical, quantum mechanical models.
Ann.Phys.(New York) 129, 378 (1980)
R.D.Deslattes, E.G.Kessler, W.C.Sauder, A.Henins
Remeasurement of γ-Ray Reference Lines
RADIOACTIVITY 198Au, 192Ir, 170Tm, 169Yb; measured Eγ for reference standard transitions. Double-crystal transmission instruments.
doi: 10.1016/0003-4916(80)90394-2
Nucl.Phys. A348, 25 (1980)
C.Ekstrom, L.Robertsson, S.Ingelman, G.Wannberg, I.Ragnarsson, and the ISOLDE Collaboration
Nuclear Ground-State Spin of 185Au and Magnetic Moments of 187,188Au: Further evidence for coexisting nuclear shapes in this mass region
NUCLEAR MOMENTS 185Au; measured hfs, J. 187Au measured hfs, a, μ. 188Au; measured a; deduced μ. ABMR technique.
doi: 10.1016/0375-9474(80)90543-6
Int.J.Appl.Radiat.Isotop. 31, 153 (1980)
H.Houtermans, O.Milosevic, F.Reichel
Half-lives of 35 Radionuclides
RADIOACTIVITY 22,24Na, 46Sc, 51Cr, 55,59Fe, 57,58,60Co, 67Ga, 75Se, 85Sr, 88Y, 95Zr, 95Nb, 99Mo, 99mTc, 103,106Ru, 110mAg, 111In, 113Sn, 125Sb, 125,131I, 134,137Cs, 133Ba, 140La, 144Ce, 169Yb, 180mHf, 192Ir, 203Hg, 203Pb; measured T1/2. 4π-γ ionization chamber, proportional counter, NaI(Tl) crystal , Ge(Li) spectrometer.
doi: 10.1016/0020-708X(80)90139-8
Phys.Rev. C21, 933 (1980)
A.J.Kreiner, A.Filevich, G.Garcia Bermudez, M.A.J.Mariscotti, C.Baktash, E.der Mateosian, P.Thieberger
High-Spin Band Structure of 192Tl
NUCLEAR REACTIONS 181Ta(18O, xnγ), E=105-125 MeV; 181Ta(16O, xnγ), E=95-105 MeV; measured Eγ, Iγ, σ(E, Eγ, θγ), γγ-coin. 192Tl levels deduced δ, J, π, T1/2. Natural target. Ge(Li) detectors.
Program and Theses, Proc.30th Ann.Conf.Nucl.Spectrosc.At.Nuclei, Leningrad, p.141 (1980)
I.A.Romany, V.A.Lutsik, Yu.N.Rakivnenko, E.A.Skakun, G.I.Yatsenko, E.A.Ivanov, A.Iordachescu, M.Ionescu-Bujor, D.Plostinaru
The Decay Scheme of the 192Au Isomer
RADIOACTIVITY 192Au [from 191Ir(α, 3n), E=38 MeV; 193Ir(3He, 4n), E=31 MeV]; measured Eγ, Iγ, I(ce), (ce)(ce)-coin; deduced levels, γ-branching, γ-multipolarity.
Nucl.Phys. A346, 329 (1980)
N.Sekine, T.Tohei, T.Nakagawa, Y.Ishizaki
Effects of Inelastic Multistep Processes on (p, t) Reactions in a Transition Region between Rare-Earth Nuclei and Double-Magic 208Pb
NUCLEAR REACTIONS 188Os, 194,196Pt, 200,202Hg(p, t), E=51.9 MeV; measured σ(Et, θ); deduced reaction mechanism. Enriched targets. DWBA, coupled-channel Born approximation analyses.
doi: 10.1016/0375-9474(80)90473-X
Program and Theses, Proc.30th Ann.Conf.Nucl.Spectrosc.At.Nuclei, Leningrad, p.140 (1980)
L.I.Simonova, N.D.Kramer, P.T.Prokofev
Multipolarity of Certain Transitions in 192Ir
NUCLEAR REACTIONS 191Ir(n, γ), E=reactor; measured I(ce). 192Ir deduced transition γ-multipolarity.
Priv.Comm. (October 1980)
C.Y.Wu, D.Cline, T.Czosnyka, L.Hasselgren, P.Russo, J.K.Sprinkle, I.Y.Lee, P.A.Butler, R.M.Diamond, F.S.Stephens, C.Baktash, S.Steadman
Nucl.Instrum.Methods 174, 133 (1980)
Y.Yoshizawa, Y.Iwata, Y.Iinuma
Precision Measurements of Gamma-Ray Intensities. II. 152Eu, 154Eu and 192Ir
RADIOACTIVITY 152,154Eu, 192Ir; measured Eγ, Iγ; deduced relative Iγ. 192Ir deduced Iγ per decay. Ge(Li) detector, high precision.
Nucl.Phys. A371, 68 (1981)
F.T.Baker, M.A.Grimm, Jr., A.Scott, R.C.Styles, T.H.Kruse, K.Jones, R.Suchannek
192Os(α, α') Reaction at Eα = 24 MeV and the IBA Model
NUCLEAR REACTIONS 192Os(α, α), (α, α'), E=24 MeV; measured σ(θ), σ(Eα', θ). 192Os deduced B(E4), deformation parameter β4. Enriched target. Interacting boson model, coupled-channels analysis.
doi: 10.1016/0375-9474(81)90745-4
Z.Phys. A301, 35 (1981)
S.A.Hjorth, A.Johnson, A.Kerek, W.Klamra, Th.Lindblad, S.Messelt, C.Pomar, W.Walus, O.Skeppstedt, Z.Sujkowski, A.Zglinski, L.Carlen, H.Ryde, M.Piiparinen
On the Decay of Compound Nuclei following Alpha-Particle and 12C Induced Reactions
NUCLEAR REACTIONS 192Os, 122Te, 166Er(α, 3n), (α, 4n), (α, 5n), E=51-55 MeV; 176Yb, 164Dy (12C, 8n), (12C, 6nα), 160Gd, 164Dy(12C, 6n), (12C, 7n), 160Gd(12C, 8n), E=118 MeV; measured Eγ, Iγ, γγ-coin; deduced average multiplicity, average side feeding multiplicity, multiplicity distribution second moment. 180Os, 170,169,168Hf, 166Yb, 192Pt, 122Xe deduced spin distribution, decay mechanism. Statistical model calculations. Ge(Li), NaI(Tl) detectors.
Phys.Rev. C24, 1667 (1981)
M.V.Hoehn, E.B.Shera, H.D.Wohlfahrt, Y.Yamazaki, R.M.Steffen, R.K.Sheline
Muonic X-Ray Study of the Even Os Nuclei
ATOMIC PHYSICS, Mesic-Atoms 186,188,190,192Os; measured muonic X-rays; deduced monopole, quadrupole charge parameters, isotope, isomer shifts.
Res.Inst.Phys., Stockholm, 1981 Ann.Rept., p.106 (1981)
Ph.Hubert, C.Roulet, H.Sergolle, Th.Lindblad, H.J.Wollersheim, E.Grosse, R.Simon, H.Emling, P.Fuchs, D.Schwalm
Multiple Coulomb Excitation in 192Pt
NUCLEAR REACTIONS 192Pt(208Pb, 208Pb'), E not given; analyzed Coulomb excitation data. 192Pt deduced levels, B(E2), J, π.
Phys.Rev. C24, 2370 (1981)
M.E.Leino, S.Yashita, A.Ghiorso
Alpha Decay of Neutron Deficient Polonium and Bismuth Isotopes
RADIOACTIVITY 192,193,193m,194Po, 191mBi; measured T1/2, Eα. Gas filled on-line mass separator.
Phys.Rev. C24, 2245 (1981)
D.C.Sousa, L.L.Riedinger, C.R.Bingham, F.E.Turner, K.S.Toth, H.K.Carter, R.L.Mlekodaj, E.H.Spejewski
Radioactive Decay of Mass-Separated 192Tl and 192Pb
RADIOACTIVITY 192,192mTl, 192Pb [from Ta, W(16O, xn), E=100, 133, 143 MeV]; measured Eγ, Iγ, I(ce), γγ-coin, T1/2; deduced log ft. 192Hg, 192Tl deduced levels, J, γ-multipolarity, δ, ICC.
IPNO-T-82-01 (1982)
V.Albin
Spectroscopie sur Faisceau des Isotopes du Plomb tres Deficients en Neutrons
NUCLEAR REACTIONS 182,184W(16O, 4n), (16O, 5n), E=100 MeV; 184W(16O, 6n), E=100 MeV; 182W(16O, 6n), (16O, 5n), E=105 MeV; measured Eγ, Iγ, γγ(θ), I(ce), E(X-ray), I(X-ray), γγ-, γ(X-ray)-coin. 195Pb deduced levels, γ-branching, γ-multipolarity, J, π, δ, T1/2. 194Pb deduced levels, T1/2, J, π, γ-branching. 193Pb deduced levels, J, π, γ-multipolarity, γ-branching.
Nucl.Phys. A388, 77 (1982)
N.Blasi, R.Bijker, M.N.Harakeh, Y.Iwasaki, W.A.Sterrenburg, S.Y.Van Der Werf, M.Vergnes
Study of the 193Ir(3He, d)194Pt and 193Ir(d, 3He)192Os Reactions: Test of a supersymmetric coupling scheme
NUCLEAR REACTIONS 193Ir(3He, d), (d, 3He), E=40 MeV; measured σ(θ). 194Pt, 192Os levels, deduced L, C2S, possible supersymmetry model breakdown. DWBA analysis, U(6/4)group.
doi: 10.1016/0375-9474(82)90509-7
Nucl.Phys. A383, 421 (1982)
E.Dafni, C.Broude, F.D.Davidovsky, M.Hass, G.Schatz
Magnetic Moments of Isomeric Bandheads in Transitional Nuclei: 119I and 192Tl
NUCLEAR REACTIONS 109Ag(13C, 3n), E=52 MeV; 181Ta(16O, 5n), E=100 MeV; measured Iγ(θ, t). 119I level deduced g, T1/2. 192Tl level deduced g, quadrupole moment, T1/2.
doi: 10.1016/0375-9474(82)90085-9
Nucl.Phys. A390, 53 (1982)
A.Neskakis, R.M.Lieder, H.Beuscher, Y.Gono, D.R.Haenni, M.Muller-Veggian
Investigation of High-Spin States in Odd-Odd 190,192,194Au Nuclei
NUCLEAR REACTIONS 191,193Ir(α, 5n), E=63, 61.5 MeV; 193Ir(α, 3n), E=40 MeV; measured E(γ), I(γ), σ(Eγ, θ), αγ(t), γγ(t). 190,192,194Au deduced levels, J, π, T1/2, ICC, B(λ) ratios, δ, γ-branching. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(82)90606-6
Izv.Akad.Nauk SSSR, Ser.Fiz. 46, 892 (1982)
V.I.Popov, I.V.Surkova
Excitation of Collective States of Nuclei in the Transition Region A ≈ 190-200 by Inelastic Scattering of Low Energy Neutrons
NUCLEAR REACTIONS 188,190,192Os, 194,196,198Pt, 198,200,202,204Hg, 206Pb(n, n'γ), E=0.15-1 MeV; measured σ; deduced optical model parmeters. 188,190,192Os, 194,196,198Pt, 198,200,202,204Hg, 206Pb level deduced β2. Coupled-channels analysis.
Z.Phys. B49, 23 (1982)
G.Schatz, E.Dafni, H.H.Bertschat, C.Broude, F.D.Davidovsky, M.Hass
Electric Quadrupole Interaction of 192Tl(8-) Nuclei in Hexagonal Tl and in Tetragonal In Metals
RADIOACTIVITY 192Tl(EC), (β+) [from 181Tl(16O, 5n), E=100 MeV]; measured γ(θ, H, t); deduced isomer electric quadrupole interaction, quadrupole moment. Recoil implantation, noncubic hosts.
Nucl.Phys. A401, 175 (1983)
H.H.Bolotin, I.Morrison, C.G.Ryan, A.E.Stuchbery
Variations of the Gyromagnetic Ratios of Low-Lying States in 192Os
NUCLEAR STRUCTURE 190,192Os; calculated g. Interacting boson approximation, broken O(6) symmetry, Nilsson basis.
NUCLEAR REACTIONS 192Os(58Ni, 58Ni'), E=220 MeV; measured γ(θ, H, T) in polarized Co, (particle)γ-coin, Coulomb excitation. 192Os levels deduced g. Enriched target, thin foil technique.
doi: 10.1016/0375-9474(83)90343-3
Phys.Rev. C28, 1570 (1983)
C.Y.Chen, J.X.Saladin, A.A.Hussein
Redetermination of the Quadrupole Moment of the First 2+ State in 192Os and 194Pt
NUCLEAR REACTIONS 192Os, 194Pt(16O, 16O'), (16O, 16O), E=53 MeV; measured σ(E(16O')), Coulomb excitation, σ(elastic)/σ(inelastic). 192Os, 194Pt level deduced E2 transition matrix element, quadrupole moment. Semi-classical, coupled-channels analyses.
Nucl.Instrum.Methods 217, 113 (1983)
A.Chalupka, W.Bertl, L.Schonauer, K.U.Bahnsen, J.Labedzki, H.J.Scheerer, H.Vonach, G.Ziegler
New MWPCs for the Munich Q3D Spectrograph
NUCLEAR REACTIONS 154Gd, 160Dy(d, p), 193Ir(d, t), E=14 MeV; measured σ(Ep), σ(Et). Position sensitive detectors, Q3D spectrograph.
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
Int.J.Appl.Radiat.Isotop. 34, 1233 (1983)
H.H.Hansen, D.Mouchel
K/LM + Internal-Conversion Ratios for Pure E2 Transitions in the Decays of 152Eu and 192Ir
RADIOACTIVITY 152Eu(EC), (β+), (β-); 192Ir(EC), (β-); measured I(ce). 152Sm, 152Gd, 192Os, 192Pt transitions deduced subshell ICC ratios.
doi: 10.1016/0020-708X(83)90192-8
Phys.Rev. C27, 2608 (1983)
E.W.Kleppinger, S.W.Yates
(n, n'γ) Study of Collective Excitations in 192Os: Comparison with the boson models for transitional nuclei
NUCLEAR REACTIONS 192Os(n, n'γ), E=1-3 MeV; measured Eγ, Iγ, γ(θ), σ(Eγ) vs E. 192Os deduced levels, J, π, γ-branching, B(E2) ratios. Enriched target, Ge(Li) detector, tof background suppression.
Hyperfine Interactions 15/16, 223 (1983)
H.-E.Mahnke, W.Semmler
Probe Atom Dependence of the Electric Field Gradient in Bismuth
NUCLEAR REACTIONS 181Ta(16O, 5n), E=100 MeV; measured γ(θ, H, t); deduced Tl electric field gradient in Bi. 192Tl deduced isomer quadrupole moment.
Program and Theses, 33rd Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Moscow, p.148 (1983)
A.V.Murzin, V.A.Libman, I.V.Kononenko
Low Excited States in 192Ir, 194Ir Observed by Fast Neutrons with Average Energy of 2 and 24 keV
NUCLEAR REACTIONS 191,193Ir(n, γ), E=2 keV; measured Eγ, Iγ. 192,194Ir levels deduced J, π.
Hyperfine Interactions 15/16, 41 (1983)
J.Rikovska, D.Novakova, J.Ferencei
Gamma-Ray Linear Polarization and Nuclear Orientation Experiments on Oriented 192,194Ir(Fe)
RADIOACTIVITY 192Ir(EC), (β-); 194Ir(β-); measured γ(θ), γ linear polarization, oriented nuclei. 192,194Pt levels deduced δ.
Nucl.Instrum.Methods 206, 441 (1983)
U.Schotzig
Photon Emission Probabilities of 192Ir
RADIOACTIVITY 192Ir; measured E(X-ray), I(X-ray), γ-emission rates; deduced γ-, X-ray-emission probabilities. 4π γ high efficiency measurement.
Nucl.Data Sheets 40, 425 (1983)
V.S.Shirley, J.M.Dairiki
Nuclear Data Sheets for A = 192
COMPILATION 192Re, 192Os, 192Ir, 192Pt, 192Au, 192Hg, 192Tl, 192Pb, 192Bi, 192Po; compiled, evaluated structure data.
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
Hyperfine Interactions 15/16, 97 (1983)
Ch.Stenzel, H.Grawe, H.Haas, H.-E.Mahnke, K.H.Maier
Magnetic Moment of the 12+-Isomer in 192Pb
NUCLEAR REACTIONS 156Gd(40Ar, 4n), E=185 MeV; measured γ(θ, H, t). 192Pb deduced isomer T1/2, μ.
Hyperfine Interactions 13, 275 (1983)
A.E.Stuchbery, C.G.Ryan, H.H.Bolotin
Disparity between the Transient Hyperfine Fields for Pt and Os in Fe; an electron vacancy sharing interpretation
NUCLEAR REACTIONS 198Pt, 192Os(32S, 32S'), E=80 MeV; 198Pt, 192Os(58Ni, 58Ni'), E=220 MeV; measured Coulomb excitation, γ(θ), oriented nuclei; deduced anomalous transient field on Pt in Fe. 198Pt, 192Os level deduced g ratio.
Nucl.Instrum.Methods 219, 123 (1984)
Y.Iwata, M.Yasuhara, K.Maeda, Y.Yoshizawa
Precision Measurements of Gamma-Ray Intensities VI. 120Sb, 124Sb and 125Sb
RADIOACTIVITY 120Sb(EC) [from 120Sn(p, n)]; 124,125Sb(β-) [from neutron irradiation of Sb]; 152Eu(EC), (β+), (β-); 154Eu, 192Ir(EC), (β-); measured Eγ, Iγ, βγ-, (X-ray)γ-coin; deduced Iγ per decay. 192Os, 192Pt, 154,152Gd, 120Sn, 124,125Te levels deduced γ-branching.
doi: 10.1016/0167-5087(84)90143-1
Yad.Fiz. 40, 73 (1984)
V.Z.Maydikov
Delayed Autoionization of Recoil Atoms from Heavy-Ion Reactions
NUCLEAR REACTIONS 113Cd(40Ar, 6n), E=50 MeV; 138Ba(22Ne, 9n), (22Ne, 8n), (22Ne, 7n), E ≈ 18 MeV; 158Gd(40Ar, 6n), E ≈ 35 MeV; measured recoil residual ionization.
Nucl.Phys. A426, 144 (1984)
S.J.Mundy, J.Lukasiak, W.R.Phillips
The Spin(6) Scheme and Electromagnetic Transitions in 191Ir and 193Ir
NUCLEAR STRUCTURE 191,193Ir, 192,194,196,198Pt; calculated levels, B(λ). Interacting boson-fermion model, Spin(6) scheme.
NUCLEAR REACTIONS Ir, Pt(p, p'), (α, α'), E=5-6 MeV; measured σ(Eγ, θ), Eγ, Iγ, Coulomb excitation. 191,193Ir, 192,194,196,198Pt deduced levels, B(λ), δ. Natural targets.
doi: 10.1016/0375-9474(84)90070-8
Phys.Lett. 137B, 32 (1984)
W.Reuter, E.B.Shera, M.V.Hoehn, F.W.Hersman, T.Milliman, J.M.Finn, C.Hyde-Wright, R.Lourie, B.Pugh, W.Bertozzi
Nuclear Charge Densities in the Transition Region: 192Os
NUCLEAR REACTIONS 192Os(e, e), (e, e'), E=150, 250, 360 MeV; measured σ(E(e)). 192Os levels deduced transition densities, B(E2), rms radii, quadrupole moment. Muonic atom data input.
doi: 10.1016/0370-2693(84)91100-6
Phys.Rev. C30, 1465 (1984)
W.Reuter, E.B.Shera, M.V.Hoehn, F.W.Hersman, T.Milliman, J.M.Finn, C.Hyde-Wright, R.Lourie, B.Pugh, W.Bertozzi
Ground-State and Transition Charge Densities in 192Os
NUCLEAR STRUCTURE 192Os, 194Pt; calculated proton densities, rms radius, quadrupole moment. 186Os; calculated rms radius, quadrupole moment. Hartree-Fock theory, other model comparisons.
NUCLEAR REACTIONS 192Os(e, e), (e, e'), E=150, 250, 355, 364 MeV; measured σ(θ), σ(E(e)). 192Os levels deduced B(λ), transition radii, charge density. Hartree-Fock calculations.
Phys.Lett. 139B, 259 (1984)
A.E.Stuchbery, I.Morrison, H.H.Bolotin
Tests of Interacting Boson Model Wave Functions from Measured Gyromagnetic Ratios of States in the Even Os Isotopes
NUCLEAR REACTIONS 188,190,192Os(58Ni, 58Ni'), E=220 MeV; measured Coulomb excitation, γ(θ), oriented nuclei. 188,190,192Os levels deduced g.
doi: 10.1016/0370-2693(84)91075-X
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.
