References quoted in the ENSDF dataset: 135 REFERENCES
468 references found.
Clicking on a keynumber will list datasets that reference the given article.
Sci.Papers, Inst.Phys.Chem.Res.(Tokyo) 18, 304 (1932)
K.Murakawa
Phys.Rev. 52, 1127 (1937)
A.N.Benson, R.A.Sawyer
The Nuclear Moment of Barium
Phys.Rev. 57, 966 (1940)
R.W.Dodson, R.D.Fowler
Products of the Uranium Fission. Radioactive Isotopes of Iodine and Xenon
Naturwissenschaften 28, 449 (1940)
H.Gotte
Eine bei der Uransplatung Auftretende Kernisomerie bei Xenon
Phys.Rev. 58, 926 (1940)
C.S.Wu
Identification of Two Radioactive Xenon from Uranium Fission
Phys.Rev. 60, 87 (1941)
E.P.Clancy
The Induced Radioactivity of Krypton and Xenon
Phys.Rev. 60, 75 (1941)
R.H.Hay
The Nuclear Magnetic Moments of C13, Ba135 and Ba137
Naturwissenschaften 31, 326 (1943)
W.Riezler
Aktivierung von Xenon durch Neutronen
Phys.Rev. 63, 67 (1943)
K.E.Weimer, M.L.Pool, J.D.Kurbatov
Radioactive Isotopes of Lanthanum
Phys.Rev. 67, 142 (1945)
C.Wu, E.Segre
Radioactive Xenons
Helv.Phys.Acta 19, 375 (1946)
E.Bleuler, W.Zunti
Zur Absorptionsmethode der Bestimmung von β- und γ-Energien
Phys.Rev. 74, 982 (1948)
J.B.Chubbuck, I.Perlman
Neutron Deficient Isotopes of Cerium and Lanthanum
Phys.Rev. 74, 34 (1948)
F.-C.Yu, J.D.Kurbatov
Energy Quanta Emitted in Disintegration of Ground State of Ba133
Phys.Rev. 76, 1068 (1949)
L.Davis, Jr., D.E.Nagle, J.R.Zacharias
Atomic Beam Magnetic Resonance Experiments with Radioactive Elements Na22, K40, Cs135, and Cs137
Phys.Rev. 76, 1408 (1949)
B.E.Robertson, M.L.Pool
28.7 h Ba-135
Phys.Rev. 75, 1473 (1949)
N.Sugarman
Characteristics of the Fission Product Cs135
Phys.Rev. 76, 871 (1949)
S.Thulin, I.Bergstrom, A.Hedgran
Mass Assignment of Xenon Activities Produced in Fission
Phys.Rev. 79, 836 (1950)
O.H.Arroe
Hyperfine Structure and Isotope Shift in Barium
NNES 9, paper 140 p.992 (1950), Radiochemical Studies: The Fission Products, Book 2, Part V, McGraw-Hill, p.992 (1951)
L.E.Glendenin, R.P.Metcalf
Characteristics of 6.7h I135 (I)
NNES 9, paper 146 p.1031 (1950), Radiochemical Studies: The Fission Products, Book 2, Part V, McGraw-Hill, p.1031 (1951)
E.J.Hoagland, N.Sugarman
Characteristics of 9.3h Xe135 (II)
NNES 9, paper 141 p.1005 (1950), Radiochemical Studies: The Fission Products, Book 2, Part V, McGraw-Hill, p.1005 (1951)
S.Katcoff, C.R.Dillard, H.Finston, B.Finkle, J.A.Seiler, N.Sugarman
Characteristics of 6.7h I135 (II)
Phys.Rev. 77, 398 (1950)
R.A.Naumann, F.L.Reynolds, I.Perlman
Mass Spectrographic Identification of Radioactive Lanthanum Isotopes
NNES 9, paper 145 p.1028 (1950), Radiochemical Studies: The Fission Products, Book 2, Part V, McGraw-Hill, p.1028 (1951)
A.S.Newton, W.H.Sullivan, O.Johnson, R.Nottorf
Characteristics of 9.2h Xe135 (I)
NNES 9, paper 148 p.1043 (1950), Radiochemical Studies: The Fission Products, Book 2, Part V, McGraw-Hill, p.1043 (1951)
T.B.Novey, J.D.Knight
Half-Life and Radiations of 13m Xe135m
NNES 9, paper 139 p.984 (1950), Radiochemical Studies: The Fission Products, Book 2, Part V. McGraw-Hill, p.984 (1951)
W.H.Sullivan, O.Johnson, R.Nottorf
Characteristics of Some Iodine Isotopes Produced in Fission
ORNL-286, p.48 (1950)
H.Zeldes, A.R.Brosi, G.W.Parker, G.M.Hebert, G.E.Creek
Characterization of Cs135
Phys.Rev. 83, 654 (1951)
W.H.Cuffey, R.Canada
The Energy of the Metastable State of Ba135
Phys.Rev. 83, 455 (1951)
R.D.Hill, F.R.Metzger
Nuclear Isomers of Ba133 and Ba135
Phys.Rev. 81, 8 (1951)
B.J.Stover
New Neutron Deficient Radioactive Isotopes of the Light Rare-Earth Region
doi: 10.1103/PhysRev.81.8
Arkiv Fysik 5, 191 (1952)
I.Bergstrom
The Isomers of Krypton and Xenon
Can.J.Chem. 31, 242 (1953)
F.Brown, L.Yaffe
The Independent Yield of Xe135 Produced in the Fission of Natural Uranium by Pile Neutrons
doi: 10.1139/v53-035
Can.J.Phys. 31, 377 (1953)
R.L.Graham, R.E.Bell
A Determination of the Half-Lives of Some Magnetic Dipole γ-Ray Transitions
doi: 10.1139/p53-037
Phys.Rev. 90, 387A (1953)
P.Lidofsky, E.Alperovitch, C.S.Wu
The Beta Spectrum of Cs135
Thesis, University of Oslo (1953); MIT Technical Report 63; AECU-2806 (1953)
A.C.Pappas
A Radiochemical Study of Fission Yields in the Region of Shell Perturbations and the Effect of Closed Shells in Fission
Physica 19, 671 (1953)
A.H.Wapstra
The Competition between d5/2 and g7/2 Levels in Sb, I, Cs, and La; The Decay of 135La
Phys.Rev. 96, 1003 (1954)
T.H.Handley, E.L.Olson
Neutron-Deficient Activities of Praseodymium
Proc.U.N.Intern.Conf.Peaceful Uses Atomic Energy, Geneva 14, 96 (1955)
G.W.Parker, W.J.Martin, G.E.Creek, P.M.Lantz
Preparation of Kilocurie Quantities of Xenon-135
Arkiv Fysik 9, 137 (1955)
S.Thulin
Studies in Nuclear Spectroscopy with Electromagnetically Separated Gaseous Isotopes II - Disintegration of Some Krypton and Xenon Isotopes
Phys.Rev. 99, 730 (1955)
A.C.Wahl
Fission of U235 by 14-MeV Neutrons: Nuclear Charge Distribution and Yield Fine Structure
Phys.Rev. 102, 1334 (1956)
H.E.Walchli, T.J.Rowland
Nuclear Magnetic Resonance Measurements of the Isotopes Barium-135 and Barium-137
Phys.Rev. 105, 590 (1957)
H.H.Stroke, V.Jaccarino, D.S.Edmonds, Jr., R.Weiss
Magnetic Moments and Hyperfine-Structure Anomalies of Cs133, Cs134, Cs135 and Cs137
Proc.U.N.Intern.Conf.Peaceful Uses At.Energy, 2nd, Geneva 14, 193 (1958)
N.Antonyeva, A.Bashilov, G.Gorodinsky, E.Grigoryev, K.Gromov, B.Dzhelepov, A.Zolotavin, O.Kraft, L.Krizhansky, A.Murin, L.Peker, V.Pokrovsky, B.Preobrazhensky, I.Rogachev, V.Sergienko, P.Tishkin, V.Yakovlev
Research in Neutron-Deficient Isotopes of Rare Earths
Can.J.Phys. 36, 1487 (1958)
G.T.Danby, J.S.Foster, A.L.Thompson
Successive Decays from Pr137 and Ce137m: Decay of Adjacent Praseodymium Isotopes
doi: 10.1139/p58-150
Izvest.Akad.Nauk SSSR, Ser.Fiz. 22, 931 (1958); Columbia Tech. Transl. 22, 923 (1959)
B.S.Dzhelepov, B.K.Preobrazhenskii, I.M.Rogachev, P.A.Tishkin
Conversion Electron Spectrum of the Cerium Fraction from the Spallation Product of Ta
Phys.Rev. 109, 100 (1958)
L.W.Fagg
Coulomb Excitation of Sb, Cs and Ba
Phys.Rev. 111, 1343 (1958)
A.C.G.Mitchell, C.B.Creager, C.W.Kocher
Disintegration of La135 and Confirmatory Experiments on Nd147
Ann.Physik 4, 39 (1959)
H.Bucka, H.Kopfermann, E.W.Otten
Bestimmung der Kernquadrupolmomente der radioaktiven Isotopes Cs135 und Cs137
JINR-P-483, Pt.3, p.40 (1959)
E.P.Grigorev, O.V.Larionov, M.K.Nikitin, S.L.Sakharov, V.O.Sergeev
Gamma Spectra of the Lanthanum and the Cerium Fraction
Zh.Eksp.Teor.Fiz. 37, 582 (1959); Soviet Phys.JETP 10, 412 (1960)
A.G.Kucheryaev, Y.K.Szhenov, S.M.Gogichaishvili
Measurements of Nuclear Magnetic Moments in the Alkali Earths by Molecular Beam Magnetic Resonance
Arkiv Fysik 17, 521 (1960)
T.Alvager
The Empirical Matrix Element of the M4 Transition in Xe135
NUCLEAR STRUCTURE 135Xe; measured not abstracted; deduced nuclear properties.
Z.Naturforsch. 15a, 593 (1960)
J.Janecke
The Half Lives of Some Positron Emitters with Superpermitted Transitions
NUCLEAR STRUCTURE 17F, 19Ne, 29P, 35Ar, 31S, 34Cl, 33Cl, 42Sc, 41Sc, 38K, 43Ti, 15O, 13N, 26Al, 25Al, 8Li; measured not abstracted; deduced nuclear properties.
Zhu.Eksp.Teor.Fiz. 39, 954 (1960); Soviet Phys.JETP 12, 661 (1961)
N.I.Kaliteevskii, E.E.Fradkin, M.P.Chaika
Quadrupole Moments of Odd Barium Isotopes
NUCLEAR STRUCTURE 137Ba, 135Ba; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 16, 231 (1960)
K.Kotajima, H.Morinaga
Isomerism in N = 81 Nuclei
NUCLEAR STRUCTURE 141Nd, 143Sm, 139Ce, 135Xe; measured not abstracted; deduced nuclear properties.
Izvest.Akad.Nauk SSSR, Ser.Fiz. 24, 1113 (1960); Columbia Tech.Transl. 24, 1117 (1961)
A.K.Lavrukhina, G.M.Kolesov, Tan Syao-en
Neutron-Deficient Cerium Isotopes. (Products of Europium Spallation by 660-MeV Protons)
NUCLEAR STRUCTURE 134Pr; measured not abstracted; deduced nuclear properties.
Phys.Rev. 118, 242 (1960)
R.G.Wille, R.W.Fink
Activation Cross Sections for 14.8 MeV Neutrons and Some New Radioactive Nuclides in the Rare Earth Region
NUCLEAR STRUCTURE 169Er, 168Ho, 167Ho, 167Dy, 165Dy, 165Er, 163Tb, 174Lu, 173Er, 174Tm, 176Lu, 175Yb, 176Tm, 177Yb, 152Pm, 152Eu, 153Sm, 154Pm, 150Eu, 151Nd, 149Nd, 157Sm, 159Gd, 161Gd, 133Ba, 136Cs, 140La, 140Pr, 139Ba, 139Ce, 141Ce, 135Ba, 138Cs, 137Ba, 147Nd, 145Ce, 143Sm, 148Pr, 142La, 141Nd, 142Pr, 143Ce; measured not abstracted; deduced nuclear properties.
Opt.Spektrosk 12, 163 (1962); Opt.Spectry.USSR (English Transl.) 12, 87 (1962)
V.S.Korolkov, A.G.Makhanek
Gradients of Electric Fields Set up by Electrons at the Sites of Atomic Nuclei
NUCLEAR STRUCTURE 17O, 181Ta, 175Lu, 27Al, 85Rb, 79Br, 79Se, 90Y, 93Nb, 90Zr, 69Ga, 73Ge, 75As, 113In, 23Na, 121Sb, 127I, 139La, 135Ba, 189Os, 11B, 199Hg, 33S, 35Cl, 39K, 51V, 63Cu, Cr, Ti, Ca, Al, Mg, Mn, F, Ne, Na, Si, C, Sc, N, K, P, Bi, Pb, Co, La, Fe, Cu, Te, Ag, Sn, Ni, Cs, Zr, Zn, Mo, Gd; measured not abstracted; deduced nuclear properties.
Nuclear Phys. 33, 639 (1962)
H.Warhanek
A 53 min Isomer of Caesium 135
NUCLEAR STRUCTURE 135Cs; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90555-2
Phys.Rev. 127, 184 (1962)
R.M.Williams, J.W.McGrath
Ratio of the Electric Quadrupole Moments of Ba137 and Ba135
NUCLEAR STRUCTURE 135Ba, 137Ba; measured not abstracted; deduced nuclear properties.
Izv.Akad.Nauk SSSR, Ser.Fiz. 27, 1363 (1963);Bull.Acad.Sci.USSR, Phys.Ser. 27, 1339 (1964)
D.G.Alkhazov, K.I.Erokhina, I.K.Lemberg
Coulomb Excitation of Levels in Odd Nuclei with A = 135 to 173
NUCLEAR STRUCTURE 173Yb, 149Sm, 157Gd, 141Pr, 135Ba, 139La, 147Sm, 143Nd, 145Nd; measured not abstracted; deduced nuclear properties.
ORNL-3488, p.1 (1963)
A.R.Brosi, B.H.Ketelle
Isomeric Transitions in Ce135 and Ba131
NUCLEAR STRUCTURE 131Ba, 135Ce; measured not abstracted; deduced nuclear properties.
Izv.Akad.Nauk SSSR, Ser.Fiz. 27, 204 (1963); Bull.Acad.Sci.USSR, Phys.Ser. 27, 214 (1964)
B.S.Dzhelepov, A.I.Medvedev, I.F.Uchevatkin, S.A.Shestopalova
Conversion Electron Spectrum of the Cerium Fraction from Proton Bombarded Tantalum
NUCLEAR STRUCTURE 137Ce, 135Ce, 134La; measured not abstracted; deduced nuclear properties.
Phys.Rev.Lett. 11, 209 (1963)
D.A.Jackson, D.H.Tuan
Hyperfine Structure of the Resonance Line of the Arc Spectra of the Isotopes 135 and 137 of Barium
NUCLEAR STRUCTURE 137Ba, 135Ba; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.11.209
J.Phys.Soc.Jpn. 18, 183 (1963)
S.Nakamura, H.Enokiya
Detection of Nuclear Quadrupole Resonances by Means of the Crossing Technique
NUCLEAR STRUCTURE 137Ba, 135Ba; measured not abstracted; deduced nuclear properties.
Ann.Physik 11, 248 (1963)
G.zu Putlitz
Bestimmung der Elektrischen Kernquadrupolmomente der Beiden Ungeraden Stabilen Bariumisotope Ba135 und Ba137
NUCLEAR STRUCTURE 137Ba, 135Ba; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 26, 213 (1964)
C.E.Bemis, G.E.Gordon, C.D.Coryell
Half-Life of Sb135 and Evidence on the Half-Life of Sb134
NUCLEAR STRUCTURE 135Sb, 134Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(64)80060-9
Can. J. Phys. 42, 213 (1964)
W.B.Clarke, H.G.Thode
Mass Spectrometric Measurements of the Half-Lives of Kr87, Kr88, Xe135, Xe138
NUCLEAR STRUCTURE 135Xe, 138Xe, 88Kr, 87Kr; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 52, 524 (1964)
I.B.Haller, B.Jung
Spin-Parity of 53 min Cs135m
NUCLEAR STRUCTURE 135Cs; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90713-8
Proc.Roy.Soc.(London) 280A, 323 (1964)
D.A.Jackson, D.H.Tuan
Hyperfine Structures of the Resonance Line of the Arc Spectra and Nuclear Quadrupole Moments of the Isotopes 135 and 137 of Barium
NUCLEAR STRUCTURE 135Ba, 137Ba; measured not abstracted; deduced nuclear properties.
J.Phys.Soc.Japan 19, 2014 (1964)
K.Takahashi, M.Fujioka, K.Hisatake
Decay of Ce135
NUCLEAR STRUCTURE 135Ce; measured not abstracted; deduced nuclear properties.
Ark.Fys. 28, 37 (1965)
G.Andersson, G.Rudstam, G.Sorensen
Decay Data on Some Xe, I, and Te Isotopes
NUCLEAR STRUCTURE 135Xe, 138Xe, 117I, 118Xe, 118Te, 118I, 121I, 121Xe, 120Xe, 120I, 119Xe, 119I, 124I, 127Te, 126I, 125Xe, 125Te, 125I, 123Xe, 123I, 123Te, 122Xe, 134I, 131Xe, 132I, 133I, 132Te, 129Xe, 129Te, 130I; measured not abstracted; deduced nuclear properties.
Izv.Akad.Nauk SSSR, Ser.Fiz. 29, 2205 (1965); Bull.Acad.Sci.USSR, Phys.Ser. 29, 2042 (1966)
V.A.Balalaev, B.S.Dzhelepov, A.I.Medvedev, I.F.Uchevatkin, S.A.Shestopalova
New Data on the Decay of Ce135
NUCLEAR STRUCTURE 135Ce; measured not abstracted; deduced nuclear properties.
Izv.Akad.Nauk SSSR, Ser.Fiz. 29, 2264 (1965); Bull.Acad.Sci.USSR, Phys.Ser. 29, 2103 (1966)
B.S.Dzhelepov, L.N.Moskvin, P.A.Tishkin, I.F.Uchevatkin, I.A.Shishelov
Conversion Electron Coincidences in Ce135 Decay
NUCLEAR STRUCTURE 135Ce; measured not abstracted; deduced nuclear properties.
Phys.Rev. 137, B483 (1965)
H.A.Grench, S.B.Burson
Excited States of Ba135 from the Decay of La135 (19.8h)
NUCLEAR STRUCTURE 135La; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 61, 613 (1965)
S.Morinobu, T.Hirose, K.Hisatake
Decay of 135La
RADIOACTIVITY 135La[from 138Ba(p, 4n)]; measured Eγ, ce; Iγ, ce; γγ-coin. 135Ba deduced levels, J, π. Enriched target.
doi: 10.1016/0029-5582(65)90611-5
Yadern.Fiz. 3, 602 (1966); Soviet J.Nucl.Phys. 3, 441 (1966)
A.A.Abdumalikov, A.A.Abdurazakov, S.B.Buribaev, K.Y.Gromov, N.A.Lebedev
Conversion-Electron Spectra of the Isotopes Ce135, Ce133, and Ce132
NUCLEAR STRUCTURE 135Ce, 132Ce, 133Ce; measured not abstracted; deduced nuclear properties.
Rev.Roumaine Phys. 11, 399 (1966)
N.Comaniciu, V.Draganescu, V.Tatu
Hyperfine Structure in BaII 4934 A and 4554 A Lines and Nuclear Magnetic Moments of Ba137 and Ba135
NUCLEAR STRUCTURE 58Co, 137Ba, 135Ba, 95Zr; measured not abstracted; deduced nuclear properties.
Compt.Rend. 262B, 1355 (1966)
N.Comaniciu, V.Draganescu, N.Ionescu-Pallas, V.Tatu
Determination des Moments Quadrupolaires Intrinseques du Baryum par des Mesures de Deplacements Isotopiques
NUCLEAR STRUCTURE 135Ba, 137Ba, 136Ba, 138Ba, 134Ba; measured not abstracted; deduced nuclear properties.
Rev.Roumaine Phys. 11, 669 (1966)
N.Comaniciu, V.Draganescu, N.J.Ionescu-Pallas, V.Tatu
Isotope Shifts and Intrinsic Deformations in Ba
NUCLEAR STRUCTURE 134Ba, 138Ba, 136Ba, 137Ba, 135Ba; measured not abstracted; deduced nuclear properties.
Compt.Rend. 262B, 915 (1966)
N.Comaniciu, V.Draganescu, V.Tatu
Les Moments Magnetiques de 135Ba et 137Ba a Partir de la Structure Hyperfine de la Raie Ba II, 4934 A
NUCLEAR STRUCTURE 135Ba, 137Ba; measured not abstracted; deduced nuclear properties.
Izv.Akad.Nauk SSSR, Ser.Fiz. 30, 1221 (1966); Bull.Acad.Sci.USSR, Phys.Ser. 30, 1271 (1967)
L.N.Galperin, G.M.Gusinskii, I.K.Lemberg
Angular Correlations of Inelastically Scattered Ions and Gamma Rays Emitted in Coulomb Excitation of Mo97, Pd105, and Ba135
NUCLEAR STRUCTURE 135Ba, 97Mo, 105Pd; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 28, 1501 (1966)
H.Hamaguchi, N.Onuma, K.Tomura, R.Kuroda
Rapid Separation of Short-Lived Xenon Nuclides from a Uranium-Fission Products Mixture by Solvent Extraction
NUCLEAR STRUCTURE 133Xe, 138Xe, 137Xe, 135Xe; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(66)80045-3
Nukleonika 11, 471 (1966)
J.Jastrzebski, M.Moszynski, A.Zglinski
Time-to-Amplitude Converter for the Measurements of Nanosecond Isomers
RADIOACTIVITY 135,137Xe(β-), 145Sm, 167Tm, 173Lu(EC); measured decay products, Eγ, Iγ, γγ(t). 125,127I, 145Pm, 167Er, 173Yb; deduced levels, T1/2.
Z.Phys. 196, 77 (1966)
L.Olschewski, E.-W.Otten
Prazisionsmessung der Kerndipolmomente von Ba135 und Ba137 mit Optischem Pumpen
NUCLEAR STRUCTURE 137Ba, 135Ba; measured not abstracted; deduced nuclear properties.
Phys.Rev. 148, 1241 (1966)
E.J.Schneid, B.Rosner
Study of (d, p) and (d, t) Reaction on the Xe136 Isotope
NUCLEAR STRUCTURE 133Xe, 137Xe, 135Xe; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 28, 287 (1966)
L.Tomlinson
Gamma Rays and Delayed Neutrons from Antimony and Arsenic Isotopes
NUCLEAR STRUCTURE 86As, 87As, 85As, 129Sb, 128Sb, 130Sb, 135Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(66)80303-2
Izv.Akad.Nauk SSSR, Ser.Fiz. 31, 1672 (1967); Bull.Acad.Sci.USSR, Phys.Ser. 31, 1712 (1968)
L.K.Batist, J.Vrzal, B.S.Dzhelepov, J.Liptak, Y.N.Podkopaev, J.Urbanets
Gamma-Ray Spectra of Barium Isotopes Obtained by (n, γ) Reactions
NUCLEAR REACTIONS 130,132,134,138Ba(n, γ), E=thermal; measured σ, σ(E), σ(θ), Eγ, Iγ. 131,133,135,139Ba deduced levels.
J.Inorg.Nucl.Chem. 29, 273 (1967)
P.Del Marmol, M.Neve De Mevergnies
Investigation of Delayed Neutron Precursors of As, Sb and Ge
NUCLEAR REACTIONS 235U(n, F)85As/86As/87As/87Se/135Sb, E thermal; measured reaction products, En, In; deduced delayed neutron T1/2, neutron emission probabilities. Comparison with available data.
doi: 10.1016/0022-1902(67)80027-7
J.Phys.Soc. Japan 23, 145 (1967)
Y.Gono, M.Ishihara, M.Sakai
Decay of La134
NUCLEAR STRUCTURE 135Ce, 134La, 134Ce; measured not abstracted; deduced nuclear properties.
Z.Phys. 199, 239 (1967)
H.Huhnermann, H.Wagner
Isotope Shift in the Resonance Lines of the Arc Spectrum of 133Cs, 135Cs, and 137Cs
NUCLEAR STRUCTURE 137Cs, 135Cs, 133Cs; measured not abstracted; deduced nuclear properties.
Czech.J.Phys. 17B, 1050 (1967)
I.Rezanka, A.Spalek, J.Frana, J.Jursik
Gamma-Radiation of 135Ce
NUCLEAR STRUCTURE 135Ce; measured not abstracted; deduced nuclear properties.
Phys.Rev. 166, 1194 (1968)
A.Abdul-Malek, R.A.Naumann
Energy Levels of La135
NUCLEAR STRUCTURE 135Ce; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A121, 612 (1968)
P.Alexander, J.P.Lau
Nuclear Structure in 133,135Xe and 133,135Cs
RADIOACTIVITY 133,133mXe [from 235U(n, F), 130Te(α, n)]; measured T1/2, Eγ, Iγ; ICC. 133Ba; measured Eγ, Iγ. 133Cs deduced levels. 135,135mXe [from 235U(n, F), 134Xe(n, γ)]; measured T1/2, Eγ, Iγ, γγ-coin. 135Cs deduced levels, log ft. Enriched targets; Ge(Li), Si(Li) detectors.
NUCLEAR REACTIONS 130Te(α, n), E=6-24 MeV; measured σ(E), isomeric ratio. Enriched target.
doi: 10.1016/0375-9474(68)90111-5
Z.Physik 216, 142 (1968)
W.Becker, W.Fischer, H.Huhnermann
Die Hyperfeinstruktur der Ba II-Resonanzlinien und die Quadrupolmomente der Ungeraden Bariumisotope
NUCLEAR MOMENTS 135Ba; measured hfs; deduced quadrupole moment.
ATOMKI Kozlemen. 10, 112 (1968)
P.Bornemisza-Pauspertl, J.Karolyi, G.Peto
Measurements of the Excitation Cross Sections of Isomeric States by Scattering of 2, 8 MeV Neutrons
NUCLEAR REACTIONS 89Y, 111Cd, 115In, 135,137Ba, 191Ir, 197Au, 199Hg(n, n'), E=2.8 MeV; measured σ. 89Y, 111Cd, 115In, 135,137Ba, 191Ir, 197Au, 199Hg deduced isomeric T1/2.
ORNL-4306, p.7 (1968)
A.R.Brosi, B.H.Ketelle
Decay of 135Pr and the New Isotope 135Nd
RADIOACTIVITY 135Pr; measured Eγ, Iγ. 135Nd; measured Eγ, Iγ. 135Ce deduced levels, J, π.
Phys.Rev. 175, 1516 (1968)
P.A.Moore, P.J.Riley, C.M.Jones, M.D.Mancusi, J.L.Foster, Jr.