Diss.Abst.Int. 45B, p.243 (1984)
C.-Y.Wu
E2 Collective Behavior in the Even-Even Osmium and Platinum Nuclei
NUCLEAR REACTIONS 186,188,190,192Os, 194Pt(40Ca, 40Ca'), (58Ni, 58Ni'), (136Xe, 136Xe'), (208Pb, 208Pb'), E=3.3-4.8 MeV/nucleon; measured γ(particle)-, (particle)(particle)γ-coin, γ yields vs Z, θ following Coulomb excitation. 186,188,190,192Os, 194Pt deduced B(E2), E2 transition matrix elements, static quadrupole moments, band intersection effects.
ATOMKI Kozlem. 26, 49 (1984)
S.W.Yates, E.W.Kleppinger
Supersymmetric Multiplets in Transitional Nuclei from (n, n'γ) Reaction Studies
NUCLEAR REACTIONS 191,193Ir, 192Os, 194Pt(n, n'γ), E not given; measured γ-spectra, γ(θ), σ(γ, E). 191,193Ir, 192Os, 194Pt deduced levels, J, π, supersymmetry multiplets.
Z.Phys. A321, 65 (1985)
P.Aufmuth, E.Wobker
Isotope Shift in Osmium I: Experiment and theory
NUCLEAR MOMENTS 188,190,192Os; calculated isotope shift; deduced modified electronic densities. Photoelectric recording Fabry-Perot spectrometer.
Phys.Rev. C32, 2212 (1985)
F.T.Baker, A.Sethi, V.Penumetcha, G.T.Emery, W.P.Jones, M.A.Grimm, M.L.Whiten
g Bosons and the Third 4+ State in 192Os
NUCLEAR REACTIONS 192Os(polarized p, p'), E=135 MeV; measured σ(Ep'), σ(θ). 192Os deduced 4+ states, reduced matrix elements, intruder characteristics.
Program and Theses, Proc.35th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Leningrad, p.529 (1985)
V.N.Danilenko, S.V.Matveev, E.K.Stepanov
Relative Intensities of Gamma-Rays from the Decay of 110mAg, 133Ba, 192Ir
RADIOACTIVITY 110mAg(β-); 133Ba(EC); 192Ir(EC), (β-); measured precise Iγ, Eγ. Ge(Li) spectrometer.
Phys.Rev. C32, 582 (1985)
R.Eder, E.Hagn, E.Zech
Measurements of Spin, Magnetic Moment, and Electric Quadrupole Moment of 41.5 h 188Ir
RADIOACTIVITY 188Ir(EC), (β+); 188Pt(EC), (α); measured γ(θ), NMR oriented nuclei; deduced electric, magnetic hfs frequencies for 188Ir in Fe, Pt. 188Ir level deduced J, μ, electric quadrupole moment.
Z.Phys. A320, 495 (1985)
E.Eid, N.M.Stewart
Studies of the Low-Lying Levels in 192Pt and 192Os
RADIOACTIVITY 192Ir(β-), (EC) [from Ir thermal neutron irradiation]; measured Eγ, Iγ, γγ-coin; deduced log ft, EC-, β-branching ratios. 192Os, 192Pt deduced levels, ICC, γ-multipolarity, J, π, γ-branching, B(E2).
Hyperfine Interactions 22, 19 (1985)
E.Hagn
Nuclear Orientation and Quadrupole Interaction
Hyperfine Interactions 24, 69 (1985)
H.-J.Kluge
Optical Measurements of Ground-State Properties of Short-Lived Nuclei in Resonance Cells
NUCLEAR MOMENTS 197Au; measured hfs. Optical spectroscopy.
RADIOACTIVITY 192,190Au(EC), (β+); 191,193Au(EC); 185Hg(EC), (β+), (α); 185mHg(IT); measured hfs, isotope shift. 190,191,192,193,195,197Au, 181,183,184,202,203,204,205,206Hg; analyzed isotope shift, B(E2) data; deduced β2. 185,187,189,191,193,195,197,199Hg; analyzed data; deduced isomer odd-even staggering parameter. 181,183,185,187,189,191,193,195,197,199,201Hg; analyzed data; deduced quadrupole moments. Optical spectroscopy.
Z.Phys. A321, 563 (1985)
V.Z.Maydikov
Delayed Autoionization of Recoil Ions by the Decay of High-Spin Isomeric States
NUCLEAR REACTIONS 138Ba(22Ne, 7n), (22Ne, 8n), (22Ne, 9n), 158Gd(40Ar, 6n), E not given; measured residual ion recoil charge spectra; deduced delayed nuclear induced autoionization, high-spin isomer internal conversion decay connection.
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
Hyperfine Interactions 22, 355 (1985)
J.Rikovska, N.J.Stone, V.R.Green
Gamma-Ray Linear Polarization Measurement on Oriented Nuclei
RADIOACTIVITY 192Ir(EC), (β-); 60Co(β-); measured γ linear polarization, oriented nuclei in Fe. 192Pt transitions deduced δ.
Nucl.Instrum.Methods 241, 461 (1985)
J.Rikovska, N.J.Stone, V.R.Green
γ-Ray Linear Polarization Measurement on Oriented Nuclei
RADIOACTIVITY 192Ir(EC), (β-); 60Co(β-); measured γ-linear polarization, oriented nuclei. 192Os, 192Pt levels deduced δ. Coaxial Ge(Li) detector assembly Compton polarimeter, 3He/4He dilution refrigerator.
Nucl.Phys. A435, 635 (1985)
A.E.Stuchbery, I.Morrison, L.D.Wood, R.A.Bark, H.Yamada, H.H.Bolotin
Critical Assessment of Interacting Boson Model Wave Functions from Measured Gyromagnetic Ratios of Lowest Eigenstates in Even Os Isotopes
NUCLEAR STRUCTURE 188,190,192Os; calculated g, mass dependent g. Interacting boson models.
NUCLEAR REACTIONS 188,190,192Os(58Ni, 58Ni'), E=220 MeV; 188,190,192Os(32S, 32S'), E=95 MeV; measured γ(θ, H, T) and γ(θ, H) in polarized Fe, (particle)-γ-coin, Coulomb excitation. 188,190,192Os levels deduced g. Enriched, natural targets, thin-foil transient, static field IMPAC techniques.
doi: 10.1016/0375-9474(85)90481-6
Z.Phys. A321, 537 (1985)
J.Streib, H.-J.Kluge, H.Kremmling, R.B.Moore, H.W.Schaaf, K.Wallmeroth, and the ISOLDE Collaboration
Isotope Shifts of Neutron-Deficient Gold Isotopes with 193 ≥ A ≥ 190
RADIOACTIVITY 190,191,192,193Au [from Hg isotope decay]; measured isotope shifts relative to 197Au; deduced rms charge radii. Resonance fluorescence spectroscopy.
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
Priv.Comm. (1985)
C.-Y.Wu
NUCLEAR STRUCTURE 186,188,190,192Os, 194Pt; measured not abtracted; deduced B(E2).
At.Data Nucl.Data Tables 35, 15 (1986)
R.Bengtsson, S.Frauendorf, F.-R.May
Quasiparticle Levels in Rotating Rare Earth Nuclei: A cranked shell-model dictionary
NUCLEAR STRUCTURE 152,154,150,156Sm, 152,154,156,158,160Gd, 154,156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 160,162,164,166,168,170,172,174,176Yb, 162,164,166,168,170,172,174,176,178,180,182,184,186Hf, 166,168,170,172,174,176,178,180,182,184,186,188W, 170,172,174,176,178,180,182,184,186,188,190Os, 176,178,180,182,184,186,188,190Pt; calculated quasiparticle levels. Rare earth nuclei, cranked shell model dictionary.
doi: 10.1016/0092-640X(86)90028-8
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.
Nucl.Instrum.Methods Phys.Res. A249, 461 (1986); Erratum Nucl.Instrum.Methods Phys.Res. A345, 215 (1994)
E.Browne
Calculated Uncertainties of Absolute γ-Ray Intensities and Decay Branching Ratios Derived from Decay Schemes
RADIOACTIVITY 192Ir(EC), (β-); calculated absolute Iγ. Analytical methods.
doi: 10.1016/0168-9002(86)90703-5
Hyperfine Interactions 30, 355 (1986)
V.R.Green, N.J.Stone
The Low Temperature Quadrupole Orientation of 103Ru in Ruthenium
RADIOACTIVITY 103Ru(β-); measured γ(θ, T), oriented nuclei, low temperature; deduced quadrupole frequency, electric field gradient for Ru, Ir in Ru. 103Ru, 192Ir deduced quadrupole moments. Low temperature quadrupole orientation technique.
Nucl.Phys. A453, 316 (1986)
H.Hubel, A.P.Byrne, S.Ogaza, A.E.Stuchbery, G.D.Dracoulis, M.Guttormsen
High-Spin Structure of 190-194Hg and the Cranked Shell Model
NUCLEAR REACTIONS 170Er(24Mg, xn), (26Mg, xn), E=120-130 MeV. 184,186W(13C, xn), E=84-87 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 190,191,192,193,194Hg deduced levels, J, π, γ-branching. Enriched targets. Compton-suppressed Ge(high purity) detectors. Cranked shell model calculations.
doi: 10.1016/0375-9474(86)90014-X
Phys.Lett. 182B, 301 (1986)
T.Ichihara, H.Sakaguchi, M.Nakamura, M.Yosoi, M.Ieiri, Y.Takeuchi, H.Togawa, T.Tsutsumi, S.Kobayashi
Mass Number Dependence of Hexadecapole (Y42) Excitation of the γ-Vibrational Band in Proton Inelastic Scattering for 152 ≤ A ≤ 192
NUCLEAR REACTIONS 152,154Sm, 160Gd, 164Dy, 166,168Er, 176Yb, 182,184W, 192Os(polarized p, p'), E=65 MeV; measured σ(θ), analyzing power vs θ. 152,154Sm, 160Gd, 164Dy, 166,168Er, 176Yb, 182,184W, 192Os deduced quadrupole, hexadecapole moments, transition strengths vs mass.
doi: 10.1016/0370-2693(86)90095-X
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.
Nucl.Instrum.Methods Phys.Res. A245, 447 (1986); see 1986Me10
D.Mehta, M.L.Garg, J.Singh, N.Singh, T.S.Cheema, P.N.Trehan
Precision Measurements of X- and Gamma-Ray Intensities in 192Ir, 160Tb, 169Yb and 152Eu Decays
doi: 10.1016/0168-9002(86)91281-7
KVI 1985 Ann.Rept., p.32 (1986)
J.Penninga, A.Balanda, W.H.A.Hesselink, J.van Klinken, B.Kotlinski, B.Kotlinski, H.J.Riezebos, A.Stolk, H.Verheul, M.J.A.de Voigt
Search for Intruder States in 192Pb
NUCLEAR REACTIONS 156Gd(40Ar, 4n), 176Hf(20Ne, 4n), E not given; measured γγ-coin. 192Pb deduced transitions.
Z.Phys. A325, 247 (1986)
G.Ulm, S.K.Bhattacherjee, P.Dabkiewicz, G.Huber, H.-J.Kluge, T.Kuhl, H.Lochmann, E.-W.Otten, K.Wendt, S.A.Ahmad, W.Klempt, R.Neugart, and the ISOLDE Collaboration
Isotope Shift of 182Hg and an Update of Nuclear Moments and Charge Radii in the Isotope Range 181Hg - 206Hg
COMPILATION 185,185m,187,189,191Hg; compiled hyperfine interaction constants, μ. 181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199Hg; compiled hfs, isotope shifts.185m,187,187m,189,189m,191,191m,193,193m,195m,197m,199m,201,203Hg; compiled, evaluated rms radii, spectroscopic quadrupole moments.
RADIOACTIVITY 182,184,186,188,190,192,194Hg; measured isotopes shifts; deduced rms radii. Collinear fast beam laser spectroscopy.
NUCLEAR MOMENTS 196,198Hg; measured isotopes shifts; deduced rms radii. Collinear fast beam laser spectroscopy.
Nucl.Instrum.Methods Phys.Res. B26, 426 (1987)
C.R.Bingham, J.A.Bounds, H.K.Carter, R.L.Mlekodaj, J.C.Griffin, W.M.Fairbank, Jr.
Application of Collinear Laser Spectroscopy on Fast Atom Beams to Measure Nuclear Properties
RADIOACTIVITY 189,190,191,192,193,194,201Tl; measured hfs, isotope shifts. Laser spectroscopy system.
NUCLEAR MOMENTS 203,205Tl; measured hfs, isotope shifts. Laser spectroscopy system.
doi: 10.1016/0168-583X(87)90789-0
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
Phys.Rev. C36, 2560 (1987)
J.A.Bounds, C.R.Bingham, H.K.Carter, G.A.Leander, R.L.Mlekodaj, E.H.Spejewski, W.M.Fairbank, Jr.
Nuclear Structure of Light Thallium Isotopes as Deduced from Laser Spectroscopy on a Fast Atom Beam
RADIOACTIVITY 189m,190m,191m,192m,193,193m,194m,201Tl; measured hfs; deduced hfs constants. 190m,192m,193,194,194m,201,203Tl deduced μ, rms radii differences. 193m,191m,189mTl deduced quadrupole moment, deformation, μ, rms radii differences. Other data input, fast atom beam laser spectroscopy.
Phys.Rev. C36, 822 (1987)
J.A.Cizewski, D.G.Burke, R.E.Brown, J.W.Sunier
Ir(t(pol), α)Os Reaction and Implications for Tests of Supersymmetries
NUCLEAR REACTIONS 191,193Ir(polarized t, α), E=17 MeV; measured σ(θ), analyzing powers. 190,192Os levels deduced population mechanism, possible supersymmetry model inadequancies. Enriched targets. DWBA calculations.
Rev.Mod.Phys. 59, 1121 (1987)
E.R.Cohen, B.N.Taylor
The 1986 Adjustment of the Fundamental Physical Constants
doi: 10.1103/RevModPhys.59.1121
Z.Phys. A328, 253 (1987)
U.Dinger, J.Eberz, G.Huber, R.Menges, S.Schroder, R.Kirchner, O.Klepper, T.Kuhl, D.Marx, G.D.Sprouse
Nuclear Moments and Change in the Charge-Radii of Neutron Deficient Lead Isotopes
RADIOACTIVITY 192,194,195,196Pb [from W(16O, xn)]; measured hfs, isotope shifts; deduced hyperfine constants. 195Pb deduced μ, spectroscopic quadrupole moments, rms charge radius. 192,194,196Pb deduced rms charge radii. Collinear laser spectroscopy.
NUCLEAR MOMENTS Pb; measured isotope shifts, hfs. 204,206,207,208Pb deduced rms charge radii. Collinear laser spectroscopy.
Nucl.Phys. A470, 415 (1987)
G.J.Gyapong, R.H.Spear, M.P.Fewell, A.M.Baxter, S.M.Burnett
Experimental Determination of the Electric Quadrupole Moment of the First Excited State of 192Pt
NUCLEAR REACTIONS 192Pt(α, α'), E=14.4-15.2 MeV; 192Pt(12C, 12C'), E=41-48 MeV; 192Pt(16O, 16O'), E=55-60 MeV; measured Coulomb excitation probabilities of the first 2+ state. 192Pt levels deduced B(E2), quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(87)90011-X
Phys.Rev. C36, 1754 (1987)
T.Ichihara, H.Sakaguchi, M.Nakamura, M.Yosoi, M.Ieiri, Y.Takeuchi, H.Togawa, T.Tsutsumi, S.Kobayashi
Inelastic Proton Scattering Exciting the γ-Vibrational Band in Deformed Nuclei (152 ≤ A ≤ 192) at 65 MeV and the Systematics of the Hexadecapole (Y42) Strength of the γ Vibration
NUCLEAR REACTIONS 152,154Sm, 160Gd, 164Dy, 166,168Er, 176Yb, 182,184W, 192Os(polarized p, p), (polarized p, p'), E=65 MeV; measured σ(θ, E), A(θ, E); deduced optical model, deformation parameters. 152,154Sm, 160Gd, 164Dy, 166,168Er, 176Yb, 182,184W, 192Os deduced quadrupole, other moments, B(λ). Coupled-channel analysis, γ-vibrational model, asymmetric rotor model. Enriched target, high resolution spectrograph, polarized beams.
Z.Phys. A328, 31 (1987)
D.Mehta, S.Singh, M.L.Garg, N.Singh, T.S.Cheema, P.N.Trehan
Study of the Radioactive Decay of 192Ir
RADIOACTIVITY 192Ir(β-), (EC); measured Eγ, Iγ, γγ(θ), oriented nuclei. 192Os levels deduced γ-branching, relative Iγ, δ(E2/M1). 192Pt deduced level J, π, γ-branching, relative Iγ, δ(E2/M1).
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.
Nucl.Instrum.Methods Phys.Res. A255, 107 (1987)
A.Reggoug, M.Berrada
X-Ray Spectrometry Applied to 14 MeV Neutron Reaction Cross-Section Measurements on Iridium
NUCLEAR REACTIONS 193,191Ir(n, 2n), E ≈ 14.7 MeV; measured E(L X-ray), I(L X-ray), E(K X-ray), I(K X-ray). 190m,192mIr deduced production σ ratio.
doi: 10.1016/0168-9002(87)91084-9
Hyperfine Interactions 36, 117 (1987)
A.E.Stuchbery, H.H.Bolotin, C.E.Doran
Transient Fields for W Ions Traversing Fe Hosts and for Os Ions Traversing Fe and Ni Hosts
NUCLEAR REACTIONS 184,186W, 188,190,192Os, 197Au(63Cu, 63Cu'), E=220, 230 MeV; 184,186W, 188,190,192Os, 197Au(58Ni, 58Ni'), E=150, 220 MeV; measured γ(projectile)-coin, γ(projectile)(θ) in polarized hosts following Coulomb excitation; deduced transient fields for W ions in Fe, Os ions in Fe, Ni hosts.
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.
Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 37 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.1, 35 (1988)
M.K.Balodis, T.V.Guseva, J.Kern
Excited-State Structures of 192Ir and 194Ir
NUCLEAR REACTIONS 191,193Ir(n, γ), E=thermal; measured I(ce), Eγ, Iγ. 192,194Ir deduced levels, J, π.
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.
Nucl.Instrum.Methods Phys.Res. A265, 468 (1988)
J.B.Cumming, P.P.Parekh, A.V.Murali
A Novel Approach to the Determination of Iridium via Ge-Coincidence/NaI(Tl)-Anticoincidence Gamma-Ray Spectrometry
RADIOACTIVITY 192Ir(EC), (β-) [from 191Ir neutron irradiation]; measured γγ-coin. Ge-coincidence, NaI(Tl)-anticoincidence γ-ray spectroscopy.
doi: 10.1016/S0168-9002(98)90015-8
Nucl.Instrum.Methods Phys.Res. A269, 202 (1988)
M.P.Fewell
Hexadecapole Reorientation in Coulomb Excitation
NUCLEAR REACTIONS 192Os(120Sn, 120Sn'), E=300-495 MeV; 184W(58Ni, 58Ni'), E=100-300 MeV; 194Pt(208Pb, 208Pb'), E=0.2-1 GeV; calculated Coulomb excitation probability, hexadecapole moment dependence; deduced hexadecapole reorientation effects.
doi: 10.1016/0168-9002(88)90878-9
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
Mem.Fac.Sci., Kyoto Univ., Ser.Phys.Astrophys., Geophys.Chem. 37, 191 (1988)
T.Ichihara
Systematics of the Hexadecapole (Y42) Strength of the γ-vibration in Deformed Nuclei (152 ≤ A ≤ 192) from Inelastic Scattering of Polarized Protons at 65 MeV
NUCLEAR REACTIONS 152,154Sm, 160Gd, 164Dy, 166,168Er, 176Yb, 182,184W, 192Os(polarized p, p), (polarized p, p'), E=65 MeV; measured σ(θ). 152,154Sm, 160Gd, 164Dy, 166,168Er, 176Yb, 182,184W, 192Os deduced hexadecapole transition strength distribution. Coupled channels model.
Nucl.Instrum.Methods Phys.Res. B34, 252 (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, and the ISOCELE Collaboration
PILIS: Post-ISOCELE Laser Isobar Separation - An Apparatus for Laser Spectroscopic Studies of Laser-Desorbed Atoms
RADIOACTIVITY 192,187,186Au; measured hfs, isotope shift. 192Au deduced μ sign. Laser desorbed radiactive sources.
doi: 10.1016/0168-583X(88)90751-3
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.