136Xe(d, p) and 136Xe(d, t) Reactions
NUCLEAR STRUCTURE 135Xe, 137Xe; measured not abstracted; deduced nuclear properties.
Z.Phys. 213, 254 (1968)
G.V.Oppen
Level-Crossing-Experiment am 6s6p 3P1-Term im Ba I-Spektrum
NUCLEAR STRUCTURE 137Ba, 135Ba; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 30, 2881 (1968)
J.P.Op de Beeck, W.B.Walters
Decay of 9.2-h 135Xe
RADIOACTIVITY 135Xe; measured Eγ, Iγ, γγ-coin; deduced log ft. 135Cs deduced levels, γ-branching, J, π.
doi: 10.1016/0022-1902(68)80146-0
J.Inorg.Nucl.Chem. 30, 1125 (1968)
L.Tomlinson, M.H.Hurdus
Delayed Neutron Precursors I. Antimony and Arsenic Precursors Separated by Electrolysis
NUCLEAR REACTIONS, Fission 235U(n, F), E= thermal; measured delayed neutron activity. 85,86As, 135Sb deduced T1/2, delayed neutron yields.
doi: 10.1016/0022-1902(68)80535-4
J.Inorg.Nucl.Chem. 30, 1649 (1968)
L.Tomlinson, M.H.Hurdus
Delayed Neutron Precursors II. Antimony and Arsenic Precursors Separated Chemically
NUCLEAR REACTIONS, Fission 235U(n, F), E= thermal; measured delayed neutron activity. 85,86As, 134,135Sb deduced T1/2, delayed neutron yields.
doi: 10.1016/0022-1902(68)80335-5
Thesis, Princeton Univ. (1969); Diss.Abst.Int. 30B, 2073 (1969)
A.B.Abdul-Malek
The Spectroscopy of Some Barium and Lanthanum Nuclei
RADIOACTIVITY 135Ce, 130,132,134Ce, 134Cs; measured Eγ, Iγ, γγ-coin, ceγ-coin, I(ce). 134La; measured T1/2. 130,132,134Ba, 135La, 132La deduced levels, J, π.
Nucl.Phys. A134, 118 (1969)
R.N.Alves, S.de Barros, P.L.Chevillon, J.Julien, J.Morgenstern, C.Samour
Determination du Spin et des Parametres des Resonances pour Cl+n, Cu+n, Ba+n et Nd+n
NUCLEAR REACTIONS Cl(n, X), E < 115 keV; Cu(n, X), E < 32 keV; Ba(n, X), E < 1300 eV; Nd(n, X), E < 740 eV; measured σ(nt)(E). 36,38Cl, 64,66Cu, 131,133,135,136,137,138Ba, 144,145,146,149,151Nd deduced resonances, resonance parameters, strength function.
doi: 10.1016/0375-9474(69)90688-5
J.Inorg.Nucl.Chem. 31, 1873 (1969)
H.O.Denschlag
Independent Yield of 135I in the Thermal Neutron Fission of 235U. The Half-Life of 135Te
NUCLEAR REACTIONS, Fission 235U(n, F), E= thermal; measured 135I yield.
RADIOACTIVITY 135Te; measured T1/2.
doi: 10.1016/0022-1902(69)90001-3
Nuovo Cimento 60B, 301 (1969)
N.Freed, W.Miles
Unified-Model Calculations for Odd-Mass Cs and La Isotopes
NUCLEAR STRUCTURE 131,133,135Cs, 133,135,137,139La; calculated levels, μ, quadrupole moment, B(E2), B(M1). Unified model, intermediate coupling.
Yadern.Fiz. 10, 681 (1969); Soviet J.Nucl.Phys. 10, 392 (1970)
L.V.Groshev, V.N.Dvoretskii, A.M.Demidov, M.S.Alvash
Radiation of Even-Odd Nuclei Near the Magic Number N = 82 after Thermal Neutron Capture
NUCLEAR REACTIONS 134,136,138Ba, 138,140,142Ce(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 135,137,139Ba, 139,141,143Ce deduced levels. Enriched targets.
Yadern.Fiz. 10, 929 (1969); Soviet J.Nucl.Phys. 10, 536 (1970)
Z.G.Gritchenko, T.P.Makarova, Y.T.Oganesyan, Y.E.Penionzhkevich, A.V.Stepanov
γ Radiation of Certain Rare-Earth Products of Fission of U by Heavy Ions
RADIOACTIVITY 140,141,142La, 135,137,139,141,143,144Ce, 138,139,142,143,145Pr, 139,140,147,149Nd, 144,148,149,150,151Pm, 153,156Sm, 150,155,156,157Eu, 147,149,159Gd[from 238U(HI, F), with HI = 12C, 20,22Ne, 40Ar]; measured Eγ, Iγ.
NUCLEAR REACTIONS 238U(HI, F), E=80-290 MeV with HI= 12C, 20,22Ne, 40Ar; measured Eγ, Iγ; deduced yields of several La, Ce, Pr, Nd, Pm, Sm, Eu, Gd isotopes. Ge(Li) detector.
Nucl.Phys. A132, 129 (1969); UCRL-TRANS-10397
J.Julien, R.Alves, S.de Barros, V.D.Huynh, J.Morgenstern, C.Samour
Variations de la Largeur Radiative Totale Gamma γ en Fonction du Nombre de Masse A et de la Valeur du Spin J = I(1/2)
NUCLEAR REACTIONS Fe, Cu, Zn, Ga, As, Se, Br, Zr, Nb, Mo, Ag, Cd, Sn, Ba, La, Pr, Nd, Gd, Tb, Tm, W, Pt, Au, Hg(n, X), E = 4-2000 eV; measured σ(nγ). 57Fe, 64,66Cu, 65,66,68Zn, 70,72Ga, 76As, 75,77,78,79Se, 80,82Br, 92,97Zr, 94Nb, 96,97,98Mo, 108,110Ag, 111,112,113,114Cd, 113,117,118,119,120,125Sn, 133,135,136Ba, 140La, 142Pr, 144,146Nd, 156,158Gd, 160Tb, 170Tm, 184W, 193,195,196,197,199Pt, 198Au, 199,200,202Hg deduced resonances, resonance parameters, γ-width, J, level spacing D.
doi: 10.1016/0375-9474(69)90618-6
Proc.Symp.Phys.Chem.Fission, 2nd, Vienna, Intern.At.En.Agency, Vienna, p.591 (1969); IAEA-SM-122/22 (1969)
H.D.Schussler, H.Ahrens, H.Folger, H.Franz, W.Grimm, G.Herrmann, J.V.Kratz, K.L.Kratz
Delayed Neutron Precursors in Fission of 235U by Thermal Neutrons
NUCLEAR REACTIONS 235U(n, F), E=thermal; measured reaction products. 83,85,87As, 86,87,88Se, 91Br, 93,94Rb, 137,140,141I, 135,136,137Te; deduced Iγ(t), delayed neutron activity(t), T1/2, delayed neutron yields.
Yadern.Fiz. 9, 906 (1969); Soviet J.Nucl.Phys. 9, 529 (1969)
O.I.Sumbaev, A.F.Mezentsev, V.I.Marushenko, A.S.Rylnikov, G.A.Ivanov
Anomalous Variations of the Nuclear Charge Radii of Barium Isotopes
NUCLEAR MOMENTS 134,135,136,137,138Ba; measured X-ray line shifts; deduced variations of charge radii.
Z.Physik 227, 216 (1969)
S.Svanberg, S.Rydberg
Level Crossing Investigation of the 6p 2P3/2 and 7p 2P3/2 Levels of Cs133, Cs135, and Cs137
NUCLEAR MOMENTS 133,135,137Cs; measured a, B; deduced quadrupole moment. Level-crossing experiment.
Izv.Akad.Nauk SSSR, Ser.Fiz. 34, 796 (1970); Bull.Acad.Sci.USSR, Phys.Ser. 34, 706 (1971)
A.A.Abdurazakov, R.Arlt, R.Babadzhanov, G.Baier, V.A.Morozov, G.Musiol, K.Tyrroff, H.Strusny
New Isotopes 133Pr, 134Nd and 135Nd; Decay Schemes of 134Pr and 135Pr
RADIOACTIVITY 134,135Nd[from Gd(660-MeV p, X)]; measured T1/2. 133,134,135Pr; measured T1/2, Eγ, Iγ. 134,135Ce deduced levels.
Phys.Rev. C1, 1491 (1970)
A.A.Delucchi, A.E.Greendale
Fission Yields of Several Iodine Isotopes and Half-Life and Fission Yield of 135Te
RADIOACTIVITY 135Te[from 235U(n, F)]; measured T1/2.
NUCLEAR REACTIONS 235U(n, F), E=thermal; measured 131,132,133,135I, 135Te yields.
Nucl.Phys. A152, 579 (1970)
C.Droste, W.Neubert, J.Lewitowicz, S.Chojnacki, T.Morek, Z.Wilhelmi, K.F.Alexander
135mCe and 137mNd: Isomeric States in N = 77 Isotones
NUCLEAR REACTIONS 128Te(12C, 5n), E=78 MeV; 119,122Sn(22Ne, xn), (20Ne, xn), E=60-160 MeV; 126Te(18O, 7n), E not given; 124,126Te(20Ne, xn), E=115, 135 MeV; measured σ(E), Eγ, Iγ, I(ce), (HI)γ-delay. 135Ce deduced levels, J, π. 137Nd deduced levels, T1/2. 139Sm deduced no isomeric with 5 ms < T1/2 < 3s. Enriched targets.
doi: 10.1016/0375-9474(70)90934-6
Phys.Lett. 33B, 474 (1970); See Also CERN-70-30, Vol.2, p.967 (1970)
J.W.Gruter, K.Sistemich, P.Armbruster, J.Eidens, H.Lawin
Identification of μs-Isomers among Primary Fission Products
NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured (fragment)(γ)-, (fragment)(X)-delay, Eγ, γγ-coin, γX-coin. 88mBr, 93m,96mRb, 96mSr, 98mY, 97mY, 99mZr, 100mNb, 132mSn, 135mSb, 134mSb, 134mTe, 134mI, 136mXe deduced T1/2.
doi: 10.1016/0370-2693(70)90221-2
Z.Naturforsch. 25a, 1750 (1970)
J.Hoeft, F.J.Lovas, E.Tiemann, T.Torring
Microwave Spectrum of BaO
NUCLEAR MOMENTS 135,137Ba; measured quadrupole moment ratios. Microwave spectroscopy.
Phys.Rev. C2, 1451 (1970)
W.John, F.W.Guy, J.J.Wesolowski
Four-Parameter Measurements of Isomeric Transitions in 252Cf Fission Fragments
RADIOACTIVITY 134mTe, 136mXe; measured T1/2, Eγ, Iγ.
RADIOACTIVITY, Fission 252Cf(SF); measured (fragment)(fragment)(γ)-coin, (fragment)(γ)-delay.
Nucl.Phys. A147, 513 (1970)
E.S.Macias, J.P.op de Beeck, W.B.Walters
Decay of 6.7 h 135I to Levels of 135Xe
RADIOACTIVITY 135I[from 235U fission]; measured Eγ, Iγ, Eβ, γγ-coin, βγ-coin; deduced Q, log ft. 135Xe deduced levels, J, π. Enriched target; Ge(Li) detector.
doi: 10.1016/0375-9474(70)90596-8
Thesis, Mass.Inst.Tech. (1970)
E.S.Macias
Spectroscopic Studies of Nuclear and Atomic Systems Using the Angular Correlation Method
RADIOACTIVITY 135I; measured Eγ, Iγ, βγ-, γγ-coin, γγ(θ), Eβ; deduced log ft. 131gTe; measured Eγ, Iγ, γγ-coin, γγ-delay; deduced log ft. 125gSn; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced log ft. 103Ru;measured Eγ, Iγ, γγ-coin, I(ce), γγ(θ); deduced log ft. 56Co; measured γγ(θ). 135Xe, 131I deduced levels, J, π. 125Sb deduced levels, J, π, γ-mixing. 103Rh deduced levels, J, π, ICC. 56Fe levels deduced J, π, γ-multipolarity.
J.Phys.Soc.Jap. 29, 790 (1970)
Y.Nagai, M.Akiba, K.Hisatake
Lifetime Measurements of the 119 and 206 keV Levels in 135La
RADIOACTIVITY 135Ce; measured ceγ-delay. 135La levels deduced T1/2.
Phys.Rev. C1, 2066 (1970)
D.von Ehrenstein, G.C.Morrison, J.A.Nolen, Jr., N.Williams
Study of the (d, p) Reaction on the Even-A Barium Isotopes 130-138
NUCLEAR REACTIONS 130,132,134,136,138Ba(d, p), E=12 MeV; measured σ(Ep, θ), Q. 131,133,135,137,139Ba deduced levels, L(n), J, π, S.
Z.Phys. 236, 97 (1970)
F.von Sichart, H.J.Stockmann, H.Ackermann, G.zu Putlitz
Optical Pumping of Free Atomic Ions with Hyperfine Structure
NUCLEAR MOMENTS 135,137Ba; measured a; deduced hyperfine anomaly Δ. Optical pumping.
Phys.Rev. C2, 1539 (1970)
N.Williams, G.C.Morrison, J.A.Nolen, Jr., Z.Vager, D.von Ehrenstein
Isobaric Analog Resonances from Proton Scattering on the Barium Isotope
NUCLEAR REACTIONS 130,132,134,136,138Ba(p, p), E=7-12 MeV; measured σ(E;θ). 131,133,135,137,139La deduced isobaric analog resonances, level-width, S, Coulomb displacement energies.
Proc.Symp.Nucl.Spectrosc.Nucl.Theory, 13th, Dubna, p.87 (1971); JINR-D6-5783 (1971)
R.Arlt, G.Baier, H.Tyrroff, Z.A.Usmanova, H.Shtrusny, E.Herrmann
On the Decay of 135Nd and 134Nd
RADIOACTIVITY 134,135Nd(EC), (β+); measured Eγ, Iγ. 135Nd deduced T1/2. 135Pr deduced levels.
Nucl.Phys. A164, 552 (1971); Priv.Comm. (1974)
F.Bazan, R.A.Meyer
Properties of Phonon-Coupled Levels: The Levels of 135Ba Populated in The Decay of 135La
RADIOACTIVITY 135La[from 135Ba(p, n), enriched targets]; measured Eγ, Iγ; deduced Q, log ft. Isotopically separated activity;Ge(Li) detector. Compton suppression spectrometer. 135Ba deduced levels, ICC, J, π, odd-particle phonon coupled level properties.
doi: 10.1016/0375-9474(71)90779-2
Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 2312 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 2099 (1972)
R.B.Begzhanov, D.A.Gladyshev, O.S.Kobilov, P.S.Radzhapov, K.S.Sabirov
Nature of the Levels of 135Ba
RADIOACTIVITY 135La; measured γγ(θ), γγ(t). 135Ba deduced γ-multipolarity, T1/2 (level).
Izv.Akad.Nauk Arm.SSR, Ser.Fiz. 6, 87 (1971)
R.B.Begzhanov, D.A.Gladyshev, O.S.Kobilov, P.S.Radzhapov, K.S.Sabirov
Nature of 135Ba Nuclear Levels
RADIOACTIVITY 135La; measured γγ(θ), γγ-delay. 135Ba levels deduced T1/2, γ-mixing, J.
Phys.Rev. C3, 1619 (1971)
D.C.Choudhury, J.N.Friedman
Application of the Intermediate-Coupling Unified Nuclear Model to Odd-Mass Cesium Isotopes
NUCLEAR STRUCTURE 131,133,135Cs; calculated levels, B(λ), μ, quadrupole moment.
An.Acad.Brasil.Cienc. 43, 63 (1971)
A.G.de Pinho, I.V.Goldstein, J.M.F.Jeronymo
The Level Spectra of Nuclei with 51 < Z < 61 and the Intermediate-Coupling Model
NUCLEAR STRUCTURE 113,115,117,119,121,123,125,127,129Sb, 125,127,129,131,133I, 131,133,135,137Cs, 133,135,137,139La, 139,141,143Pr, 143,145,147,149Pm; calculated levels, μ, quadrupole moment, B(M1), B(E2). Intermediate- coupling model.
Can.J.Phys. 49, 785 (1971)
R.C.Hawkings, W.J.Edwards, W.J.Olmstead
Independent Yields of Mass-135 Xenons in the Thermal Neutron Fission of 233U, 235U, 239Pu, and 241Pu
NUCLEAR REACTIONS, Fission 239,241Pu, 233,235U(n, F), E=thermal; measured 135Xe yields.
Nucl.Phys. A169, 305 (1971)
E.S.Macias, W.B.Walters
Gamma-Gamma Directional Correlations in 135Xe Following the Decay of 135I
RADIOACTIVITY 135I [from 235U fission]; measured γγ(θ). 135Xe deduced levels, J, π. Enriched target. Ge(Li), NaI(Tl) detectors.
doi: 10.1016/0375-9474(71)90886-4
Thesis, Univ.Wisconsin (1971); Diss.Abst.Int. 32B, 2339 (1971)
W.M.Roney, Jr.
Magnetic Moments of Excited States of Odd A Nuclei
NUCLEAR MOMENTS 103Rh, 107,109Ag, 111,113Cd, 123,125Te, 135Ba levels measured g.
Nucl.Phys. A171, 593 (1971)
R.N.Saxena, H.D.Sharma
Energy Levels of 133Xe
RADIOACTIVITY 133I, 135I[from 235U(n, F) or 238U(γ, F)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 133Xe deduced levels, J, π. Natural target, Ge(Li) detectors.
doi: 10.1016/0375-9474(71)90605-1
Z.Phys. 246, 369 (1971)
J.van Klinken, S.Goring, D.Habs, M.von Hartrott, H.Klewe-Nebenius, R.Lohken, H.Rebel, G.Schatz
139Sm, a New Nuclide of Relevance for the Systematics of the N = 77 Isomers
RADIOACTIVITY 139Sm, 139mSm, 137mNd, 135mCe; measured T1/2, Eγ, Iγ, I(ce). 135Ce, 137Nd, 139Sm deduced levels, ICC, γ-multipolarity.
Nucl.Phys. A177, 393 (1971)
R.E.Van De Vyver, N.J.Pattenden
Neutron Resonances in Barium Isotopes
NUCLEAR REACTIONS 134Ba, 135Ba, 136Ba, 137Ba(n, X), E=4-2000 eV; measured σ(nT)(E). 135,136,137,138Ba deduced resonance parameters, n-width, n-width, γ-width, strength function. Enriched targets.
doi: 10.1016/0375-9474(71)90299-5
Phys.Rev. C3, 1199 (1971)
B.H.Wildenthal, E.Newman, R.L.Auble
Study of the Level Structure of N = 82 Nuclei via Proton-Transfer Reactions
NUCLEAR REACTIONS 144Sm, 142Nd, 140Ce, 138Ba, 136Xe(3He, d), E=40, 24 MeV; measured σ(Ed, θ); deduced Q for 142Nd(3He, d). 144Sm, 142Nd, 140Ce, 138Ba, 136Xe(d, 3He), E=40 MeV; measured σ(E(3He), θ); deduced Q for 136Xe(d, 3He). 135I, 137Cs, 139La, 141Pr, 143Pm, 145Eu deduced levels, J, π, L, S.
Phys.Lett. 37B, 266 (1971)
B.H.Wildenthal, D.Larson
The Structure of the Lighter N = 82 Nuclei
NUCLEAR STRUCTURE 133Sb, 134Te, 135I, 136Xe; calculated levels, wave functions. Shell model.
doi: 10.1016/0370-2693(71)90014-1
Phys.Rev. C5, 1759 (1972)
E.Achterberg, F.C.Iglesias, A.E.Jech, J.A.Moragues, D.Otero, M.L.Perez, A.N.Proto, J.J.Rossi, W.Scheuer, J.F.Suarez
Conversion-Coefficient Measurements and Spin-Parity Assignments for Excited Levels in 133,135,136Xe, 135,137,139Cs, and 138Ba
RADIOACTIVITY 133mXe, 135Xe, 135mXe, 137,139Xe, 133,135,136I, 138Cs; measured Eγ, Iγ, I(ce); deduced log ft. 133,135,136Xe, 138Ba, 135,137,139Cs deduced levels, J, π, ICC, γ-multipolarity. Solid-state detectors.
JINR-P6-6426 (1972)
V.P.Afanasiev, I.I.Gromova, N.A.Lebedev, V.A.Morozov, T.M.Muminov, H.Fuia, A.B.Khalikulov, F.S.Khamraev
Measurement of Excited State Life-Times in Neutron-Deficient Nuclei of 165Er, 163Er, 157Tb, 153Gd, 151Gd and 135La
NUCLEAR REACTIONS 135Ba, 151,153Eu, 157Gd, 163,165Ho(p, nγ), E=660 MeV; measured ceγ-delay. 135La, 151,153Gd, 157Tb, 163,165Er deduced T1/2.
J.Phys.Soc.Jap. 32, 567 (1972)
M.Akiba, Y.Nagai, K.Hisatake
Remeasurement of the Lifetime of the 119 keV Level in 135La
RADIOACTIVITY 135Ce; measured ceγ-delay. 135La level deduced T1/2.
Nucl.Instrum.Methods 102, 253 (1972)
R.Arlt, V.A.Bystrov, W.Habenicht, E.Herrmann, V.I.Raiko, H.Strusny, H.Tyrroff
Isobars from the Spallation Reaction for Nuclear Spectroscopy
Izv.Akad.Nauk SSSR, Ser.Fiz. 36, 744 (1972); Bull.Acad.Sci.USSR, Phys.Ser. 36, 673 (1973)
R.Arlt, G.Beyer, V.A.Morozov, G.Musiol, T.M.Muminov, H.Tyrroff, H.Strusny, Z.A.Usmanova, V.I.Fominykh, H.Fuya, A.B.Khalikulov, E.Herrmann
On the 135Pr → 135Ce Decay Scheme
RADIOACTIVITY 135Pr [from Gd(660-MeV p, X)]; measured Eγ, Iγ, I(ce), γγ-coin, γce(t); deduced ICC, log ft. 135Ce deduced levels, J, π, T1/2.
J.Phys.(Paris) 33, 829 (1972)
V.Berg, J.Letessier, C.Bourgeois, R.Foucher
Mesures de Vies Moyennes d'Etats Excites dans les Lanthanes 135 et 133
RADIOACTIVITY 133,135Ce; measured ceγ-, (ce)(ce)-delay. 133,135La levels deduced T1/2.
Izv.Akad.Nauk SSSR, Ser.Fiz. 36, 2520 (1972); Bull.Acad.Sci.USSR, Phys.Ser. 36, 2190 (1973)
R.B.Begzhanov, O.S.Kobilov, K.S.Sabirov, S.K.Salimov, U.K.Khudaibergenov
The Angular Correlation of γ-Rays of Neutron-Rich Xenon Isotopes
RADIOACTIVITY 131,132,133,134,135I [from 239Pu(n, F)]; measured γγ(θ). 131,132,133,134,135Xe deduced γ-mixing.
Nucl.Phys. A196, 178 (1972)
C.Ekstrom, S.Ingelman, M.Olsmats, B.Wannberg, G.Andersson, A.Rosen
Nuclear Spins of Neutron-Deficient Pr and Nd Isotopes
NUCLEAR MOMENTS 133,134,135,136,137,138m,139,140Pr, 134,135,136,137,138,139,139m,140Nd; measured J. Atomic-beam magnetic resonance.
doi: 10.1016/0375-9474(72)90959-1
NP-19337, p.26 (1972)
O.C.Jonsson, E.Lund, G.Rudstam
Total Decay Energies for Neutron-Rich Nuclei
RADIOACTIVITY 79Ga, 90Rb, 115,116,117Ag, 119Cd, 120,121In, 127,128,133Sb, 129,131,132Sn, 132,135,136,137I, 133Te, 139,140Cs, 141Ba; measured Eβ. Deduced Q.
Z.Phys. 249, 205 (1972)
L.Olschewski
Messung der magnetischen Kerndipolmomente an freien 43Ca-, 87Sr-, 135Ba-, 137Ba-, 171Yb- und 173Yb-Atomen mit optischem Pumpen
NUCLEAR MOMENTS 43Ca, 87Sr, 135,137Ba, 171,173Yb; measured μ. Optical pumping.
Phys.Scr. 5, 209 (1972)
S.Rydberg, S.Svanberg
Investigation of the np 2P3/2 Level Sequence in the Cs I Spectrum By Level Crossing Spectroscopy
NUCLEAR MOMENTS 133Cs; measured a, b. 135,137Cs deduced quadrupole moment. Level-crossing methods.
Phys.Rev. C6, 2201 (1972)
S.Sen, P.J.Riley, T.Udagawa
136Xe(p, p')136Xe and 136Xe(p, d)135Xe Reactions
NUCLEAR REACTIONS 136Xe(p, p'), (p, d), E=13.982 MeV; measured σ(θ); deduced optical model parameters. 136Xe deduced levels, J, π, S, β. 135Xe deduced levels, J, π.
Izv.Akad.Nauk SSSR, Ser.Fiz. 36, 753 (1972); Bull.Acad.Sci.USSR, Phys.Ser. 36, 681 (1973)
V.Zhuk, E.Krupa, V.A.Morozov, T.M.Muminov, K.Fuya, A.B.Khalikulov
Spin and Parity Assignments for Certain 135La Levels
RADIOACTIVITY 135Ce [from Gd(660-MeV p, X)]; measured γγ(θ). 135La deduced level J, π, γ-mixing.
Nucl.Phys. A212, 197 (1973)
S.Borg, G.B.Holm, B.Rydberg
Proton Particle States in the Region Around 132Sn
RADIOACTIVITY 133Sn, 135Te [from 235U fission]; measured T1/2, Eγ, Iγ, Eβ-, βγ-coin, γγ-coin. 133Sb, 135I deduced levels, J, π, log ft. Isotopically separated sources, Ge(Li), anthracene detectors.
doi: 10.1016/0375-9474(73)90045-6
Nucl.Phys. A213, 445 (1973)
T.W.Conlon
New M2 Isomers in Neutron Deficient I, La and Pr Associated with a Deformed Nuclear Shape
NUCLEAR REACTIONS 107,109Ag, 127I, 123Sb(12C, xnγ), E=88 MeV; measured Eγ, Iγ(t), E(X-ray), I(X), deduced ICC. 115mI or 117mI, 131mLa, 135mPr deduced levels, J, π, γ-multipolarities, T1/2.
doi: 10.1016/0375-9474(73)90745-8
ANCR-1129, p.23 (1973)
R.J.Gehrke, L.D.McIsaac, R.L.Heath
γ-Ray Energy and Relative Intensity Measurements of Several Fission Product Radionuclides
RADIOACTIVITY 87Kr, 88Kr, 88Rb, 134I, 135I; measured Eγ, Iγ.
Z.Phys. 259, 15 (1973)
K.Heyde, P.J.Brussaard
Neutron Hole States in the N=81 Nuclei
NUCLEAR STRUCTURE 133Te, 135Xe, 137Ba, 139Ce, 141Nd, 143Sm; calculated levels, J, π, S, γ-branching, transition probabilities.