Z.Phys. A329, 307 (1988)
Y.Liu, D.Hu, H.Sun, Z.Ding
Studies on the Low-Lying Levels in 192Pt and 192Os Populated in 192Ir Decay
RADIOACTIVITY 192Ir(EC), (β-); measured Eγ, Iγ, γγ-coin. 192Os, 192Pt deduced levels, γ-multipolarity, ICC, B(λ), J, π. Interacting boson model.
NUCLEAR STRUCTURE 192Os, 192Pt; calculated levels, B(E2). Interacting boson model.
Nucl.Phys. A485, 399 (1988)
C.S.Lim, R.H.Spear, W.J.Vermeer, M.P.Fewell, G.J.Gyapong
Electric Quadrupole Moments of the First Excited State of 192Os
NUCLEAR REACTIONS 192Os(α, α'), E=14.2-16.5 MeV; 192Os(12C, 12C'), E=40-55 MeV; 192Os(12C, 12C'), E=44-47 MeV; measured Coulomb excitation probabilities. 192Os levels deduced B(E2), static quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(88)90110-8
Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2216 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 135 (1988)
A.V.Murzin
Gamma Spectroscopy Based on Filtered Neutron Beams of an Atomic Reactor
NUCLEAR REACTIONS 179Hf, 191Ir, 143,145Nd, 50V(n, γ), E=reactor; measured γ-spectra, reduced intensities; deduced correlation coefficient.
Hyperfine Interactions 43, 493 (1988)
E.Scheidemann, R.Eder, E.Hagn, E.Zech
A Transmission γ-Ray Polarimeter for Sign Measurements of Magnetic Moments of Radioactive Nuclei
RADIOACTIVITY 60Co, 193Os, 191m,192,194Ir, 195mPt; measured γ(θ), γ CP, oriented nuclei; deduced μ sign. Transmission γ-ray polarimeter, low temperature nuclear orientation.
Nucl.Phys. A501, 546 (1989)
F.T.Baker, A.Sethi, V.Penumetcha, G.T.Emery, W.P.Jones, M.A.Grimm, M.L.Whiten
192Os(p(pol), p') Reaction at 135 MeV
NUCLEAR REACTIONS 192Os(polarized p, p'), E=134.5 MeV; measured σ(θ), analyzing power vs θ; deduced matrix elements for excitation of 4+ states. 192Os levels deduced deformation lengths. Enriched target. Coupled-channels analysis.
doi: 10.1016/0375-9474(89)90147-4
Phys.Rev. C40, 2527 (1989)
T.B.Clegg, G.Haouat, J.P.Delaroche, Ch.Lagrange, J.Chardine, M.T.McEllistrem, S.E.Hicks, G.R.Shen
Dynamics of Collective Excitations in 190,192Os and 194Pt Observed by 8 MeV Neutron Scattering
NUCLEAR REACTIONS 190,192Os, 194Pt(n, n), (n, n'), E=8 MeV; measured σ(θ); deduced model parameters. 190Os, 194Pt deduced deformation features.
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
Nucl.Instrum.Methods Phys.Res. A278, 484 (1989)
P.Durner, T.von Egidy, F.J.Hartmann
Neutron-Capture Gamma Rays below 40 keV
NUCLEAR REACTIONS 27Al, 39K, 51V, 127I, 133Cs, 159Tb, 165Ho, 169Tm, 175Lu, 181Ta, 191Ir, 197Au, 232Th(n, γ), E=low; meaured Eγ, absolute Iγ. 28Al, 40K, 52V, 128I, 134Cs, 160Tb, 166Ho, 170Tm, 176Lu, 182Ta, 192Ir, 198Au, 233Th deduced transitions. Si-Li detector.
doi: 10.1016/0168-9002(89)90869-3
Phys.Rev. C40, 2509 (1989)
S.E.Hicks, Z.Cao, M.C.Mirzaa, J.L.Weil, J.M.Hanly, J.Sa, M.T.McEllistrem
Nuclear Dynamics of 192Os as Probed in Neutron Scattering
NUCLEAR REACTIONS 192Os(n, n), (n, n'), E=0.25-4.2 MeV; measured σ(θ), σ(E); deduced model parameters. 192Os deduced deformation features. Coupled-channels analysis.
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
Hyperfine Interactions 50, 793 (1989)
M.Trhlik, B.Sedlak, S.Kapusta, P.Cizek, M.Finger, J.Konicek, E.Kisdi-Koszo, A.Lovas, M.Vobecky, J.Kovac
Nuclear Spin-Lattice Relaxation of 192Ir in Ferromagnetic Amorphous Alloy Fe-B Studied by Nuclear Orientation
RADIOACTIVITY 192Ir(EC), (β-); measured γ(θ, T), oriented nuclei; deduced spin-lattice relaxation in ferromagnetic amorphous alloy.
Phys.Rev. C41, R9 (1990)
J.A.Becker, N.Roy, E.A.Henry, M.A.Deleplanque, C.W.Beausang, R.M.Diamond, J.E.Draper, F.S.Stephens, J.A.Cizewski, M.J.Brinkman
Observation of Superdeformation in 192Hg
NUCLEAR REACTIONS 176Yb(22Ne, 6n), E=122 MeV; measured γγ-coin. 192Hg deduced levels, J, π, superdeformed band structure. HERA detector array.
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.Rev. C42, R1791 (1990)
J.E.Draper, F.S.Stephens, M.A.Deleplanque, W.Korten, R.M.Diamond, W.H.Kelly, F.Azaiez, A.O.Macchiavelli, C.W.Beausang, E.C.Rubel, J.A.Becker, N.Roy, E.A.Henry, M.J.Brinkman, A.Kuhnert, S.W.Yates
Spins in Superdeformed Bands in the Mass 190 Region
NUCLEAR STRUCTURE 192,194Hf, 233U; analyzed superdeformed band structure; deduced level J. Pseudospin formalism.
doi: 10.1103/PhysRevC.42.R1791
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.
Nucl.Phys. A520, 169c (1990)
T.L.Khoo, R.V.F.Janssens, E.F.Moore, K.B.Beard, Ph.Benet, I.Ahmad, M.P.Carpenter, R.R.Chasman, P.J.Daly, M.W.Drigert, U.Garg, Z.W.Grabowski, F.L.H.Wolfs, D.Ye
Population of Superdeformed Bands, the Competition with Fission, and the Barrier between Normal and Superdeformed States
NUCLEAR REACTIONS 160Gd(36S, 4n), E=154-172 MeV; 120Sn(36S, 4n), E=170 MeV; measured γγ-coin, γ-multiplicity. 152Dy, 192Hg deduced superdeformed band level entry, feeding spin features.
doi: 10.1016/0375-9474(90)91144-G
Phys.Rev.Lett. 64, 3127 (1990)
E.F.Moore, R.V.F.Janssens, I.Ahmad, M.P.Carpenter, P.B.Fernandez, T.L.Khoo, S.L.Ridley, F.L.H.Wolfs, D.Ye, K.B.Beard, U.Garg, M.W.Drigert, Ph.Benet, P.J.Daly, R.Wyss, W.Nazarewicz
Lifetime Measurements in the Superdeformed Band of 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin, DSA. 192Hg deduced levels, T1/2, B(E2), transition quadrupole moment, J, π, superdeformed band structure.
doi: 10.1103/PhysRevLett.64.3127
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
Phys.Rev.Lett. 64, 2623 (1990)
F.S.Stephens, M.A.Deleplanque, J.E.Draper, R.M.Diamond, C.W.Beausang, W.Korten, W.H.Kelly, F.Azaiez, J.A.Becker, E.A.Henry, N.Roy, M.J.Brinkman, J.A.Cizewski, S.W.Yates, A.Kuhnert
Spin Alignment in Superdeformed Hg Nuclei
RADIOACTIVITY 192,194Hg; analyzed spectra; deduced superdeformed band spin alignment.
doi: 10.1103/PhysRevLett.64.2623
Z.Phys. A335, 475 (1990)
W.H.Trzaska, J.Kantele, R.Julin, J.Kumpulainen, P.Van Duppen, M.Huyse, J.Wauters
Comparison of Experimental and Calculated K/L Ratios of E0 Transitions in Some Heavy Nuclei
RADIOACTIVITY 154Gd, 192,194,196,198,202,204,206,208Pb, 208Po; compiled measured, calculated I(ce) ratios; deduced no major differences.
Phys.Rev. C41, R13 (1990)
D.Ye, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, R.R.Chasman, I.Ahmad, K.B.Beard, Ph.Benet, M.W.Drigert, P.B.Fernandez, U.Garg, T.L.Khoo, S.L.Ridley, F.L.H.Wolfs
Superdeformed Band in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=162 MeV; measured γγ-coin. 192Hg deduced levels, J, π, superdeformed band structure.
Z.Phys. A338, 469 (1991)
E.A.Henry, A.Kuhnert, J.A.Becker, M.J.Brinkman, T.F.Wang, J.A.Cizewski, W.Korten, F.Azaiez, M.A.Deleplanque, R.M.Diamond, J.E.Draper, W.H.Kelly, A.O.Macchiavelli, F.S.Stephens
Observation of Superdeformed Band in 192Pb
NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=128, 132 MeV; measured γγ-coin. 192Pb deduced levels, J, π, superdeformed band dynamic moment of inertia.
Nucl.Phys. A534, 77 (1991)
J.Kern, A.Raemy, W.Beer, J.-Cl.Dousse, W.Schwitz, M.K.Balodis, P.T.Prokofjev, N.D.Kramer, L.I.Simonova, R.W.Hoff, D.G.Gardner, M.A.Gardner, R.F.Casten, R.L.Gill, R.Eder, T.von Egidy, E.Hagn, P.Hungerford, H.J.Scheerer, H.H.Schmidt, E.Zech, A.Chalupka, A.V.Murzin, V.A.Libman, I.V.Kononenko, C.Coceva, P.Giacobbe, I.A.Kondurov, Yu.E.Loginov, P.A.Sushkov, S.Brant, V.Paar
Nuclear Levels in 192Ir
NUCLEAR REACTIONS 191Ir(n, γ), E=thermal; measured Eγ, Iγ, I(ce), γγ-coin; 191Ir(n, γ), E=0.66, 5.4, 6.1 eV, 2, 24 keV; measured Eγ, Iγ; 191Ir(d, p), E=15, 22 MeV; measured E(p), σ; 193Ir(d, t), E=14, 15, 22 MeV; measured E(t), σ, Iγ(θ) from oriented nuclei in Fe. 192Ir deduced levels, J, π, ICC, γ-multipolarity. Nilsson configurations, comparison with interacting boson-fermion-fermion model calculations. Curved-crystal spectrometer, Ge detectors, magnetic spectrometer, Q3D spectrograph. Enriched targets.
doi: 10.1016/0375-9474(91)90559-O
Nucl.Phys. A530, 437 (1991)
J.M.Lagrange, M.Pautrat, J.S.Dionisio, Ch.Vieu, J.Vanhorenbeeck
High-Spin States in the 192Pb and 193Pb Isotopes
NUCLEAR REACTIONS 182W(16O, 5n), (16O, 6n), E=109 MeV; measured Eγ, Iγ, I(ce), γγ-, (ce)γ-coin, Iγ(θ). 192Pb, 193Pb deduced levels, J, π, T1/2, ICC. Enriched targets, intrinsic Ge detectors, magnetic spectrometer with Si(Li) detector.
doi: 10.1016/0375-9474(91)90812-K
Phys.Lett. 258B, 284 (1991)
E.F.Moore, R.V.F.Janssens, I.Ahmad, M.P.Carpenter, A.M.Baxter, M.E.Bleich, P.B.Fernandez, T.Lauritsen, T.L.Khoo, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, W.Reviol, D.Ye
K X-Ray Yields Associated with the Superdeformed Band of 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γ-, X-ray spectra, γ(X-ray)-coin, X-ray yields. 192Hg; deduced no strong superdeformed band E0 decay.
doi: 10.1016/0370-2693(91)91086-B
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, 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
Nucl.Instrum.Methods Phys.Res. A321, 506 (1992)
I.Alfter, E.Bodenstedt, B.Hamer, J.van den Hoff, W.Knichel, H.Munning, S.Piel, J.Schuth, R.Sajok
A Twelve Detector Coincidence Spectrometer for On-Line and Off-Line Measurements of Nuclear g-Factors
RADIOACTIVITY 192Ir(EC), (β-); measured γγ(θ, H) in Fe. 158Er(EC), (β+) [from 150Sm(12C, 4n)]; measured γγ(θ). 158Dy, 192Pt levels deduced g. Twelve detector coincidence spectrometer.
NUCLEAR REACTIONS 156Gd(α, 2n), E=27 MeV; measured γγ(θ, H) in-beam. 158Dy levels deduced integral rotations. Twelve detector coincidence spectrometer.
doi: 10.1016/0168-9002(92)90061-8
Z.Phys. A342, 249 (1992)
E.Bodenstedt, B.Hamer, P.Herzog, J.van den Hoff, H.Munning, S.Piel, J.Prinz, R.Sajok
Measurement of the g-Factor of the 2+1 State of 192Pt in an External Magnetic Field First Experiments with a New Twelve Detector IPAC Apparatus
RADIOACTIVITY 192Ir(β-), (EC) [from 191Ir(n, γ), E=thermal]; measured γγ(θ, H), γγ-coin; deduced 192Pt hyperfine field in Fe. 192Pt level deduced g-factor.
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
Phys.Lett. 279B, 239 (1992)
T.Lauritsen, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, I.Ahmad, P.B.Fernandez, T.L.Khoo, J.A.Kuehner, D.Prevost, J.C.Waddington, U.Garg, W.Reviol, D.Ye, M.W.Drigert
Dynamic Moment of Inertia of the 192Hg Superdeformed Band at High Rotational Frequencies
NUCLEAR REACTIONS 160Gd(36S, 4n), E=154-167 MeV; measured γγγ-coin. 192Hg deduced superdeformed states, relative Iγ, increasing dynamic moment of inertia.
doi: 10.1016/0370-2693(92)90386-I
Phys.Rev.Lett. 69, 2479 (1992)
T.Lauritsen, Ph.Benet, T.L.Khoo, K.B.Beard, I.Ahmad, M.P.Carpenter, P.J.Daly, M.W.Drigert, U.Garg, P.B.Fernandez, R.V.F.Janssens, E.F.Moore, F.L.H.Wolfs, D.Ye
Feeding of Superdeformed Bands: The mechanism and constraints on band energies and the well depth
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 192Hg deduced superdeformed band feeding, entry distribution features.
doi: 10.1103/PhysRevLett.69.2479
Phys.Rev. C46, R2136 (1992)
Y.Liang, M.P.Carpenter, R.V.F.Janssens, I.Ahmad, R.G.Henry, T.L.Khoo, T.Lauritsen, F.Soramel, S.Pilotte, J.M.Lewis, L.L.Riedinger, C.-H.Yu, U.Garg, W.Reviol, I.G.Bearden
Double Blocking in the Superdeformed 192Tl Nucleus
NUCLEAR REACTIONS 160Gd(37Cl, 5n), E=178, 181 MeV; measured Eγ, Iγ, γγ(θ). 192Tl deduced levels, J, π, superdeformed band features, moments of inertia. Cranked shell model.
doi: 10.1103/PhysRevC.46.R2136
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.
J.Phys.(London) G18, 1401 (1992)
J.Sinatkas, L.D.Skouras, D.Strottman, J.D.Vergados
Shell-Model Calculations in the A = 80-100 Mass Region: II. A study of the N = 49, 48 nuclei
NUCLEAR STRUCTURE 91Mo, 89Zr, 93Ru, 87Sr, 90Nb, 88Y, 92Ru, 90Mo, 88Zr, 86Sr, 91Tc, 89Nb; calculated levels, B(λ). 87Y; caluclated levels. Shell model.
doi: 10.1088/0954-3899/18/8/013
Pramana 39, 571 (1992)
K.Singh, K.S.Dhillon
Sum Peak Method Applied to the Study of Decay of Ir-192
RADIOACTIVITY 192Ir(β-), (EC); measured Eγ, Iγ, (K X-ray)γ-sum peaks, I (X-ray); deduced K-shell flourescence yields for Os, Pt. 192Os, 192Pt levels deduced absolute K-conversion ICC, relative K-capture probabilities.
Z.Phys. A342, 373 (1992)
A.E.Stuchbery, S.S.Anderssen, H.H.Bolotin, A.P.Byrne, G.D.Dracoulis, B.Fabricius, T.Kibedi
Transient Field Measurements of First-Excited State g-Factors in 188,190,192Os
NUCLEAR REACTIONS 188,190,192Os(58Ni, 58Ni'), E=150 MeV; measured γ(58Ni)-coin, (particle)γ(θ), transient field prcessions. 188,190,192Os levels deduced g-factors. Nuclei traversing thin polarized Fe foil.
Z.Phys. A342, 277 (1992)
J.Wauters, P.Dendooven, P.Decrock, M.Huyse, R.Kirchner, O.Klepper, G.Reusen, E.Roeckl, P.Van Duppen
The Alpha-Branching Ratios of the 188,190,192Pb Isotopes
RADIOACTIVITY 190,192Pb(α) [from 181Ta(20Ne, xnp), E < 240 MeV]; 188Pb(α) [from 155Gd(40Ar, 7n), E=240 MeV]; measured Eα, Iα, Eγ, Iγ, E X-ray, I X-ray; deduced α-branching ratios.
Nucl.Instrum.Methods Phys.Res. A312, 346 (1992)
M.J.Woods, S.E.M.Lucas, D.F.G.Reher, G.Sibbens
The Half-Life of 192Ir
RADIOACTIVITY 192Ir(EC), (β-); measured T1/2; deduced recommended T1/2. High pressure re-entrant ionization chambers.
doi: 10.1016/0168-9002(92)90179-8
Nucl.Phys. A557, 57c (1993)
M.P.Carpenter, R.V.F.Janssens, Y.Liang, I.G.Bearden, I.Ahmad, M.W.Drigert, U.Garg, R.G.Henry, J.M.Lewis, T.L.Khoo, T.Lauritsen, S.Pilotte, W.Reviol, L.L.Riedinger, F.Soramel, C.-H.Yu
New Results on Superdeformed Bands in Hg and Tl Nuclei
NUCLEAR REACTIONS 159Tb(36S, 4n), E=165 MeV; 160Gd(37Cl, 5n), E=178, 181 MeV; analyzed data. 191,192Tl, 190Hg deduced levels, J, π, superdeformed bands. Other data input.
doi: 10.1016/0375-9474(93)90530-B
Nucl.Phys. A557, 615c (1993)
D.Cline
Quadrupole and Octupole Shapes in Nuclei
NUCLEAR STRUCTURE 184W, 186,188,190,192Os, 148,150Nd, 226Ra; compiled, reviewed Coulomb excitation data; deduced deformation related features extraction possibility.
doi: 10.1016/0375-9474(93)90574-H
J.Phys.(London) G19, L177 (1993)
A.Dewald, R.Kruecken, P.Sala, J.Altmann, O.Stuch, P.von Brentano, D.Bazzacco, C.Rossi-Alvarez, G.de Angelis, J.Rico, G.Vedovato, G.lo Bianco
RDDS Coincidence Lifetime Measurement for Two Superdeformed States in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=168 MeV; measured Eγ, γγ-coin. 192Hg deduced superdeformed states T1/2, B(λ), transition quadrupole moments. Recoil distance Doppler shift coincidence plunger, differential decay curve method, Ge detectors, anti-Compton shields, BGO ball, enriched target.
doi: 10.1088/0954-3899/19/11/005
Nucl.Phys. A557, 75c (1993)
F.Hannachi, C.Schuck, G.Bastin, I.Deloncle, B.Gall, M.G.Porquet, A.G.Smith, F.Azaiez, C.Bourgeois, J.Duprat, A.Korichi, N.Perrin, N.Poffe, H.Sergolle, A.Astier, Y.Le Coz, M.Meyer, N.Redon, M.Bentley, J.Simpson, J.F.Sharpey-Schafer, M.J.Joyce, C.W.Beausang, P.Fallon, E.S.Paul, P.J.Dagnall, S.A.Forbes, S.Gale, P.M.Jones, R.Wadsworth, R.M.Clark, M.M.Aleonard, D.Curien, G.De France, M.Carpenter, R.Henry, T.Lauritsen, P.Willsau
Study of the Superdeformed Band in 194Pb and 192Hg with EUROGAM
NUCLEAR REACTIONS 162Dy(36S, 4n), E=162 MeV; measured Eγ, Iγ, γγ-coin, DSA. 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 194Pb deduced decay out of superdeformed band.
doi: 10.1016/0375-9474(93)90532-3
Nucl.Phys. A557, 635c (1993)
M.Oshima, T.Morikawa, H.Kusakari, N.Kobayashi, M.Sugawara, Y.H.Zhang, A.Ferragut, S.Ichikawa, N.Shinohara, Y.Nagame, M.Shibata, Y.Gono, T.Inamura
Double-γ Vibrational States in 168Er and 192Os
NUCLEAR REACTIONS 168Er(74Ge, 74Ge'), E=295 MeV; 192Os(58Ni, 58Ni'), E=240 MeV; measured γ(particle)-coin following Coulomb excitation. 168Er, 192Os deduced levels, J, π, B(λ), ratios.
doi: 10.1016/0375-9474(93)90575-I
Phys.Rev. C47, 2378 (1993)
A.J.M.Plompen, M.N.Harakeh, W.H.A.Hesselink, G.van't Hof, N.Kalantar-Nayestanaki, J.P.S.van Schagen, R.V.F.Janssens, I.Ahmad, I.G.Bearden, M.P.Carpenter, T.L.Khoo, T.Lauritsen, Y.Liang, U.Garg, W.Reviol, D.Ye
Lack of Evidence for a Superdeformed Band in 192Pb
NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=132 MeV; measured γγ-coin, DSA. 192Pb deduced no superdeformed band.
Nucl.Phys. A562, 61 (1993)
A.J.M.Plompen, M.N.Harakeh, W.H.A.Hesselink, G.van't Hof, N.Kalantar-Nayestanaki, J.P.S.van Schagen, M.P.Carpenter, I.Ahmad, I.G.Bearden, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, Y.Liang, U.Garg, W.Reviol, D.Ye
Collective and Quasiparticle Structure in 192Pb
NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=132 MeV; measured Eγ, Iγ, γγ(θ), γγ(t), γγ-coin. 192Pb deduced levels, J, π. Enriched target, Compton-suppressed Ge-detectors, central array of BGO detectors. Cranked shell model calculations.
doi: 10.1016/0375-9474(93)90032-S
Nucl.Phys. A562, 88 (1993)
A.J.M.Plompen, J.Blomqvist, M.P.Carpenter, M.N.Harakeh, W.H.A.Hesselink, R.V.F.Janssens, R.J.Liotta, N.Sandalescu
Non-Collective Degrees of Freedom in 192Pb
NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=132 MeV; measured Iγ(θ), DCO. 192Pb deduced levels, J, π, configuration. Quasiparticle multi-step shell model.
doi: 10.1016/0375-9474(93)90033-T
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.
Z.Phys. A349, 5 (1994)
J.Duprat, B.J.P.Gall, M.G.Porquet, F.Hannachi, F.Azaiez, M.Aiche, G.Bastin, C.W.Beausang, R.Beraud, C.Bourgeois, R.M.Clark, I.Deloncle, R.Duffait, K.Hauschild, H.Hubel, M.J.Joyce, M.Kaci, A.Korichi, Y.Le Coz, M.Meyer, E.S.Paul, N.Perrin, N.Poffe, N.Redon, C.Schuck, H.Sergolle, J.F.Sharpey-Schafer, J.Simpson, A.G.Smith, R.Wadsworth
First Observation of a Superdeformed Nucleus Produced in an αxn Reaction Channel
NUCLEAR REACTIONS 184W(16O, 4nα), E=113 MeV; measured γγ-coin. 192Hg deduced superdeformed high-spin band feeding, decay-out patterns.
Nucl.Phys. A568, 445 (1994)
P.E.Garrett, D.G.Burke
Nuclear Structure of 192Ir Studied with Direct Transfer Reactions
NUCLEAR REACTIONS 191Ir(d, p), E=16 MeV; measured σ(θ, Ep); 193Ir(d, t), E=18 MeV; measured σ(θ, Et); 193Ir(3He, α), E=25.5 MeV; measured σ(Eα); 195Pt(p, α), E=18 MeV; measured σ(Eα). 192Ir deduced levels, J, π, L, spectroscopic strengths. Comparison with interacting boson-fermion-fermion model, Nilsson predictions. Enriched targets, magnetic spectrograph.
doi: 10.1016/0375-9474(94)90390-5
Z.Phys. A347, 223 (1994)
B.J.P.Gall, M.G.Porquet, F.Hannachi, A.Korichi, I.Ahmad, M.Aiche, F.Azaiez, G.Bastin, C.W.Beausang, R.Beraud, C.Bourgeois, M.P.Carpenter, R.M.Clark, I.Deloncle, R.Duffait, J.Duprat, K.Hauschild, R.Henry, R.V.F.Janssens, M.J.Joyce, T.L.Khoo, M.Kaci, T.Lauritsen, Y.Le Coz, M.Meyer, E.S.Paul, N.Perrin, N.Poffe, N.Redon, C.Schuck, H.Sergolle, J.F.Sharpey-Schafer, J.Simpson, A.G.Smith, R.Wadsworth, P.Willsau
New Results on the Superdeformed Band in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 192Hg deduced superdeformed band dynamical moment of inertia features. Cranked HFB model comparison.
Phys.Rev. C49, 2849 (1994)
E.A.Henry, A.Kuhnert, J.A.Becker, M.J.Brinkman, T.F.Wang, J.A.Cizewski, W.Korten, F.Azaiez, M.A.Deleplanque, R.M.Diamond, J.E.Draper, W.H.Kelly, A.O.Macchiavelli, F.S.Stephens
Comment on ' Lack of Evidence for a Superdeformed Band in 192Pb '
NUCLEAR REACTIONS 148Sm(48Ca, 4n), E=205 MeV; 173Yb(24Mg, 5n), E=128, 132 MeV; measured Eγ, Iγ. 192Pb deduced superdeformed band.
Phys.Rev.Lett. 73, 777 (1994)
R.G.Henry, T.Lauritsen, T.L.Khoo, I.Ahmad, M.P.Carpenter, B.Crowell, T.Dossing, R.V.F.Janssens, F.Hannachi, A.Korichi, C.Schuck, F.Azaiez, C.W.Beausang, R.Beraud, C.Bourgeois, R.M.Clark, I.Deloncle, J.Duprat, B.Gall, H.Hubel, M.J.Joyce, M.Kaci, Y.Lecoz, M.Meyer, E.S.Paul, N.Perrin, N.Poffe, M.G.Porquet, N.Redon, H.Sergolle, J.F.Sharpey-Schafer, J.Simpson, A.G.Smith, R.Wadsworth, P.Willsau
Spectrum of γ Rays Connecting Superdeformed and Normal States in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 192Hg deduced superdeformed to normal high-spin states transition, band coupling features.
doi: 10.1103/PhysRevLett.73.777
Z.Phys. A348, 87 (1994)
Y.Le Coz, N.Redon, A.Astier, R.Beraud, R.Duffait, M.Meyer, F.Hannachi, G.Bastin, I.Deloncle, B.Gall, M.Kaci, M.G.Porquet, C.Schuck, F.Azaiez, C.Bourgeois, J.Duprat, A.Korichi, N.Perrin, N.Poffe, H.Sergolle, J.F.Sharpey-Schafer, C.W.Beausang, S.J.Gale, M.J.Joyce, E.S.Paul, R.M.Clark, K.Hauschild, R.Wadsworth, J.Simpson, M.A.Bentley, A.G.Smith, H.Hubel, P.Willsau, G.De France, I.Ahmad, M.Carpenter, R.Henry, R.V.F.Janssens, T.L.Khoo, T.Lauritsen
Two Proton High-Spin Excitations and Dipole Bands in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γ yields, γγ-coin. 192Hg deduced high-spin levels, J, π, band structure, configuration, B(λ) ratios. Mean field Hartree-Fock+BCS model.
Phys.Rev. C50, 2602 (1994)
I.Y.Lee, C.Baktash, D.M.Cullen, J.D.Garrett, N.R.Johnson, F.K.McGowan, D.F.Winchell, C.H.Yu
Lifetimes of Low-Spin States in the Superdeformed Band of 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 192Hg deduced superdeformed high-spin states T1/2. Recoil distance method.
Nucl.Instrum.Methods Phys.Res. A339, 203 (1994)
H.Miyahara, H.Matumoto, C.Mori, N.Takeuchi, T.Genka
Determination of Gamma-Ray Emission Probabilities for 75Se, 166mHo and 192Ir by a Self-Consistent Method
RADIOACTIVITY 75Se(EC); 166mHo(β-); 75As, 166Er, 192Pt levels deduced emission probabilities.
doi: 10.1016/0168-9002(94)91805-8
Nucl.Phys. A580, 173 (1994)
G.Passler, J.Rikovska, E.Arnold, H.-J.Kluge, L.Monz, R.Neugart, H.Ravn, K.Wendt, and the ISOLDE Collaboration
Quadrupole Moments and Nuclear Shapes of Neutron-Deficient Gold Isotopes
RADIOACTIVITY 193,191Au(EC); 192,194Au(EC), (β+); measured istope shifts, hfs; deduced quadrupole moment, deformation parameter β2, hyperfine constants. Particle-triaxial-rotor model applied to 183-197Au.
doi: 10.1016/0375-9474(94)90769-2
Phys.Rev. C49, 2851 (1994)
A.J.M.Plompen, M.N.Harakeh, W.H.A.Hesselink, G.van't Hof, N.Kalantar-Nayestanaki, J.P.S.van Schagen, R.V.F.Janssens, I.Ahmad, I.G.Bearden, M.P.Carpenter, T.L.Khoo, T.Lauritsen, Y.Liang, U.Garg, W.Reviol, D.Ye
Reply to ' Comment on ' Lack of Evidence for a Superdeformed Band in 192Pb ' '
NUCLEAR STRUCTURE 192Pb; analyzed, reviewed existing data; deduced need for more definitive experiments to determine superdeformed band evidence.
Phys.Rev.Lett. 72, 1329 (1994)
J.Wauters, N.Bijnens, P.Dendooven, M.Huyse, H.Y.Hwang, G.Reusen, J.von Schwarzenberg, P.Van Duppen, R.Kirchner, E.Roeckl, and the ISOLDE Collaboration
Fine Structure in the Alpha Decay of Even-Even Nuclei as an Experimental Proof for the Stability of the Z = 82 Magic Shell at the Very Neutron-Deficient Side
RADIOACTIVITY 202Rn, 194,196,198Po, 186,188Pb, 180,182,184Hg(α); calculated α-decay T1/2, hindrance factors; deduced shell closure role, 0+ level configuration in daughter nuclei.
doi: 10.1103/PhysRevLett.72.1329
Nucl.Phys. A574, 560 (1994)
P.Willsau, A.Korichi, F.Hannachi, H.Hubel, W.Korten, M.Neffgen, F.Azaiez, C.Bourgeois, J.Duprat, N.Perrin, N.Poffe, H.Sergolle, G.Bastin, I.Deloncle, B.Gall, M.Kaci, M.G.Porquet, C.Schuck, J.Simpson, R.Duffait, Y.Le Coz, M.Meyer, N.Redon, G.De France, A.G.Smith, C.W.Beausang, M.J.Joyce, E.S.Paul, J.F.Sharpey-Schafer, R.M.Clark, R.Wadsworth, I.Ahmad, M.P.Carpenter, R.G.Henry, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, J.H.Hughes, H.J.Maier
Lifetimes of the Superdeformed Band in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin, Doppler shifts. 192Hg deduced T1/2 of high-spin superdeformed states, transition quadrupole moments. EUROGAM Ge detector spectrometer array.
doi: 10.1016/0375-9474(94)90244-5
Nucl.Phys. A593, 212 (1995)
S.S.Anderssen, A.E.Stuchbery, S.Kuyucak
Measured Magnetic Moments of 2+1 States in 190-198Pt and Interacting Boson Model Description of M1 Systematics in the Platinum Isotopes
NUCLEAR REACTIONS 190,192,194,196,198Pt(58Ni, 58Ni'), E=160 MeV; measured γ(θ, H, T) in thin polarized Gd, (particle)γ-coin, Coulomb excitation. 190,192,194,196,198Pt levels deduced g-factors. 190Pt levels deduced B(E2;0+1 → 2+1). Enriched target, thin-foil transient-field IMPAC technique.
NUCLEAR STRUCTURE 190,192,194,196,198Pt; calculated levels, B(E2), B(M1), δ, g. Proton-neutron interacting boson model (IBM-2), F-spin symmetry breaking.
doi: 10.1016/0375-9474(95)00350-A
Z.Phys. A352, 239 (1995)
S.J.Asztalos, P.Fallon, R.M.Clark, J.A.Becker, L.A.Bernstein, B.Cederwall, M.A.Deleplanque, R.M.Diamond, L.P.Farris, E.A.Henry, W.H.Kelly, I.Y.Lee, A.O.Macchiavelli, F.S.Stephens
Confirmation of the Superdeformed Band in 192Pb
NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=140 MeV; measured γγγ-coin. 192Pb deduced high-spin levels, J, π, superdeformed band dynamic moment of inertia.
Phys.Rev.Lett. 74, 3939 (1995)
D.S.Delion, A.Florescu, M.Huyse, J.Wauters, P.Van Duppen, A.Insolia, R.J.Liotta, and the ISOLDE Collaboration
Microscopic Description of Alpha Decay to Intruder 0+2 States in Pb, Po, Hg, and Pt Isotopes
RADIOACTIVITY 194,196,198Po(α); 200,202Rn(α); 188,186Pb; 180,182,184Hg; calculated hindrance factors. Quasiparticle RPA.
doi: 10.1103/PhysRevLett.74.3939
Nucl.Instrum.Methods Phys.Res. A357, 150 (1995)
I.Deloncle, M.-G.Porquet, M.Dziri-Marce
New Approach in the Off-Line Treatment of High-Fold Data
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; 184W(16O, 6n), (16O, 7n), (16O, 4nα), E=113 MeV; measured individual multi-gated γ-spectra, γγ-coin, excited, yrast superdeformed bands associated relative Iγ.
doi: 10.1016/0168-9002(94)01733-6
Z.Phys. A352, 13 (1995)
L.Ducroux, A.Astier, R.Beraud, R.Duffait, Y.Le Coz, M.Meyer, S.Perries, N.Redon, J.F.Sharpey-Schafer, A.N.Wilson, R.Collatz, I.Deloncle, F.Hannachi, M.Kaci, A.Lopez-Martens, M.G.Porquet, C.Schuck, F.Azaiez, S.Bouneau, C.Bourgeois, J.Duprat, A.Korichi, N.Perrin, N.Poffe, H.Sergolle, D.Goutte, R.Lucas, V.Meot, I.Hibbert, R.Wadsworth, F.Beck, D.Curien, G.De France, G.Duchene, B.Gall, B.Haas, J.P.Vivien
Configuration of the Existence of a Superdeformed Rotational Band in 192Pb
NUCLEAR REACTIONS 168Er(30Si, 6n), E=159 MeV; measured γγ-coin. 192Pb deduced superdeformed band.
Phys.Rev. C51, R1609 (1995)
P.Fallon, T.Lauritsen, I.Ahmad, M.P.Carpenter, B.Cederwall, R.M.Clark, B.Crowell, M.A.Deleplanque, R.M.Diamond, B.Gall, F.Hannachi, R.G.Henry, R.V.F.Janssens, T.L.Khoo, A.Korichi, I.Y.Lee, A.O.Macchiavelli, C.Schuck, F.S.Stephens
Quasiparticle Excitations in Superdeformed 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-, γγγ-coin. 192Hg deduced high-spin levels, J, π, superdeformed bands, dynamic moment of inertia.
doi: 10.1103/PhysRevC.51.R1609
Phys.Lett. 345B, 403 (1995)
A.Korichi, F.Hannachi, I.Deloncle, W.Korten, I.Ahmad, F.Azaiez, G.Bastin, C.W.Beausang, C.Bourgeois, M.P.Carpenter, R.M.Clark, R.Duffait, J.Duprat, B.J.P.Gall, R.G.Henry, H.Hubel, R.V.F.Janssens, M.Joyce, M.Kaci, T.L.Khoo, T.Lauritsen, Y.Le Coz, M.Meyer, E.S.Paul, N.Perrin, N.Poffe, M.G.Porquet, N.Redon, C.Schuck, H.Sergolle, J.F.Sharpey-Schafer, J.Simpson, A.G.Smith, R.Wadsworth, P.Willsau
Observation and Lifetime of the First Excited Superdeformed Band in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγγ-coin, DSA. 192Hg deduced high-spin levels, J, π, superdeformed band two-quasineutron excitation, T1/2, deformation features, B(λ), transition quadrupole moments.
doi: 10.1016/0370-2693(94)01608-F
Phys.Scr. T56, 234 (1995)
Y.Le Coz, A.Astier, R.Beraud, R.Duffait, M.Meyer, N.Redon, G.Bastin, I.Deloncle, B.Gall, F.Hannachi, M.Kaci, M.G.Porquet, C.Schuck, F.Azaiez, C.Bourgeois, J.Duprat, A.Korichi, N.Perrin, N.Poffe, H.Sergolle, C.W.Beausang, S.J.Gale, M.J.Joyce, E.S.Paul, J.F.Sharpey-Schafer, R.M.Clark, K.Hauschild, R.Wadsworth, J.Simpson, M.A.Bentley, G.Smith, H.Hubel, P.Willsau, G.De France, I.Ahmad, M.Carpenter, R.Henry, R.V.F.Janssens, T.L.Khoo, T.Lauritsen
Two Proton High Spin Excitations and Dipole Bands in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin. 192Hg deduced high-spin levels, J, π, band structure, configuration. Mean-field HF plus BCS formalism calculations.
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.
At.Data Nucl.Data Tables 61, 43 (1995)
V.I.Tretyak, Yu.G.Zdesenko
Tables of Double Beta Decay Data
RADIOACTIVITY A=36-238; compiled, reviewed 2β decay T1/2 data.
doi: 10.1016/S0092-640X(95)90011-X
Z.Phys. A356, 3 (1996)
N.Bijnens, I.Ahmad, A.N.Andreyev, J.C.Batchelder, C.R.Bingham, D.Blumenthal, B.C.Busse, X.S.Chen, L.F.Conticchio, C.N.Davids, M.Huyse, R.V.F.Janssens, P.Mantica, H.Penttila, W.Reviol, D.Seweryniak, P.Van Duppen, W.B.Walters, J.Wauters, B.E.Zimmerman
Fine Structure in the α Decay of 192Po
RADIOACTIVITY 192Po(α) [from 160Dy(36Ar, X), E=175.6 MeV]; measured α-spectra; deduced T1/2, fine structure, α-branching ratio. 188Pb deduced level, J, π.
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. C53, 2126 (1996)
S.M.Fischer, M.P.Carpenter, R.V.F.Janssens, B.Crowell, I.Ahmad, D.J.Blumenthal, T.L.Khoo, T.Lauritsen, D.Nisius, W.Reviol, W.F.Mueller, L.L.Riedinger, B.H.Smith, B.Cederwall
Alignment Additivity in the Two-Quasiparticle Superdeformed Bands of 192Tl
NUCLEAR REACTIONS 160Gd(37Cl, 5n), E=178 MeV; measured Eγ, γγγ-coin, Iγ. 192Tl deduced levels, J, π, superdeformed bands, configurations, quasiparticle alignments.
Hyperfine Interactions 97/98, 409 (1996)
E.Hagn
Recent Developments and New Trends in NMR on Oriented Nuclei
NUCLEAR MOMENTS 169,171,172,173,174,177,177mLu; compiled, reviewed hfs, μ, quadrupole moments, quadrupole interaction in Co. 184,186,186m,188,186,191,193,195,197,198,199Au, 185,187,189Pt, 189,191,192,193Ir; compiled reviewed quadrupole moments, ratio. 90,95,96Nb, 90m,95Zr, 111In, 193m,195m,197mAu, 197mHg; compiled, reviewed quadrupole interaction changes. 90Nb, 90mZr; compiled, reviewed NMR data, oriented nuclei.