Phys.Scr. 7, 24 (1973)
S.Ingelman, C.Ekstrom, M.Olsmats, B.Wannberg
Nuclear Spins of Neutron-Deficient Lanthanum and Cerium Isotopes
NUCLEAR MOMENTS 131,132,132m,133,135,136La, 130,132,133,133m,134,135,137,137m,139Ce; measured J. Atomic beam magnetic resonance method.
Nucl.Phys. A213, 1 (1973)
J.R.Leigh, K.Nakai, K.H.Maier, F.Puhlhofer, F.S.Stephens, R.M.Diamond
Energy-Level Systematics of Odd-Mass Lanthanum Isotopes; a New Coupling Scheme
NUCLEAR REACTIONS 130,128,126,124,122Te(11B, 4nγ), E=40, 45, 50, 52.6, 56.5 MeV; 124Sn(14N, 5nγ), 120,118,116Sn(14N, 3nγ), E=50.5, 53, 58, 62, 64.8, 67, 68.5, 72, 76 MeV; 112Sn(16O, 2npγ), E=72, 76, 82, 88, 94 MeV; measured σ(Eγ, θ), γγ-coin, γγ(t). 125,127,129,131,133,135,137La deduced levels, J, π, T1/2, γ-multipolarity. Enriched targets. Ge(Li) detector.
doi: 10.1016/0375-9474(73)90178-4
CEA-R-4427 (1973)
J.Legrand, M.Blondel, P.Magnier, C.Perrot, J.P.Brethon
Accurate Measurement of Some Internal Conversion Coefficients (109Ag:88 keV, 99Tc:140 keV, 139La:166 KeV, 135Ba:268 keV)
RADIOACTIVITY 99mTc, 109Cd, 135mBa, 139Ce; measured I(ce), Eγ. Deduced ICC.
Phys.Rev. C7, 1678 (1973)
G.R.Lucas, Jr., P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins, R.J.Powers, A.R.Kunselman
Neutron Emission Following Muon Capture in 142Ce, 140Ce, 138Ba, and 120Sn
NUCLEAR REACTIONS 120Sn, 138Ba, 140,142Ce(μ-, nγ); measured Eγ, Iγ, 139,140,141,142La, 135,136,137,138Ba, 117,118,119,120In deduced levels, absolute yield per muon capture.
J.Phys.Soc.Jap. 35, 1251 (1973)
A.Morinaga, M.Akiba, M.Fujioka, H.Nakayama, M.Sekikawa, K.Hisatake
Penetration Effect and Transition Probability of the 5/2+' → 7/2+ Transition in 135La
RADIOACTIVITY 135Ce; measured I(ce), Eγ, Iγ, βce(t). Deduced ICC. 135La transitions deduced, γ-mixing, penetration parameter, T1/2.
Phys.Lett. 44B, 443 (1973)
K.Nakai, P.Kleinheinz, J.R.Leigh, K.H.Maier, F.S.Stephens, R.M.Diamond, G.Lovhoiden
Prolate Deformation in Neutron-Deficient Lanthanum Isotopes
NUCLEAR REACTIONS 116,118,120,122Sn(14N, xnγ), E=not given; measured Eγ, Iγ(θ), γγ-coin. 130Ba(α, t), E=27 MeV; 138Ba(3He, d), E=22 MeV; measured σ(Et), σ(Ed), L. 125,127,129,131,133,135,137,139La deduced levels, J, π.
doi: 10.1016/0370-2693(73)90329-8
J.Nucl.Energy 27, 409 (1973)
D.C.Santry, R.D.Werner
Neutron Capture Cross-Section of 135Xe
RADIOACTIVITY 135Xe; measured T1/2.
NUCLEAR REACTIONS 135Xe(n, γ), E=thermal; measured σ.
doi: 10.1016/0022-3107(73)90095-6
KFK-1768 (1973)
J.van Klinken, D.Habs, H.Klewe-Nebenius, K.Wisshak, G.Nowicki, J.Buschmann, S.Goring, R.Lohken, H.Rebel, G.Schatz
Systematic Experiments on Neutron Deficient Nuclei in the Region 50 ≤(N, Z) ≤ 82
RADIOACTIVITY 135,137Nd, 137,138,139,139m,140,142mPm, 139,140,141,143mSm, 140,141,141m,142,142mEu, 142,143,144Gd; measured T1/2, Eγ, Iγ. 135,137Pr, 139,140,142Nd, 140,141,143Pm, 142Sm, 144Eu deduced levels.
Rev.Roum.Phys. 19, 629 (1974)
A.Calboreanu, E.Cincu, I.Minzatu, C.Pencea, O.Salagean
Delayed Gamma Rays from Fission Induced by 13.3 MeV Protons on 232Th, 235U and Natural Uranium
RADIOACTIVITY 87,88Kr, 91mY, 91Sr, 97Nb, 97Zr, 99Mo, 99mTc, 101Mo, 105Ru, 112Ag, 131m,132,134Te, 131,132,133I, 135Xe, 139Ba, 143Ce, 162Tb; measured T1/2.
NUCLEAR REACTIONS 232Th, 235U(p, F), E=13.3 MeV; measured delayed γ.
Proc.Symp.Phys.Chem.Fission, 3rd, Rochester, N.Y. (1973), Int.At.En.Agency, Vienna, Vol.2, p.221 (1974)
R.G.Clark, L.E.Glendenin, W.L.Talbert, Jr.
Fission Fragment Isomers from Spontaneous Fission of 252Cf
RADIOACTIVITY, Fission 252Cf(SF); measured Eγ, Iγ, γf(t), Xγ-, γγ-coin. 87Br, 89Kr, 92Rb, 95,96,97Sr, 97,98Y, 99,100,101,102,103Zr, 102Nb, 103,104,106,107Mo, 105,107,108Tc, 109,110,111Ru, 109,111Rh, 132,134Sb, 134,135Te, 134,136,137I, 136,137Xe, 147,148,149Ce, 139,140,141Cs, 141,143,144,146Ba, 146,147La, 149,150,151Pr, 154Nd, 156,158Sm deduced transitions, T1/2, fission yields.
J.Inorg.Nucl.Chem. 36, 201 (1974)
W.R.Daniels, G.P.Ford, D.C.Hoffman, K.Wolfsberg
Branching Ratio for the Decay of 135I to the Isomers of 135Xe
RADIOACTIVITY 135I; measured Eγ, Iγ. 135Xe levels deduced γ-branching.
doi: 10.1016/0022-1902(74)80684-6
Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2022 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 11 (1974)
M.A.Deleplanque, C.Gerschel, N.Perrin, P.Quentin
Coriolis Interaction in Transitional Nuclei
NUCLEAR STRUCTURE 77Br, 135La; calculated levels, K, J, π.
Priv.Comm. (January 1974)
B.S.Dzhelepov, I.F.Uchevatkin
RADIOACTIVITY 135Ce; measured T1/2.
Bull.Amer.Phys.Soc. 19, No.4, 501, EH11 (1974)
J.Fontanilla, A.L.Prindle, J.H.Landrum, R.A.Meyer
Half-Lives and β-Decay of the 133 and 135 Isomers of Xe
RADIOACTIVITY 133,133m,135Xe; measured T1/2, Eγ; deduced log ft. 135Cs deduced levels.
Phys.Rev.Lett. 33, 859 (1974)
H.Franz, J.-V.Kratz, K.-L.Kratz, W.Rudolph, G.Herrmann, F.M.Nuh, S.G.Prussin, A.A.Shihab-Eldin
Delayed-Neutron Spectra Following Decay of 85As and 135Sb
RADIOACTIVITY 84,85As, 135Sb; measured delayed neutrons, Eγ, Iγ, γγ-coin. 84,85As deduced β-branching ratios. 85As, 135Sb deduced resonances in β-strength function. 84Se deduced levels.
doi: 10.1103/PhysRevLett.33.859
Nucl.Phys. A222, 557 (1974)
J.Gizon, A.Gizon, M.R.Maier, R.M.Diamond, F.S.Stephens
Deformed States of Neutron-Deficient Cerium and Neodymium Nuclei
NUCLEAR REACTIONS 120,122Sn(16O, 3nγ), 124Sn(16O, 5nγ), 122,124Te(16O, 3nγ), E=60-90 MeV; measured σ(E;Eγ, θ), γγ-coin, γ-γdelay. 133,135Ce, 135,137Nd deduced levels, J, π, T1/2, γ-mixing, prolate shape. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(74)90339-X
J.Inorg.Nucl.Chem. 36, 2409 (1974)
B.Grapengiesser, E.Lund, G.Rudstam
Survey of Short-Lived Fission Products Obtained Using the Isotope-Separator-on-Line Facility at Studsvik
RADIOACTIVITY 74,75,76Zn, 75,76,77,78,79Ga, 77,79,80Ge, 85,86,87,88,89Br, 90,91Kr, 90,91,92,93,94Rb, 93,94,95,97Sr, 94,95,97Y, 111,113,114,115,116,117,118,120Ag, 119,120,121,122,123,125,127,128Cd, 120,121,122,123,124,125,126,127,128In, 127,129,131,132Sn, 130,132,134Sb, 135,136Te, 137,138,139I, 137,139,140,141Xe, 140,141,142Cs, 142,143,144,145Ba, 145La, 145,147Ce; measured T1/2.
doi: 10.1016/0022-1902(74)80448-3
Bull.Amer.Phys.Soc. 19, No.4, 452, BG12 (1974)
J.H.Landrum, A.L.Prindle, W.B.Walters, R.A.Meyer
The Unique First Forbidden β-Decay of 6.61 +/- 0.01 Hour 135I
RADIOACTIVITY 135I; measured T1/2, Eγ, Iγ; deduced log ft. 135Xe deduced levels.
Priv.Comm. (April 1974)
R.A.Meyer
RADIOACTIVITY 135,135mXe; measured Eγ, Iγ. 135Cs deduced levels, J, π.
J.Phys.Soc.Jap. 36, 1501 (1974)
Y.Nagai, K.Hisatake
Excited States of 135La Populated by the Decay of 135Ce
RADIOACTIVITY 135Ce; measured γe(t), γe-coin, I(ce), Eγ, Iγ, γγ(θ). 135La deduced levels, γ-mixing, multipolarities, ICC, T1/2, EC-ratios, log ft, J, π.
Nucl.Instrum.Methods 120, 333 (1974)
G.Rudstam, S.Shalev, O.C.Jonsson
Delayed Neutron Emission from Separated Fission Products
RADIOACTIVITY 87,88Br, 136Te, 137I; measured En(t).
Nucl.Phys. A230, 153 (1974)
S.Shalev, G.Rudstam
Energy Spectra of Delayed Neutrons from Separated Fission Products (I). The Precursors 85As, 87Br, 134Sn, 135Sb, 136Te and 137I
RADIOACTIVITY 85As, 87Br, 134Sn, 135Sb, 136Te, 137I; measured En, In for β-delayed neutrons. 86Kr, 136Xe deduced level density.
doi: 10.1016/0375-9474(74)90535-1
Nucl.Phys. A248, 157 (1975)
F.Ackermann, E.W.Otten, G.zu Putlitz, A.Schenck, S.Ullrich
Determination of the Spectroscopic Quadrupole Moments of 131Cs, 132Cs and 136Cs
NUCLEAR MOMENTS 131,132,136Cs; measured hfs, a, b; deduced μ, quadrupole moment.
doi: 10.1016/0375-9474(75)90160-8
Nucl.Phys. A246, 425 (1975)
K.Aleklett, G.Nyman, G.Rudstam
Beta-Decay Properties of Strongly Neutron-Rich Nuclei
RADIOACTIVITY 76,77Zn, 76,77,78,79,80,81Ga, 79,81Ge, 82,83As, 85Se, 85,86,87,88,89Br, 89,90,91,92Kr, 90,91,92,93,94Rb, 114,116,117,118,119,120Ag, 120,121,122,123,124,125,126,127,128,129In, 132,134Sb, 135Te, 136,137,139I, 137,139,140,141Xe, 139,140,141,142,143Cs, 143,144,145Ba, 144,145La; measured total-absorption γ-spectra, deduced β-strength functions, average reduced transition rates. Mass-separated fission products.
doi: 10.1016/0375-9474(75)90657-0
Nucl.Phys. A248, 249 (1975)
V.L.Alexeev, B.A.Emelianov, L.P.Kabina, D.M.Kaminker, Y.I.Khazov, I.A.Kondurov, E.K.Leushkin, Y.E.Loginov, V.L.Rumjantsev, S.L.Sakharov, A.I.Smirnov, P.A.Sushkov
Low-Lying 134Cs Excited States from the (n, γ) Reaction
NUCLEAR REACTIONS 133Cs(n, nγ), E=fission; measured Eγ, Iγ, 133Cs(n, γ), E=th; measured Eγ, Iγ, E(ce), I(ce), γγ-coin, γγ-delay; deduced isomeric cross-section ratio, Q. 134Cs(n, γ), E=th; measured Eγ, Iγ. 134Cs deduced levels, J, π, γ-multipolarity, γ-branching, T1/2. Ge(Li), Si(Li), NaI(Tl) detectors, bent crystal spectrometer, magnetic spectrometer, natural target.
RADIOACTIVITY 134Cs [from 133Cs(n, γ)]; measured Eγ, Iγ. 134mCs [from 133Cs(n, γ)]; measured Eγ, Iγ, E(ce), I(ce). 134Cs levels deduced J, π, γ-multipolarity, γ-branching, ICC. Bent crystal spectrometer, Ge(Li) detector, magnetic spectrometer.
doi: 10.1016/0375-9474(75)90165-7
J.At.Energy Soc.Jap. 17, 177 (1975)
T.Fukuda, S.Omori
A Dry Method for Separating Xenon from its Precursor Fission-Iodine: Measurements of the 135I Branching Ratio and Half-Life of 135mXe
RADIOACTIVITY 135I; measured Iγ(t); deduced β-branching. 135mXe deduced T1/2.
Nucl.Data Sheets 14, 191 (1975)
E.A.Henry
Nuclear Data Sheets for A = 135
COMPILATION 135Sb, 135Te, 135I, 135Xe, 135Cs, 135Ba, 135La, 135Ce, 135Pr, 135Nd; compiled, evaluated structure data.
Phys.Rev. C12, 1321 (1975)
E.A.Henry, R.A.Meyer
Systematic Study of the Structure of Odd-Mass Lanthanum Nuclei. II. Levels in 135La from 135Ce Decay
RADIOACTIVITY 135Ce; measured Eγ, Iγ, I(ce), γγ-coin; deduced ICC, log ft. 135La deduced levels, J, π, λ, hindrance factors.
J.Inorg.Nucl.Chem. 37, 2336 (1975)
D.C.Hoffman, J.W.Barnes, B.J.Dropesky, F.O.Lawrence, G.M.Kelley, M.A.Ott
Half-Lives of 129mXe, 131mXe, 133mXe, 133gXe and 135gXe
RADIOACTIVITY 129m,131m,133m,133,135Xe; measured T1/2.
doi: 10.1016/0022-1902(75)80745-7
Nucl.Sci.Eng. 57, 117 (1975)
T.Izak-Biran, S.Amiel
Reevaluation of the Emission Probabilities of Delayed Neutrons from Fission Products
COMPILATION 84,85,86As, 87,88,89Se, 87,88,89,90,91,92Br, 92,93,94Kr, 92,93,94,95,96,97,98Rb, 97,98,99Y, 134,135Sb, 136,137Te, 137,138,139,140,141I, 141,142Xe, 141,142,143,144,145,146Cs; compiled, evaluated delayed neutron emission probabilities.
Progr.Theor.Phys. 53, 489 (1975)
A.Kuriyama, T.Marumori, K.Matsuyanagi, R.Okamoto
Microscopic Structure of a New Type of Collective Excitation in Odd-Mass Mo, Ru, I, Cs and La Isotopes
NUCLEAR STRUCTURE 129,131I, 131,133Cs, 133,135La, 95,97,99Mo, 97,99,101Ru; calculated B(E2).
Z.Phys. A274, 15 (1975)
B.Martin, D.Merkert, J.L.Campbell
Intensity Ratios of L, M, N, O Subshell Conversion Electrons in M3 and M4 Transitions
RADIOACTIVITY 103mRh, 109mAg, 115mIn, 125mTe, 134mCs, 135mBa, 193mIr; measured Eγ, I(ce). 103Rh, 109Ag, 115In, 125Te, 134Cs, 135Ba, 193Ir transitions deduced δ.
Nucl.Phys. A249, 141 (1975)
J.Meyer-ter-Vehn
Collective Model Description of Transitional Odd-A Nuclei (II). Comparison with Unique Parity States of Nuclei in the A = 135 and A = 190 Mass Regions
NUCLEAR STRUCTURE 199Tl, 195Au, 193Hg, 187Ir, 135Pr, 129,131La, 137Nd, 133Ce; calculated levels, K, β.
doi: 10.1016/0375-9474(75)90096-2
J.Phys.Soc.Jap. 38, 322 (1975)
A.Morinaga, K.Hisatake
Penetration Effects for Internal Conversions in the Odd-Mass Isotopes of La and Cs
RADIOACTIVITY 131Ba, 135,137m,139Ce; measured Iγ, I(ce); deduced ICC. 131Cs, 135,137,139La levels deduced γ-mixing.
Nucl.Phys. A253, 231 (1975)
H.Toki, A.Faessler
Asymmetric Rotor Model for Decoupled Bands in Transitional Odd-Mass Nuclei
NUCLEAR STRUCTURE 191,193,195Hg, 189,191,193,195Au, 187,189Ir, 135Pr, 133La; calculated levels, B(λ), μ, quadrupole moment, δ.
doi: 10.1016/0375-9474(75)90129-3
Nucl.Phys. A248, 173 (1975)
S.Ullrich, E.W.Otten
Determination of the Isotopic Shift of the First Resonance Line in Cs(I) Spectrum for the Isotopes 131Cs, 132Cs, and 136Cs
NUCLEAR MOMENTS 131,132,133,134,135,136,137Cs; measured optical isotopic shift; deduced change of mean squared radius, deformation parameters.
doi: 10.1016/0375-9474(75)90161-X
Phys.Rev. C12, 2111 (1975)
J.van Klinken, S.J.Feenstra
Shape Implications of Unhindered 11/2- → 11/2- β Decays in the Region with N < 82 and Z > 50
RADIOACTIVITY 139Eu, 139mSm, 135Pm; measured βγ-coin, γ(t), I(ce); deduced log ft. 139mPm deduced T1/2, J, π. 139Sm deduced K/L.
Nucl.Phys. A247, 59 (1975)
K.Wisshak, H.Klewe-Nebenius, D.Habs, H.Faust, G.Nowicki, H.Rebel
The Level Scheme of 135Pr: Prolate Deformation of the 11/2- Isomer
RADIOACTIVITY 135Nd [from 138Ce(α, 7n), 136Ce(α, 5n)]; measured Eγ, Iγ, γγ-coin, I(ce), E(ce); deduced ICC, K/L. 135Pr deduced levels, J, π. Enriched targets, mass separated sources, Ge(Li) detectors, Si(Li) detector with magnetic filter for background suppression.
NUCLEAR REACTIONS 139La(α, 8n), E=80-104 MeV; measured σ(E, Eγ, θ), γγ-coin. 135Pr deduced levels, J, π. Natural target, Ge(Li) detectors.
doi: 10.1016/0375-9474(75)90277-8
Nucl.Phys. A256, 173 (1976)
A.R.de L.Musgrove, B.J.Allen, J.W.Boldeman, R.L.Macklin
keV Neutron Capture Cross Sections of 134Ba and 136Ba
NUCLEAR REACTIONS 134Ba(n, γ), E=3-60 keV; 136Ba(n, γ), E=3-100 keV; measured σ(n, γ). 135,137Ba deduced resonance parameters.
doi: 10.1016/0375-9474(76)90102-0
Inorg.Nucl.Chem.Lett. 12, 243 (1976)
H.Feuerstein, J.Oschinski
Determination of the Branching Ratios of the Decay of I-135 and Xe-135m
RADIOACTIVITY 135I, 135mXe; measured γ, β branching.
Program and Theses, Proc.25th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Baku, p.98 (1976)
M.G.Gasior, V.G.Kalinnikov, T.Kretsu
Positron Decay of 135Ce and 141Nd
RADIOACTIVITY 135Ce, 141Nd; measured Eβ+; deduced Q+. Mass-separator.
J.Inorg.Nucl.Chem. 38, 1929 (1976)
R.J.Gehrke, R.G.Helmer
Half-Lives of 134La and 132-135Ce
RADIOACTIVITY 134La, 132,133,134,135Ce; measured T1/2.
doi: 10.1016/0022-1902(76)80440-X
Phys.Lett. 65B, 231 (1976)
K.-L.Kratz, W.Rudolph, H.Ohm, H.Franz, G.Herrmann, C.Ristori, J.Crancon, M.Asghar, G.I.Crawford, F.M.Nuh, S.G.Prussin
Decay of Individual Levels in Delayed Neutron Emitters to Excited States in the Final Nuclei
RADIOACTIVITY 85As, 135Sb, 94Rb; measured β-delayed neutrons, γ spectra. 135Te levels deduced delayed neutron branching. 134Te deduced levels.
doi: 10.1016/0370-2693(76)90170-2
Izv.Akad.Nauk SSSR, Ser.Fiz. 40, 1249 (1976); Bull.Acad.Sci.USSR, Phys.Ser. 40, No.6, 125 (1976)
A.I.Levon, O.F.Nemets, V.A.Stepanenko, V.P.Chepak
g-Factors for the 21/2+, 2679-keV 107Cd and 27/2+, 2737-keV 135La Three-Quasi-Particle States
NUCLEAR REACTIONS 105Pd, 133Cs(α, 2nγ), E=27 MeV; measured γ(θ, H, t). 107Cd, 135La deduced g for 3 quasiparticle state.
Phys.Rev. C13, 1544 (1976)
E.Lund, G.Rudstam
Delayed-Neutron Activities Produced in Fission: Mass Range 122-146
RADIOACTIVITY 123,122Ag, 127,128,129,130,131,132In, 128Cd, 133,134Sn, 134,135,136Sb, 136Te, 137,138,139,140,141I, 141,142,143,144,145,146Cs; measured delayed neutrons, T1/2.
Nucl.Instrum.Methods 134, 173 (1976)
E.Lund, G.Rudstam
Spectrometer for Measuring Total Beta Decay Energies
RADIOACTIVITY 127Sn, 106Rh, 135,136I; measured Eβ; deduced Q.
Z.Phys. A277, 107 (1976)
I.-J.Ma, G.zu Putlitz
On the Electric Nuclear Quadrupole Moments of 135,137Ba
NUCLEAR MOMENTS 135,137Ba; measured hfs; deduced quadrupole moment. Level-crossing.
J.Phys.(London) G2, 421 (1976)
D.C.Palmer, R.C.Morgan, J.R.Cresswell, P.D.Forsyth, I.Hall, M.Maynard, D.J.Thomas
Coulomb Excitation of 135Ba
NUCLEAR REACTIONS 135Ba(α, α'γ), E=8.0, 10.0 MeV; measured Coulomb excitation, Iγ. 135Ba levels deduced B(E2), T1/2. Ge(Li) detector.
doi: 10.1088/0305-4616/2/6/010
Thesis, Univ.Grenoble (1976)
R.Sellam
Etude des Etats Isomeriques de μsec des Produits de Fission de l'235U apres Separation en Masse par 'Lohengrin'
RADIOACTIVITY 88mBr, 94m,95m,98m,100mY, 97mSr, 99mZr, 131m,133mSb, 132m,135m,136mXe [from 235U fission]; measured T1/2 in μs range, Eγ, Iγ.
At.Energ. 43, 201 (1977); Sov.At.Energy 43, 828 (1977)
V.A.Anufriev, T.S.Belanova, S.I.Babich, Y.S.Zamyatnin, A.G.Kolesov, E.I.Shkokov, S.M.Kalebin, V.S.Artamonov, R.N.Ivanov
Resonance Parameters of 133Cs and 134Cs Isotopes at Energies up to 400 eV
NUCLEAR REACTIONS 133,134Cs(n, n'), E=th; measured transmission. 133,134Cs deduced neutron resonance parameters.
Nucl.Phys. A275, 229 (1977)
D.D.Bogdanov, A.V.Demyanov, V.A.Karnaukhov, L.A.Petrov, A.Plochocki, V.G.Subbotin, J.Voboril
New Neutron-Deficient Isotopes of Barium and Rare-Earth Elements
RADIOACTIVITY 117,120,122Ba, 129,130,131Pr, 129,130,131,132,133Nd, 132,133,134,135Pm, 133,134,135Sm, 138Eu; measured T1/2, X-ray, γ-ray, delayed proton spectra; deduced average β+ strength functions. Enriched targets, mass-separated heavy-ion reaction products.
doi: 10.1016/0375-9474(77)90285-8
J.Phys.Soc.Jap. 43, 1109 (1977)
J.Chiba, R.S.Hayano, M.Sekimoto, H.Nakayama, K.Nakai
Band Structures of the 135La, 133La and 129Cs Nuclei
NUCLEAR REACTIONS 133Cs, 127I(α, 2n), E=28 MeV; 133Cs(3He, 3n), E=33 MeV; measured Eγ, σ(Eγ, θ), γγ(t). 135,133La, 129Cs deduced levels, K, J, π, T1/2. Natural targets. Ge(Li) detectors.
Nucl.Phys. A292, 144 (1977)
C.Ekstrom, S.Ingelman, G.Wannberg, M.Skarestad
Nuclear Spins and Magnetic Moments of Some Cesium Isotopes
NUCLEAR MOMENTS 120,121,121m,122,122m,123,124,126,128,130m,135mCs; measured J. 121,122,123,124,126,128,130,130mCs; measured a; deduced μ. Atomic-beam magnetic resonance.
doi: 10.1016/0375-9474(77)90363-3
Phys.Lett. 62A, 131 (1977)
H.Kruger, O.Lutz, H.Oehler
Nuclear Magnetic Moments and Ratios of Quadrupole Moments 135Ba, 137Ba, 138La, 139La by NMR Spectroscopy
NUCLEAR MOMENTS 135,137Ba, 138,139La; measured μ, quadrupole moment. NMR.
doi: 10.1016/0375-9601(77)90974-4
Nucl.Phys. A286, 403 (1977)
E.Lund, K.Aleklett, G.Rudstam
Total β-Decay Energies and Masses of Tin, Antimony and Tellurium Isotopes in the Vicinity of 132Sn
RADIOACTIVITY 127,128,129,130,131Sn, 128,130,131,134Sb, 134,135Te; measured β-spectra; deduced Qβ, mass excesses. 127mSn; measured T1/2. 129,131Sb deduced levels. 130mSn deduced Qβ, β-branching, level energy. Comparison with mass formula predictions. Mass-separated fission products.
doi: 10.1016/0375-9474(77)90592-9
Progr.Theor.Phys. 58, 376 (1977)
R.Okamoto
Low-Lying Collective States in Odd-Mass I, Cs, La and Pr N = 80 Isotones
NUCLEAR STRUCTURE 133I, 135Cs, 137La, 139Pr; calculated low-lying collective states.