Phys.Rev. C54, R2799 (1996)
K.Helariutta, T.Enqvist, P.Jones, R.Julin, S.Juutinen, P.Jamsen, H.Kankaanpaa, P.Kuusiniemi, M.Leino, M.Muikku, M.Piiparinen, A.Savelius, W.H.Trzaska, S.Tormanen, J.Uusitalo, R.G.Allatt, P.A.Butler, P.T.Greenlees, R.D.Page
First Observation of Excited States in 192Po
NUCLEAR REACTIONS 160Dy(36Ar, 4n), E=178 MeV; measured Eα, Iα, Eγ, Iγ, (recoil)γ-coin. 192Po deduced levels, possible J, π, band structure.
doi: 10.1103/PhysRevC.54.R2799
Phys.Rev.Lett. 77, 1707 (1996)
A.Lopez-Martens, F.Hannachi, T.Dossing, C.Schuck, R.Collatz, E.Gueorguieva, Ch.Vieu, S.Leoni, B.Herskind, T.L.Khoo, T.Lauritsen, I.Ahmad, D.J.Blumenthal, M.P.Carpenter, D.Gassmann, R.V.F.Janssens, D.Nisius, A.Korichi, C.Bourgeois, A.Astier, L.Ducroux, Y.Le Coz, M.Meyer, N.Redon, J.F.Sharpey-Schafer, A.N.Wilson, W.Korten, A.Bracco, R.Lucas
Fragmentation of the Decay from the Superdeformed Yrast Band in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=195 MeV; measured γγ-coin. 192Hg deduced superdeformed yrast band decay characteristics.
doi: 10.1103/PhysRevLett.77.1707
Proc.Workshop Gammasphere Physics, Berkeley, California, 1-2 December 1995, World Scientific, Singapore, p.98 (1996)
L.L.Riedinger, W.Reviol, J.M.Lewis, W.F.Mueller, B.H.Smith, J.-Y.Zhang, S.M.Fischer, M.P.Carpenter, R.V.F.Janssens, B.Crowell, I.Ahmad, D.J.Blumenthal, T.L.Khoo, T.Lauritsen, D.Nisius, B.Cederwall
The Multiplicity of Shapes in Tl Nuclei
NUCLEAR REACTIONS 156Gd(37Cl, 4n), E not given; measured Eγ, Iγ, γγ-coin. 189Tl deduced levels, J, π, configurations. Gammasphere array.
NUCLEAR STRUCTURE 192Tl; analyzed data; deduced levels, J, π, superdeformed bands. 189,191,193Tl analyzed superdeformed bands moments of inertia. 189,191,193,195Tl; calculated deformation parameters.
Phys.Rev.Lett. 77, 5016 (1996)
G.Seewald, E.Hagn, B.Hinfurtner, E.Zech, D.Forkel-Wirth, R.Eder, and the ISOLDE Collaboration
Measurements of Spectroscopic Quadrupole Moments of Neutron Deficient Ir Isotopes and Shape Coexistence in 186Ir
RADIOACTIVITY 184Ir(EC), (β+); 186,186mIr(EC), (β+); 187Ir(EC); 188Ir(EC), (β+); 189Ir(EC); measured quadrupole-interaction resolved NMR, oriented nuclei; deduced spectroscopic quadrupole moments, ratios.
doi: 10.1103/PhysRevLett.77.5016
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.
Z.Phys. A355, 129 (1996)
P.Willsau, M.Neffgen, Y.Le Coz, H.Hubel, W.Korten, F.Hannachi, A.Korichi, M.G.Porquet, M.Kaci, N.Redon, M.Meyer, C.W.Beausang, E.S.Paul, J.Simpson, J.R.Hughes
Lifetimes of a Dipole Cascade in 192Hg
NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γγ-coin, Doppler shift recoil distance. 192Hg deduced high-spin levels, J, π, B(λ), T1/2.
Nucl.Phys. A607, 178 (1996)
C.Y.Wu, D.Cline, T.Czosnyka, A.Backlin, C.Baktash, R.M.Diamond, G.D.Dracoulis, L.Hasselgren, H.Kluge, B.Kotlinski, J.R.Leigh, J.O.Newton, W.R.Phillips, S.H.Sie, J.Srebrny, F.S.Stephens
Quadrupole Collectivity and Shapes of Os-Pt Nuclei
NUCLEAR REACTIONS 186,188,190,192Os, 194Pt(40Ca, 40Ca'), (58Ni, 58Ni'), (136Xe, 136Xe'), (208Pb, 208Pb'), E=3.3-4.8 MeV/nucleon; measured Eγ, Iγ following Coulomb excitation. 186,188,190,192Os, 194Pt deduced levels, J, π, E2, M1 matrix elements.
doi: 10.1016/0375-9474(96)00181-9
Phys.Lett. 382B, 214 (1996)
C.Y.Wu, D.Cline
Fragmentation of Two-Phonon γ Vibration Strength in Deformed Nuclei
NUCLEAR STRUCTURE 186,188,190,192Os, 232Th, 156Gd, 160Dy, 168Er; analyzed interband E2 transition matrix elements; deduced intrinsic E2 matrix elements between ΔK=2 bands. Rotational, intrinsic motions coupling effects included.
doi: 10.1016/0370-2693(96)00658-2
Phys.Rev. C54, 2356 (1996)
C.Y.Wu, D.Cline
Triaxiality in Quadrupole Deformed Nuclei
NUCLEAR STRUCTURE 150Nd, 152,154Sm, 156,158,160Gd, 160,162,164Dy, 166,168Er, 168,174Yb, 176,178Hf, 184,186W, 186,188,190,192Os, 230,232Th, 234,238U; analyzed interband E2 matrix elements; deduced instrinsic E2 moments, triaxiality parameter (δ), E(2+) ratio.
Proc.9th Intern.Symposium on Capture Gamma-Ray Spectroscopy and Related Topics, Budapest, Hungary, October 1996, G.L.Molnar, T.Belgya, Zs.Revay, Eds., Vol.1, p.147 (1997)
M.Balodis
The Revised Nilsson Model Interpretation of Transitional Nucleus 192Ir
NUCLEAR STRUCTURE 192Ir; analyzed levels, J, π; deduced Nilsson configurations.
Nucl.Instrum.Methods Phys.Res. A391, 289 (1997)
C.J.Barton, R.L.Gill, R.F.Casten, D.S.Brenner, N.V.Zamfir, A.Zilges
Coulomb Excitation of Radioactive Nuclear Beams in Inverse Kinematics
NUCLEAR REACTIONS C(188Os, 188Os'), (192Os, 192Os'), E=270 MeV; measured Eγ, Iγ(t) following projectile Coulomb excitation. 188,192Os levels deduced T1/2, B(E2). Application to radioactive beams discussed.
doi: 10.1016/S0168-9002(97)00416-6
Phys.Rev. C55, 1724 (1997)
N.Fotiades, W.Younes, J.A.Cizewski, D.P.McNabb, K.Y.Ding, 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.Andreev, L.F.Conticchio
Spectroscopy of 192Po
NUCLEAR REACTIONS 164Er(32S, 4n), E=164 MeV; measured Eγ, Iγ, (recoil)γγ-, (recoil)γ-coin, Eα, Iα. 192Po deduced levels. Particle-core model. Recoil decay tagging technique.
NUCLEAR STRUCTURE 192,194,196,198,200,202,204,206,208Po; analyzed level systematics; deduced model parameters. Particle-core model, quasiparticle RPA.
Acta Phys.Pol. B28, 269 (1997)
R.Julin, R.G.Allatt, P.A.Butler, K.J.Cann, J.F.C.Cocks, T.Enqvist, P.T.Greenlees, K.Helariutta, G.D.Jones, P.M.Jones, S.Juutinen, P.Jamsen, H.Kankaanpaa, P.Kuusiniemi, M.Leino, M.Muikku, R.D.Page, M.Piiparinen, A.Savelius, W.H.Trzaska, S.Tormanen, J.Uusitalo
Studies of Neutron-Rich and Heavy Nuclei with the New In-Beam Facilities at JYFL
NUCLEAR REACTIONS 116Cd(84Kr, X), E=370 MeV; measured Eγ, Iγ, γγ-coin. 114,116Cd deduced levels, J, π. 170Yb(28Si, 4n), 160Dy(36Ar, 4n), E not given; measured recoil α-decay associated Eγ, Iγ, γγ-coin. 192,194Po deduced levels, J, π. 208Pb(18O, 4n), E=95 MeV; measured E(ce), I(ce), (ce)(ce)-coin. 222Th deduced levels, J, π.
Acta Phys.Hung.N.S. 6, 169 (1997)
R.Julin, K.Helariutta, P.Jones, S.Juutinen, H.Kankaanpaa, P.Kuusiniemi, M.Leino, M.Muikku, A.Savelius, W.Trzaska, J.Uusitalo, R.G.Allatt, P.A.Butler, J.F.C.Cocks, P.T.Greenlees, R.D.Page, J.Simpson, R.Lemmon
Probing Shapes of Very Neutron Deficient Z ≈ 82 Nuclei using the Recoil-Decay Tagging Method
NUCLEAR REACTIONS 160Dy(36Ar, 4n), E=178 MeV; 144Sm(36Ar, 4n), E=190 MeV; measured Eγ, Iγ, α-spectra following recoil decay, α-tagged (recoil)γ-coin.
Phys.Rev. C56, 2474 (1997)
D.P.McNabb, J.A.Cizewski, K.Y.Ding, N.Fotiades, D.E.Archer, J.A.Becker, L.A.Bernstein, K.Hauschild, W.Younes, R.M.Clark, P.Fallon, I.Y.Lee, A.O.Macchiavelli, R.W.MacLeod
Decay and Properties of the Yrast Superdeformed Band in 192Pb
NUCLEAR REACTIONS 173Yb(24Mg, 5n), E=134.5 MeV; measured Eγ, Iγ, γγ-coin. 192Pb deduced high-spin, superdeformed levels, band structure, possible discrete linking transition.
Phys.Rev. C55, R2150 (1997)
E.F.Moore, T.Lauritsen, R.V.F.Janssens, T.L.Khoo, D.Ackermann, I.Ahmad, H.Amro, D.Blumenthal, M.P.Carpenter, S.M.Fischer, G.Hackman, D.Nisius, F.Hannachi, A.Lopez-Martens, A.Korichi, S.Asztalos, R.M.Clark, M.A.Deleplanque, R.M.Diamond, P.Fallon, I.Y.Lee, A.O.Macchiavelli, F.S.Stephens, J.A.Becker, L.Bernstein, L.P.Farris, E.A.Henry
Differential Lifetime Measurements and Identical Superdeformed Bands 192,194Hg
NUCLEAR REACTIONS 148Nd(48Ca, 4n), E=205 MeV; 150Nd(48Ca, 4n), E=202 MeV; measured γγγ-, higher-fold coincidences, DSA. 192,194Hg deduced superdeformed bands differential T1/2, intrinsic quadrupole moments, β2.
doi: 10.1103/PhysRevC.55.R2150
Z.Phys. A358, 219 (1997)
E.F.Moore, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, D.Ackermann, I.Ahmad, H.Amro, D.Blumenthal, S.Fischer, G.Hackman, D.Nisius, F.Hannachi, A.Lopez-Martens, S.J.Asztalos, R.M.Clark, M.A.Deleplanque, R.M.Diamond, P.Fallon, R.Kruecken, I.-Y.Lee, A.O.Macchiavelli, F.S.Stephens, J.A.Becker, L.Bernstein, L.P.Farris, E.A.Henry, A.Korichi
Lifetime Measurements and Decay of Superdeformed Bands in Hg Isotopes
NUCLEAR REACTIONS 148Nd(48Ca, 4n), E=205 MeV; 150Nd(48Ca, 4n), E=202 MeV; measured Eγ, Iγ, γγ-coin, DSA. 192Hg deduced superdeformed bandsintrinsic quadrupole moments, high-spin levels T1/2. 194Hg deduced superdeformed bands intrinsic quadrupole moments, high-spin levels T1/2, linking transitions. Centroid shift analysis.
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.
Proc.9th Intern.Symposium on Capture Gamma-Ray Spectroscopy and Related Topics, Budapest, Hungary, October 1996, G.L.Molnar, T.Belgya, Zs.Revay, Eds., Vol.1, p.63 (1997)
N.Pietralla, C.Fransen, P.von Brentano, R.-D.Herzberg, A.Zilges, O.Beck, J.Besserer, T.Eckert, D.Jager, U.Kneissl, B.Krischok, H.Maser, J.Margraf, A.Nord, H.H.Pitz
Low-Lying Collective Dipole Excitations in Stable Even-A Nuclei and Their Relation to Phase Transition of Nuclear Deformation
NUCLEAR REACTIONS 178,180Hf, 190,192Os(γ, γ'), E not given; analyzed data. 178,180Hf, 190,192Os deduced excitation B(M1), deformation dependence. Other nuclei compared.
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.
Nucl.Data Sheets 84, 1 (1998)
Y.A.Akovali
Review of Alpha-Decay Data from Doubly-Even Nuclei
COMPILATION A=106-256; compiled, evaluated α-decay data for even-even nuclei.
Phys.Lett. 437B, 29 (1998)
R.G.Allatt, R.D.Page, M.Leino, T.Enqvist, K.Eskola, P.T.Greenlees, P.Jones, R.Julin, P.Kuusiniemi, W.H.Trzaska, J.Uusitalo
Fine Structure in 192Po α-Decay and Shape Coexistence in 188Pb
RADIOACTIVITY 192Po(α) [from 160Dy(36Ar, 4n)]; measured α spectra; deduced branching, hindrance factors. 188Pb deduced levels, J, π, configurations.
doi: 10.1016/S0370-2693(98)00939-3
Phys.Rev. C57, R1017 (1998)
B.C.Busse, P.Fallon, R.Krucken, D.Ackermann, I.Ahmad, S.J.Asztalos, D.J.Blumenthal, M.P.Carpenter, R.M.Clark, M.A.Deleplanque, R.M.Diamond, S.M.Fischer, F.Hannachi, R.V.F.Janssens, T.L.Khoo, A.Korichi, T.Lauritsen, I.Y.Lee, A.Lopez-Martens, A.O.Macchiavelli, R.W.MacLeod, E.F.Moore, D.Nisius, G.Schmid, D.Seweryniak, F.S.Stephens, K.Vetter
Lifetime Measurements of Yrast and Excited Superdeformed Bands in 192,193Hg
NUCLEAR REACTIONS 176Yb(22Ne, 5n), (22Ne, 6n), E=118 MeV; measured Eγ, Iγ, γγ-coin, DSA. 192,193Hg deduced superdeformed bands T1/2, average quadrupole moments, configurations.
doi: 10.1103/PhysRevC.57.R1017
Nucl.Data Sheets 84, 487 (1998)
B.Singh, J.L.Rodriguez, S.S.M.Wong, J.K.Tuli
Review of Log ft Values in β Decay
COMPILATION A=1-250; compiled log ft values.
Nucl.Phys. A660, 87 (1999); Erratum Nucl.Phys. A674, 578 (2000)
J.Benlliure, K.-H.Schmidt, D.Cortina-Gil, T.Enqvist, F.Farget, A.Heinz, A.R.Junghans, J.Pereira, J.Taieb
Production of Neutron-Rich Isotopes by Cold Fragmentation in the Reaction 197Au + Be at 950 A MeV
NUCLEAR REACTIONS Be(197Au, X), E=950 MeV/nucleon; measured neutron-rich fragments isotopic production σ, momentum distributions; deduced evidence for 193,194Re, 191,192W, 189Ta, 187,188Hf. Cold fragmentation process, analytical model description.
doi: 10.1016/S0375-9474(99)00386-3
CEA-ISBN 2-7272-0200-8 (1999)
M.-M.Be, B.Duchemin, J.Lame, C.Morillon, F.Piton, E.Browne, V.Chechev, R.Helmer, E.Schonfeld
Table of Radionuclides
COMPILATION 3H, 14C, 22Na, 26Al, 35S, 36Cl, 40K, 55Fe, 58,60Co, 65Zn, 68Ga, 68Ge, 75Se, 95Zr, 95Nb, 111,113In, 113Sn, 123Te, 125I, 137Cs, 139,141Ce, 188Re, 192,194Ir, 207Bi; compiled, evaluated decay data.
CEA-ISBN 2-7272-0211-3 (1999)
M.-M.Be, B.Duchemin, E.Browne, S.-C.Wu, V.Chechev, R.Helmer, E.Schonfeld
Table of Radionuclides: Comments on Evaluations
COMPILATION 3H, 14C, 22Na, 26Al, 35S, 36Cl, 40K, 55Fe, 58,60Co, 65Zn, 68Ga, 68Ge, 75Se, 95Zr, 95Nb, 111,113In, 113Sn, 123Te, 125I, 137Cs, 139,141Ce, 188Re, 192Ir, 207Bi; compiled, evaluated decay data. Comments on evaluations.
Phys.Rev. C59, 2264 (1999)
C.Fransen, B.Krischok, O.Beck, J.Besserer, P.von Brentano, T.Eckert, R.-D.Herzberg, U.Kneissl, J.Margraf, H.Maser, A.Nord, N.Pietralla, H.H.Pitz, A.Zilges
Low-Lying Dipole Excitations in the Transitional Nuclei 190, 192Os
NUCLEAR REACTIONS 190,192Os(γ, γ'), E=4 MeV bremsstrahlung; measured Eγ, Iγ(θ). 190,192Os deduced levels, J, π, B(M1), dipole excitation strength distribution, scissors mode. Comparison with IBM-2 predictions.
Nucl.Instrum.Methods Phys.Res. A433, 592 (1999)
O.Helene, V.R.Vanin, S.P.Tsai
Improvement of 192Ir and 152Eu Gamma-Ray Calibration Energies by using a Self-Calibration Procedure
RADIOACTIVITY 192Ir, 152Eu(β-), (EC); measured Eγ, Iγ; deduced uncertainties. Self-calibration procedure.
doi: 10.1016/S0168-9002(99)00474-X
Eur.Phys.J. A 6, 289 (1999)
K.Helariutta, J.F.C.Cocks, T.Enqvist, P.T.Greenlees, P.Jones, R.Julin, S.Juutinen, P.Jamsen, H.Kankaanpaa, H.Kettunen, P.Kuusiniemi, M.Leino, M.Muikku, M.Piiparinen, P.Rahkila, A.Savelius, W.H.Trzaska, S.Tormanen, J.Uusitalo, R.G.Allatt, P.A.Butler, R.D.Page, M.Kapusta
Gamma-Ray Spectroscopy of 192-195Po
NUCLEAR REACTIONS 160Dy(36Ar, 4n), (36Ar, 2n), (36Ar, n), E=178, 196 MeV; 170Yb(28Si, 4n), (28Si, 3n), E=143 MeV; 171Yb(28Si, 5n), (28Si, 4n), E=155 MeV; 166Er(32S, 4n), E=172 MeV; measured prompt, delayed Eγ, Iγ, γγ-, (recoil)γ-coin. 192,193,194,195Po deduced levels, J, π, configurations, collective features. Level systematics of Po isotopes discussed. Mass separator, recoil decay tagging.
Phys.Scr. T88, 141 (2000)
J.A.Cizewski, D.P.McNabb
Probing Nuclear Structure at Finite Temperature and Spin via Decay of Superdeformed Bands in Lead Nuclei
NUCLEAR REACTIONS 174Yb(25Mg, 5n), E not given; 173Yb(24Mg, 5n), E not given; measured Eγ, Iγ, γγ-coin. 192,194Pb deduced quasicontinuum spectra from superdeformed band decay, related parameters. Gammasphere array.
doi: 10.1238/Physica.Topical.088a00141
Nucl.Instrum.Methods Phys.Res. A450, 35 (2000)
R.G.Helmer, C.van der Leun
Recommended Standards for γ-Ray Energy Calibration (1999)
COMPILATION 7Be, 22,24Na, 44Ti, 46Sc, 51Cr, 54Mn, 56,57,58,60Co, 59Fe, 65Zn, 66Ga, 75Se, 82Br, 84Rb, 85Sr, 88Y, 94Nb, 95Zr, 95mTc, 99Mo, 106Ru, 108m,110mAg, 109Cd, 113,125Sn, 124,125Sb, 132,137Cs, 133Ba, 139,141,144Ce, 152,154Eu, 153Sm, 153Gd, 160,161Tb, 166mHo, 169Yb, 170Tm, 172Hf, 182Ta, 185Os, 192Ir, 198,199Au, 203,210Pb, 203Hg, 207Bi, 228Th, 241Am; compiled γ-ray calibration standards.
doi: 10.1016/S0168-9002(00)00252-7
Phys.Rev. C62, 044316 (2000)
T.Lauritsen, T.L.Khoo, I.Ahmad, M.P.Carpenter, R.V.F.Janssens, A.Korichi, A.Lopez-Martens, H.Amro, S.Berger, L.Calderin, T.Dossing, S.M.Fischer, G.Hackman, F.Hannachi, C.J.Lister, E.F.Moore, D.T.Nisius, C.Schuck, S.Siem
Experimental Determination of the Excitation Energy of Superdeformed Bands in 192, 194Hg by Analysis of the Decay Quasicontinuum γ Rays
NUCLEAR REACTIONS 150Nd(48Ca, 4n), E=199 MeV; 160Gd(36S, 4n), E=157 MeV; measured Eγ, Iγ, γγ-coin. 192,194Hg deduced quasicontinuum decay features, superdeformed bands excitation energy, spin. Gammasphere array.
doi: 10.1103/PhysRevC.62.044316
Phys.Rev. C61, 031304 (2000)
D.P.McNabb, J.A.Cizewski, T.L.Khoo, T.Lauritsen, K.Hauschild, K.Y.Ding, N.Fotiades, W.Younes, D.E.Archer, R.W.Bauer, J.A.Becker, L.A.Bernstein, R.M.Clark, M.A.Deleplanque, R.M.Diamond, P.Fallon, I.Y.Lee, A.O.Macchiavelli, R.W.MacLeod, F.S.Stephens, A.Lopez-Martens, W.H.Kelly
Quasicontinuous Decay Spectra of Superdeformed Bands in 192, 194Pb and Energy Gaps in Level Density at Moderate Angular Momenta
NUCLEAR REACTIONS 174Yb(25Mg, 5n), E=130.0 MeV; 173Yb(24Mg, 5n), E=134.5 MeV; measured Eγ, Iγ, γγ-coin. 192,194Pb deduced superdeformed band decay quasicontinuum transitions, level density features. Constant temperature level density model.
doi: 10.1103/PhysRevC.61.031304
Proc.2nd Intern.Conf Fission and Properties of Neutron-Rich Nuclei, St Andrews, Scotland, June 28-July 3, 1999, J.H.Hamilton, W.R.Phillips, H.K.Carter, Eds., World Scientific, Singapore, p.156 (2000)
Zs.Podolyak, P.H.Regan, M.Pfutzner, J.Gerl, M.Hellstrom, M.Caamano, P.Mayet, M.Mineva, M.Sawicka, Ch.Schlegel, for the GSI Isomer Collaboration
High Spin Fragmentation Spectroscopy
NUCLEAR REACTIONS Be(208Pb, X)138Gd/167Tb/170Dy/178Tm/181Yb/187Hf/188Hf/187Ta/188Ta/189Ta/179W/190W/191W/192W/192Re/193Re/194Re/195Re/197Os/198Ir/201Pt/202Pt, E=1 GeV/nucleon; measured relative isotopic yields, residue energy, Eγ following projectile fragmentation. 138Gd, 179,190W, 188Ta, 192Re, 198Ir, 201,202Pt; deduced transitions following isomer decay.