J.Phys.(Paris) 38, 9 (1977)
B.Pfeiffer, J.P.Bocquet, J.A.Pinston, R.Roussille, M.Asghar, G.Bailleul, R.Decker, J.Greif, H.Schrader, G.Siegert, H.Wollnik, J.Blachot, E.Monnand, F.Schussler
Gamma Spectroscopy of Some Short-Lived Fission Products with the Isotope Separator Lohengrin
RADIOACTIVITY 100Y, 100Zr, 149,150Ce, 150Pr, 136Te, 87Se; measured Eγ, Iγ, T1/2. 149Pr, 135,137Te, 86Se; measured Eγ, Iγ. 88Se; measured Eγ, Iγ; deduced ground state β-branching. 85Se; measured Eγ, Iγ, T1/2; deduced ground state β-branching.
J.Inorg.Nucl.Chem. 39, 753 (1977)
W.Rudolph, K.-L.Kratz, G.Herrmann
Half-Lives, Fission Yields and Neutron Emission Probabilities of Neutron-Rich Antimony Isotopes
RADIOACTIVITY 134,135,136Sb, 136Te; measured T1/2, delayed neutrons.
NUCLEAR REACTIONS 235U(n, F), E=th; measured fission yields, yields for 134,135Sb. 134,135,136Sb, 136Te deduced neutron emission probabilities.
doi: 10.1016/0022-1902(77)80148-6
J.Radioanal.Chem. 36, 591 (1977)
G.Rudstam
Characterization of Delayed-Neutron Spectra
NUCLEAR STRUCTURE 79,80,81Ga, 85As, 87,88,89,90,91Br, 93,94,95Rb, 129,130In, 134,135Sb, 136Te, 137,138,139,140,141I, 142,143,144Cs, 93Kr, 96,97Rb, 97,99Y; analyzed β-delayed neutron spectra features, other data. 235U, 239Pu; analyzed delayed neutron spectra in fission; deduced mass formulae systematic deviations.
KFA-IKP-10/77, p.50 (1977)
R.Sellam, J.P.Bocquet, J.Blachot, E.Monnand, F.Schussler, J.W.Gruter, K.Sistemich
Microsecond Isomers in Fission Products of 235U
RADIOACTIVITY 88mBr, 94m,95mY, 97mSr, 98m,100mY, 99mZr, 131m,133mSb, 132m,135mTe, 136mXe; measured T1/2.
Phys.Rev. C18, 530 (1978)
W.J.Baldridge
Shell-Model Studies for the 132Sn Region. I. Few Proton Cases
NUCLEAR STRUCTURE 135I, 136Xe, 137Cs; calculated levels. Shell model.
Nucl.Phys. A306, 29 (1978)
H.Bartsch, W.Gunther, K.Huber, U.Kneissl, H.Krieger, H.J.Maier
Search for a γ-Decay of the 236U Shape Isomer
RADIOACTIVITY 236mU shape isomer [from 238U(γ, 2n), E=45 MeV bremsstrahlung]; measured Eγ, Iγ; deduced Γγ/Γf.
doi: 10.1016/0375-9474(78)90308-1
Z.Phys. A287, 45 (1978)
J.Crancon, C.Ristori, H.Ohm, W.Rudolph, K.-L.Kratz, M.Asghar
Half-Lives and P(n) Values of Delayed-Neutron Precursors in the Mass Chains 85-87, 92, 135, 136 and 145
RADIOACTIVITY 85,86,87As, 92Br, 135,136Sb, 136Te, 145Cs; measured T1/2, neutron emission probability.
Atlas of Gamma-Ray Spectra from the Inelastic Scattering of Reactor Fast Neutrons, Part I and II, Atomizdat, Moscow (1978)
A.M.Demidov, I.Govor, Yu.K.Cherepantsev, M.R.Ahmed, S.Al-Najjar, M.A.Al-Amili, N.Al-Assafi, N.Rammo
COMPILATION Z=3-92; compiled experimental values of Eγ, Iγ, decay schemes, energy levels.
Hyperfine Interactions 4, 165 (1978)
C.Ekstrom, S.Ingelman, G.Wannberg, M.Skarestad, and the ISOLDE Collaboration
Hyperfine Structure, Nuclear Spins and Moments of Short-Lived Nuclides Studied by On-Line Atomic-Beam Magnetic Resonance Techniques
NUCLEAR MOMENTS 77,78,78m,79,84m,89,90,90mRb, 120,121,121m,122,122m,123,124,126,128,130m,135m,139,140,141,142Cs, 185Au, 208,209,210,211,212,213,220,221,222Fr; measured J. 78m,79Rb, 121,122,123,124,126,128,130,130mCs, 188Au; measured hfs, μ. ABMR.
Z.Phys. A288, 327 (1978)
H.Gerhardt, E.Matthias, F.Schneider, A.Timmermann
Isotope Shifts and Hyperfine Structure of the 6s-7p Transitions in the Cesium Isotopes 133, 135, and 137
NUCLEAR STRUCTURE 133,135,137Cs; measured hfs; deduced isotope shift. Laser spectrometer.
Z.Phys. A288, 11 (1978)
O.Lutz, H.Oehler
135Ba and 137Ba Fourier Transform NMR and NQR Studies
NUCLEAR MOMENTS 135,137Ba, 35Cl; measured Larmor frequencies, μ, atomic shielding, quadrupole moment; deduced hyperfine anomalies.
Proc.Roy.Soc.(London), Ser.A 365, 567 (1979)
P.E.G.Baird, R.J.Brambley, K.Burnett, D.N.Stacey, D.M.Warrington, G.K.Woodgate
Optical Isotope Shifts and Hyperfine Structure in λ553.5 nm of Barium
NUCLEAR MOMENTS 138,137,136,135,134Ba; measured optical isotope shifts, hfs; deduced hyperfine constants. 137,136,135,134Ba deduced charge distribution mean square radius relative to 138Ba. 135Ba deduced quadrupole moment.
Z.Phys. A291, 219 (1979)
K.Bekk, A.Andl, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz
Laserspectroscopic Studies of Collective Properties of Neutron Deficient Ba Nuclei
NUCLEAR MOMENTS 126,129m,129,135mBa; measured optical isotope shift, hfs. 126,129m,129,135mBa deduced differences of rms charge radii, μ, quadrupole moment. Laser spectroscopy. Quasiparticle-plus-triaxial rotor, droplet model.
Nucl.Instrum.Methods 164, 579 (1979)
H.G.Borner, W.F.Davidson, J.Almeida, J.Blachot, J.A.Pinston, P.H.M.Van Assche
High Precision Gamma-Ray Energy Measurements of Fission Products
NUCLEAR REACTIONS 235U, 239Pu(n, F), E=reactor spectrum; measured Eγ. 79Ge, 85,87,88,89,90,91,92,93,94Kr, 92,93,95,98Rb, 92,93,96,98Sr, 92,94,96,97,98,99,100Y, 97,99,100,101Zr, 99,100,101,102,103,104Nb, 99,101,103,104,105,108Mo, 99,101,102,103,104,105,106Tc, 105,109Ru, 105,107,109Rh, 109Pd, 121Cd, 125,128,130,131,132Sn, 128,130,132,133,134Sb, 131,132,133,134,135,136Te, 131,132,133,134,135,136,138,140I, 133,138,139,140,141,142Xe, 138,140,141,143,144,145,146Cs, 139,140,141,142,143,144,145,146Ba, 141,143,144,146,147,148Ce, 140,142,144,146,147,148La, 146,147,148Pr deduced transitions. 234,235U targets.
Z.Phys. A290, 231 (1979)
M.Gustavsson, G.Olsson, A.Rosen
Hyperfine-Structure Investigation in the 6s 5d Configuration of 135Ba and 137Ba
NUCLEAR MOMENTS 135,137Ba; measured hfs. 135,137Ba deduced magnetic dipole, electric quadrupole interaction constants a, b, quadrupole moments. Atomic-beam magnetic resonance method, dye-laser detection.
ATOMIC PHYSICS 135,137Ba; measured hfs. 135,137Ba deduced magnetic dipole, electric quadrupole interaction constants a, b, quadrupole moments. Atomic-beam magnetic resonance method, dye-laser detection.
Z.Phys. A289, 407 (1979)
U.Keyser, H.Berg, F.Munnich, K.Hawerkamp, H.Schrader, B.Pfeiffer, E.Monnand
Experimental Beta-Decay Energies of Several Neutron-Rich Nuclides with Mass Number 131 < A < 146
RADIOACTIVITY 131Sn, 134Sb, 135,136Te, 143,146Ba, 146La; measured Eβ; deduced Qβ. Comparison with mass formulae.
Nucl.Phys. A317, 335 (1979)
K.-L.Kratz, W.Rudolph, H.Ohm, H.Franz, M.Zendel, G.Herrmann, S.G.Prussin, F.M.Nuh, A.A.Shihab-Eldin, D.R.Slaughter, W.Halverson, H.V.Klapdor
Investigation of Beta Strength Functions by Neutron and Gamma-Ray Spectroscopy (I). The Decay of 87Br, 137I, 85As and 135Sb
RADIOACTIVITY 85As, 87Br, 135Sb, 137I [from 235U(n(th), F), fast chemical separations]; measured delayed neutron spectra, γ-ray spectra; deduced β- strength functions. 85Se, 87Kr, 135Te, 137Xe deduced Γn, En, partial n-emission probability.
doi: 10.1016/0375-9474(79)90486-X
INDC(NDS)-107/G+SP, p.103 (1979)
K.-L.Kratz
Review of Delayed Neutron Energy Spectra
COMPILATION 75As, 87Br, 92,93,94,95,96,97,98Rb, 135Sb, 136Te, 137,138I, 141,142,143,144,145,146,147Cs; compiled, evaluated fission product β-delayed neutron spectra; deduced <En>.
Bull.Am.Phys.Soc. 25, No7, 734, CC4 (1980)
E.A.Henry, R.A.Meyer
Possible Evidence for Structural Control of Neutrons Emitted from Levels above Neutron Binding Energy in the Decay Sequence 136Te(β-)136I(n)135I
RADIOACTIVITY 136Te; measured βγ-, γγ-coin, β-delayed En. 135I deduced levels.
Z.Phys. A295, 37 (1980)
W.Jitschin, G.Meisel
Doppler-Free Two-Photon Laser Spectroscopy of Barium I: Hyperfine Splitting and Isotope Shift of High Lying Levels
ATOMIC PHYSICS 134,135,136,137,138Ba; measured optical isotope shift, hfs; deduced configuration interaction effects. Laser spectroscopy.
Z.Phys. A298, 273 (1980)
K.Kawade, G.Battistuzzi, H.Lawin, K.Sistemich, J.Blomqvist
A μs-Isomer in 135Te
RADIOACTIVITY 135Te [from fission product separator]; measured γγ-, (X-ray)γ-coin, (fission fragment)γ-coin, Eγ, Iγ, E(K X-ray), I(K X-ray). 135Te level deduced T1/2. 135Te deduced levels, T1/2, J, π, ICC, γ-multipolarity, B(E2), configuration. 135Sb [from fission product separator]; measured Eγ, Iγ. 135Te level deduced upper limit for Iβ.
Z.Phys. A294, 233 (1980)
E.Lund, P.Hoff, K.Aleklett, O.Glomset, G.Rudstam
Delayed Neutron Emission Probabilities of Gallium, Bromine, Rubidium, Indium, Antimony, Iodine, and Cesium Precursors
RADIOACTIVITY 79,80,81,82,83Ga, 87,88,89Br, 92,93,94,95,96Rb, 127,128,129,130,131,132In, 134,135Sb, 137,138,139I, 141,142,143,144,145Cs [from on-line separation]; measured β-delayed En, Eβ, Iβ; deduced delayed-n emission probabilities. 127,129,132In deduced T1/2.
Z.Phys. A295, 311 (1980)
R.E.Silverans, G.Borghs, G.Dumont, J.M.Van den Cruyce
Collinear Fast Beam-Laser Spectroscopy on 5d2D3/2, 5/2 Barium Ions
NUCLEAR MOMENTS 138,137,136,135,134,132,130Ba; measured optical isotope shift, hfs. 138,137,136,135,134,132,130Ba deduced differences of rms charge radii. 135,137Ba deduced hfs constants.
Spectra of Radiations of Radioactive Nuclides, Publishing House Fan, Tashkent (1980)
Ts.Vylov, V.M.Gorozhankin, Zh.Zhelev, A.I.Ivanov, R.B.Ivanov, V.G.Kalinnikov, M.Ya.Kuznetsova, N.A.Lebedev, M.A.Mikhailova, A.I.Muminov, A.F.Novgorodov, Yu.V.Norseev, Sh.Omanov, B.P.Osipenko, E.K.Stepanov, V.G.Chumin, A.F.Shchus, Yu.V.Yushkevich
RADIOACTIVITY A=1-249; measured Eγ, Iγ, I(ce), Eα, Iα. Other data input.
Bulg.J.Phys. 8, 556 (1981)
A.Abdurazakov, Tz.Vylov, M.Enikova, Zh.Zhelev, T.Islamov, N.Lebedev, G.Kononenko, A.Ioushkevitch
Experimental Study of the Excited Nuclear States in the 50 ≤ Z, N ≤ 82 Region. III. 135La Excited State Features, Determined on the Basis of Electromagnetic Transitions
RADIOACTIVITY 135Ce(EC), (β+); measured Eγ, Iγ, I(ce). 135La deduced levels, J, π, γ-branching, γ-multipolarity, ICC.
JINR-P6-81-565 (1981)
M.Budzynski, N.A.Lebedev, G.I.Lizurei, T.M.Muminov, R.G.Nazmitdinov, Ya.Sarzhinski, T.Khazratov, A.B.Kalikulov
Properties of Excited States in 135La
RADIOACTIVITY 135Ce; measured γγ(θ). 135La levels deduced J, π, γ-multipolarity, δ. Quasiparticle-phonon model.
Nucl.Phys. A359, 9 (1981)
P.Hoff
The Population of Excited States in Residual Nuclei via Delayed Neutrons
RADIOACTIVITY 81Ga, 88,89Br, 93,94,95,96Rb, 135Sb, 138,139I; measured Eγ, Iγ, β-delayed neutrons, Iγ/In. 80Ge, 87,88Kr, 92,93,94,95Sr, 134Te, 137Xe deduced levels.
doi: 10.1016/0375-9474(81)90209-8
Phys.Rev. C23, 1713 (1981)
T.Saito, T.Toriyama, M.Kanbe, K.Hisatake
Atomic Mass Difference Between 135Ce and 135La
RADIOACTIVITY 135Ce [from 139La(p, 5n), E=43 MeV, chemical separation]; measured Eβ+, γγγ-coin; deduced Q(EC). 135La levels deduced γ-branching, EC/β+. 135Ce, 135La deduced mass difference.
Nucl.Phys. A367, 1 (1981)
C.Thibault, F.Touchard, S.Buttgenbach, R.Klapisch, M.De Saint Simon, H.T.Duong, P.Jacquinot, P.Juncar, S.Liberman, P.Pillet, J.Pinard, J.L.Vialle, A.Pesnelle, G.Huber, and the ISOLDE Collaboration
Hyperfine Structure and Isotope Shift of the D2 Line of 118-145Cs and Some of Their Isomers
NUCLEAR MOMENTS 118,119,119m,120,121,121m,122,122m,123,124,125,126,127,128,129,130,130m,131,132,133,134,134m,135,135m,136,136m,137,138,138m,139,140,141,142,143,144,145Cs; measured hfs, hyperfine constants, spins, isotope shifts; deduced μ, quadrupole moment, rms charge radii, deformation parameter β. High-resolution laser spectroscopy on thermal atomic beams.
doi: 10.1016/0375-9474(81)90274-8
Nucl.Instrum.Methods 186, 177 (1981)
H.Wagner, K.Dorschel, C.Hohle, H.Huhnermann, Th.Meier
Laser Fluorescence Spectroscopy on Fast Ion Beams at the Marburg Separator
NUCLEAR MOMENTS 130,132,134,135,136,137,138Ba; measured isotope shifts. Laser fluorescence spectroscopy, fast ions, doppler tuning.
Program and Theses, 32nd Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Kiev, p.78 (1982)
G.D.Alkhazov, V.P.Afanasev, N.Ganbaatar, K.Ya.Gromov, V.G.Kalinnikov, Ya.Kormitski, A.Lyatushinski, K.A.Mezilev, Yu.N.Novikov, V.N.Panteleev, A.G.Polyakov, A.Potempa, E.Senyavski, F.Tarkani, Yu.V.Yushkevich
Short Lived Neutron Deficient Isotopes of the Isobars A = 135 and 136. New Isotope 136Sm
RADIOACTIVITY 135Pm, 136Sm(β+), (EC); measured Eγ, Iγ, E(K X-ray), T1/2. 135Nd deduced levels.
Nucl.Phys. A378, 443 (1982)
G.Audi, M.Epherre, C.Thibault, A.H.Wapstra, K.Bos
Masses of Rb, Cs and Fr Isotopes
ATOMIC MASSES A=74-99; A=117-147; A=204-228; analyzed direct mass measurement data for Rb, Cs, Fr isotopes; deduced mass excesses. 78,81,82,84,86,90,98Rb, 119,121,123,135,116,118,120,122,124,130,134,136,138Cs deduced mass isomeric corrections.
doi: 10.1016/0375-9474(82)90459-6
Nucl.Phys. A382, 501 (1982)
V.S.Butsev, D.Chultem, I.N.Zhivotov
Negative Pion Capture in Atomic Nuclei near the Closed Neutron Shell at N = 82
NUCLEAR REACTIONS 142,143,144,145,146,148,150Nd, 141Pr, 140Ce, 139La, 138Ba(π-, xnyp)138Pr/132La/137Ba/135Ba/133Ba/131Ba/135Cs/134Cs/135Xe/, E at rest; measured Eγ, Iγ; deduced reaction mechanism. 134m,135mCs deduced isomer, J, π, T1/2, σ(production) ratio. 137m,135m,133m,131mBa, 132mLa, 137mCe, 138mPr deduced isomer, J, π. 133,131Ba deduced σ(isomer)/σ(ground state).
doi: 10.1016/0375-9474(82)90357-8
Phys.Rev. C26, 2607 (1982)
Y.-S.Chen, G.A.Leander
Quasicontinuum Properties of M1 Spectra in the Particle-Rotor Model
NUCLEAR STRUCTURE 159,161,163,165,167,169,171,173,175,177Yb, 127,129,131,133,135,137,139Ce, 131Pr, 129La, 127Cs, 125I, 123Sb; calculated M1 quasicontinuum γ-spectra; deduced particle, quasiparticle number dependence. Core-quasiparticle coupling models.
Phys.Lett. 112B, 103 (1982)
H.Dias, F.Krmpotic
Projected BCS-Tamm-Dancoff Approximation with Blocking Effect
NUCLEAR STRUCTURE 135I; calculated levels; deduced blocking effect role. Projected BCS, pairing, TDA.
doi: 10.1016/0370-2693(82)90306-9
Z.Phys. A306, 195 (1982)
P.Grundevik, H.Lundberg, L.Nilsson, G.Olsson
Hyperfine Structure in the 6p5d Configuration and Isotope Shifts in Transitions between the 6s5d and the 6p5d Configurations in Ba I
NUCLEAR MOMENTS 135,137Ba; measured isotope shifts, hfs; deduced electric quadrupole moments. 137,136,135,134,130Ba deduced charge rms radii change relative to 138Ba. High resolution laser fluoresence spectroscopy. Self-consistent field calculations.
Z.Phys. A306, 281 (1982)
P.Grafstrom, Jiang Zhan-Kui, G.Jonsson, S.Kroll, C.Levinson, H.Lundberg, S.Svanberg
Hyperfine Structure and Isotope Shift of Highly Excited Barium-I States
NUCLEAR MOMENTS 135,136,137,138Ba; measured hfs. 135,136,137Ba deduced isotope shift relative to 138Ba. High resolution laser spectroscopy.
J.Phys.(London) B15, 3787 (1982)
J.Neukammer, H.Rinneberg
Configuration Interaction and Singlet-Triplet Mixing Probed by Hyperfine Structure of 6s14d 1D2 and 3D1, 3D2, 3D3 Barium Rydberg States
NUCLEAR MOMENTS 134,135,136,137,138Ba; measured hfs; deduced configuration interaction, singlet-triplet mixing. Optical-optical double resonance technique.
doi: 10.1088/0022-3700/15/21/005
J.Phys.(London) B15, L425 (1982)
J.Neukammer, H.Rinneberg
Hyperfine Structure of Perturbed 6sns 3S1 Rydberg States of Barium
NUCLEAR MOMENTS 135,137Ba; measured hfs. Tunable cw dye lasers.
doi: 10.1088/0022-3700/15/13/002
J.Phys.(London) B15, L723 (1982)
J.Neukammer, H.Rinneberg
Fine Structure Perturbations of Hyperfine Structure of 6snd 3D2 Rydberg States of Barium
NUCLEAR MOMENTS 134,135,136,137,138Ba; measured hfs; deduced fine structure perturbation effects, Rydberg series singlet-triplet mixing parameter.
doi: 10.1088/0022-3700/15/20/001
Z.Phys. A306, 11 (1982)
H.Rinneberg, J.Neukammer, E.Matthias
Isotope Shifts of Perturbed 6sns 1S0 and 3S1 Rydberg States of Odd Barium Isotopes
NUCLEAR MOMENTS 135,137,138Ba; measured optical isotope shifts.
J.Phys.(London) B15, L825 (1982)
H.Rinneberg, J.Neukammer
Hyperfine Structure and Configuration Interaction of the 5d7d 1D2 Perturbing State of Barium
NUCLEAR MOMENTS 134,135,136,137,138Ba; measured hfs, isotope shifts. Tunable cw dye lasers.
doi: 10.1088/0022-3700/15/23/002
Nucl.Sci.Eng. 80, 238 (1982)
G.Rudstam
Six-Group Representation of the Energy Spectra of Delayed Neutrons from Fission
RADIOACTIVITY 87,88,89,90,91,92Br, 84,85,86,87As, 87,88,89,91Se, 92,93,94,95,96,97,98,99Rb, 98m,99,97mY, 137,138,139,140,141I, 134,135,136Sb, 136,137,138Te, 141,142,143,144,145,146,147Cs, 147La, 79,80,81,83Ga, 92,93,94Kr, 127,128,129,130,131,132In, 141,142Xe, 97,98,99Sr, 134Sn, 147,148Ba [from fission]; analyzed β-delayed neutron precursor data; deduced group parameters, average neutron energy.
NUCLEAR REACTIONS, Fission 233U, 241Pu(n, F), E=thermal; 232Th, 236,238U, 237Np, 240,242Pu(n, F), E=0.5 MeV; calculated β-delayed neutron precursor group abundances, decay constants.
RADIOACTIVITY, Fission 252Cf(SF); calculated β-delayed neutron precursor group abundances, decay constants.
Phys.Lett. 112B, 124 (1982)
E.B.Shera, H.D.Wohlfahrt, M.V.Hoehn, Y.Tanaka
Charge Distributions of Barium Isotopes from Muonic X-Rays
NUCLEAR MOMENTS 134,135,136,137,138Ba; measured muonic X-rays; deduced charge distributions, isotope shifts. Droplet model, interacting boson approximation calculations.
ATOMIC PHYSICS, Mesic-Atoms 134,135,136,137,138Ba; measured E(X-ray), I(X-ray); deduced charge distributions, isotope shifts. Droplet model, interacting boson approximation calculations.
doi: 10.1016/0370-2693(82)90311-2
Phys.Rev. C26, 2273 (1982)
W.B.Walters, S.M.Lane, N.L.Smith, R.J.Nagle, R.A.Meyer
Shell Model Description of N = 81 Five-Excition 135Xe and the Decay of 135I
NUCLEAR STRUCTURE 135Xe; calculated levels; deduced configurations. Shell model.
RADIOACTIVITY 135I(β-) [from fission product radiochemical separation]; measured Eγ, Iγ, T1/2, γγ-coin; deduced Iβ, log ft. 135Xe deduced levels, J, π, γ-branching. Shell model.
Z.Phys. A304, 269 (1982)
A.Zemel, C.Broude, E.Dafni, A.Gelberg, M.B.Goldberg, J.Gerber, G.J.Kumbartzki, K.-H.Speidel
Magnetic Moment of the 19/2+ Isomer in 135Ce
NUCLEAR REACTIONS 122Sn(16O, 3n), E=62 MeV; measured Eγ, Iγ, γ(t), recoil, γ(θ, H). 135Ce level deduced g, configuration, T1/2.
Z.Phys. A311, 41 (1983)
W.Becker, G.Werth
Precise Determination of the Ground State Hyperfine Splitting of 135Ba+
NUCLEAR MOMENTS 135Ba; measured hfs. High precision, microwave optical double resonance experiment.
Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2089 (1983)
V.A.Bondarenko, I.L.Kuvaga, P.T.Prokofev, G.L.Rezvaya, T.l.Solomonova
Study of 135Ba by the (n, n'γ)-Reaction
NUCLEAR REACTIONS 135Ba(n, n'γ), E=fast; measured Eγ, Iγ, Iγ(θ); deduced σ(inelastic). 135Ba deduced levels, J, π. Statistical model analysis. Enriched target, Ge(Li) detector.
Lat.PSR Zinat.Akad.Vestis, Fiz.Teh.Ser. No.6, 8 (1983)
V.Bondarenko, N.Kramer, I.Kuvaga, P.Prokofev, G.Rezvaya, T.Solomonova
The γ-Spectrum of 135,137Ba from the (n, n'γ) Reaction
NUCLEAR REACTIONS 135,137Ba(n, n'γ), E=0.1-2.6 MeV; measured Eγ, Iγ. 135,137Ba deduced isomer production σ, γ-branching.
Phys.Rev. C28, 2437 (1983)
Y.S.Chen, S.Frauendorf, G.A.Leander
Shape of Rotating Quasiparticle Orbits and Signature Splitting in La, Ce, and Pr Nuclei
NUCLEAR STRUCTURE 129,130,131,133,134,135Ce, 129,130,133,134La, 130,131,134,135Pr; calculated yrast, near-yrast band Routhians, (γ) deformation signature splitting. Cranking model.
Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2108 (1983)
R.V.Dzholos, Ts.Vylov, Zh.T.Zhelev, M.M.Mikhailova
Study of the Excited States of 135Ba
NUCLEAR STRUCTURE 135Ba; calculated ground state μ, B(λ).
RADIOACTIVITY 135La(EC), (β+); measured Eγ, Iγ, I(ce); deduced log ft. 135Ba levels deduced γ-, EC-branching ratio, ICC, γ-multipolarity.