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
Hyperfine Interactions 129, 149 (2000)
P.Van Duppen, M.Huyse
Shape coexistence around the Z=82 closed shell probed by α-decay
RADIOACTIVITY 196,200Po, 200At, 199,200,201,202Rn(α); measured Eα, Iα, (α)x-ray coin. 176,178,180Pt, 180,182,184,186Hg, 186,188,190,192,194Pb, 192,194,198,200,202,204,206,208,210Po, 198,200,202Rn(α); analyzed hindrance factors.Po; analyzed energy systematics for even-even isotopes. Z=80, 82, 84, 86, 88; analyzed reduced α widths.
Nucl.Phys. A682, 223c (2001)
M.Caamano, P.H.Regan, Zs.Podolyak, C.J.Pearson, P.Mayet, J.Gerl, Ch.Schlegel, M.Pfutzner, M.Hellstrom, M.Mineva, and the GSI ISOMER Collaboration
Nuclear Structure of Heavy Neutron Rich Systems: Fragmentation spectroscopy with a 1 GeV per nucleon 208Pb beam
NUCLEAR REACTIONS 9Be(208Pb, X), E=1 GeV/nucleon; measured fragment yields, delayed Eγ, Iγ(t), γγ-, (fragment)γ-coin. 190W, 188Ta, 192,193Re, 200,201,202Pt, 197Ir, 206Hg deduced transitions following isomer decay. Fragment separator.
doi: 10.1016/S0375-9474(00)00643-6
Phys.Rev. C63, 061302 (2001)
G.D.Dracoulis, T.Kibedi, A.P.Byrne, A.M.Baxter, S.M.Mullins, R.A.Bark
Effect of Oblate Deformation on E3 Strengths in Light Lead and Polonium Isotopes
NUCLEAR REACTIONS 166,168Er(28Si, 4n), E=140 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin, E(ce), I(ce). 190,192Pb deduced levels, J, π, ICC, isomeric states T1/2, configurations. Comparisons with neighboring polonium isotopes.
doi: 10.1103/PhysRevC.63.061302
Appl.Radiat.Isot. 54, 141 (2001)
K.A.Fonseca, M.F.Koskinas, M.S.Dias
Disintegration Rate Measurement of a 192Ir Solution
RADIOACTIVITY 192Ir(EC), (β-); measured Eγ, βγ-coin, decay rate.
doi: 10.1016/S0969-8043(00)00158-5
Phys.Rev. C64, 064304 (2001)
E.Gueorguieva, Ch.Vieu, C.Schuck, A.Minkova, B.Kharraja, M.Kaci, F.Hannachi, J.S.Dionisio, A.Korichi, A.Lopez-Martens, Z.Meliani, Ts.Venkova
First Identification of 20+ Isomeric States in Odd-Odd 190, 192Au Nuclei
NUCLEAR REACTIONS 186W(11B, 7n), (11B, 6n), (11B, 5n), E=84, 86 MeV; measured prompt and delayed Eγ, Iγ, E(ce), I(ce), γγ-, (ce)γ-coin, γ-ray polarization. 190,192Au deduced high-spin levels, J, π, ICC, configurations, B(E2), isomeric states T1/2, triaxial deformation. Eurogam II array, electron spectrometer, recoil shadow anisotropy technique. Total Routhian surface calculations.
doi: 10.1103/PhysRevC.64.064304
J.Phys.(London) G27, R109 (2001)
R.Julin, K.Helariutta, M.Muikku
Intruder States in Very Neutron-Deficient Hg, Pb and Po Nuclei
NUCLEAR REACTIONS 144Sm(36Ar, 4n), (36Ar, 3n), E=190 MeV; 112Sn(64Zn, 2n), E not given; 148Sm(40Ca, 4n), E=195, 200 MeV; 144Sm(42Ca, 4n), E=209 MeV; 170Yb(28Si, 4n), (28Si, 3n), E not given; 171Yb(28Si, 5n), (28Si, 4n), E not given; 160Dy(36Ar, 4n), E=178 MeV; 142Nd(52Cr, 4n), (52Cr, 3n), E not given; 160Dy(36Ar, n), (36Ar, 3n), E not given; measured Eγ, Iγ, γγ-, (recoil)γ-coin. 174,176,177Hg, 182,184Pb, 190,191,192,193,194,195Po deduced levels, J, π, configurations, rotational bands. Jurosphere array, gas-filled separator, recoil-decay tagging.
doi: 10.1088/0954-3899/27/7/201
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
Yad.Fiz. 64, No 5, 908 (2001); Phys.Atomic Nuclei 64, 843 (2001)
I.B.Kovgar, A.I.Levon, R.S.Poznyak, O.V.Sevastyuk
Anomalies in the Orbital Magnetism of Neutrons in the 190, 192Pt Nuclei
NUCLEAR REACTIONS 188,190Os(α, 2n), E=26.8 MeV; measured Eγ, Iγ(θ, H, t). 190,192Pt deduced high-spin isomeric states g factors, neutron orbital g factor anomalies. Integrated disturbed angular distribution technique.
doi: 10.1134/1.1378873
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
Acta Phys.Pol. B32, 1015 (2001)
J.Uusitalo, H.Kettunen, A.N.Andreyev, K.Eskola, P.T.Greenlees, K.Helariutta, M.Huyse, P.Jones, R.Julin, S.Juutinen, H.Kankaanpaa, P.Kuusiniemi, M.Leino, M.Muikku, P.Nieminen, P.Rahkila, K.Van del Vel, P.Van Duppen
Alpha Decay Studies of Translead Nuclei at the Proton Drip Line
RADIOACTIVITY 191,192Po, 195,196Rn(α); measured Eα, T1/2, hindrance factors.
Yad.Fiz. 64, No 2, 195 (2001); Phys.Atomic Nuclei 64, 153 (2001)
E.V.Vasilieva, A.M.Sukhovoj, V.A.Khitrov
Direct Experimental Estimate of Parameters That Determine the Cascade Gamma Decay of Compound States of Heavy Nuclei
NUCLEAR REACTIONS 113Cd, 123Te, 127I, 149Sm, 155Gd, 159Tb, 169Tm, 180Hf, 189Os, 191Ir, 195Pt, 199Hg(n, γ), E=thermal; measured Eγ, 2-step photon cascades. 114Cd, 124Te, 128I, 150Sm, 156Gd, 160Tb, 170Tm, 181Hf, 190Os, 192Ir, 196Pt, 200Hg deduced level densities vs excitation energy, sum of radiative strengths for E1 and M1 transitions. Comparison with Statistical Model calculations.
doi: 10.1134/1.1349436
Phys.Rev. C64, 014307 (2001); Comment Phys.Rev. C66, 039801 (2002)
C.Y.Wu, D.Cline, A.B.Hayes, M.W.Simon, R.Krucken, J.R.Cooper, C.J.Barton, C.W.Beausang, C.Bialik, M.A.Caprio, R.F.Casten, A.A.Hecht, H.Newman, J.Novak, N.Pietralla, K.Zyromski, N.V.Zamfir
Two-Phonon γ-Vibrational Strength in Osmium Nuclei
NUCLEAR REACTIONS 188,190Os(58Ni, 58Ni'), E=275 MeV; measured Doppler-shifted Eγ, Iγ, γγ-, (particle)γ-coin following Coulomb excitation. 188,190Os deduced levels, J, π, B(E2), two-phonon γ-vibration strength. Recoil-distance technique.
doi: 10.1103/PhysRevC.64.014307
Appl.Radiat.Isot. 56, 125 (2002)
M.P.Unterweger
Half-Life Measurements at the National Institute of Standards and Technology
RADIOACTIVITY 22Na, 133Ba, 207Bi(EC); 60Co, 85Kr, 125Sb, 137Cs, 155Eu(β-); 152,154Eu(EC), (β-); measured T1/2. Comparison with previous results.
COMPILATION 3H, 18F, 22,24Na, 32P, 46Sc, 51Cr, 54Mn, 57,58,60Co, 59Fe, 62Cu, 65Zn, 67Ga, 75Se, 85Kr, 85Sr, 88Y, 99Mo, 99mTc, 103Ru, 109Cd, 110mAg, 111In, 113,117mSn, 123,125,131I, 125Sb, 127,131m,133Xe, 133,140Ba, 134,137Cs, 139,141,144Ce, 140La, 152,154,155Eu, 153Gd, 153Sm, 166Ho, 169Yb, 177Lu, 181,188W, 186,188Re, 192Ir, 195,198Au, 201,202Tl, 203Hg, 203Pb, 207Bi, 228Th; compiled T1/2.
doi: 10.1016/S0969-8043(01)00177-4
GSI 2002-1, p.14 (2002)
K.Van de Vel, A.N.Andreyev, D.Ackermann, S.Antalic, H.J.Boardman, P.Cagarda, J.Gerl, F.P.Hessberger, S.Hofmann, M.Huyse, D.Karlgren, B.Kindler, I.Kozhoukharov, M.Leino, B.Lommel, G.Munzenberg, C.Moore, R.D.Page, C.Schlegel, P.Van Duppen
Fine Structure in the Alpha Decay of Neutron-Deficient Polonium Isotopes
RADIOACTIVITY 192Po(α) [from 142Nd(52Cr, 2n)]; measured electronα-coin, Eα. 188Pb; deduced population intensity of oblate/prolate states, shape coexistence. 188Po(α) [from 142Nd(50Cr, 4n)]; measured Eα, T1/2. Comparison with neighboring isotopes.
Nucl.Phys. A729, 3 (2003)
G.Audi, O.Bersillon, J.Blachot, A.H.Wapstra
The NUBASE evaluation of nuclear and decay properties
COMPILATION A=1-293; compiled, evaluated ground- and isomeric-states mass excess, J, π, decay properties.
doi: 10.1016/j.nuclphysa.2003.11.001
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
Priv.Comm. (2003)
H.D.Choi, R.B.Firestone, R.M.Lindstrom, G.L.Molnar, S.F.Mughabghab, R.Paviotti Corcuera, Zs.Revay, A.Trkov, V.Zerkin, C.M.Zhou
Database of Prompt Gamma Rays from Slow Neutron Capture for Elemental Analysis
COMPILATION Z=1-92; compiled Eγ, Iγ from neutron capture.
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.
Eur.Phys.J. A 17, 537 (2003)
H.Kettunen, T.Enqvist, T.Grahn, P.T.Greenlees, P.Jones, R.Julin, S.Juutinen, A.Keenan, P.Kuusiniemi, M.Leino, A.-P.Leppanen, P.Nieminen, J.Pakarinen, P.Rahkila, J.Uusitalo
Alpha-decay studies of the new isotopes 191At and 193At
NUCLEAR REACTIONS 141Pr(54Fe, 4n), (56Fe, 4n), E ≈ 248-272 MeV; measured excitation functions. Recoil-decay tagging.
RADIOACTIVITY 191,193At, 187,189Bi(α) [from 141Pr(54Fe, 4n), (56Fe, 4n) and subsequent decay]; measured Eα, T1/2 for ground and excited states; deduced hindrance factors. 191,193At, 187,189Bi deduced levels, J, π, configurations.
doi: 10.1140/epja/i2002-10162-1
Eur.Phys.J. A 17, 167 (2003)
K.Van de Vel, A.N.Andreyev, R.D.Page, H.Kettunen, P.T.Greenlees, P.Jones, R.Julin, S.Juutinen, H.Kankaanpaa, A.Keenan, P.Kuusiniemi, M.Leino, M.Muikku, P.Nieminen, P.Rahkila, J.Uusitalo, K.Eskola, A.Hurstel, M.Huyse, Y.Le Coz, M.B.Smith, P.Van Duppen, R.Wyss
In-beam γ-ray spectroscopy of 190Po: First observation of a low-lying prolate band in Po isotopes
NUCLEAR REACTIONS 142Nd(52Cr, 4n), E=255 MeV; measured Eγ, Iγ, (recoil)γ-coin. 190Po deduced levels, J, π, configurations, deformation. Jurosphere array, recoil-decay tagging. Level systematics in neighboring nuclides discussed.
RADIOACTIVITY 187,188Pb, 188,190,191,193Bi, 190,191,192Po(α) [from 142Nd(52Cr, xnyp)]; measured Eα. Mass separator.
doi: 10.1140/epja/i2003-10002-x
Phys.Rev. C 68, 054311 (2003)
K.Van de Vel, A.N.Andreyev, D.Ackermann, H.J.Boardman, P.Cagarda, J.Gerl, F.P.Hessberger, S.Hofmann, M.Huyse, D.Karlgren, I.Kojouharov, M.Leino, B.Lommel, G.Munzenberg, C.Moore, R.D.Page, S.Saro, P.van Duppen, R.Wyss
Fine structure in a α decay of 188, 192Po
RADIOACTIVITY 188,192Po(α) [from 142Nd(50Cr, 4n), (52Cr, 4n)]; measured Eα, Iα, αγ-coin; deduced hindrance factors. 192Po deduced levels, isomeric state T1/2. 184,188Pb deduced excited 0+ states features. Potential energy surface calculations.
doi: 10.1103/PhysRevC.68.054311
Phys.Rev.Lett. 90, 142501 (2003)
A.N.Wilson, G.D.Dracoulis, A.P.Byrne, P.M.Davidson, G.J.Lane, R.M.Clark, P.Fallon, A.Gorgen, A.O.Macchiavelli, D.Ward
Direct Decays from Superdeformed States in 192Pb Observed Using Time-Correlated γ-Ray Spectroscopy
NUCLEAR REACTIONS 168Er(29Si, 5n), E=154 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 192Pb deduced linking transitions between normal-deformed and superdeformed states, superdeformed band excitation energy, J, π. Gammasphere array. Comparison with model predictions.
doi: 10.1103/PhysRevLett.90.142501
Priv.Comm. (2003)
A.N.Wilson
At.Data Nucl.Data Tables 87, 185 (2004)
I.Angeli
A consistent set of nuclear rms charge radii: properties of the radius surface R(N, Z)
COMPILATION A=1-248; compiled, analyzed charge radii.
doi: 10.1016/j.adt.2004.04.002
Nucl.Instrum.Methods Phys.Res. A533, 409 (2004)
A.N.Andreyev, D.Ackermann, F.P.Hessberger, S.Hofmann, M.Huyse, G.Munzenberg, R.D.Page, K.Van de Vel, P.Van Duppen
Conversion electron and beta decay spectroscopy at SHIP
RADIOACTIVITY 192Po(α) [from 142Nd(52Cr, 2n)]; 192Bi(α), (EC), (β+) [from 142Nd(52Cr, 2n)]; measured Eα, Eβ, Eγ, conversion electron spectra. 188Pb deduced transition. Mass separator.
NUCLEAR REACTIONS 142Nd(52Cr, 2n), (52Cr, np), E=255 MeV; measured delayed (recoil)α-, (recoil)γ-coin, Eβ, conversion electron spectra. 188Pb deduced transition. Mass separator.
doi: 10.1016/j.nima.2004.07.204
Thesis, Leuven Univ. Belgium (2004)
H.De Witte
Probing the nuclear structure along the Z=82 closed shell: decay- and laser spectroscopic studies of exotic Pb, Bi and Po nuclei
RADIOACTIVITY 213Pb, 215Pb, 218Bi(β-); 193Bi, 196,197,199,201At, 200,201,203,205Fr(α); measured Eγ, Iγ, Eα, Iα, βγ-, αγ-, γγ-coin, half-lives, conversion coefficients. 213,215Bi, 218Po; deduced levels, J, π, logft, multipolarity. Sources produced at ISOLDE-CERN facility using 232Th, 238U(p, X), E=1.4 GeV reaction. RILIS and surface ionization sources, and pulsed-release technique. 210,211,213,214,215Tl(β-n); measured neutron spectra, non-observation of resonantly ionized Tl isotopes. No delayed neutron emission probabilities deduced.
NUCLEAR MOMENTS 183,184,185,186,187,188,190,208Pb; measured hyperfine structure using In Source laser spectroscopy; deduced isotope shifts, rms charge radii, magnetic moments.
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
Laser Phys.Lett. 1, 317 (2004)
P.H.Regan, J.J.Valiente-Dobon, C.Wheldon, C.Y.Wu, J.F.Smith, A.O.Macchiavelli, D.Cline, R.S.Chakrawarthy, R.Chapman, M.Cromaz, P.Fallon, S.J.Freeman, A.Gorgen, W.Gelletly, A.Hayes, S.D.Langdown, I.Y.Lee, X.Liang, C.J.Pearson, Zs.Podolyak, R.Teng, D.Ward, D.D.Warner, A.D.Yamamoto
Production of exotic nuclear isomers in multi-nucleon transfer reactions
NUCLEAR REACTIONS 198Pt(136Xe, X), E=850 MeV; measured prompt and delayed Eγ, Iγ, γγ-, (particle)γ-coin following multinucleon transfer reactions. 198Pt deduced levels, J, π. 184W, 185Re, 191,192,195Os, 192,198Pt, 193Au deduced transitions, high-spin isomeric states T1/2. 136Ba, 133,134,136Xe deduced delayed transitions. Gammasphere, Chico arrays.
Phys.Rev. C 69, 024316 (2004)
J.J.Valiente-Dobon, P.H.Regan, C.Wheldon, C.Y.Wu, N.Yoshinaga, K.Higashiyama, J.F.Smith, D.Cline, R.S.Chakrawarthy, R.Chapman, M.Cromaz, P.Fallon, S.J.Freeman, A.Gorgen, W.Gelletly, A.Hayes, H.Hua, S.D.Langdown, I.Y.Lee, X.Liang, A.O.Macchiavelli, C.J.Pearson, Zs.Podolyak, G.Sletten, R.Teng, D.Ward, D.D.Warner, A.D.Yamamoto
136Ba studied via deep-inelastic collisions: Identification of the (νh11/2)-210+ isomer
NUCLEAR REACTIONS 198Pt(136Xe, X), E=850 MeV; measured prompt and delayed Eγ, Iγ, γγ-, (particle)γ-coin. 136Ba deduced levels, J, π, B(E2), isomer T1/2. 128,130Te, 131,133I, 132,136Xe, 138Ba, 137La, 184W, 185Re, 191,192,195Os, 192,198Pt, 193Au; deduced isomers T1/2. Gammasphere, Chico arrays.
doi: 10.1103/PhysRevC.69.024316
Nucl.Phys. A734, 156 (2004)
H.W.Wilschut, V.L.Kravchuk
Developing an "Atomic Clock" for Fission Lifetime Measurements
NUCLEAR REACTIONS 232Th(20Ne, F), E=30 MeV/nucleon; measured Eγ, pre-fission X-ray spectra, (fragment)γ-coin; deduced fission lifetime.
doi: 10.1016/j.nuclphysa.2004.01.024
Appl.Radiat.Isot. 60, 257 (2004)
M.J.Woods, S.M.Collins
Half-life data - a critical review of TECDOC-619 update
COMPILATION 23,24Na, 40K, 46Sc, 51Cr, 54,56Mn, 55,59Fe, 56,57,58,60Co, 64Cu, 65Zn, 66,67,68Ga, 75Se, 85Kr, 85Sr, 88Y, 93m,94,95Nb, 99Mo, 99mTc, 103,106Ru, 106Rh, 109Cd, 110mAg, 111In, 113Sn, 123,125,129,131I, 123mTe, 125Sb, 133Ba, 134,137Cs, 139,141,144Ce, 152,154,155Eu, 153Sm, 166,166mHo, 169Yb, 170Tm, 198Au, 201Tl, 203Hg, 207Bi, 226Ra, 228Th, 234mPa, 241,243Am; compiled, analyzed T1/2.
doi: 10.1016/j.apradiso.2003.11.026
GSI 2005-1, p.77 (2005)
A.N.Andreyev, S.Antalic, D.Ackermann, S.Franchoo, F.P.Hessberger, S.Hofmann, M.Huyse, I.Kojouharov, B.Kindler, P.Kuusiniemi, S.R.Lesher, B.Lommel, R.Mann, G.Munzenberg, K.Nishio, R.D.Page, J.Ressler, B.Streicher, B.Sulignano, P.Van Duppen, D.Wiseman
New isotopes 186, 187Po and 192At
NUCLEAR REACTIONS 144Sm(46Ti, xn), E not given; measured Eγ, Eα, αα-, αγ-coin following residual nucleus decay; deduced evidence for 186,187Po. 144Sm(51V, xn), E not given; measured Eγ, Eα, αα-, αγ-coin following residual nucleus decay; deduced evidence for 192At.
RADIOACTIVITY 186,187Po, 183Pb, 179Hg, 175Pt(α) [from 144Sm(46Ti, xn) and subsequent decay]; measured Eα, T1/2. 183Pb deduced excited state energy. 187Po deduced isomeric states. 192At(α) [from 144Sm(51V, xn)]; measured Eα, αα-coin, T1/2; deduced isomeric states.
Eur.Phys.J. A 23, 201 (2005)
M.Caamano, P.M.Walker, P.H.Regan, M.Pfutzner, Zs.Podolyak, J.Gerl, M.Hellstrom, P.Mayet, M.N.Mineva, A.Aprahamian, J.Benlliure, A.M.Bruce, P.A.Butler, D.Cortina Gil, D.M.Cullen, J.Doring, T.Enqvist, C.Fox, J.Garces Narro, H.Geissel, W.Gelletly, J.Giovinazzo, M.Gorska, H.Grawe, R.Grzywacz, A.Kleinbohl, W.Korten, M.Lewitowicz, R.Lucas, H.Mach, C.D.O'Leary, F.De Oliveira, C.J.Pearson, F.Rejmund, M.Rejmund, M.Sawicka, H.Schaffner, C.Schlegel, K.Schmidt, K.-H.Schmidt, P.D.Stevenson, Ch.Theisen, F.Vives, D.D.Warner, C.Wheldon, H.J.Wollersheim, S.Wooding, F.Xu, O.Yordanov
Isomers in neutron-rich A ≈ 190 nuclides from 208Pb fragmentation
NUCLEAR REACTIONS Be(208Pb, X), E=1 GeV/nucleon; measured fragments isotopic yields, delayed Eγ, γγ-, (particle)γ-coin; deduced isomer production ratios.
RADIOACTIVITY 188Ta, 190W, 192,193Re, 195Os, 197,198Ir, 200,201,202Pt, 203Au(IT) [from Be(208Pb, X)]; measured Eγ, Iγ, γγ-coin, T1/2. 188Ta, 190W, 192,193Re, 195Os, 197,198Ir, 200,201,202Pt, 203Au deduced transitions. 190W, 200,201,202Pt deduced levels, J, π. 174,175Er, 185Hf, 191,194Re, 199Ir(IT) [from Be(208Pb, X)]; measured Eγ, Iγ.
doi: 10.1140/epja/i2004-10079-7
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 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
Eur.Phys.J. A 25, Supplement 1, 179 (2005)
J.Uusitalo, S.Eeckhaudt, T.Enqvist, K.Eskola, T.Grahn, P.T.Greenlees, P.Jones, R.Julin, S.Juutinen, H.Kettunen, P.Kuusiniemi, M.Leino, A.-P.Leppanen, P.Nieminen, M.Nyman, J.Pakarinen, P.Rahkila, C.Scholey
Alpha-decay studies using the JYFL gas-filled recoil separator RITU
RADIOACTIVITY 188,190,192,194,196,198,200,202,204Po, 191,193,195,197,199At, 196,198,200,202,204,206Rn, 199,201,203,205,207Fr(α); measured reduced widths using gas filled recoil separator; deduced hindrance factors, proton intruder states and deformation effects.
doi: 10.1140/epjad/i2005-06-089-9
Nucl.Phys. A748, 12 (2005)
A.N.Wilson, G.D.Dracoulis, P.M.Davidson, A.P.Byrne, R.M.Clark, P.Fallon, A.Gorgen, G.J.Lane, A.O.Macchiavelli, D.Ward
Quadrupole moment of the yrast superdeformed band in 192Pb
NUCLEAR REACTIONS 168Er(29Si, 5n), E=154 MeV; measured Eγ, Iγ, γγ-coin, DSA. 192Pb deduced superdeformed band levels T1/2, quadrupole moment. Gammasphere array, total Routhian surface calculations.
doi: 10.1016/j.nuclphysa.2004.10.017
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
Phys.Rev. C 73, 024317 (2006)
A.N.Andreyev, S.Antalic, D.Ackermann, S.Franchoo, F.P.Hessberger, S.Hofmann, M.Huyse, I.Kojouharov, B.Kindler, P.Kuusiniemi, S.R.Lesher, B.Lommel, R.Mann, G.Munzenberg, K.Nishio, R.D.Page, J.J.Ressler, B.Streicher, S.Saro, B.Sulignano, P.Van Duppen, D.R.Wiseman
α-decay spectroscopy of the new isotope 192At
NUCLEAR REACTIONS 144Sm(51V, X), E=230 MeV; measured Eγ, Eα, (recoil)α-, αα-, αγ-coin following residual nucleus decay; deduced evidence for 192At.
RADIOACTIVITY 192,192mAt(α) [from 144Sm(51V, 3n)]; measured Eα, Eγ, αγ-coin, T1/2; deduced isomeric states energies, configurations.
doi: 10.1103/PhysRevC.73.024317
Hyperfine Interactions 171, 217 (2006)
M.Avgoulea, M.Mahgoub, J.Billowes, P.Campbell, A.Ezwam, D.H.Forest, M.Gardner, J.Huikari, A.Jokinen, A.Nieminen, G.Tungate, J.Aysto
Laser spectroscopy of stable Os isotopes
NUCLEAR MOMENTS 184,186,187,188,189,190,192Os; measured hfs, isotope shifts. Laser spectroscopy.
doi: 10.1007/s10751-006-9485-0
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
Bull.Rus.Acad.Sci.Phys. 70, 1822 (2006)
A.I.Levon, I.B.Kovgar, Yu.V.Nosenko, V.A.Onishchuk, A.A.Shevchuk
Nuclear g-factors of high-spin isomers in 190, 192, 194Pt
NUCLEAR REACTIONS 188,190,192Os(α, 2n)190,192,194Pt, E=27 MeV; measured g-factors of isomeric states using integral perturbed angular distribution of γ-rays in an external magnetic field of 2.9T.
NUCLEAR MOMENTS 190,192,194Pt; measured Eγ, Iγ; deduced g-factors.
Atlas of Neutron Resonances, 5ed., Resonance Parameters and Thermal Cross Sections, Z = 1-100, Elsevier, Amsterdam (2006)
S.F.Mughabghab
COMPILATION Z=1-100; compiled, evaluated thermal neutron induced σ, resonance parameter data.
Proc.Fusion06: Reaction Mechanisms and Nuclear Structure at the Coulomb Barrier, San Servolo, Venice, Italy, 19-23 March 2006, L.Corradi, et al. Eds. p. 271 (2006); AIP Conf.Proc. 853 (2006)
P.H.Regan, G.A.Jones, Zs.Podolyak, G.de Angelis, Y.H.Zhang, A.Gadea, C.A.Ur, M.Abdullah, M.Axiotis, D.Bazzacco, R.Broda, D.Bucurescu, E.Farnea, W.Gelletly, M.Ionescu-Bujor, A.Iordachescu, Th.Kroll, S.D.Langdown, S.Lenzi, S.Lunardi, N.Marginean, T.Martinez, N.Medina, R.Menegazzo, D.R.Napoli, B.Quintana, B.Rubio, C.Rusu, R.Schwengner, D.Tonev, J.J.Valiente-Dobon, W.von Oertzen, G.Wollel
Nuclear Structure and Reaction Mechanism Studies with Multinucleon Reactions
NUCLEAR REACTIONS 192Os(82Se, 84Se), E=460 MeV; measured Eγ, Iγ, γγ-coin. 84Se, 190Os deduced levels, J, π. 192Os(82Se, X)74Ge/76Ge/78Ge/80Ge/82Ge/192Pt/194Pt/196Pt, E=460 MeV; measured Eγ, Iγ, γγ-coin, γ-ray multiplicity. 74,76,78,80,82Ge, 192,194,196Pt deduced levels, J, π. GASP array.
doi: 10.1063/1.2338389
Phys.Rev.C 74, 067303 (2006)
P.M.Walker, F.R.Xu
Shapes of neutron-rich A ≈ 190 odd-odd nuclei
NUCLEAR STRUCTURE 188,190Ta, 190,192Re; calculated total Routhian surfaces, deformation.
doi: 10.1103/PhysRevC.74.067303
IAEA-STI/PUB/1263 (2007)
H.D.Choi, R.B.Firestone, R.M.Lindstrom, G.L.Molnar, S.F.Mughabghab, R.Paviotti Corcuera, Z.Revay, A.Trkov, V.Zerkin, C.Zhou
Database of Prompt Gamma Rays from Slow Neutron Capture for Elemental Analysis
COMPILATION Z=1-92; compiled Eγ, Iγ from neutron capture.
Acta Phys.Pol. B38, 1249 (2007)
M.Ionescu-Bujor, A.Iordachescu, N.Marginean, C.A.Ur, G.Suliman, D.Bucurescu, D.L.Balabanski, F.Brandolini, S.Chmel, K.A.Gladnishki, H.Hubel, R.Marginean, G.Neyens
Quadrupole Moments for Isomeric States with Normal and Intruder Configurations in Neutron-Deficient Pb Nuclei
NUCLEAR REACTIONS 168Er(28Si, 4n)192Pb, 170Er(29Si, 5n)170Er, E not given; measured Eγ, Iγ(θ, E, t). 192,194Pb deduced quadrupole moments of isomeric states using the TDPAD method.
Phys.Lett. B 650, 141 (2007)
M.Ionescu-Bujor, A.Iordachescu, N.Marginean, C.A.Ur, D.Bucurescu, G.Suliman, D.L.Balabanski, F.Brandolini, S.Chmel, P.Detistov, K.A.Gladnishki, H.Hubel, S.Mallion, R.Marginean, N.H.Medina, D.R.Napoli, G.Neyens, P.Pavan, R.V.Ribas, C.Rusu, K.Turzo, N.Vermeulen
Shape coexistence in neutron-deficient Pb nuclei probed by quadrupole moment measurements
NUCLEAR REACTIONS 168Er(28Si, 4n), 170Er(28Si, 5n), E=143 MeV; measured Eγ, Iγ, γγ-coin, time differential perturbed angular distributions, lifetimes. 192Pb, 194Pb deduced levels, J, π, spectroscopic quadrupole moments.
doi: 10.1016/j.physletb.2007.05.002
Phys.Rev. C 76, 044315 (2007); Erratum Phys.Rev. C 78, 069904 (2008)
Y.Oktem, D.L.Balabanski, B.Akkus, C.W.Beausang, M.Bostan, R.B.Cakirli, R.F.Casten, M.Danchev, M.Djongolov, M.N.Erduran, S.Erturk, K.A.Gladniski, G.Gurdal, J.Tm.Goon, D.J.Hartley, A.A.Hecht, R.Krucken, N.Nikolov, J.R.Novak, G.Rainovski, L.L.Riedinger, I.Yigitoglu, N.V.Zamfir, O.Zeidan
High-spin states in 191, 193Au and 192Pt: Evidence for oblate deformation and triaxial shapes
NUCLEAR REACTIONS 186W(11B, 4n), (11B, 4np), (11B, 6n), E=68 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ), linear polarization.191,193Au, 192Pt deduced levels, J, π; calculated deformation parameters using Particle-Plus-Triaxial Rotor model.
doi: 10.1103/PhysRevC.76.044315
Nucl.Instrum.Methods Phys.Res. A589, 202 (2008)
T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr.
Evaluation of theoretical conversion coefficients using BrIcc
COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.
doi: 10.1016/j.nima.2008.02.051
Phys.Rev. C 78, 014320 (2008)
E.A.McCutchan, R.F.Casten, V.Werner, R.Winkler, R.B.Cakirli, G.Gurdal, X.Liang, E.Williams
β decay spectroscopy of 192Pt and the nature of 0+ excitations
RADIOACTIVITY 192Au(β+)(EC); measured Eγ, Iγ, γγ-coin. 192Pt; deduced levels, J, π, B(E2). 172,174,176,178,180,182,184,186,188,190,192,194Pt; systematics. Comparison with model calculations.
doi: 10.1103/PhysRevC.78.014320
University of Surrey (2008)
S.J.Steer
Isomer Decay Spectroscopy of N ≤ 126 Neutron-Rich Nuclei
NUCLEAR REACTIONS 9Be(208Pb, X)195Ir/198Ir/199Ir/200Ir/201Ir/202Ir/203Ir/197Pt/198Pt/199Pt/200Pt/201Pt/202Pt/203Pt/204Pt/201Au/202Au/203Au/204Au/205Au/193Os/195Os/197Os/198Os/199Os/190W/191W/203Hg/204Hg/205Hg/206Hg/191Re/192Re/193Re/194Re/196Re/188Ta/189Ta; measured Eγ, Iγ; Deduced levels, J, π.
Nucl.Phys. A803, 1 (2008)
C.Weber, G.Audi, D.Beck, K.Blaum, G.Bollen, F.Herfurth, A.Kellerbauer, H.-J.Kluge, D.Lunney, S.Schwarz
Atomic mass measurements of short-lived nuclides around the doubly-magic 208Pb
ATOMIC MASSES 145,147Cs, 181,183,186,187,196,205Tl, 197,208Pb, 190,191,192,193,194,195,196,197,209,215,216Bi, 203,205,229Fr, 214,229,230Ra; measured masses using the ISOLTRAP Penning trap mass spectrometer.
doi: 10.1016/j.nuclphysa.2007.12.014
Acta Phys.Pol. B40, 875 (2009)
N.Alkhomashi, P.H.Regan, Zs.Podolyak, S.B.Pietri, A.B.Garnsworthy, S.J.Steer, J.Benlliure, E.Caserejos, M.Gorska, J.Gerl, H.J.Wollersheim, J.Grebosz, N.Kurz, I.Kojouharov, H.Schaffner, A.Algora, G.Benzoni, A.Blazhev, P.Boutachkov, A.M.Bruce, L.Caceres, P.Doornenbal, A.M.D.Bacelar, I.J.Cullen, M.E.Estevez, G.Farrelly, Y.Fujita, W.Gelletly, R.Hoischen, R.Kumar, S.Lalkovski, Z.Liu, C.Mihai, F.Molina, D.Mucher, B.Rubio, A.Tamii, S.Tashenov, J.J.Valiente-Dobon, P.M.Walker, P.J.Woods
β--Delayed and Isomer Spectroscopy of Neutron-Rich Ta and W Isotopes
RADIOACTIVITY 188Ta, 190,191W, 192,193Re, 189Ta(IT), 188Ta(β-); measured Eγ, Iγ, βγ-coin., isomeric states.
Phys.Rev. C 80, 064308 (2009)
N.Alkhomashi, P.H.Regan, Zs.Podolyak, S.Pietri, A.B.Garnsworthy, S.J.Steer, J.Benlliure, E.Caserejos, R.F.Casten, J.Gerl, H.J.Wollersheim, J.Grebosz, G.Farrelly, M.Gorska, I.Kojouharov, H.Schaffner, A.Algora, G.Benzoni, A.Blazhev, P.Boutachkov, A.M.Bruce, A.M.D.Bacelar, I.J.Cullen, L.Caceres, P.Doornenbal, M.E.Estevez, Y.Fujita, W.Gelletly, R.Hoischen, R.Kumar, N.Kurz, S.Lalkovski, Z.Liu, C.Mihai, F.Molina, A.I.Morales, D.Mucher, W.Prokopowicz, B.Rubio, Y.Shi, A.Tamii, S.Tashenov, J.J.Valiente-Dobon, P.M.Walker, P.J.Woods, F.R.Xu
β+-delayed spectroscopy of neutron-rich tantalum nuclei: Shape evolution in neutron-rich tungsten isotopes
NUCLEAR REACTIONS Be(208Pb, X)186Hf/187Hf/188Hf/189Hf/188Ta/189Ta/190Ta/191Ta/192Ta/190W/191W/192W/193W/194W/192Re/193Re/194Re/195Re/196Re, E=1 GeV/nucleon; measured yields. 187Hf, 188,189,190Ta, 190,191W, 192,193Re; measured delayed γ; deduced isomers and half-lives.
RADIOACTIVITY 188,190,192Ta(β-)[from Be(208Pb, X), E=1 GeV/nucleon]; measured Eγ, Iγ, γγ-coin, βγ correlations, and half-lives using GSI Fragment separator, MUSIC ionization chamber; and RISING array. 188,190,192W; deduced levels, J, π, logft. Comparison with interacting boson approximation (IBA-1) calculations for 190W. Z=56-80, N=84-122; discussed systematics of first 2+ and 4+ states, B(E2), and γ deformation parameter in even-even nuclei.
doi: 10.1103/PhysRevC.80.064308
Nucl.Phys. A825, 39 (2009)
J.E.Garcia-Ramos, K.Heyde
The Pt isotopes: Comparing the Interacting Boson Model with configuration mixing and the extended consistent-Q formalism
NUCLEAR STRUCTURE 172,174,176,178,180,182,184,186,188,190,192,194Pt; calculated level energies, B(E2), quadrupole moments and effect of intruder states using interacting boson model. Comparison with previous results and data.
doi: 10.1016/j.nuclphysa.2009.04.003
Acta Phys.Pol. B40, 545 (2009)
I.Mazumdar, D.A.Gothe, G.Anil kumar, M.Aggarwal, P.K.Joshi, R.Palit, H.C.Jain
Search for Rare Shape Transition and GQR Decay in Hot Rotating 188Os Nucleus
NUCLEAR REACTIONS 12C(180Hf, X), E=65 MeV; measured Eγ, Iγ;188Os, 192Pt; deduced giant dipole resonance strength distributions.