Z.Phys. A311, 1 (1983)
E.R.Eliel, W.Hogervorst, T.Olsson, L.R.Pendrill
High Resolution Laser Spectroscopy of Low-Lying p-States in Sr I and Ba I
NUCLEAR MOMENTS 84,86,87,88Sr, 134,135,136,137,138Ba; measured hfs, isotope shifts. 87Sr, 135,137Ba deduced hfs constants. High resolution laser spectroscopy in Sr I and Ba I.
J.Phys.(London) B16, 1881 (1983)
E.R.Eliel, W.Hogervorst
Hyperfine Structure in 6snd Rydberg Configurations in Barium
NUCLEAR MOMENTS 135,137Ba; measured hfs; deduced singlet-triplet mixing coefficient asymptotic behavior. Atomic beam two-step excitation, CW dye lasers.
doi: 10.1088/0022-3700/16/11/010
Z.Phys. A312, 1 (1983)
P.Grundevik, M.Gustavsson, G.Olsson, T.Olsson
Hyperfine-Structure and Isotope-Shift Measurements in the 6s5d → 6p5d, 6p5d → 6s5d Transitions of Ba I in the Far-Red Spectral Region
NUCLEAR MOMENTS 135,137Ba; measured optical hfs, isotope shift; deduced magnetic dipole interaction constants. Atomic beam, high resolution laser spectroscopy.
Z.Phys. A310, 19 (1983)
W.Hogervorst, E.R.Eliel
High Resolution Spectroscopy on 6sns Rydberg States of Barium
NUCLEAR MOMENTS 135,136,137,138Ba; measured hfs, isotope shifts. High resolution laser atomic beam experiment.
Nucl.Phys. A408, 109 (1983)
S.T.Hsieh, H.C.Chiang, M.C.Wang
Phenomenological Weak-Coupling Analysis on N = 81 Isotones
NUCLEAR STRUCTURE 135Xe, 137Ba, 139Ce, 141Nd, 143Sm, 134I, 138La, 140Pr, 142Pm, 144Eu; calculated levels, binding energies, spectroscopic factors, B(λ). Phenomenological weak coupling analysis.
doi: 10.1016/0375-9474(83)90352-4
Nucl.Phys. A403, 234 (1983)
A.C.Mueller, F.Buchinger, W.Klempt, E.W.Otten, R.Neugart, C.Ekstrom, J.Heinemeier
Spins, Moments and Charge Radii of Barium Isotopes in the Range 122-146Ba Determined by Collinear Fast-Beam Laser Spectroscopy
NUCLEAR MOMENTS 122,123,125,127,131m,137m,139,140,141,142,143,144,145,146Ba; measured hfs, isotope shifts; deduced hyperfine constants, rms charge radii, deformation β. 123,125,127,129,129m,131,131m,132,133,133m,135,135m,137,137m,139,141,143,145Ba levels deduced J, π, μ, quadrupole moment. Collinear fast beam laser spectroscopy.
NUCLEAR REACTIONS La, U(p, X), E=600 MeV; measured thick target production yields for Ba, Cs isotopes.
doi: 10.1016/0375-9474(83)90226-9
Phys.Rev. A27, 1779 (1983)
H.Rinneberg, J.Neukammer
Hyperfine Structure and Three-Channel Quantum-Defect Theory of 6snd 1D2 Rydberg States of Ba
NUCLEAR MOMENTS 135,137Ba; measured hfs; deduced singlet-triplet mixing coefficients.
Phys.Rev. C29, 1033 (1984)
A.Abbas
Quasi-Shell Closure for Even Z = 58 to 70, N = 82 and the Similarity of these Nuclei
NUCLEAR STRUCTURE 138,137,136,135,134Ba, 140,139,138,137,136Ce, 142,141,140,139,138Nd, 144,143,142,141,140Sm, 146,145,144,142Gd, 148,147,146Dy, 148Er; analyzed yrast levels, other data; deduced seniority mixing, stability, quasishell closure effects.
J.Phys.(London) G10, 1099 (1984)
E.Dragulescu, M.Ivascu, R.Mihu, D.Popescu, G.Semenescu, A.Velenik, V.Paar
Coulomb Excitation of Levels in 135Ba and 137Ba
NUCLEAR REACTIONS 135,137Ba(α, α'), E=9.6-12.2 MeV; 135,137Ba(16O, 16O'), E=35-45 MeV; measured Eγ, Iγ, γ(θ), σ(Eγ, E) following Coulomb excitation. 135Ba(14N, 14N'), E=40 MeV; measured Eγ, Iγ, γ(θ) following Coulomb excitation. 135,137Ba deduced levels, J, π, δ, γ-branching, B(E2). Enriched targets, Ge(Li) detectors, Compton suppression spectrometer.
doi: 10.1088/0305-4616/10/8/015
Bull.Am.Phys.Soc. 29, No.4, 661, BK14 (1984)
J.C.Hill, F.K.Wohn, R.L.Gill, A.Wolf, K.Sistemich
Structure of the N=82 Isotone 135I from the Decay 135Te
RADIOACTIVITY 135Te(β-); measured Eγ, Iγ, γγ-coin. 135I deduced levels, configuration. Shell model calculation.
Nucl.Sci.Eng. 87, 418 (1984)
F.M.Mann, M.Schreiber, R.E.Schenter, T.R.England
Evaluation of Delayed-Neutron Emission Probabilities
RADIOACTIVITY A=79-148; analyzed delayed neutron precursor data; deduced role in fission yields, delayed neutron emission probability systematics.
Z.Phys. A316, 275 (1984)
L.R.Pendrill
Estimation of the Specific Mass Effect in the Isotope Shifts of Energy Levels in the Optical Spectrum of Ba I and Ba II
NUCLEAR MOMENTS 134,135,136,137,138Ba; analyzed optical isotope shift data; deduced specific mass effect estimates.
Z.Phys. A316, 149 (1984)
K.A.H.van Leeuwen, W.Hogervorst
Stark Effect, Hyperfine Structure and Isotope Shifts in Highly Excited States of Ba I and Ca I
ATOMIC PHYSICS 40Ca; measured electric dipole polarizability; deduced departure from quadratic Stark effect, large Rydberg state polarizability role. High resolution laser atomic beam spectroscopy.
NUCLEAR MOMENTS 134,135,136,137Ba; measured hfs, isotope shifts, electric dipole polarizability. 135,137Ba deduced magnetic dipole, electric quadrupole coupling constants. High resolution laser atomic beam spectroscopy.
Priv.Comm. (April 1985)
M.Bogdanovic
Hyperfine Interactions 24, 43 (1985)
B.Cagnac
Applications of the Two-Photon Doppler-Free Method: Hyperfine interactions and isotope shift measurements
NUCLEAR MOMENTS 20,21,22Ne, 4,3He; analyzed hfs, isotope shift data. 203,205Tl, 85,87Rb, 43,40,42,44,48Ca, 86,87,88Sr, 206,207,208Pb, 135,137,138Ba, 113,115In; compiled, evaluated hfs, isotope shift data. Two-photon Doppler-free techniques, theoretical models.
ATOMIC PHYSICS Na, Ne, K, Rb, Ba; analyzed fine structure data. 87Sr; analyzed Rydberg level hfs data; deduced hyperfine constants.
Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 85 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.1, 88 (1985)
M.A.Dolgopolov, I.V.Kopytin
Spin-Orbit Interaction and L-Foridden Proton γ M1-Transitions
NUCLEAR STRUCTURE 133,135,137,139La, 139Pr, 141Pm; calculated levels, B(M1). Finite Fermi system, two-particle spin-orbit interaction.
Nucl.Phys. A437, 1 (1985)
E.Hammaren, K.W.Schmid, F.Grummer, A.Faessler, B.Fladt
Microscopic Description of Odd-Mass Nuclei in the Mass A = 130 Region
NUCLEAR REACTIONS 130,132,134,136Ba(d, p), E not given; calculated spectroscopic amplitudes. Microscopic model.
NUCLEAR STRUCTURE 127,129,131,133Ce, 125,127,129,131Ba, 123,125,127,129Xe, 127,129,131La, 123,125,127,129Cs, 121,123,125,127I; calculated levels, rotational parameters. 132,134,136Ba; calculated one-neutron pickup spectroscopic amplitudes. 130,132,134,136Ba; calculated one-proton stripping, one-proton pickup stripping spectroscopic amplitudes. Microscopic model.
doi: 10.1016/0375-9474(85)90225-8
Phys.Rev.Lett. 55, 1457 (1985); Erratum Phys.Rev.Lett. 55, 2739 (1985)
J.Jolie, P.Van Isacker, K.Heyde, A.Frank
F-Spin Multiplets and Supersymmetry in Nuclei
NUCLEAR STRUCTURE 138,136,134,139,137,135Ce, 130,132,134,131,133,135Ba, 130,128,126,127,129,131Xe, 126,124,122,127,125,123Te; calculated levels, B(E2); deduced F-spin multiplet, supersymmetry connecting group structure. Interacting boson model, U(B)(12) dynamical group.
doi: 10.1103/PhysRevLett.55.1457
Z.Phys. A321, 417 (1985)
M.Kortelahti, R.Julin, J.Hattula, A.Pakkanen, M.Piiparinen
Non-Yrast Level Structure of 135Pr
NUCLEAR REACTIONS 136Ce(p, 2n), E=19.9 MeV; measured σ(Eγ), Eγ, Iγ, γγ-coin, γ(t), γ(θ), I(ce). 135Pr deduced levels, J, π, T1/2, ICC, γ-multipolarity, deformation. Triaxial rotor-plus-particle model.
Z.Phys. A322, 105 (1985)
L.Koester, K.Knopf, W.Waschkowski
Neutron Scattering Lengths and Cross Sections of the Barium Isotopes
NUCLEAR REACTIONS Ba, 130,132,134,135,136,137,138Ba(n, n), E=0.5 meV-132 eV; measured σ, coherent scattering lengths. Ba, 136,137,138Ba deduced absorption, zero-energy σ. Christiansen filter measurements, BaF2, BaCo3, α-BaF2, β-BaF2 compounds.
LPNI-1139 (1985)
I.A.Kondurov, P.A.Sushkov, E.I.Fedorova, M.Bogdanovic, G.Barreau, H.G.Borner, R.Brissot, S.Kerr, H.Seyfarth
High-Energy γ-Lines from 133Cs(n, γ) Reaction and Levels of 134Cs Nucleus
NUCLEAR REACTIONS 133Cs(n, γ), E=1.4-8 MeV; measured Eγ, Iγ. 134Cs deduced levels, γ-branching, neutron binding energy.
Z.Phys. A321, 255 (1985)
M.Samri, G.J.Costa, G.Klotz, D.Magnac, R.Seltz, J.P.Zirnheld
The β Decay of Tellurium 135 and 137
RADIOACTIVITY 135,137Te(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, γγ-, βγ-coin; deduced T1/2, log ft, mass excess. 135,137I deduced levels, J, π, β-branching. Shell model comparison.
Hyperfine Interactions 24, 181 (1985)
R.E.Silverans, G.Borghs, P.De Bisschop, M.Van Hove
Fast Ion Beam Collinear Laser Spectroscopy: Some aspects of recent applications, sensitivity and resolution
NUCLEAR MOMENTS 137,136,135,134,132,130Ba; measured isotope shifts. 137Ba, 87Br; measured hfs. 87Sr deduced g. Fast ion beam collinear laser spectroscopy.
Z.Phys. A321, 215 (1985)
M.Van Hove, G.Borghs, P.De Bisschop, R.E.Silverans
Hyperfine Structure of 5d2D3/2 135,137Ba Ions by Collinear Fast Beam Laser-rf Double Resonance Spectroscopy
NUCLEAR MOMENTS 135,137Ba; measured hfs; deduced coupling constants. Collinear laser-rf double resonance spectroscopy.
Hyperfine Interactions 23, 179 (1985)
D.Wegener
Calculated Perturbed Angular Correlations for 111In Doped Cubic Single Crystals
RADIOACTIVITY 111In(EC); calculated γγ(θ, H, t). Doped cubic single crystals, various low index crystallographic orientations.
J.Phys.(London) B19, L593 (1986)
J.Bauche, H.T.Duong, P.Juncar, S.Liberman, J.Pinard, A.Coc, C.Thibault, F.Touchard, J.Lerme, J.L.Vialle, S.Buttgenbach, A.C.Mueller, A.Pesnelle, and the ISOLDE Collaboration
Accurate Wavenumbers of the First Resonance Doublet of Francium Atoms and Relativistic Contribution to Isotope Shifts in the Resonance Doublets of Francium and Caesium Atoms
RADIOACTIVITY 212,221Fr [from Th, U(p, X), E=600 MeV]; 135,137,139,141,143Cs; measured isotope shifts. Semi-empirical, relativistic Dirac-Fock models.
doi: 10.1088/0022-3700/19/18/001
J.Phys.(Paris) 47, 1709 (1986)
M.A.Bouchiat, J.Guena, L.Pottier, L.Hunter
Atomic Parity Violation Measurements in the Highly Forbidden 6S1/2 - 7S1/2 Caesium Transition. III. Data Acquisition and Processing. Results and Implications
NUCLEAR MOMENTS 135Cs; measured hfs; deduced parity violating effect, nuclear charge, rms radii.
J.Phys.(London) B19, 2853 (1986)
M.Carre, J.Lerme, J.L.Vialle
Larmor Precession Measurement of the Nuclear g(I) Factor of 135,137Ba Isotopes in a Fast Atomic Beam
NUCLEAR MOMENTS 135,137Ba; measured hfs; deduced nuclear Lande g factor. Fast atomic beam laser spectroscopy technique, static magnetic field.
doi: 10.1088/0022-3700/19/18/015
Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1021 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.5, 190 (1986)
M.A.Dolgopolov, I.V.Kopytin
Description of l-Forbidden γ(M1)-Transitions in Odd Nuclei with A ≈ 125
NUCLEAR STRUCTURE 111,113Cd, 117,119Sn, 123,125Te, 131Xe, 133,135,137,139La, 139Pr, 141Pm; calculated B(M1). Finite Fermi system theory.
Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1994 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 120 (1986)
I.A.Kondurov, P.A.Sushkov, E.I.Fedorova, M.Bogdanovich, G.Barro, Kh.G.Berner, P.Brisso, S.Kerr, H.Zaifart
Hard γ-Rays from the Reaction 133Cs(n, γ) and Level Scheme of 134Cs
NUCLEAR REACTIONS 134,133Cs(n, γ), E=thermal; measured Eγ, Iγ. 134Cs deduced levels, neutron binding energy. 135Cs deduced transitions. Pair spectrometer.
Proc.Conf. on Nuclear Structure with Heavy Ions, Bologna, Italy, Vol.2, p.145 (1986)
S.Lunardi, M.Morando, F.Scarlassara, F.Soramel, S.Beghini, C.Signorini, W.Meczynski, W.Starzecki, G.Fortuna, A.M.Stefanini
Nuclear Deformation in Neutron Deficient Samarium Isotopes
NUCLEAR REACTIONS 112,110Cd(32S, xnyp), E=126-170 MeV; 142Nd(α, 6n), E=90 MeV; 106Cd(37Cl, 2np), E=138-145 MeV; 107Ag(32S, 2np), (32S, 2n2p), E=125-150 MeV; measured γ(X-ray)-coin, γγ(t), γ(θ), Doppler shift recoil distance. 136,140,138Sm deduced levels, J, π, T1/2, γ-branching, nuclear deformation characteristics, B(λ). 139Eu, 140Gd, 135Pm deduced levels, J, π, T1/2, γ-branching, B(λ).
Phys.Rev. C34, 523 (1986)
T.M.Semkow, D.G.Sarantites, K.Honkanen, V.Abenante, L.A.Adler, C.Baktash, N.R.Johnson, I.Y.Lee, M.Oshima, Y.Schutz, Y.S.Chen, J.X.Saladin, C.Y.Chen, O.Dietzsch, A.J.Larabee, L.L.Riedinger, H.C.Griffin
Spectroscopic Study of the High-Spin States in 135Pr
NUCLEAR STRUCTURE 135Pr; calculated levels, alignments, crossing frequencies. Cranked shell model.
NUCLEAR REACTIONS 120Sn(19F, 4n), E=91 MeV; measured Eγ, Iγ, γγ(θ). 135Pr deduced levels, J, π, alignments, crossing frequencies, signature splittings, γ-deformation parameter. Cranked shell model comparison.
Phys.Rev. A33, 2117 (1986)
R.E.Silverans, G.Borghs, P.De Bisschop, M.Van Hove
Hyperfine Structure of the 5d 2D(J) States in the Alkaline-Earth Ba Ion by Fast-Ion-Beam Laser-rf Spectroscopy
NUCLEAR MOMENTS 135,137Ba; measured hfs; deduced constants. Collinear fast-beam laser-rf double resonance spectroscopy.
J.Phys.(London) G13, 1269 (1987)
C.E.Alonso, J.M.Arias, M.Lozano
Nuclear Structure Studies of the Odd-Mass Ba and La Isotopes with the IBFA-2 Model
NUCLEAR STRUCTURE 121,123,125,127,129,131,133,134Ba, 127,129,131,133,135,137,139La; calculated levels, B(λ), μ, isotope shifts, charge radii. Interacting boson-fermion model.
doi: 10.1088/0305-4616/13/10/015
Pisma Zh.Eksp.Teor.Fiz. 46, 136 (1987); JETP.Lett.(USSR) 46, 170 (1987)
G.D.Alkhazov, A.E.Barzakh, N.B.Buyanov, V.P.Denisov, V.S.Ivanov, V.S.Letokhov, V.I.Mishin, S.K.Sekatsky, V.N.Fedoseev, I.Ya.Chubukov
Differences in the Isotopic Changes in the Charge Radii of Nuclei with 50 ≤ (N, Z) ≤ 82
RADIOACTIVITY 138,139,140Eu; measured isotope shifts. 137,138,139,140,141,142,143Eu; deduced rms radius isotopic dependence. 127,128,129,130,131,132,133,134,135,136Cs, 128,129,130,131,132,133,134,135Xe, 128,129,130,131,132,133,134,135,136,137Ba, 133,134,135,136,137,138,139,140,141Nd, 137,138,139,140,141,142,143Sm deduced rms radius isotopic dependence.
Phys.Rev. C36, 602 (1987)
C.W.Beausang, L.Hildingsson, E.S.Paul, W.F.Piel, Jr., P.K.Weng, N.Xu, D.B.Fossan
Collective Band Structures in the Odd-Proton Nuclei 135,137Pm
NUCLEAR REACTIONS 116Sn(24Mg, 4np), E=144 MeV; 114Cd(27Al, 4n), E=131 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, σ(Eγ, E). 135,137Pm deduced levels, J, π, γ multipolarity. Enriched targets. Cranked shell model calculations.
Phys.Rev.Lett. 58, 2182 (1987)
E.M.Beck, F.S.Stephens, J.C.Bacelar, M.A.Deleplanque, R.M.Diamond, J.E.Draper, C.Duyar, R.J.McDonald
Superdeformed Band in 135Nd
NUCLEAR REACTIONS 100Mo(40Ar, 5n), E=173, 177 MeV; measured γγ-coin. 135Nd deduced levels, J, π, superdeformed band, moment of inertia.
doi: 10.1103/PhysRevLett.58.2182
Phys.Rev. C36, 974 (1987)
J.Billowes, K.P.Lieb, J.W.Noe, W.F.Piel, Jr., S.L.Rolston, G.D.Sprouse, O.C.Kistner, F.Christancho
Lifetime and g-Factor Measurements of Yrast States in 134Nd and 136Nd
NUCLEAR REACTIONS 110Pd(28Si, 4n), (30Si, 4n), E=120-125 MeV; measured nγ-coin, recoil distance Doppler shift. 76Ge(62Ni, 4n), (62Ni, 3n), (64Ni, 4n), (64Ni, 5n), E=235 MeV; measured nγ-coin vs H, γ-anisotropy. 136,134Nd deduced levels, J, π, T1/2, transition quadrupole moment, B(λ), g-factors. 135Nd level deduced g. 146,148Nd(16O, 16O'), E=38 MeV; measured γ correlation anisotropy following Coulomb excitation; deduced Nd paramagnetic relaxation time in Ni.
Bull.Am.Phys.Soc. 32, No.8, 1563, CD5 (1987)
F.P.Calaprice, M.Kitano, M.Pitt, J.Clayhold, M.Kadar-Kallen, M.Musolf, W.Happer, G.Ulm, K.Wendt, T.Chupp, J.Bonn, R.Neugart, E.Otten, H.T.Duong, and the ISOLDE Collaboration
Nuclear Alignment and Magnetic Moments of 135Xe and 135mXe by Spin Exchange Optical Pumping
RADIOACTIVITY 135m,135Xe; measured γ(θ), NMR, aligned nuclei; deduced μ.
Rev.Roum.Phys. 32, 485 (1987)
E.Dragulescu, M.Ivascu, M.Ionescu-Bujor, A.Iordachescu, C.Petrache, D.Popescu, G.Pascovici, G.Semenescu, M.Duma, I.Gurgu, F.Baciu, R.A.Meyer, V.Paar, S.Brant, D.Vorkapic, D.Vretenar, H.Ajazaj
High-Spin Spectroscopy of Pr Nuclei
NUCLEAR REACTIONS 118,119,120,122,124Sn, 121,123Sb, 125,126,128,130Te, 136,138Ce(19F, X), (16O, X), (14N, X), E not given; measured Eγ, Iγ, γ(θ), γγ(t), X-ray(γ)(t). 133,134,135,136,137,138,139Pr deduced levels, J, π, band structure, γ-branching. In-beam γ-ray spectroscopy. Interacting boson model calculations.
Rev.Roum.Phys. 32, 743 (1987)
E.Dragulescu, M.Ivascu, D.Popescu, G.Semenescu, I.Gurgu, L.Marinescu, F.Baciu
Levels in 134,135,136Ba Excited by the (9Be, xnγ) Reactions
NUCLEAR REACTIONS 128,130Te(9Be, xn), E=30-37 MeV; measured σ(E, Eγ), γ-spectra. 134,135,136Ba deduced levels, band characteristics.
Rev.Roum.Phys. 32, 947 (1987)
E.Dragulescu, M.Ivascu, C.Petrache, D.Popescu, G.Semenescu, M.Duma, I.Gurgu, F.Baciu, S.Brant, V.Paar, D.Vorkapic
Shape Transition in Pr Nuclei
NUCLEAR REACTIONS 118,119,120Sn(19F, xn), E=72-76 MeV; 125Te(14N, 4n), E=52-58 MeV; measured γγ(t), γ(X-ray)(t), σ(Eγ, E). 133,135Pr deduced levels, J, π.
J.Phys.(London) G13, L149 (1987)
M.M.Michailova
Application of Spinor Symmetry to 131,133Xe and 135Ba
NUCLEAR STRUCTURE 131,133Xe, 135Ba; calculated levels, B(E2). Spinor symmetry.
doi: 10.1088/0305-4616/13/8/004
J.Phys.(London) G13, L201 (1987)
S.M.Mullins, R.Wadsworth, J.M.O'Donnell, P.J.Nolan, A.J.Kirwan, P.J.Bishop, M.J.Godfrey, D.J.G.Love
First Observation of the i13/2 Neutron Orbital in the A = 130 Region: Spectroscopy of 135Sm
NUCLEAR REACTIONS 92Mo(46Ti, n2p), E=210 MeV; 64Zn(74Se, n2p), E=290 MeV; measured Eγ, Iγ, γγ-, γ(recoil nucleus)-coin, γγ(θ). 135Sm deduced levels, J, π, γ-branching, configuration, band structure. Ge detectors, bismuth germanate suppression shields, recoil separator, enriched targets. Cranked shell model.
doi: 10.1088/0305-4616/13/9/006
Phys.Rev. C35, 959 (1987)
W.F.Piel, Jr., C.W.Beausang, D.B.Fossan, L.Hildingsson, E.S.Paul
Collective Band Structures in the γ-Soft Nucleus 135Nd
NUCLEAR REACTIONS 112Cd(27Al, 3np), E=110-142 MeV; measured γ(θ), γγ-coin. 116Sn(24Mg, 3n2p), E=124-144 MeV; measured γγ-coin. 135Nd deduced levels, J, π, δ, band structure, B(λ) ratios, configuration. Enriched targets, n-type Ge detectors, bismuth germanate anti-Compton shields. Cranked shell model calculations.
Nucl.Data Sheets 52, 205 (1987)
Yu.V.Sergeenkov
Nuclear Data Sheets for A = 135
COMPILATION 135Sb, 135Te, 135I, 135Xe, 135Cs, 135Ba, 135La, 135Ce, 135Pr, 135Nd, 135Pm, 135Sm; compiled, evaluated structure data.
J.Phys.(London) B20, 2383 (1987)
W.Vassen, E.Bente, W.Hogervorst
CW Laser Excitation of the Barium 6sng and 6snh Rydberg Series from the Metastable 6s5d 1,3D and 5d2 1G4 States
NUCLEAR MOMENTS 137,135Ba; measured hfs. 132,134,130,136Ba deduced isotope shift relative to 138Ba.
doi: 10.1088/0022-3700/20/11/010
J.Phys.(London) G13, 205 (1987)
R.Wadsworth, J.M.O'Donnell, D.L.Watson, P.J.Nolan, P.J.Bishop, D.J.Thornley, A.Kirwan, D.J.G.Love
Lifetimes of Low-Lying Levels in Light Rare Earth Nuclei around A = 135
NUCLEAR REACTIONS 46Ti, 50Cr(92Mo, X)132Nd/134Nd/133Pm/135Pm/134Sm/136Sm, E=210, 230 MeV; measured Eγ, Iγ, nγ-coin, residual nucleus recoil distances. 132,134Nd, 133,135Pm, 134,136Sm deduced T1/2, B(E2), deformations. Enriched targets. Model comparison.
doi: 10.1088/0305-4616/13/2/009
J.Phys.(London) G13, L207 (1987)
R.Wadsworth, A.Kirwan, D.J.G.Love, Y.-X.Luo, J.-Q.Zhong, P.J.Nolan, P.J.Bishop, M.J.Godfrey, R.Hughes, A.N.James, I.Jenkins, S.M.Mullins, J.Simpson, D.J.Thornley, K.L.Ying
The New Spectroscopy of Superdeformed States: Systematics in the light rare earths and unexpected feeding patterns
NUCLEAR REACTIONS 104Pd(32S, 2n2p), (32S, n2p), E=152 MeV; 104Ru(34S, 4n), (34S, 3n), E=155 MeV; 104Ru(36S, 4n), (36S, 3n), E=150 MeV; 104Ru(34S, 4np), E=162 MeV; 106Pd(34S, 4np), (34S, 4n), E=152 MeV; 100Mo(36S, 4n), E=150 MeV; measured Eγ, Iγ, γγ-coin. 132Ce, 133,134,135,137Nd deduced transitions, feeding level J, π, dynamical moments of inertia, superdeformed bands.
doi: 10.1088/0305-4616/13/9/007
Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 1651 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.8, 170 (1988)
G.D.Alkhazov, A.E.Barzakh, N.B.Buyanov, V.P.Denisov, V.S.Ivanov, V.S.Letokhov, V.I.Mishin, S.K.Sekatsky, V.N.Fedoseev, I.Ya.Chubukov
Trends in Mean-Square Charge Radius and Electromagnetic Moments for Samarium and Neodymium Isotopes having N < 82
NUCLEAR STRUCTURE 147,144,143,142,141,141m,140,139,138Sm; 143,142,141,140,139,138,137,136,135,134,132Nd; analyzed isotope shift, hyperfine constants data; deduced rms charge radius, μ, quadrupole moments systematics.
Phys.Rev. C37, 370 (1988)
A.Goswami, S.Bhattacharya, M.Saha, S.Sen
Band Structure in 133,135Pr
NUCLEAR STRUCTURE 133,135Pr; calculated levels, γ-branching ratio.
Phys.Rev. C38, 2902 (1988)
L.Losano, H.Dias, F.Krmpotic, B.H.Wildenthal
Comparisons between Shell-Model Calculations, Seniority Truncation, and Quasiparticle Approximations: Application to the odd Ni isotopes and odd N = 82 isotones
NUCLEAR STRUCTURE 59,61,63,65Ni, 135I, 137Cs, 139La, 141Pr, 143Pm; calculated levels, μ, quadrupole moments, B(λ). Shell model.
ORNL/TM-10766 (1988)
R.L.Macklin
Search for 136Xe Resonance Neutron Capture
NUCLEAR REACTIONS 136Xe(n, γ), E=2.154-18.4 keV; measured capture σ(E); deduced σ(thermal).
ATOMKI 1987 Ann.Rept., p.39 (1988)
B.M.Nyako, M.Jozsa, L.Zolnai, V.Barci, J.Gizon
Search for Unfavoured Transitions in 135La and 129Cs
NUCLEAR REACTIONS 133Cs, 127I(α, 2n), E=20 MeV; measured γγ-coin, energy correlation.
Phys.Scr. T23, 37 (1988)
J.Simpson
Nuclear Shapes and Phases at Very High Spin
NUCLEAR REACTIONS 114Cd, 108Pd(48Ca, 4n), E=205 MeV; analyzed data. 152Dy, 158Er deduced levels, superdeformed band features.
NUCLEAR STRUCTURE 133,135,137Nd, 131Ce; analyzed data; deduced superdeformed band features.
J.Phys.(London) G14, 239 (1988)
R.Wadsworth, J.M.O'Donnell, D.L.Watson, P.J.Nolan, A.Kirwan, P.J.Bishop, M.J.Godfrey, D.J.Thornley, D.J.G.Love
Investigation of the Band Structure of 132,134Nd and 135Pm at Medium Spin
NUCLEAR REACTIONS 92Mo(46Ti, 2pα), (46Ti, 4p), (46Ti, 3p), E=210 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 132,134Nd, 135Pm deduced levels, J, π, band characteristics, γ-multipolarity. Model calculations.
NUCLEAR STRUCTURE 132,134Nd, 135Pm; calculated levels, band characteristics.
doi: 10.1088/0305-4616/14/2/016
Z.Phys. A329, 407 (1988)
K.Wendt, S.A.Ahmad, C.Ekstrom, W.Klempt, R.Neugart, E.W.Otten
Hyperfine Structure and Isotope Shift of the Neutron-Rich Barium Isotopes 139-146Ba and 148Ba
NUCLEAR MOMENTS 134,135,136,137,138Ba; measured isotope shift, hfs; deduced hyperfine parameters. 134,135,136,137Ba level deduced μ, electric quadrupole moment, rms charge radius.
RADIOACTIVITY 139,140,141,142,143,144,145,146,148Ba; measured isotope shift, hfs; deduced hyperfine parameters. 139,140,141,142,143,144,145Ba level deduced μ, electric quadrupole moment, rms charge radius. 146Ba deduced rms charge radius.
Phys.Lett. 215B, 211 (1988)
R.Wyss, J.Nyberg, A.Johnson, R.Bengtsson, W.Nazarewicz
Highly Deformed Intruder Bands in the A ≈ 130 Mass Region
NUCLEAR STRUCTURE A ≈ 130; calculated total routhians; deduced model parameters. 131,132Ce; calculated total routhians. 135Nd, 132Ce; calculated moments of inertia; deduced deformed band features. Deformed shell model.
doi: 10.1016/0370-2693(88)91422-0
J.Nucl.Sci.Technol.(Tokyo) 25, 641 (1988)
K.Yamada, N.Ozaki, M.Yamamoto, K.Ueyanagi
Separation of Barium Isotopes by Selective Two-Step Photoionization Process
NUCLEAR MOMENTS 130,132,134,135,136,137,138Ba; measured hfs, isotope shifts. Two-step photoionization process.
Thesis, Texas A-M Univ. (1989); LA-11534-T (1989)
M.C.Brady
Evaluation and Application of Delayed Neutron Precursor Data
COMPILATION 79,80,81Ga, 85As, 87,88,89,90,91,92Br, 92,93,94,95,96,97,98Rb, 129,130In, 134,135Sb, 136Te, 137,138,139,140,141I, 141,142,143,144,145,146,147Cs; compiled, evaluated β-delayed neutron spectra, precursor data.
Z.Phys. A332, 407 (1989)
P.Hoff, B.Ekstrom, B.Fogelberg
The Low Energy β-Strength of 135Sb
RADIOACTIVITY 135Sb(β-); measured Eγ, Iγ, γγ-coin; deduced β-strength function. 135Te deduced levels, configuration.
Z.Phys. A332, 229 (1989)
M.O.Kortelahti, H.K.Carter, R.A.Braga, R.W.Fink, B.D.Kern
Non-Yrast Level Structure of 135Nd via Beta Decay of 135Pm
RADIOACTIVITY 135Pm(β+), (EC) [from 92Mo(46Ti, X), E=240 MeV]; measured γγ-coin, I(ce). 135Nd deduced levels, possible J, π.
Thesis, Univ.York (1989)
S.M.Mullins
Normal and Highly Deformed Rotational Bands in 135Sm and 133Nd
NUCLEAR REACTIONS 64Zn(74Se, n2p), E=290 MeV; 92Mo(46Ti, n2p), E=210 MeV; 104Pd(32S, n2p), E=152 MeV; measured γγ-coin, DSA. 135Sm deduced levels, band structure, configuration. 133Nd deduced levels, J, π, superdeformed band, quadrupole moment. Cranked shell model, total Routhian surface calculations.
At.Data Nucl.Data Tables 42, 189 (1989)
P.Raghavan
Table of Nuclear Moments
COMPILATION Z=1-99; compiled μ, electric quadrupole moments.
doi: 10.1016/0092-640X(89)90008-9
Nucl.Phys. A499, 1 (1989)
K.S.Vierinen, J.M.Nitschke, P.A.Wilmarth, R.B.Firestone, J.Gilat
Decay of Neutron Deficient Eu, Sm and Pm Isotopes Near the Proton Drip Line
RADIOACTIVITY 134,135,136Eu, 134,135,136Sm, 134,135,136Pm(β+p) [from 92Mo(46Ti, xnyp), E=192-212 MeV mass separated sources]; measured T1/2, β-delayed Ep, Ip, Eγ; deduced log ft, γγ-, (X-ray)γ-, βγ-, p(X-ray)-, pγ-coin. 135,136Sm, 134,135,136Pm, 134,135,136Nd deduced levels, J, π. n-Ge, planar Ge, plastic scintillator, surface barrier Si(Au) detectors, ΔE-E telescope, enriched targets.
doi: 10.1016/0375-9474(89)90266-2
Phys.Rev. C41, R1327 (1990)
R.M.Diamond, C.W.Beausang, A.O.Macchiavelli, J.C.Bacelar, J.Burde, M.A.Deleplanque, J.E.Draper, C.Duyar, R.J.McDonald, F.S.Stephens
Line Shape and Lifetimes in the 135Nd Superdeformed Band
NUCLEAR REACTIONS 100Mo(40Ar, 5n), E=175 MeV; measured γγγ-coin, DSA. 135Nd deduced levels, J, π, superdeformed band features, transition quadrupole moment.
doi: 10.1103/PhysRevC.41.R1327
Z.Phys. A337, 131 (1990)
V.Lopac, S.Brant, V.Paar
Quantum Chaos for N = 79 Nuclei in the IBFM Model
NUCLEAR STRUCTURE 131Te, 135Ba, 137Ce; calculated levels, spectral rigidity. Quantum chaos, interacting boson-fermion model.
Phys.Rev. C41, 2624 (1990)
R.Ma, E.S.Paul, D.B.Fossan, Y.Liang, N.Xu, R.Wadsworth, I.Jenkins, P.J.Nolan
Rotational Bands in 135Ce: Collective prolate and oblate rotation
NUCLEAR REACTIONS 122Sn(18O, 5n), E=85, 89 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 135Ce deduced levels, J, π, γ-multipolarity, band features, alignment, Routhians. Cranked shell model.
Proc.8th Seminar on Precise Measurements in Nucl.Spectrosc., Uzhgorod, p.55 (1990)
N.M.Miftakhov, A.A.Rodionov, Yu.P.Smirnov, V.V.Fedorov
Measurements of Magnetic Moments of 114In, 123,125Te, 133,135Ba, 191Os Nuclei
NUCLEAR MOMENTS 114In, 123,125Te, 133,135Ba, 191Os; measured X-ray hyperfine shifts; deduced μ. Bend-crystal spectrometer.
Priv.Comm. (1990)
R.Neugart
NUCLEAR STRUCTURE 117,119,121,123,125,125m,127,127m,129,129m,131,131m,133,133m,135,135m,137,139,141,143Xe; compiled μ, quadrupole moment data.
Phys.Rev. C42, R1805 (1990)
P.H.Regan, R.Wyss, R.Wadsworth, D.B.Fossan, Y.-J.He, J.R.Hughes, I.Jenkins, R.Ma, M.S.Metcalfe, S.M.Mullins, P.J.Nolan, E.S.Paul, R.J.Poynter, N.Xu
Lifetime Measurements in 135Sm: Large deformation in the N = 6 intruder band and evidence for quenched proton pairing
NUCLEAR REACTIONS 92Mo(46Ti, n2p), E=210 MeV; measured γ-spectra, DSA. 135Sm levels deduced T1/2, deformed band quadrupole moment.
doi: 10.1103/PhysRevC.42.R1805
Phys.Rev.Lett. 65, 3104 (1990)
H.Stolzenberg, St.Becker, G.Bollen, F.Kern, H.-J.Kluge, Th.Otto, G.Savard, L.Schweikhard, G.Audi, R.B.Moore
Accurate Mass Determination of Short-Lived Isotopes by a Tandem Penning-Trap Mass Spectrometer
ATOMIC MASSES 118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,135,137Cs; measured masses. Tandem Penning-trap mass spectrometer, comparison with other methods.
doi: 10.1103/PhysRevLett.65.3104
Thesis, State Univ.of New York (1990); Diss.Abst.Int. 51B, 2954 (1990)
N.Xu
High-Spin Studies for the N = 78 Odd-A Isotones in the A ≈ 130 Mass Region
NUCLEAR REACTIONS 128Te(11B, 4n), E=57-61 MeV; 122Sn(19F, 4n), E=81 MeV; 116Cd(27Al, 4n), E=124 MeV; 110Cd(35Cl, 2n2p), E=167 MeV; measured γγ-coin, γ(t), Eγ, Iγ. 135La deduced high-spin levels, J, π, γ-multipolarity, B(λ) ratios. 137Pr, 139Pm, 141Eu deduced high-spin levels.
Bull.Am.Phys.Soc. 35, No.4, 996, G6 4 (1990)
N.Xu, Y.Liang, R.Ma, E.S.Paul, D.B.Fossan
High Spin States in the Odd-Z 135La Nucleus
NUCLEAR REACTIONS 128Te(11B, 4nγ), E=61 MeV; measured not given. 135La deduced levels, J, π, band structure, configuration.
Astrophys.J. 375, 823 (1991)
H.Beer
Capture Cross Section Measurements of Krypton and Xenon Isotopes and the Fundamental Parameters of the s-Process
NUCLEAR REACTIONS 78,80,84,86Kr, 124,126,128,132,134,136Xe(n, γ), E=low; measured capture σ; deduced s-process fundamental parameters. Neutrons from 7Li(p, n) reaction, fast cyclic activation technique.
doi: 10.1086/170246
Phys.Rev. C43, 2586 (1991)
J.A.C.Goncalves, R.N.Saxena
Directional Correlations of γ Transitions in 135Xe following the Decay of 135I
RADIOACTIVITY 135I [from 235U(n, F)]; measured γγ(θ). 135Xe levels deduced J, π, δ(E2/M1). Ge, Ge(Li) detectors.
J.Phys.(London) G18, 1177 (1992)
V.S.Letokhov, V.I.Mishin, S.K.Sekatsky, V.N.Fedoseyev, G.D.Alkhazov, A.E.Barzakh, V.P.Denisov, V.E.Starodubsky
Laser Spectroscopic Studies of Nuclei with Neutron Number N < 82 (Eu, Sm and Nd Isotopes)
RADIOACTIVITY 135,137,139,141Nd, 139,141,141m,143,145Sm; measured hfs; deduced parameters a, b, quadrupole moments. 132,134,135,136,137,138,139,140,141Nd, 138,139,140,141,141m,142,143,145Sm, 138,139,140,141,142,143,144,145Eu; measured isotope shifts; deduced mean square charge radii. Resonance ionization spectroscopy.
NUCLEAR MOMENTS 142Nd, 144Sm; measured isotope shifts; deduced mean square charge radii. Resonance ionization spectroscopy.
doi: 10.1088/0954-3899/18/7/008
J.Phys.(London) G18, 847 (1992)
P.H.Regan, R.Wadsworth, S.M.Mullins, J.Nyberg, A.Atac, S.A.Forbes, D.B.Fossan, Y.-J.He, J.R.Hughes, I.Jenkins, R.Ma, M.S.Metcalfe, P.J.Nolan, E.S.Paul, R.J.Poynter, D.Santonicio, A.Virtanen, N.Xu
Measurement of the Intrinsic Quadrupole Moments in the νi13/2 Bands of 135,137Sm
NUCLEAR REACTIONS 92Mo(46Ti, n2p), E=210 MeV; 104Pd(37Cl, 3np), E=168 MeV; measured γγ-coin, DSA. 137Sm deduced levels, J, π, T1/2, deformation parameter β2, quadrupole moments, band structure. 135Sm deduced levels, J, π, T1/2, deformation parameter β2, quadrupole moments, band structure, superdeformation features.
doi: 10.1088/0954-3899/18/5/013
Hyperfine Interactions 75, 85 (1992)
P.B.Semmes
Nuclear Spins and Moments: Fundamental structural information
NUCLEAR STRUCTURE 133Pm, 135,133Sm; calculated μ. Particle-rotor model.
Phys.Rev. C46, R39 (1992)
J.-y.Zhang, J.R.Hughes
Search for Identical Bands at Normal Deformation in the A = 130 Mass Region
NUCLEAR STRUCTURE 117,119,121,123,125,127,129,131Xe, 121,123,125,127,129,131Ba, 127,129,131,133,135Ce, 133,135,137Nd, 133,135,137,139Sm, 119,121,123,125,127,129,131Cs, 123,127,129,131,133La, 131,133,135,137Pr, 135,137,139Pm, 139,141Eu; analyzed transition energies average deviation. Identical bands, normal deformation, cancellation picture.
Nucl.Phys. A551, 54 (1993)
V.A.Bondarenko, I.L.Kuvaga, P.T.Prokofjev, V.A.Khitrov, Yu.V.Kholnov, L.H.Kkhem, Yu.P.Popov, A.M.Sukhovoi, S.Brant, V.Paar, V.Lopac
Thermal-Neutron-Capture Studies on 135Ba
NUCLEAR REACTIONS 134Ba(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin; deduced σ (tot), isomer production σ. 135Ba deduced levels, J, π, γ-branching ratios. Comparison with calculations of interacting boson-fermion model. Enriched target, hyperpure Ge detectors.
doi: 10.1016/0375-9474(93)90303-F
Bull.Rus.Acad.Sci.Phys. 57, 50 (1993)
V.A.Bondarenko, I.L.Kuvaga, L.K.Khiem, Yu.P.Popov, P.T.Prokofev, A.M.Sukhovoy, P.D.Khang, V.A.Khitrov, Yu.V.Kholnov
γ-Decay of 135Ba Compound State
NUCLEAR REACTIONS 134Ba(n, γ), E=thermal; measured γγ-coin, Iγ. 135Ba deduced levels, two quantum cascade Iγ. Enriched target.
Proc.6th Intern.Conf.on Nuclei Far from Stability + 9th Intern.Conf.on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R.Neugart, A.Wohr, Eds., p.575 (1993)
J.Breitenbach, R.A.Braga, J.L.Wood, P.B.Semmes, J.Kormicki
Deformation Studies in the Extremely Neutron-Deficient Praseodymium, Neodymium and Promethium Isotopes
RADIOACTIVITY 137,133,135Eu, 137Sm, 133,135,137Pm, 133,135,137Nd(β+), (EC); measured Eγ, Iγ, E X-ray, I(ce), γγ(t), γ(X-ray)(t), (ce)γ(t), (ce)(X-ray)(t). 133Pm deduced levels. 133Nd deduced levels, isomer decay features.
Phys.Rev. C48, 109 (1993)
R.E.Chrien, B.K.S.Koene, M.L.Stelts, R.A.Meyer, S.Brant, V.Paar, V.Lopac
Neutron-Capture Gamma-Ray Study of Levels in 135Ba and Description of Nuclear Levels in the Interacting-Boson-Fermion Model
NUCLEAR REACTIONS Ba, 134Ba(n, γ), E=thermal, resonance; measured Eγ, Iγ. 135Ba deduced levels, J, π, spin cut off parameters. Interacting-boson-fermion, cluster vibration models.
Phys.Lett. 312B, 272 (1993)
S.M.Mullins, J.Nyberg, A.Maj, M.S.Metcalfe, P.J.Nolan, P.H.Regan, R.Wadsworth, R.A.Wyss
Population Effects in the Highly-Deformed Bands of 131Ce and 135Nd from 18,16O-Induced Reactions
NUCLEAR REACTIONS 117Sn(18O, 4n), E=85 MeV; measured Eγ, Iγ, γγ-coin, DSA. 122Te(16O, 3n), E=85 MeV; measured Eγ, Iγ, γγ-coin. 131Ce, 135Nd deduced levels, J, π, highly deformed band structure.
doi: 10.1016/0370-2693(93)91080-7
J.Phys.(London) G19, L23 (1993)
E.S.Paul, C.W.Beausang, R.M.Clark, R.A.Cunningham, P.Fallon, S.A.Forbes, C.J.Gross, F.Hannachi, A.N.James, A.Korichi, P.J.Nolan, J.Simpson, R.Wadsworth, J.N.Wilson
Resolution of the Highly Deformed Band Assignment Anomaly in 134Nd/131Ce
NUCLEAR REACTIONS 104Ru(32S, xnypzα), E=155, 160 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin; deduced relative Iγ for many exit channels. 133,135Nd, 131Ce deduced highly deformed bands.
doi: 10.1088/0954-3899/19/2/004
At.Data Nucl.Data Tables 53, 1 (1993)
G.Rudstam, K.Aleklett, L.Sihver
Delayed- Neutron Branching Ratios of Precursors in the Fission Product Region
COMPILATION A=75-150; compiled β--decay T1/2, neutron emission probability; deduced average delayed-neutron branching ratios.
RADIOACTIVITY 80,81,83,79,82Ga, 84Ge, 84,85,86,87As, 88,89,91,87Se, 100,99,98mY, 100,98Sr, 99,98,97,96,95,94,93,92Rb, 91,90,89,88,87Br, 129m,129,130m,131,128m,128,132In, 150,149,148,147La, 149,148,147,146Ba, 148,147,146,145,144,143,142,141Cs, 139,138,137I, 137,136Te, 136,135,134Sb, 134,133Sn(β-n); measured β-, neutron activity simultaneously; deduced revised neutron emission probability, T1/2, delayed neutron branching ratios.
J.Phys.(London) B26, 4289 (1993)
P.Villemoes, A.Arnesen, F.Heijkenskjold, A.Wannstrom
Isotope Shifts and Hyperfine Structure of 134-138Ba II by Fast Ion Beam-Laser Spectroscopy
NUCLEAR MOMENTS 134,135,136,137,138Ba; measured hfs, isotope shifts; deduced magnetic dipole, electric quadrupole hyperfine parameters for 135,137Ba. Ion beam-laser spectroscopy.
doi: 10.1088/0953-4075/26/22/030
Phys.Rev. C47, 1428 (1993)
P.K.Weng, P.F.Hua, S.G.Li, S.X.Wen, L.H.Zhu, L.K.Zhang, G.J.Yuan, G.S.Li, P.S.Yu, C.X.Yang, X.F.Sun, Y.X.Guo, X.G.Lei
High Spin Structure in Odd-Proton Nuclei 129,131Pr
NUCLEAR REACTIONS 107Ag(28Si, 2n2p), (28Si, 4n2p), E=128 MeV; 116Sn(19F, 4n), E=93 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), K X-ray spectra. 129,131Pr deduced levels, J, π, configuration, γ-multipolarity, band structure. 107Ag(28Si, xnypzα), E=120-144 MeV; measured σ(E) for production of 129,131Pr, 128Ce, 132Nd. Cranked shell model comparison.
NUCLEAR STRUCTURE 129,131,133,135,137Pr; calculated levels; deduced systematics. Cranked shell model.
Phys.Rev. C48, R494 (1993)
P.Willsau, H.Hubel, R.M.Diamond, M.A.Deleplanque, A.O.Macchiavelli, J.R.Oliveira, F.S.Stephens, H.Kluge, J.A.Becker, E.A.Henry, A.Kuhnert, M.Stoyer
Lifetimes of the Decay from Superdeformed to Normal Deformed in 135Nd
NUCLEAR REACTIONS 100Mo(40Ar, 5n), E=175 MeV; measured γγ-coin, Doppler shift recoil distance. 135Nd deduced superdeformed states T1/2, transition probabilities, quadrupole moments.
Phys.Lett. 331B, 19 (1994)
M.Bernas, S.Czajkowski, P.Armbruster, H.Geissel, Ph.Dessagne, C.Donzaud, H.-R.Faust, E.Hanelt, A.Heinz, M.Hesse, C.Kozhuharov, Ch.Miehe, G.Munzenberg, M.Pfutzner, C.Rohl, K.-H.Schmidt, W.Schwab, C.Stephan, K.Summerer, L.Tassan-Got, B.Voss
Projectile Fission at Relativistic Velocities: A novel and powerful source of neutron-rich isotopes well suited for in-flight isotopic separation
NUCLEAR REACTIONS Pb(238U, F)86Ge/88As/89As/90Se/96Kr/103Y/104Y/105Y/106Zr/107Zr/108Nb/109Nb/110Nb/111Mo/112Mo/113Mo/114Tc/115Tc/116Ru/118Ru/118Rh/119Rh/120Rh/121Rh/121Pd/122Pd/123Pd/125Ag/126Ag/135Sn/136Sn/137Sn/137Sb/138Sb/139Sb/139Te/140Te/141Te/142Te/143I/144I/147Xe/151Ba/151La/152La/153La/153Ce/154Ce/155Ce, E at 750 MeV/nucleon; measured reaction products; deduced projectile fission fragment yields, production σ. Fragment separator, energy-loss, tof techniques.
doi: 10.1016/0370-2693(94)90937-7
Phys.Rev. C50, 2582 (1994)
F.Voss, K.Wisshak, K.Guber, F.Kappeler, G.Reffo
Stellar Neutron Capture Cross Sections of the Ba Isotopes
NUCLEAR REACTIONS 134,135,136,137Ba(n, γ), E=5-225 keV; measured capture σ(E); deduced stellar neutron capture σ for kT=10 to 100 keV.
Acta Phys.Pol. B26, 221 (1995)
M.A.Deleplanque
New Features in Superdeformed Nuclei
NUCLEAR REACTIONS 100Mo(40Ar, X), E=176, 182 MeV; measured γγγ-coin. 135Nd deduced superdeformed band to normal states linking transitions features. Data on 194Hg, 153Dy discussed.
Phys.Rev. C52, R2302 (1995)
M.A.Deleplanque, S.Frauendorf, R.M.Clark, R.M.Diamond, F.S.Stephens, J.A.Becker, M.J.Brinkman, B.Cederwall, P.Fallon, L.P.Farris, E.A.Henry, H.Hubel, J.R.Hughes, W.Korten, I.Y.Lee, A.O.Macchiavelli, M.A.Stoyer, P.Willsau, J.E.Draper, C.Duyar, E.Rubel
Low-Spin Termination of the Superdeformed Band in 135Nd
NUCLEAR REACTIONS 100Mo(40Ar, 5n), E=176-182 MeV; measured γγγ-coin, Eγ, Iγ. 135Nd deduced high-spin levels, J, π, superdeformed band decay, termination.
doi: 10.1103/PhysRevC.52.R2302
J.Phys.(London) G21, 1491 (1995)
J.Toivanen, J.Suhonen
Microscopic Quasiparticle-Phonon Description of Odd-A Xe Isotopes
NUCLEAR STRUCTURE 127,129,131,133Xe; calculated levels. 127,133,135Xe, 129,131Cs, 131,133I; calculated Gamow-Teller β-decay log ft. Microscopic quasiparticle-phonon model.
doi: 10.1088/0954-3899/21/11/007
Can.J.Phys. 73, 484 (1995)
W.A.van Wijngaarden, J.Li
Hyperfine Splittings and Isotope Shifts of (6s)2 1S0 → (6s6p) 1P1 Transition in Barium
NUCLEAR MOMENTS 135,136,137,138Ba; measured hfs, isotope shifts; deduced magnetic dipole, electric quadrupole hyperfine coupling constants.
Bull.Rus.Acad.Sci.Phys. 59, 1851 (1995)
G.V.Veselov, V.A.Sergienko, A.V.Potempa, K.Ya.Gromov, V.G.Kalinnikov, N.Yu.Kotovsky, V.I.Fominykh, M.B.Yuldashev
Determination of β-Decay Energy for A = 134-141 Nuclei of Rare-Earth Elements
RADIOACTIVITY 135,137,138,139,140,134Pm(β+); 137Sm(β+), (EC); 139,140,141Eu(β+), (EC); 134Pr(β+), (EC); measured β endpoint energies, Q(EC).