Nucl.Phys. A828, 348 (2009)
D.Ni, Z.Ren
α-Decay calculations of medium mass nuclei within generalized density-dependent cluster model
RADIOACTIVITY 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156,158Yb, 156,158,160,162Hf, 158,160,162,164,166,168W, 162,164,166,168,170,172,174,186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190Pt, 172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194Pb, 190,192,194,196,198,200,202,204,206,208,210Po, 196,198,200,202,204,206,208,210,212Rn, 202,204,206,208,210,212Ra, 212,214,216Th, 218U(α); calculated α-decay T1/2 using generalized density-dependent cluster model with double-folded or Woods-Saxon potentials. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.07.014
Phys.Rev. C 79, 014316 (2009)
Y.Z.Wang, H.F.Zhang, J.M.Dong, G.Royer
Branching ratios of α decay to excited states of even-even nuclei
RADIOACTIVITY 180,182,184Hg(α), 186,188Pb(α), 190,194,196,198Po(α), 202Rn(α), 226,228,230,232Th(α), 230,232,234,236U(α), 236,238,240,242Pu(α), 242,244Cm(α), 246Cf(α); calculated branching ratios for decays to ground excited states in the framework of generalized liquid-drop model. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.014316
Phys.Rev. C 79, 014312 (2009)
A.N.Wilson, S.S.Szigeti, P.M.Davidson, J.I.Rogers, D.M.Cardamone
Intensity profiles of superdeformed bands in Pb isotopes in a two-level mixing model
NUCLEAR STRUCTURE 192,194,196Pb; calculated γ decay widths, spins, fractional intensity loss profiles of superdeformed bands. Two-level mixing model. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.014312
J.Phys.:Conf.Ser. 205, 012020 (2010)
D.Bonatsos, I.Boztosun, I.Inci
A long sought result: Closed analytical solutions of the Bohr Hamiltonian with the Morse potential
NUCLEAR STRUCTURE 98,100,102,104Ru, 102,104,106,108,110,112,114,116Pd, 106,108,110,112,114,116,118,120Cd, 118,120,122,124,126,128,130,132,134Xe, 130,132,134,136,142Ba, 134,136,138Ce, 140,148,150Nd, 140,142,152,154Sm, 142,144,152,154,156,158,160,162Gd, 158,160,162,164,166Dy, 156,160,162,164,166,168,170Er, 164,166,168,170,172,174,176,178Yb, 168,170,172,174,176,178,180Hf, 176,178,180,182,184,186W, 178,180,184,186,188Os, 186,188,190,192,194,196,198,200Pt, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242,248Cm, 250Cf; calculated low-lying 0+, 2+, 4+ states, β and γ bandheads, deformation using Bohr Hamiltonian with Morse potential; deduced Morse potential shapes. Compared with data.
doi: 10.1088/1742-6596/205/1/012020
Phys.Rev. C 82, 024303 (2010)
G.Ilie, R.F.Casten, P.von Brentano, D.Bucurescu, T.Faestermann, G.Graw, S.Heinze, R.Hertenberger, J.Jolie, R.Krucken, D.A.Meyer, D.Mucher, C.Scholl, V.Werner, R.Winkler, H.-F.Wirth
Investigation of 0+ states in 192Pt and 194Pt isotopes
NUCLEAR REACTIONS 194,196Pt(p, t), E=25 MeV: measured triton spectra, σ(θ). 192,194Pt; deduced levels, L-transfers, J, π. DWBA analysis of σ(θ) data. Systematics of low-lying states of even-even Pt nuclei from A=170-202, and 0+ states in 152,154,158Gd, 162Dy, 168Er, 170Yb, 176Hf, 180,184W, 190Os, 192,194Pt.
doi: 10.1103/PhysRevC.82.024303
Eur.Phys.J. A 45, 153 (2010)
M.Kmiecik, A.Maj, J.Gerl, G.Neyens, L.Atanasova, D.L.Balabanski, F.Becker, P.Bednarczyk, G.Benzoni, N.Blasi, A.Bracco, S.Brambilla, L.Caceres, F.Camera, M.Ciemala, F.C.L.Crespi, S.K.Chamoli, S.Chmel, J.M.Daugas, P.Detistov, P.Doornenbal, G.Georgiev, K.Gladnishki, M.Gorska, H.Grawe, J.Grebosz, M.Hass, R.Hoischen, G.Ilie, M.Ionescu-Bujor, J.Jolie, I.Kojuharov, A.Krasznahorkay, R.Kulessa, M.Lach, S.Lakshmi, S.Leoni, G.Lo Bianco, R.Lozeva, K.H.Maier, S.Mallion, K.Mazurek, W.Meczynski, B.Million, D.Montanari, S.Myalski, C.Petrache, M.Pfutzner, S.Pietri, Zs.Podolyak, W.Prokopowicz, D.Rudolph, N.Saito, T.R.Saito, A.Saltarelli, G.S.Simpson, J.Styczen, N.Vermeulen, E.Werner-Malento, O.Wieland, H.J.Wollersheim, M.Zieblinski
Spin-alignment and g-factor measurement of the Iπ = 12+ isomer in 192Pb produced in the relativistic-energy fragmentation of a 238U beam
doi: 10.1140/epja/i2010-11003-4
J.Phys.:Conf.Ser. 205, 012005 (2010)
H.Laftchiev, J.Libert, P.Quentin, T.L.Ha
Higher Tamm-Dankoff approximation for rotational nuclear states
NUCLEAR STRUCTURE 192,194Pb; calculated moments of inertia, pairing strength using Cr.HTDA (Cranking version of Higher Tamm-Dankoff approximation). Compared with data.
doi: 10.1088/1742-6596/205/1/012005
Phys.Rev. C 82, 064605 (2010)
K.P.Santhosh, J.G.Joseph, S.Sahadevan
α decay of nuclei in the range 67≤Z≤91 from the ground state and isomeric state
RADIOACTIVITY 151,152,153,154Ho, 153,154,155Tm, 155,156,157Lu, 156Hf, 157,158,159,160,161Ta, 158W, 161,162,163,164,165Re, 165,166,167,169,171,174Ir, 172Pt, 170,171,173,175,176,177Au, 176,177,187Hg, 177,179,181,183,185Tl, 179,180,181,183,185,187Pb, 186,187,188,189,190,191,192,193,194,195,196Bi, 187,188,192,193,195,197,199,201Po, 191,192,193,194,195,197,198,200,202,212,214At, 195,197,199,201,203Rn, 201,202,203,204,206Fr, 201,203,205,207Ra, 206,208,216Ac, 216Th, 217Pa(α), 245Md, 257Db, 263Sg; calculated half-lives for favored and unfavored transitions for ground states and isomers using Coulomb and proximity potential model for deformed nuclei (CPPMDN). Comparison with experimental data.
doi: 10.1103/PhysRevC.82.064605
Nucl.Phys. A847, 42 (2010)
K.P.Santhosh, S.Sahadevan
Systematic decay studies of even-even 132-138Nd, 144-158Gd, 176-196Hg and 192-198Pb isotopes
RADIOACTIVITY 132,134,136,138Nd, 144,146,148,150,152,154,156,158Gd, 176,178,180,182,184,186,188,190,192,194,196Hg, 192,194,196,198Pb(α); analyzed T1/2 using Coulomb and Proximity Potential Model. 132,134,136,138Nd(8Be), (12C), (14C), (16O), (18O), (20O), (20Ne), (22Ne), (24Ne), (24Mg), (26Mg), (28Mg), (28Si), (30Si), (32Si), (34Si), (34S), (36S); 144,146,148,150,152,154,156,158Gd(8Be), (12C), (14C), (16C), (16O), (18O), (22O), (26O), (22Ne), (24Ne), (26Ne), (24Mg), (26Mg), (28Mg), (30Mg), (30Si), (32Si), (34Si), (36Si), (34S), (36S); 176,178,180,182,184,186,188,190,192,194,196Hg(8Be), (12C), (14C), (16O), (18O), (20O), (20Ne), (22Ne), (24Ne), (24Mg), (26Mg), (28Mg), (30Mg), (28Si), (30Si), (32Si), (34Si), (34S), (36S); 192,194,196,198Pb(8Be), (12C), (14C), (16O), (18O), (20O), (22Ne), (24Ne), (26Mg), (28Mg), (30Mg), (30Si), (32Si), (34Si), (36S); calculated cluster decay T1/2 systematics and effect of deformation using Coulomb and Proximity Potential Model.
doi: 10.1016/j.nuclphysa.2010.07.001
J.Phys.:Conf.Ser. 205, 012024 (2010)
P.Sarriguren, R.R.Rodriguez-Guzman, L.M.Robledo
Microscopic description of shape evolution in medium-mass nuclei
NUCLEAR STRUCTURE 130Xe, 144,146,148,150,152,154,156,158Sm, 184,186,188,190,192,194,196W; calculated quadrupole moment, deformation including tri-axial degrees of freedom, potential energy surface, evolution of ground-state nuclear shapes. 190W; calculated single-particle levels. Self-consistent HFB with Gogny and Skyrme density-dependent interactions.
doi: 10.1088/1742-6596/205/1/012024
Eur.Phys.J. A 43, 145 (2010)
A.N.Wilson, M.C.East, G.D.Dracoulis, A.P.Byrne, R.M.Clark, P.M.Davidson, P.Fallon, A.Gorgen, G.J.Lane, A.O.Macchiavelli, D.Ward
On the character of three 8+ states in 192Pb
NUCLEAR REACTIONS 168Er(29Si, 5n), E=154 MeV; measured Eγ, Iγ, γγ-coin using Gammasphere HPGe detector array. 192Pb; deduced levels, J, π, multipolarities, deformation, configurations. Time-correlated spectroscopy, DCO analysis. Comparison with systematics.
doi: 10.1140/epja/i2010-10905-3
Priv.Comm. (2011)
G.Audi, W.Meng
Atomic Mass Evaluation 2011
Phys.Rev. C 83, 034603 (2011)
P.Belli, R.Bernabei, F.Cappella, R.Cerulli, F.A.Danevich, A.Incicchitti, M.Laubenstein, S.S.Nagorny, S.Nisi, O.G.Polischuk, V.I.Tretyak
First observation of α decay of 190Pt to the first excited level (Eexc = 137.2 keV) of 186Os
RADIOACTIVITY 190Pt(α); measured Eγ, Iγ; deduced α-decay branching ratio to the excited states in 186Os, α-decay half-life. 192,194,195,196,198Pt(α); measured Eγ, Iγ, half-life limits for α decay to the excited states. Comparison of half-lives with the cluster model calculations.
doi: 10.1103/PhysRevC.83.034603
Phys.Rev.Lett. 106, 052503 (2011)
T.E.Cocolios, W.Dexters, M.D.Seliverstov, A.N.Andreyev, S.Antalic, A.E.Barzakh, B.Bastin, J.Buscher, I.G.Darby, D.V.Fedorov, V.N.Fedosseyev, K.T.Flanagan, S.Franchoo, S.Fritzsche, G.Huber, M.Huyse, M.Keupers, U.Koster, Yu.Kudryavtsev, E.Mane, B.A.Marsh, P.L.Molkanov, R.D.Page, A.M.Sjoedin, I.Stefan, J.Van de Walle, P.Van Duppen, M.Venhart, S.G.Zemlyanoy, M.Bender, P.-H.Heenen
Early Onset of Ground State Deformation in Neutron Deficient Polonium Isotopes
NUCLEAR REACTIONS U(p, X)192Po/194Po/196Po/198Po/200Po/202Po/204Po/206Po/208Po/210Po/216Po/218Po, E=1.4 GeV; measured reaction products, Ee, Ie, Eα, Iα; deduced isotope shifts, mean-square charge radii. Comparison with systematics and FRDM calculations.
doi: 10.1103/PhysRevLett.106.052503
Acta Phys.Pol. B42, 643 (2011)
I.Mazumdar, D.A.Gothe, G.Anil Kumar, M.Aggarwal
Shape Transition and Isovector Giant Quadrupole Resonance Decay in Hot Rotating Nuclei
NUCLEAR REACTIONS 180Hf(12C, X)192Pt/188Os, E=65 MeV; measured Eγ, Iγ; deduced deformed non-spherical shape, excess yield of high-energy γ-rays, possible first observation of the Isovector Giant Quadrupole Resonance (IVGQR) on excited state.
Int.J.Mod.Phys. E20, 459 (2011)
T.Niksic, D.Vretenar, P.Ring
Beyond the relativistic mean-field approximation: configuration mixing calculations
NUCLEAR STRUCTURE 190,192,194,196,198,200Pt; calculated triaxial quadrupole binding-energy maps, proton canonical single-particle energy levels, low-energy spectra, J, π. Comparison with experimental data.
doi: 10.1142/S0218301311017855
Phys.Rev. C 83, 014309 (2011)
K.Nomura, T.Otsuka, R.Rodriguez-Guzman, L.M.Robledo, P.Sarriguren
Structural evolution in Pt isotopes with the interacting boson model Hamiltonian derived from the Gogny energy density functional
NUCLEAR STRUCTURE 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200Pt; calculated potential energy surfaces in the β-γ plane, low-lying spectra of g.s., quasi β and quasi γ bands, B(E2) values, Level schemes for 184,186,188,190,192,194Pt nuclei. Interacting boson model (IBM) Hamiltonian from constrained Hartree-Fock-Bogoliubov (HFB) calculations with the finite range and density-dependent Gogny-D1S energy density functional. Shape transition in Pt nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014309
Phys.Rev. C 84, 054316 (2011)
K.Nomura, T.Otsuka, R.Rodriguez-Guzmin, L.M.Robledo, P.Sarriguren
Collective structural evolution in neutron-rich Yb, Hf, W, Os, and Pt isotopes
NUCLEAR STRUCTURE 180,182,184,186,188,190,192Yb, 182,184,186,188,190,192,194Hf, 184,186,188,190,192,194,196W, 186,188,190,192,194,196,198Os, 188,190,192,194,196,198,200Pt; calculated potential energy surfaces, ground-state correlation energies, moments of inertia, low-lying levels, J, π, B(E2) ratios. Interacting-boson-model (IBM) Hamiltonian from constrained Hartree-Fock-Bogoliubov calculations with the Gogny-DIM energy density functional. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.054316
Acta Phys.Pol. B42, 629 (2011)
C.Parascandolo, D.Pierroutsakou, R.Silvestri, C.Agodi, R.Alba, V.Baran, A.Boiano, M.Colonna, R.Coniglione, E.De Filippo, A.Del Zoppo, M.Di Toro, U.Emanuele, F.Farinon, A.Guglielmetti, G.Inglima, M.La Commara, C.Maiolino, B.Martin, M.Mazzocco, C.Mazzocchi, P.Molini, C.Rizzo, M.Romoli, M.Sandoli, D.Santonocito, C.Signorini, F.Soramel, A.Trifiro, M.Trimarchi
Investigation of the Dynamical Dipole Mode in the 192Pb Mass Region
NUCLEAR REACTIONS 152Sm(40Ca, X)192Pb, E=11 MeV/nucleon; 144Sm(48Ca, X)192Pb, E=10.1 MeV/nucleon; measured Eγ, Iγ; deduced γ-spectra difference for fusion-evaporation and fission events.
Phys.Rev. C 84, 064307 (2011)
Y.Qian, Z.Ren
Systematic study of new data for extreme α decays
RADIOACTIVITY 109I, 112,113Cs, 142Ce, 146,147,148,149Sm, 151Eu, 152Gd, 156Dy, 162,164Er, 168Yb, 174,176Hf, 180W, 159Re, 161,184,188Os, 167,169Ir, 172,190,192Pt, 172,175,177Au, 176,196Hg, 179,181Tl, 179,180,181,204Pb, 187Bi, 187Po, 238U, 244Pu, 233,236Cm, 237Cf, 249Md, 253Lr, 257Db, 260,265,267,282Sg, 261,262,274Bh, 263,265Hs, 278Mt, 281Ds, 285Cn, 285,286Nh, 288,289Fl, 289,290Mc, 293,294Ts(α); calculated half-lives using Modified two-potential approach (MTPA) for deformed nuclei associated with the density-dependent cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064307
Phys.Rev. C 83, 034313 (2011)
A.A.Raduta, P.Buganu
Toward a new description of triaxial nuclei
NUCLEAR STRUCTURE 188,190,192Os, 228,230Th; calculated levels, J, π, B(E2), level staggering in ground, β and γ bands using liquid drop Hamiltonian. Transition from γ unstable to triaxial shape. Signature for triaxiality. Sextic and Mathieu approach (SMA), and Coherent state model (CSM). Comparison with experimental data.
doi: 10.1103/PhysRevC.83.034313
Nucl.Phys. A850, 34 (2011)
K.P.Santhosh, S.Sahadevan, J.G.Joseph
Alpha decay of even-even nuclei in the region 78 ≤ Z ≤ 102 to the ground state and excited states of daughter nuclei
NUCLEAR STRUCTURE Z=78-102; calculated α-decay T1/2, branching ratios. Coulomb and proximity potential model for deformed nuclei, comparison with experimental data.
doi: 10.1016/j.nuclphysa.2010.12.002
Phys.Rev. C 84, 044313 (2011)
S.J.Steer, Zs.Podolyak, S.Pietri, M.Gorska, H.Grawe, K.H.Maier, P.H.Regan, D.Rudolph, A.B.Garnsworthy, R.Hoischen, J.Gerl, H.J.Wollersheim, F.Becker, P.Bednarczyk, L.Caceres, P.Doornenbal, H.Geissel, J.Grebosz, A.Kelic, I.Kojouharov, N.Kurz, F.Montes, W.Prokopwicz, T.Saito, H.Schaffner, S.Tashenov, A.Heinz, M.Pfutzner, T.Kurtukian-Nieto, G.Benzoni, A.Jungclaus, D.L.Balabanski, M.Bowry, C.Brandau, A.Brown, A.M.Bruce, W.N.Catford, I.J.Cullen, Zs.Dombradi, M.E.Estevez, W.Gelletly, G.Ilie, J.Jolie, G.A.Jones, M.Kmiecik, F.G.Kondev, R.Krucken, S.Lalkovski, Z.Liu, A.Maj, S.Myalski, S.Schwertel, T.Shizuma, P.M.Walker, E.Werner-Malento, O.Wieland
Isomeric states observed in heavy neutron-rich nuclei populated in the fragmentation of a 208Pb beam
NUCLEAR REACTIONS 9Be(208Pb, X)183Hf/184Hf/185Hf/186Hf/187Hf/188Hf/186Ta/187Ta/188Ta/189Ta/190Ta/189W/190W/191W/192W/193W/194W/192Re/193Re/194Re/195Re/196Re/197Re/195Os/196Os/197Os/198Os/199Os/200Os/197Ir/198Ir/199Ir/200Ir/201Ir/202Ir/203Ir/200Pt/201Pt/202Pt/203Pt/204Pt/204Au/205Au, E=1 GeV/nucleon; measured magnetic rigidity, energy loss, time of flight, Eγ, Iγ, isomeric half-lives and ratios. FRS at GSI facility. 206Tl, 203,204,205,206Hg, 201,202,203,204,205Au, 197,198,199,200,201,202,203,204Pt, 195,198,199,200,201,202,203Ir, 193,195,197,198,199Os, 191,192,193,194,196Re, 190,191W, 188,189Ta; deduced levels, isomers, J, π, half-lives, B(E2), B(M2), B(E3), B(M4). Comparison with shell-model and BCS calculations.
doi: 10.1103/PhysRevC.84.044313
INDC(NDS)-0594 (2011)
N.J.Stone
Table of nuclear magnetic dipole and electric quadrupole moments
COMPILATION Z=1-99, N=1-254; compiled experimental data on nuclear magnetic and electrical quadrupole moments.
Phys.Rev. C 85, 034301 (2012); Pub.Note Phys.Rev. C 85, 039904 (2012)
N.Al-Dahan, P.H.Regan, Zs.Podolyak, P.M.Walker, N.Alkhomashi, G.D.Dracoulis, G.Farrelly, J.Benlliure, S.B.Pietri, R.F.Casten, P.D.Stevenson, W.Gelletly, S.J.Steer, A.B.Garnsworthy, E.Casarejos, J.Gerl, H.J.Wollersheim, J.Grebosz, M.Gorska, I.Kojouharov, H.Schaffner, A.Algora, G.Benzoni, A.Blazhev, P.Boutachkov, A.M.Bruce, I.J.Cullen, A.M.D.Bacelar, A.Y.Deo, M.E.Estevez, Y.Fujita, R.Hoischen, R.Kumar, S.Lalkovski, Z.Liu, P.J.Mason, C.Mihai, F.Molina, D.Mucher, B.Rubio, A.Tamii, S.Tashenov, J.J.Valiente-Dobon, P.J.Woods
Multiple Β- decaying states in 194Re: Shape evolution in neutron-rich osmium isotopes
NUCLEAR REACTIONS 9Be(208Pb, X)186Hf/187Hf/188Hf/189Hf/188Ta/189Ta/190Ta/191Ta/190W/191W/192W/193W/192Re/193Re/194Re/195Re/196Re/195Os/196Os/197Os/198Os, E=1 GeV/nucleon; measured fragment yields, ion identification by energy loss and time-of-flight methods; deduced decay properties. GSI FRagment Separator (FRS), RISING spectrometer.
RADIOACTIVITY 192,194Re[from 9Be(208Pb, X), E=1 GeV/nucleon](β-); 194Os[from 194Re decay](α); measured Eγ, Iγ, βγ-, (implants)γ-coin, recoil-decay tagging method, half-life. 194Os; deduced levels, J, π. 187Hf, 188,189,190Ta, 190,191W, 192,193Re(IT); measured Eγ, Iγ, half-lives. GSI FRagment Separator (FRS), RISING spectrometer. Systematics of low-lying 0+, 2+, 4+ and 6+ states in N=110-122 Os and W nuclei.
NUCLEAR STRUCTURE 194Re; calculated levels, J, π, configurations using Nilsson multi-quasiparticle (MQP) model.
doi: 10.1103/PhysRevC.85.034301
Thesis, University of Surrey (2012)
M.W.Reed
Exploring Long-lived Exotic Isomers in Deformed Atomic Nuclei with Schottky Mass Spectrometry at the GSI Storage Ring
NUCLEAR REACTIONS 9Be(197Au, X), E=478-492 MeV/nucleon; measured Shottkey mass spectra using Experimental Storage Ring (ESR) and Fragment Separator (FRS) at GSI. 183,184,186Hf, 185,186,187,188Ta, 185,186W, 191,192,194Re, 195Os, 195Ir; deduced isomers, half-lives, level energies, multi-quasiparticle structures.