Nucl.Phys. A608, 176 (1996)
A.V.Afanasjev, I.Ragnarsson
The Coexistence of the Intruder νi13/2, Superdeformed and Terminating Bands in the A ∼ 135 Mass Region
NUCLEAR STRUCTURE 131,132,133Ce, 133,135,137Nd; Z=57-61; N=72-78; analyzed high-spin spectra systematics in mass region where superdeformed bands are observed; deduced coexistence with intruder, terminating bands. Configuration-dependent shell correction approach, cranked Nilsson potential.
doi: 10.1016/S0375-9474(96)00257-6
Nucl.Phys. A597, 427 (1996)
A.Granderath, P.F.Mantica, R.Bengtsson, R.Wyss, P.von Brentano, A.Gelberg, F.Seiffert
Shapes and Rotational Structures of Neutron h11/2 Configurations in the Xe-Ba-Ce Region
NUCLEAR STRUCTURE 127,131Ce; analyzed experimental Routhians. 129,117,119,121,123,125,127Xe, 127,129,133,131,135Ce, 121,123,125,127,129,131,133Ba; analyzed band structure systematics, spectra; calculated signature splitting, crossing frequencies, rotational bands; deduced decoupling parameter. Strutinsky mean field concept.
doi: 10.1016/0375-9474(95)00484-X
Phys.Rev. C54, 1463 (1996)
P.E.Koehler, R.R.Spencer, R.R.Winters, K.H.Guber, J.A.Harvey, N.W.Hill, M.S.Smith
Resonance Neutron Capture and Transmission Measurements and the Stellar Neutron Capture Cross Sections of 134Ba and 136Ba
NUCLEAR REACTIONS 134,136Ba(n, γ), (n, X), E=20 eV-500 keV; measured capture σ(E), transmission; deduced σ vs E; calculated astrophysical reaction rates. 135,137Ba levels deduced l, J, π, Γn, Γγ, (gΓnΓγ)/Γ. Enriched targets. R-matrix analysis.
Int.J.Mod.Phys. E5, 153 (1996)
L.Losano, H.Dias
Quasiparticle and Phonon Excitations in Odd-Mass N = 83 Isotones
NUCLEAR STRUCTURE 135Te, 137Xe, 139Ba, 141Ce, 143Nd, 145Sm, 147Gd, 149Dy, 151Er; calculated levels J, π, spectroscopic factors. Quasiparticle-phonon coupling model.
doi: 10.1142/S0218301396000074
Priv.Comm. (1996)
S.Mullins
NUCLEAR STRUCTURE 135Sm; measured not given; deduced high-spin levels associated γ transitions.
Z.Phys. A356, 227 (1996)
S.Xu, Y.Xie, Z.Li, R.Ma, Y.Ge, C.Wang, B.Guo, J.Xing, W.Huang, T.Zhang, Z.Liu, S.Zhu
New β-Delayed Proton Precursor 135Gd
NUCLEAR REACTIONS 106Cd(32S, 3n), E=171 MeV; measured γ(X-ray)p-coin, β-delayed proton spectrum. 135Gd deduced T1/2.
RADIOACTIVITY 135Gd(β+p) [from 106Cd(32S, 3n), E=171 MeV]; measured γ(X-ray)p-coin, β-delayed proton spectrum, T1/2.
Nucl.Instrum.Methods Phys.Res. A383, 441 (1996)
M.Yoshida, T.Oishi, T.Honda, T.Torii
A Calibration Technique for Gas-Flow Ionization Chambers with Short Half-Lived Rare Gases
RADIOACTIVITY 41Ar, 133Xe, 135Xe(β-) [from 40Ar, 132Xe, 134Xe(n, γ);E=reactor]; measured Eγ, Iγ; deduced prepared gas purity.
doi: 10.1016/S0168-9002(96)00834-0
Phys.Rev.Lett. 77, 3743 (1996)
C.T.Zhang, P.Bhattacharyya, P.J.Daly, R.Broda, Z.W.Grabowski, D.Nisius, I.Ahmad, T.Ishii, M.P.Carpenter, L.R.Morss, W.R.Phillips, J.L.Durell, M.J.Leddy, A.G.Smith, W.Urban, B.J.Varley, N.Schulz, E.Lubkiewicz, M.Bentaleb, J.Blomqvist
Yrast Excitations Around Doubly Magic 132Sn from Fission Product γ-Ray Studies
RADIOACTIVITY 248Cm(SF); measured γγ-coin; deduced possible accepted masses inconsistencies for N=82 isotones. 132,134Te, 135I deduced yrast high-spin levels, J, π, configuration.
doi: 10.1103/PhysRevLett.77.3743
Phys.Rev. C56, R16 (1997); Comment Phys.Rev. C59, 546 (1999)
F.Andreozzi, L.Coraggio, A.Covello, A.Gargano, T.T.S.Kuo, A.Porrino
Structure of Neutron-Rich Nuclei Around 132Sn
NUCLEAR STRUCTURE 134Te; calculated levels, B(λ), binding energies, g, μ. 135I calculated levels, binding energies. Shell model, realistic effective interaction.
Nucl.Phys. A626, 343c (1997)
D.Beck, and the ISOLDE Collaboration
Direct Mass Measurements of Unstable Rare Earth Isotopes with the ISOLTRAP Mass Spectrometer
ATOMIC MASSES 123,125,127,131Ba, 133,134,135,136,137Pr, 132,134,135,136,137,138Nd, 136,137,138,139,140m,141,143Pm, 136,137,138,139,140,141g,141m,142,143Sm, 139,141,142m,143,144,145,146,147,148,149Eu, 148,149,154Dy, 150Ho; measured cyclotron frequency; deduced masses. Penning trap mass spectrometer, on-line isotope separation.
doi: 10.1016/S0375-9474(97)00556-3
Phys.Rev. C56, R2363 (1997)
P.Bhattacharyya, C.T.Zhang, B.Fornal, P.J.Daly, Z.W.Grabowski, I.Ahmad, T.Lauritsen, L.R.Morss, W.R.Phillips, J.L.Durell, M.J.Leddy, A.G.Smith, W.Urban, B.J.Varley, N.Schulz, E.Lubkiewicz, M.Bentaleb, J.Blomqvist
Yrast States of Neutron-Rich N = 83 Nuclei from Fission Product γ-Ray Studies
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 134Sb, 135Te, 136I deduced levels, possible J, π, configurations. Shell model analysis.
doi: 10.1103/PhysRevC.56.R2363
Z.Phys. A358, 203 (1997)
P.J.Daly, C.T.Zhang, P.Bhattacharyya, R.Broda, Z.W.Grabowski, D.Nisius, I.Ahmad, M.P.Carpenter, L.R.Morss, W.R.Phillips, J.L.Durell, M.J.Leddy, A.G.Smith, W.Urban, B.J.Varley, N.Schulz, E.Lubkiewicz, M.Bentaleb, J.Blomqvist
Few-Valence-Particle Excitations Around Doubly Magic 132Sn
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-, (X-ray)γ-coin. 134Te, 135I deduced high-spin levels, J, π, configurations, γ-branching.
J.Phys.(London) G23, 1183 (1997)
S.Flibotte, J.M.Nieminen
Superdeformation: A tool to study fusion reactions
NUCLEAR REACTIONS 116Sn(30Si, X), 70Ge(76Ge, X), E not given; analyzed GDR spectra vs γ multiplicity; 64Ni(74Ge, X), E=239 MeV; 112Cd(26Mg, X), E=94 MeV; analyzed compound-nucleus spin distribution; 64Ni(74Ge, 2n), (74Ge, 4n), E=239 MeV; analyzed relative σ. 134,135,136Nd deduced superdeformed band feeding enhancement related features.
doi: 10.1088/0954-3899/23/10/005
Nucl.Sci.Eng. 126, 324 (1997)
R.C.Greenwood, K.D.Watts
Delayed Neutron Energy Spectra of 87Br, 88Br, 89Br, 90Br, 137I, 138I, 139I, and 136Te
RADIOACTIVITY 87,88,89,90Br, 137,138,139I, 136Te(β-); measured delayed En, In. Isotope separation on line.
Phys.Rev. C56, 2865 (1997)
P.Hoff, J.P.Omtvedt, B.Fogelberg, H.Mach, M.Hellstrom
The Z = 52 and N = 84 Nucleus 136Te: Low spin states observed in the decay of 136Sb
RADIOACTIVITY 136Sb(β-); measured Eγ, Iγ, γγ-, βγ-coin, log ft. 136Sb deduced ground state J, π. 136Te deduced levels, J, π, configurations. Data from other N=84 nuclei compared.
Z.Phys. A358, 217 (1997)
W.Korten, B.Schulze, H.Hubel, S.Chmel, A.Gorgen, U.J.van Severen, W.Pohler, R.Zinken, T.Hartlein, C.Ender, F.Kock, P.Reiter, D.Schwalm, F.Schindler, J.Gerl, R.Schubart, F.Azaiez, S.Bouneau, J.Duprat, I.Deloncle
Conversion-Electron Spectroscopy in the Decay of Superdeformed 135Nd
NUCLEAR REACTIONS 124Te(16O, 5n), E=111 MeV; measured Eγ, Iγ, γγ-, (ce)γ-coin. 135Nd deduced high-spin, superdeformed band linking transitions ICC, γ-multipolarity, no evidence for E0 transitions. Mini-orange filter detectors.
Phys.Rev. C55, R2760 (1997)
R.Krucken, I.Y.Lee
Do Superdeformed Bands Decay Via Electric Monopole Transitions ( Question )
NUCLEAR STRUCTURE 194Pb, 133,135Nd; calculated E0 transition strength between normal deformed, superdeformed states; deduced transition probability, branching ratios.
doi: 10.1103/PhysRevC.55.R2760
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.
Phys.Rev.Lett. 78, 3832 (1997)
J.M.Nieminen, S.Flibotte, M.Cromaz, A.Galindo-Uribarri, G.Gervais, D.S.Haslip, V.P.Janzen, D.C.Radford, C.E.Svensson, J.C.Waddington, D.Ward, J.N.Wilson
Enhancement of Superdeformed Band Population in 135Nd
NUCLEAR REACTIONS 64Ni(74Ge, X), 112Cd(26Mg, X), E not given; measured γγ-coin; deduced 134,135,136Nd, 132Ce production relative σ. 135Nd deduced superdeformed band population enhancement entrance channel dependence.
doi: 10.1103/PhysRevLett.78.3832
Bull.Rus.Acad.Sci.Phys. 61, 1611 (1997)
A.M.Sukhovoi, V.A.Khitrov
Cascade Gamma Decay of the Compound State of Heavy Nucleus as Seen Experimentally
NUCLEAR REACTIONS 113Cd, 127I, 123Te, 134,136,137,138Ba, 142,143,145Nd, 149Sm, 155,157Gd, 159Tb, 165Ho, 162,163,164Dy, 167Er, 169Tm, 173,174,176Yb, 175,176Lu, 177,178,179,180Hf, 195Pt, 199Hg, 181Ta, 182,186W, 191Ir, 197Au(n, γ), E=thermal; analyzed γ spectra, γγ-coin. 114Cd, 124Te, 137,138,139Ba, 146Nd, 150Sm, 156,158Gd, 160Tb, 164Dy, 168Er, 170Tm, 174Yb, 181Hf, 196Pt, 200Hg, 182Ta, 183W, 192Ir, 198Au deduced two-quantum cascade intensities vs excitation energy, level density parameters, pairing features.
Acta Phys.Pol. B28, 233 (1997)
C.T.Zhang, P.Bhattacharyya, P.J.Daly, , R.Broda, Z.W.Grabowski, D.Nisius, I.Ahmad, T.Ishii, M.P.Carpenter, L.R.Morss, W.R.Phillips, J.L.Durell, M.J.Leddy, A.G.Smith, W.Urban, B.J.Varley, N.Schulz, E.Lubkiewicz, M.Bentaleb, J.Blomqvist
Shell-Model High-Spin Yrast States of Fission Product Nuclei Above Doubly Magic 132Sn
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 134Te, 135I deduced levels, J, π, configurations. Shell model analysis.
Eur.Phys.J. A 1, 359 (1998)
B.Aengenvoort, W.Korten, H.Hubel, S.Chmel, A.Gorgen, U.J.van Severen, W.Pohler, R.Zinken, T.Hartlein, C.Ender, F.Kock, P.Reiter, D.Schwalm, F.Schindler, J.Gerl, R.Schubart, F.Azaiez, S.Bouneau, J.Duprat, I.Deloncle
Conversion-Electron Gamma-Ray Coincidence Spectroscopy of Superdeformed 135Nd
NUCLEAR REACTIONS 124Te(16O, 5n), E=111 MeV; measured Eγ, Iγ, E(ce), I(ce), γγ-, (ce)γ-coin. 135Nd deduced high-spin, superdeformed levels, J, π, linking transitions, no E0 transitions. Mini-orange spectrometers.
Eur.Phys.J. A 3, 109 (1998)
P.Bhattacharyya, C.T.Zhang, P.J.Daly, B.Fornal, Z.W.Grabowski, I.Ahmad, T.Lauritsen, L.R.Morss, W.Urban, A.Nowak, W.R.Phillips, J.L.Durell, M.J.Leddy, A.G.Smith, B.J.Varley, N.Schulz, E.Lubkiewicz, M.Bentaleb, J.Blomqvist
Three-Valence-Particle Fission Product 51135Sb84
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 135Sb deduced levels, possible J, π, configurations. Eurogam II array.
Phys.Rev. C58, 3726 (1998)
S.Botelho, W.A.Seale, L.G.R.Emediato, J.R.B.Oliveira, M.N.Rao, R.V.Ribas, N.H.Medina, E.W.Cybulska, M.A.Rizzutto, F.R.Espinoza-Quinones, G.Garcia-Bermudez, H.Somacal, M.A.Cardona
Lifetime Measurements in 135Pr
NUCLEAR REACTIONS 123Sb(16O, 4n), E=76 MeV; measured Eγ, Iγ, DSA. 135Pr levels deduced T1/2, B(E2). TRS calculations.
Eur.Phys.J. A 1, 407 (1998)
C.Donzaud, S.Czajkowski, P.Armbruster, M.Bernas, C.Bockstiegel, P.Dessagne, H.Geissel, E.Hanelt, A.Heinz, C.Kozhuharov, Ch.Miehe, G.Munzenberg, M.Pfutzner, W.Schwab, C.Stephan, K.Summerer, L.Tassan-Got, B.Voss
Low-Energy Fission Investigated in Reactions of 750 AMeV 238U-Ions on 208Pb. II: Isotopic distributions
NUCLEAR REACTIONS Pb(238U, X), E=750 MeV/nucleon; measured projectile fission fragments mass, charge, velocity distributions, production σ, low-energy fission component features; deduced evidence for 90,91Se, 96Kr, 103,104,105Y, 106,107Zr, 108,109,110Nb, 111,112,113Mo, 114,115Tc, 116,117,118Ru, 118,119,120,121Rh, 121,122,123Pd, 125,126Ag, 135,136,137Sn, 137,138,139Sb, 139,140,141,142Te. Fragment separator.
Phys.Rev. C58, 3212 (1998)
N.J.O'Brien, R.Wadsworth, D.E.Archer, P.Fallon, I.M.Hibbert, D.T.Joss, D.R.LaFosse, P.J.Nolan, E.S.Paul, J.Pfohl, M.A.Riley, D.G.Sarantites, R.Wyss
Highly Deformed Structures in 135, 136Sm
NUCLEAR REACTIONS 105Pd(35Cl, 3np), (35Cl, 4np), E=180 MeV; measured Eγ, Iγ, (charged particle)γ-, γγ-coin. 135,136Sm deduced high-spin levels, J, π, highly-deformed rotational bands. Cranked shell model calculations. Gammaspere, Microball.
Phys.Rev. C57, R10 (1998)
C.M.Petrache, R.Wyss, Zs.Podolyak, D.Bazzacco, G.de Angelis, D.de Acuna, M.De Poli, A.Dewald, E.Farnea, J.Gableske, A.Gadea, S.Lunardi, D.R.Napoli, M.N.Rao, C.Rossi Alvarez, T.Scanferla, C.A.Ur, R.Venturelli, P.von Brentano, L.H.Zhu
Lifetime Measurements of Highly Deformed Bands in 134,135Nd and 131Ce
NUCLEAR REACTIONS 110Pd(28Si, 3n), (28Si, 4n), (28Si, 3nα), E=132 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin, DSA. 134,135Nd, 131Ce deduced high-spin levels T1/2, quadrupole moments, deformation, configurations.
Nuovo Cim. 111A, 657 (1998)
C.M.Petrache, Zs.Podolyak, D.Bazzacco, S.Lunardi, R.Menegazzo, M.N.Rao, C.Rossi Alvarez, T.Scanferla, C.A.Ur, R.Venturelli, G.de Angelis, D.de Acuna, M.de Poli, E.Farnea, A.Gadea, D.R.Napoli, A.Dewald, J.Gableske, P.von Brentano, R.Wyss
Deformation of Highly Deformed Bands in Nd Nuclei
NUCLEAR REACTIONS 110Pd(28Si, 3n), (28Si, 4n), (28Si, 3nα), E=132 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin, DSA. 131Ce, 134,135Nd deduced high-spin levels T1/2, quadrupole moments. GASP array.
Nucl.Data Sheets 84, 115 (1998)
Yu.V.Sergeenkov, B.Singh
Nuclear Data Sheets for A = 135
COMPILATION 135Sn, 135Sb, 135Te, 135I, 135Xe, 135Cs, 135Ba, 135La, 135Ce, 135Pr, 135Nd, 135Pm, 135Sm, 135Eu, 135Gd; compiled, evaluated structure data.
Nucl.Phys. A628, 41 (1998)
J.Suhonen, J.Toivanen, A.Holt, T.Engeland, E.Osnes, M.Hjorth-Jensen
Study of Odd-Mass N = 82 Isotones with Realistic Effective Interactions
NUCLEAR STRUCTURE 135I, 137Cs, 139La, 141Pr, 143Pm, 145Eu; calculated levels, J, π. Microscopic quasiparticle-phonon model, realistic G-matrix-based effective interactions.
doi: 10.1016/S0375-9474(97)00615-5
Nucl.Phys. A644, 277 (1998)
G.N.White, N.J.Stone, J.Rikovska, S.Ohya, J.Copnell, T.J.Giles, Y.Koh, I.S.Towner, B.A.Brown, B.Fogelberg, L.Jacobsson, P.Rahkila, M.Hjorth-Jensen
Magnetic Dipole Moments Near 132Sn: New measurement on 135I by NMR/ON
RADIOACTIVITY 135I(β-) [from 233U(n, F), E=thermal]; measured Iγ(θ, H, T), NMR on oriented nuclei. 135I deduced ground state g, μ. Shell model, core polarization, mesonic exchange currents.
NUCLEAR STRUCTURE 125,127,129,131,133Sb, 133,135I, 137Cs, 139La; calculated μ. Shell model.
doi: 10.1016/S0375-9474(98)00597-1
Nucl.Phys. A651, 3 (1999)
F.Ames, G.Audi, D.Beck, G.Bollen, M.de Saint Simon, R.Jertz, H.-J.Kluge, A.Kohl, M.Konig, D.Lunney, I.Martel, R.B.Moore, T.Otto, Z.Patyk, H.Raimbault-Hartmann, G.Rouleau, G.Savard, E.Schark, S.Schwarz, L.Schweikhard, H.Stolzenberg, J.Szerypo, and the ISOLDE Collaboration
High-Accuracy Mass Determination of Unstable Cesium and Barium Isotopes
ATOMIC MASSES 117,118,119,120,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142Cs, 123,124,125,126,127,128,131,138,139,140,141,142,143,144Ba; measured masses. Online mass spectrometry, Penning trap, least-squares adjustment of data. Macroscopic-microscopic model calculations.
doi: 10.1016/S0375-9474(99)00111-6
Yad.Fiz. 62, No 5, 892 (1999); Phys.Atomic Nuclei 62, 832 (1999)
S.T.Boneva, E.V.Vasilieva, L.I.Simonova, V.A.Bondarenko, A.M.Sukhovoi, V.A.Khitrov
(n, γ) Reactions in Heavy Nuclei: Manifestations of nuclear structure at excitation energies up to the neutron binding energy
NUCLEAR REACTIONS 113Cd, 123,124Te, 127I, 134,136,137,138Ba, 139La, 142,143,145Nd, 149Sm, 155,157Gd, 159Tb, 162,163,164Dy, 165Ho, 167Er, 169Tm, 173,174,176Yb, 175,176Lu, 177,178,179,180Hf, 181Ta, 182,186W, 187,189Os, 191Ir, 195Pt, 197Au, 199Hg(n, γ), E not given; analyzed two-photon γ cascade data; deduced structure effects.
Pramana 53, 447 (1999)
E.Dragulescu, G.Semenescu, I.Iftimia
Nuclear Structure Studies of Nuclei Near N = 80
NUCLEAR STRUCTURE 135,136Ba, 136La, 137Ce, 139Nd; analyzed data; deduced levels, J, π. Comparison with IBM calculations.
Phys.Rev.Lett. 82, 1823 (1999)
B.Fogelberg, K.A.Mezilev, H.Mach, V.I.Isakov, J.Slivova
Precise Atomic Mass Values Near 132Sn: The resolution of a puzzle
RADIOACTIVITY 131,132Sn, 131,132,133Sb, 132,133,134Te, 132,133,134,135I, 133,135Xe(β-); measured βγ-coin; deduced Qβ, mass excess. 131,132In, 133,134Sn, 134Sb(β-); analyzed data; deduced Qβ, mass excess. Comparison with previous results, theory. Shell model analysis.
ATOMIC MASSES 131,132Sn, 131,132,133Sb, 132,133,134Te, 132,133,134,135I, 133,135Xe(β-); measured βγ-coin; deduced Qβ, mass excess. 131,132In, 133,134Sn, 134Sb(β-); analyzed data; deduced Qβ, mass excess. Comparison with previous results, theory. Shell model analysis.
doi: 10.1103/PhysRevLett.82.1823
Acta Phys.Pol. B30, 1219 (1999)
B.Fornal, R.Broda, W.Krolas, T.Pawlat, J.Wrzesinski, P.J.Daly, P.Bhattacharyya, Z.W.Grabowski, C.T.Zhang, D.Bazzacco, S.Lunardi, C.Rossi Alvarez, G.Viesti, G.De Angelis, M.Cinausero, D.R.Napoli
Spectroscopy at the Neutron-Rich Edge of β-Stability Valley
NUCLEAR REACTIONS 208Pb(76Ge, X)211Po, E=450 MeV; measured Eγ, Iγ, γγ-coin, γγ(t). 211Po deduced yrast high-spin states J, π, isomer T1/2 and B(E3). Shell model comparison. GASP array.
RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 135Te deduced yrast high-spin levels, J, π. Shell model comparison. GASP array.
Phys.Rev. C60, 034301 (1999)
T.Klemme, A.Fitzler, A.Dewald, S.Schell, S.Kasemann, R.Kuhn, O.Stuch, H.Tiesler, K.O.Zell, P.von Brentano, D.Bazzacco, F.Brandolini, S.Lunardi, C.M.Petrache, C.Rossi Alvarez, G.De Angelis, P.Petkov, R.Wyss
Lifetimes Measurements for 134Nd and Neighboring Nuclei with the Coincidence-Plunger Technique
NUCLEAR REACTIONS 110Pd(28Si, xnyp)134Nd/130Ce/131Ce/132Ce/133Pr/134Pr/135Nd, E=125 MeV; measured Doppler shifted Eγ, Iγ(θ), γγ-coin. 134,135Nd deduced high-spin levels, J, π, T1/2, B(E2), deformation. 130,131,132Ce, 133,134Pr levels deduced T1/2, B(E2), transition quadrupole moments. Rotor Model and Interacting Boson Model Calculations. GASP array, coincidence recoil-distance method.
doi: 10.1103/PhysRevC.60.034301
Phys.Rev. C60, 011303 (1999)
F.G.Kondev, M.A.Riley, D.J.Hartley, T.B.Brown, R.W.Laird, M.Lively, J.Pfohl, R.K.Sheline, E.S.Paul, D.T.Joss, P.J.Nolan, S.L.Shepherd, R.M.Clark, P.Fallon, D.G.Sarantites, M.Devlin, D.R.LaFosse, F.Lerma, R.Wadsworth, I.M.Hibbert, N.J.O'Brien, J.Simpson, D.E.Archer
Differential Quadrupole Moment Measurements of the 1/2+ [660](i13/2) Neutron Intruder Band in 133Nd and 135Nd
NUCLEAR REACTIONS 105Pd(35Cl, 2npα), (35Cl, 2n3p), E=173 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin, DSA. 133,135Nd deduced rotational bands quadrupole moments. Gammasphere, Microball arrays.
doi: 10.1103/PhysRevC.60.011303
Nucl.Phys. A650, 133 (1999)
G.A.Lalazissis, D.Vretenar, P.Ring
Ground-State Properties of Deformed Proton Emitters in the Relativistic Hartree-Bogoliubov Model
NUCLEAR STRUCTURE Z=53-69; calculated one-proton separation energy, ground-state deformations for odd-Z nuclei near drip line. 107,108,109I, 111,112,113Cs, 115,116La, 119,120Pr, 124,125Pm, 130,131Eu, 135,136Tb, 140,141Ho, 145,146,147Tm; calculated ground-state deformation, configurations, single-particle levels. Relativistic Hartree-Bogoliubov model. Comparisons with data, other models.
doi: 10.1016/S0375-9474(99)00121-9
Eur.Phys.J. A 8, 307 (2000)
D.Beck, F.Ames, G.Audi, G.Bollen, F.Herfurth, H.-J.Kluge, A.Kohl, M.Konig, D.Lunney, I.Martel, R.B.Moore, H.Raimbault-Hartmann, E.Schark, S.Schwarz, M.de Saint Simon, J.Szerypo, and the ISOLDE Collaboration
Accurate Masses of Unstable Rare-Earth Isotopes by ISOLTRAP
ATOMIC MASSES 133Cs, 123,125,127Ba, 133,134,135,136,137Pr, 130,132,134,135,136,137,138Nd, 136,137,138,139,140,141,143Pm, 136,137,138,139,140,141,142,143Sm, 139,141,142,143,144,145,146,147,148,149,151,153Eu, 148,149,154Dy, 150Ho; measured mass. Penning trap.
COMPILATION Z=55-80; compiled, evaluated atomic mass data.
NUCLEAR REACTIONS 181Ta(p, X)133Ce/133Pr/133Nd/138Nd/138Pm/139Pm/140Pm/142Pm/139Sm/140Sm/141Sm/142Sm/143Sm/138Eu/140Eu/141Eu/142Eu/143Eu/144Eu/143Gd/144Tb/148Tb/150Tb/151Tb/148Dy/150Dy/151Dy/150Ho/151Ho/176Yb/168Lu/176W/176Ta, E=1 GeV; measured Eγ, secondary beam intensity yield. Isolde mass separator.
Nucl.Phys. A674, 168 (2000)
V.F.Dmitriev, V.B.Telitsin
Many-Body Corrections to the Nuclear Anapole Moment II
NUCLEAR STRUCTURE 133Cs, 135,137Ba, 205Tl, 207Pb, 209Bi; calculated anapole moments, many-body contributions. Core polarization, parity-violating effective interaction.
doi: 10.1016/S0375-9474(00)00158-5
Phys.Rev. C62, 065501 (2000)
P.K.Panda, B.P.Das
Effects of Nuclear Structure on Parity Nonconservation in Atomic Cesium in Relativistic Mean Field Theory
NUCLEAR STRUCTURE 125,127,129,131,133,135,137,139Cs; calculated binding energies, radii, nuclear structure corrections to weak charge. Relativistic mean field theory, several parameter sets compared.
doi: 10.1103/PhysRevC.62.065501
Nucl.Phys. A677, 75 (2000)
T.Radon, H.Geissel, G.Munzenberg, B.Franzke, Th.Kerscher, F.Nolden, Yu.N.Novikov, Z.Patyk, C.Scheidenberger, F.Attallah, K.Beckert, T.Beha, F.Bosch, H.Eickhoff, M.Falch, Y.Fujita, M.Hausmann, F.Herfurth, H.Irnich, H.C.Jung, O.Klepper, C.Kozhuharov, Yu.A.Litvinov, K.E.G.Lobner, F.Nickel, H.Reich, W.Schwab, B.Schlitt, M.Steck, K.Summerer, T.Winkler, H.Wollnik
Schottky Mass Measurements of Stored and Cooled Neutron-Deficient Projectile Fragments in the Element Range of 57 ≤ Z ≤ 84
ATOMIC MASSES 133La, 134Ce, 135,138Nd, 138Pm, 156Ho, 158Er, 158,160Tm, 160,161,162,164Yb, 162,163,164,166Lu, 164,165,166,167,168,170,171Hf, 167,168,169,170,171,173,175Ta, 170,171,172,173,174,175,176,177W, 172,173,174,175,176,177,178Re, 174,175,176,177,178,179,180,181Os, 177,178,179,180,181,183,184,185Ir, 178,179,180,181,182,183,184,185,187Pt, 181,182,183,184,185,187,188,189Au, 184,185,186,187,188,189,190,192Hg, 186,187,188,189,190,191,192,193,194,195Tl, 188,189,190,191,192,193,194,195,196,197,198Pb, 192,193,194,195,196,197,198Bi, 197,198,199,200,201,202Po; measured masses. Schottky mass spectrometry.
doi: 10.1016/S0375-9474(00)00304-3
Trans.Bulg.Nucl.Soc. 5, 121 (2000)
L.L.Riedinger, D.J.Hartley, W.Reviol, O.Zeidan, J.-Y.Zhang
Rotational Bands Built on Intruder States in Deformed Nuclei
NUCLEAR STRUCTURE 131,133,135,137Nd, 131,132Pr, 163Lu, 177Re, 179Ir, 181Au; analyzed rotational bands excitation energies, moments of inertia, deformation effects, related features.
Hyperfine Interactions 127, 57 (2000)
S.Trapp, G.Marx, G.Tommaseo, A.Klaas, A.Drakoudis, G.Revalde, G.Szawiola, G.Werth
Hyperfine structure and g-factor measurements on Ba+ and Eu+ isotopes
NUCLEAR MOMENTS 131,133,135,137Ba, 148,149,150,151,153Eu; measured hfs; deduced coupling constants. 137Ba; measured g factor. Paul and Penning traps, laser resonance fluorescence.
Phys.Rev. C62, 024309 (2000)
N.Yoshinaga, Y.D.Devi, A.Arima
Microscopic Derivation of Interacting Boson-Fermion Model Hamiltonian and Its Application to Singly Magic Nuclei
NUCLEAR STRUCTURE 134Te, 135I, 136Xe, 137Cs, 138Ba, 139La, 125,126,127,128,129,130Sn; calculated levels, J, π. Interacting boson-fermion model, comparison with data.
doi: 10.1103/PhysRevC.62.024309
Phys.Rev. C63, 024322 (2001)
B.Fornal, R.Broda, P.J.Daly, P.Bhattacharyya, C.T.Zhang, Z.W.Grabowski, I.Ahmad, D.Seweryniak, I.Wiedenhover, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, C.J.Lister, P.Reiter, J.Blomqvist
Few Particle Excitations of N = 83 Isotones 134Sb and 135Te from 248Cm Fission
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 134Sb, 135Te deduced levels, J, π, configurations. Gammasphere array.
doi: 10.1103/PhysRevC.63.024322
Phys.Rev. C64, 021302 (2001)
A.Korgul, H.Mach, B.Fogelberg, W.Urban, W.Kurcewicz, V.I.Isakov
Structure Information on the r-Process Nucleus 135Sn
RADIOACTIVITY 135Sn(β-) [from 238U(n, F)]; measured Eγ, Iγ, γγ-, βγ-coin, T1/2. 135Sb deduced levels, possible J, π. Online fission-product mass separator. Astrophysical r-process and level systematics in neighboring nuclides discussed. Comparisons with model predictions.
doi: 10.1103/PhysRevC.64.021302
Phys.Rev. C 64, 054306 (2001); Erratum Phys.Rev. C 104, 069902 (2021)
Y.X.Luo, J.O.Rasmussen, A.V.Ramayya, J.H.Hamilton, X.Q.Zhang, J.K.Hwang, C.J.Beyer, J.Kormicki, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.V.Daniel, K.E.Gregorich, T.N.Ginter, P.Zielinski, C.M.Folden, I.Y.Lee, P.Fallon, A.Macchiavelli, R.Donangelo, M.A.Stoyer, S.Asztalos, S.C.Wu
Fission γ Spectra and Levels in 139Ba
RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 135Te, 139Ba deduced high-spin levels, J, π. Gammasphere array.
doi: 10.1103/PhysRevC.64.054306
Eur.Phys.J. A 11, 9 (2001)
M.N.Mineva, M.Hellstrom, M.Bernas, J.Gerl, H.Grawe, M.Pfutzner, P.H.Regan, M.Rejmund, D.Rudolph, F.Becker, C.R.Bingham, T.Enqvist, B.Fogelberg, H.Gausemel, H.Geissel, J.Genevey, M.Gorska, R.Grzywacz, K.Hauschild, Z.Janas, I.Kojouharov, Y.Kopatch, A.Korgul, W.Korten, J.Kurcewicz, M.Lewitowicz, R.Lucas, H.Mach, S.Mandal, P.Mayet, C.Mazzocchi, J.A.Pinston, Zs.Podolyak, H.Schaffner, Ch.Schlegel, K.Schmidt, K.Summerer, H.J.Wollersheim
A New μs Isomer in 136Sb Produced in the Projectile Fission of 238U
RADIOACTIVITY 134,135Te, 136Sb(IT) [from 9Be(238U, X)]; measured Eγ, Iγ, T1/2. 136Sb deduced isomeric level J, π. Fragment separator.
NUCLEAR REACTIONS 9Be(238U, X), E=750 MeV/nucleon; measured delayed Eγ, Iγ, (fragment)γ-coin. 134,135Te, 136Sb deduced isomers T1/2. 136Sb deduced isomeric level J, π. Fragment separator.
Acta Phys.Pol. B32, 2683 (2001)
M.A.Riley, R.W.Laird, F.G.Kondev, D.J.Hartley, D.E.Archer, T.B.Brown, R.M.Clark, M.Devlin, P.Fallon, I.M.Hibbert, D.T.Joss, D.R.LaFosse, P.J.Nolan, N.J.O'Brien, E.S.Paul, J.Pfohl, D.G.Sarantites, R.K.Sheline, S.L.Shepherd, J.Simpson, R.Wadsworth, M.T.Matev, A.V.Afanasjev, J.Dobaczewski, G.A.Lalazissis, W.Nazarewicz, W.Satula
Global Lifetime Measurements of Highly-Deformed and Other Rotational Structures in the A ∼ 135 Light Rare-Earth Region: Probing the single-particle motion in a rotating potential
NUCLEAR REACTIONS 105Pd(35Cl, xnypzα), E=173 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin, DSA. 130,131,132,133Pr, 132,133,134,135Nd, 133,134,136Pm, 135,136,137Sm deduced rotational bands T1/2, transition quadrupole moments. Gammasphere, Microball arrays. Comparisons with model predictions.
Nucl.Phys. A682, 493c (2001)
J.Shergur, M.Hannawald, D.Seweryniak, H.Fynbo, U.Koester, A.Woehr, D.Fedorov, V.Fedoseyev, V.Mishin, P.Hoff, J.Ressler, A.Bickley, B.Pfeiffer, H.Simon, T.Nilsson, H.Mach, K.Wilhelmsen Rolander, H.Ravn, K.-L.Kratz, W.Walters, and the ISOLDE Collaboration
Decay of 135, 136Sn Isolated by Use of a Laser Ion Source and Evidence for a More Harmonic-Oscillator-Like Nuclear Potential
RADIOACTIVITY 135Sn(β-); measured Eβ, Eγ, β-delayed neutron spectra, T1/2. 136Sn(β-); measured T1/2. 134,135Sb deduced levels, J, π. Level systematics in neighboring nuclides discussed.
doi: 10.1016/S0375-9474(00)00678-3
Chin.Phys.Lett. 18, 30 (2001)
P.-K.Weng, G.-J.Yuan, Z.-J.Zhang, S.-G.Li, S.-X.Wen, G.-S.Li, Z.-Y.Dai, C.-X.Yang, Z.-H.Peng, X.-A.Liu, X.-G.Wu, Y.-W.Pu
High-Spin States in the Odd-Proton Nucleus 135Pm
NUCLEAR REACTIONS 107Ag(32S, 2n2p), E=146 MeV; measured Eγ, Iγ, γγ-coin. 135Pm deduced high-spin levels, J, π, configurations.
doi: 10.1088/0256-307X/18/1/311
At.Data Nucl.Data Tables 81, 1 (2002)
I.M.Band, M.B.Trzhaskovskaya, C.W.Nestor, Jr., P.O.Tikkanen, S.Raman
Dirac-Fock Internal Conversion Coefficients
NUCLEAR STRUCTURE Z=10-126; A=20-310; calculated ICC. Relativistic self-consistent-field Dirac-Fock approach.
Phys.Rev. C65, 051306 (2002)
L.Coraggio, A.Covello, A.Gargano, N.Itaco
Structure of Sn Isotopes Beyond N = 82
NUCLEAR STRUCTURE 134,135Sn; calculated levels, J, π. 134Sn calculated transitions B(E2). Shell model, realistic effective interaction, comparison with data.
doi: 10.1103/PhysRevC.65.051306
Eur.Phys.J. A 13, 281 (2002)
I.Dillmann, M.Hannawald, U.Koster, V.N.Fedoseyev, A.Wohr, B.Pfeiffer, D.Fedorov, J.Shergur, L.Weissman, W.B.Walters, K.-L.Kratz
Selective Laser Ionization of N ≥ 82 Indium Isotopes: The new r-process nuclide 135In
RADIOACTIVITY 135,134,133,132In(β-n) [from 238U(n, F)]; measured β-delayed neutron intensity vs time, T1/2. Comparison with RPA results, earlier data. ISOL method, laser ionization source.
doi: 10.1007/s10050-002-8756-7
Eur.Phys.J. A 15, 175 (2002)
J.H.Hamilton, A.V.Ramayya, J.K.Hwang, X.Y.Luo, J.O.Rasmussen, E.F.Jones, X.Q.Zhang, S.J.Zhu, P.M.Gore, T.N.Ginter, I.Y.Lee, R.V.F.Janssens, I.Ahmed, J.D.Cole, W.Greiner, G.Ter-Akopian, Y.Oganessian
New insights into neutron-rich nuclei at high spin
RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 135Te, 139,141Ba, 106Mo; deduced high-spin levels, J, π. 104,106Mo, 108,110,112Ru, 112,114,116,118Pd; deduced rotational band features. 162,164Gd deduced levels.
doi: 10.1140/epja/i2001-10249-1
Phys.Rev. C65, 054317 (2002)
K.Higashiyama, N.Yoshinaga, K.Tanabe
Shell Model Study of Backbending Phenomena in Xe Isotopes
NUCLEAR STRUCTURE 130,131,132,133,134,135,136Xe; calculated levels, J, π, rotational bands features. Shell model, comparison with data.
doi: 10.1103/PhysRevC.65.054317
Phys.Rev.Lett. 88, 152501 (2002)
R.W.Laird, F.G.Kondev, M.A.Riley, D.E.Archer, T.B.Brown, R.M.Clark, M.Devlin, P.Fallon, D.J.Hartley, I.M.Hibbert, D.T.Joss, D.R.LaFosse, P.J.Nolan, N.J.O'Brien, E.S.Paul, J.Pfohl, D.G.Sarantites, R.K.Sheline, S.L.Shepherd, J.Simpson, R.Wadsworth, M.T.Matev, A.V.Afanasjev, J.Dobaczewski, G.A.Lalazissis, W.Nazarewicz, W.Satula
Quadrupole Moments of Highly Deformed Structures in the A ∼ 135 Region: Probing the single-particle motion in a rotating potential
NUCLEAR REACTIONS 105Pd(35Cl, xnypzα), E=173 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin, DSA. 130,131,132Pr, 133,135Nd, 133,134,136Pm, 135,137Sm deduced rotational bands transition quadrupole moments, additivity of single-particle moments. Cranked Skyrme-Hartree-Fock and cranked relativistic mean field calculations. Gammasphere, Microball arrays.
doi: 10.1103/PhysRevLett.88.152501
Nucl.Phys. A704, 179c (2002)
G.J.Mathews, M.T.Ressell
Shell-Model Studies Near the N = 82 r-Process Waiting Point
NUCLEAR STRUCTURE 112In, 127,135I, 131Sn, 133Sb; calculated levels, J, π. 130Cd, 128Pd; calculated Gamow-Teller strength distributions. Z=40-49; calculated β-decay T1/2.
doi: 10.1016/S0375-9474(02)00778-9
Prog.Nucl.Energy 41, 39 (2002)
B.Pfeiffer, K.Kratz, P.Moller
Status of delayed-Neutron Precursor Data: Half-Lives and Neutron Emission Probabilities
COMPILATION Z=27-63; compiled, analyzed β-decay T1/2, neutron emission probabilities, model predictions.
Eur.Phys.J. A 15, 171 (2002)
D.C.Radford, C.Baktash, A.Galindo-Uribarri, C.J.Gross, T.A.Lewis, P.E.Mueller, P.A.Hausladen, D.Shapira, D.W.Stracener, C.H.Yu, B.Fuentes, E.Padilla, D.J.Hartley, C.J.Barton, M.Caprio, N.V.Zamfir
Physics with heavy neutron-rich RIBs at the HRIBF
NUCLEAR REACTIONS C(126Te, 126Te'), (126Sn, 126Sn'), (128Te, 128Te'), (128Sn, 128Sn'), (132Te, 132Te'), (134Ba, 134Ba'), (134Te, 134Te'), (136Te, 136Te'), (136Ba, 136Ba'), E ≈ 3 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 126,128,132,134,136Te, 126,128Sn, 134,136Ba deduced transitions B(E2). 9Be(134Te, αX)135Te, E ≈ 4 MeV/nucleon; measured Eγ, Iγ, αγ-, αα-coin. 135Te deduced levels, J, π.
doi: 10.1140/epja/i2001-10248-2
Phys.Rev. C65, 017302 (2002)
S.K.Saha, C.Constantinescu, P.J.Daly, P.Bhattacharyya, C.T.Zhang, Z.W.Grabowski, B.Fornal, R.Broda, I.Ahmad, D.Seweryniak, I.Wiedenhover, M.P.Carpenter, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, C.J.Lister, P.Reiter
Excitations of Two- and Three-Valence-Proton Nuclei 134Te and 135I
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 134Te, 135I deduced levels, J, π, configurations. Gammasphere array.
doi: 10.1103/PhysRevC.65.017302
Phys.Rev. C65, 034313 (2002)
J.Shergur, B.A.Brown, V.Fedoseyev, U.Koster, K.L.Kratz, D.Seweryniak, W.B.Walters, A.Wohr, D.Fedorov, M.Hannawald, M.Hjorth-Jensen, V.Mishin, B.Pfeiffer, J.J.Ressler, H.O.U.Fynbo, P.Hoff, H.Mach, T.Nilsson, K.Wilhelmsen-Rolander, H.Simon, A.Bickley, and the ISOLDE Collaboration
β-Decay Studies of 135-137Sn using Selective Resonance Laser Ionization Techniques
RADIOACTIVITY 135,136,137Sn(β-), (β-n) [from U(p, X)]; measured β-delayed neutron spectra, Eγ, Iγ, γγ-coin, T1/2; deduced delayed neutron emission probabilities. 135Sb deduced levels, J, π, β-branching ratio. Resonance laser ionization, mass separator.
RADIOACTIVITY 137Sb(β-), (β-n); estimated T1/2 and %P(n) from extrapolation.
doi: 10.1103/PhysRevC.65.034313
Phys.Rev. C66, 044302 (2002)
W.Urban, W.R.Phillips, I.Ahmad, J.Rekawek, A.Korgul, T.Rzaca-Urban, J.L.Durell, M.J.Leddy, A.G.Smith, B.J.Varley, N.Schulz, L.R.Morss
Near-yrast structure of neutron-rich, N = 85 isotones
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 139Xe, 141Ba deduced levels, J, π, γ-ray polarization. 143Ce, 135Sn, 137Te analyzed levels, J, π. Eurogam 2 array.
doi: 10.1103/PhysRevC.66.044302
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
Fizika(Zagreb) B 12, 85 (2003)
J.H.Hamilton, S.J.Zhu, Y.X.Luo, J.K.Hwang, A.V.Ramayya, P.M.Gore, J.O.Rasmussen, and the GANDS Collaborations
Collective and single-particle structures in neutron-rich nuclei
RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 104,106Mo, 133,135Te, 139,141Ba, 139Xe, 115,117Ag deduced levels, J, π, rotational bands. Gammasphere array.
Phys.Rev. C 68, 054328 (2003)
H.Iimura, M.Koizumi, M.Miyabe, M.Oba, T.Shibata, N.Shinohara, Y.Ishida, T.Horiguchi, H.A.Schuessler
Nuclear moments and isotope shifts of 135La, 137La, and 138La by collinear laser spectroscopy
NUCLEAR MOMENTS 135,137,138,139La; measured hfs, isotope shifts, μ, quadrupole moments. Collinear laser spectroscopy.
doi: 10.1103/PhysRevC.68.054328
Phys.Rev.Lett. 91, 132501 (2003)
S.Zhu, U.Garg, B.K.Nayak, S.S.Ghugre, N.S.Pattabiraman, D.B.Fossan, T.Koike, K.Starosta, C.Vaman, R.V.F.Janssens, R.S.Chakrawarthy, M.Whitehead, A.O.Macchiavelli, S.Frauendorf
A Composite Chiral Pair of Rotational Bands in the Odd-A Nucleus 135Nd
NUCLEAR REACTIONS 110Pd(30Si, 5n), E=133 MeV; measured Eγ, Iγ, γγ-coin. 135Nd deduced high-spin levels, J, π, three-quasiparticle chiral structure. Gammasphere array.
doi: 10.1103/PhysRevLett.91.132501
INDC(CCP)-439 (2004)
T.V.Alenicheva, L.P.Kabina, I.A.Mitropolsky, T.M.Tyukavina
Atlas of rotational bands in odd-mass nuclei
COMPILATION A=43-253; compiled, analyzed rotational band data, related parameters; calculated rotational energies. Variable moment of inertia model.
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.Phys. A746, 150c (2004)
H.Geissel, Yu.A.Litvinov, F.Attallah, K.Beckert, P.Beller, F.Bosch, D.Boutin, T.Faestermann, M.Falch, B.Franzke, M.Hausmann, M.Hellstrom, E.Kaza, Th.Kerscher, O.Klepper, H.-J.Kluge, C.Kozhuharov, K.-L.Kratz, S.A.Litvinov, K.E.G.Lobner, L.Maier, M.Matos, G.Munzenberg, F.Nolden, Yu.N.Novikov, T.Ohtsubo, A.Ostrowski, Z.Patyk, B.Pfeiffer, M.Portillo, T.Radon, C.Scheidenberger, V.Shishkin, J.Stadlmann, M.Steck, D.J.Vieira, H.Weick, M.Winkler, H.Wollnik, T.Yamaguchi
New results with stored exotic nuclei at relativistic energies
ATOMIC MASSES 116,135,136,137,138,139,140Te, 117,119I, 117,118,119,120,121,122Xe, 116,117,118,119,120,121,122Pd, 143Sm; measured masses. Tl; analyzed proton separation energies, mass values. Schottky mass spectrometer.
doi: 10.1016/j.nuclphysa.2004.09.030
Int.J.Mod.Phys. E13, 87 (2004)
I.Ragnarsson, F.G.Kondev, E.S.Paul, M.A.Riley, J.Simpson
The nuclear mass at finite angular momenta
NUCLEAR STRUCTURE Nd, Yb; analyzed data; deduced shell energies, pair correlation features. 109,110Sb, 113I, 114Xe, 135Nd, 152,154,156Dy, 163Lu, 194Hg, 192,194Pb; analyzed rotational band energies, superdeformation.
doi: 10.1142/S0218301304001771
Nucl.Phys. A746, 83c (2004)
D.C.Radford, C.Baktash, J.R.Beene, B.Fuentes, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, Y.Larochelle, T.A.Lewis, J.F.Liang, J.Mas, P.E.Mueller, E.Padilla, D.Shapira, D.W.Stracener, R.L.Varner, C.-H.Yu, C.J.Barton, M.A.Caprio, D.J.Hartley, N.V.Zamfir
Nuclear structure studies with heavy neutron-rich RIBS at the HRIBF
NUCLEAR REACTIONS C(126Sn, 126Sn'), (128Sn, 128Sn'), (130Sn, 130Sn'), (132Sn, 132Sn'), (134Sn, 134Sn'), (132Te, 132Te'), (134Te, 134Te'), (136Te, 136Te'), E < 3 MeV/nucleon; measured Eγ, Iγ, (recoil)γ-coin following projectile Coulomb excitation. 126,128,130,132,134Sn, 132,134,136Te deduced excitation B(E2). 9Be(134Te, 8Be), 13C(134Te, 12C), E ≈ 4 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin.
doi: 10.1016/j.nuclphysa.2004.09.056
Eur.Phys.J. A 21, 61 (2004)
S.Sarkar, M.S.Sarkar
Shell model calculations with modified empirical Hamiltonian in the 132Sn region
NUCLEAR STRUCTURE 134,135,136,137Sn, 134,135,136,137Sb, 134,135,136,137Te, 135,136,137I, 136,137Xe, 137Cs; calculated binding energies. 135Sb, 137I, 136,137Te; calculated levels, J, π. 134Sn, 135Sb, 134,136Te; calculated transitions B(E2). Shell model, modified Hamiltonian, comparison with data.
doi: 10.1140/epja/i2003-10198-7
Phys.Rev. C 70, 044319 (2004)
M.Scheck, H.von Garrel, N.Tsoneva, D.Belic, P.von Brentano, C.Fransen, A.Gade, J.Jolie, U.Kneissl, C.Kohstall, A.Linnemann, A.Nord, N.Pietralla, H.H.Pitz, F.Stedile, C.Stoyanov, V.Werner
Dipole strength distributions in the stable Ba isotopes 134-138Ba: A study in the mass region of a nuclear shape transition
NUCLEAR REACTIONS 135,137Ba(γ, γ'), E=2.5, 3.1, 4.1 MeV bremsstrahlung; measured Eγ, Iγ. 135,137Ba deduced level energies, widths, branching ratios, dipole strength distributions. Comparison with quasiparticle-phonon model predictions.
doi: 10.1103/PhysRevC.70.044319
Phys.Rev. C 69, 051302 (2004)
P.J.Woods, P.Munro, D.Seweryniak, C.N.Davids, T.Davinson, A.Heinz, H.Mahmud, F.Sarazin, J.Shergur, W.B.Walters, A.Woehr
Proton decay of the highly deformed nucleus 135Tb
RADIOACTIVITY 135Tb(p) [from 92Mo(50Cr, 6np)]; measured Ep, T1/2. 135Tb deduced level J, π, configuration, deformation. Mass separator.
NUCLEAR REACTIONS 92Mo(50Cr, 6np), E=310 MeV; measured delayed Ep, (recoil)(decay)-coin; deduced production σ.
doi: 10.1103/PhysRevC.69.051302
Phys.Rev. C 69, 054309 (2004)
N.Yoshinaga, K.Higashiyama
Systematic studies of nuclei around mass 130 in the pair-truncated shell model
NUCLEAR STRUCTURE 126,128,130,132,134Xe, 128,130,132,134,136Ba, 130,132,134,136,138Ce, 132,134,136,138,140Nd; calculated levels, J, π, B(E2). 129,131,133Xe, 131,133,135Ba, 133,135,137Ce; calculated levels, J, π, μ. Pair-truncated shell model, comparisons with data.
doi: 10.1103/PhysRevC.69.054309
Yad.Fiz. 68, 517 (2005); Phys.Atomic Nuclei 68, 488 (2005)
Chr.Bargholtz, B.A.Chernyshev, L.Geren, V.N.Grebenev, Yu.B.Gurov, B.Hoistad, I.V.Laukhin, K.Lindberg, V.G.Sandukovsky, R.R.Shafigullin, P.-E.Tegner
A Search for Deeply bound Pionic States of Xenon Produced in the 136Xe(d, 3He)135Xeπ-bound Reaction
NUCLEAR REACTIONS 136Xe(d, 3HeX)135Xe, E=500 MeV; 1H(d, π0), E=500 MeV; measured helium spectra. 135Xe deduced pionic state binding energy.
doi: 10.1134/1.1891199
Phys.Rev. C 72, 057302 (2005); Erratum Phys.Rev. C 73, 069901 (2006)
L.Coraggio, A.Covello, A.Gargano, N.Itaco
Shell-model structure of exotic 135Sb
NUCLEAR STRUCTURE 135Sb; calculated levels, J, π, B(M1). Shell model, realistic effective interaction, comparison with data.
doi: 10.1103/PhysRevC.72.057302
J.Phys.(London) G31, S1639 (2005)
C.J.Gross
Recent results at HRIBF using neutron-rich radioactive ion beams
NUCLEAR REACTIONS 64Ni(132Sn, X), (134Sn, X), E=450-620 MeV; measured fusion σ. C(130Te, 130Te'), (132Te, 132Te'), E=3 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 132Te level deduced g factor. 13C(134Te, 135Te), E=550 MeV; measured Eγ, Iγ. 135Te level deduced J, π.
doi: 10.1088/0954-3899/31/10/047
Proc.Nuclei at the Limits, Argonne, Illinois, D.Seweryniak and T.L.Khoo, eds., p.99 (2005); AIP Conf. Proc 764 (2005)
H.C.Jain, S.Lakshmi, P.K.Joshi
Identification Of Chiral Bands In 135Ce
NUCLEAR REACTIONS 124Sn(16O, 5n), E=80 MeV; measured Eγ, Iγ, γγ-coin, DSA. 135Ce deduced high-spin levels, J, π, T1/2, B(M1), B(E2), chiral doublet bands.
doi: 10.1063/1.1905297
Eur.Phys.J. A 25, Supplement 1, 123 (2005)
A.Korgul, H.Mach, B.A.Brown, A.Covello, A.Gargano, B.Fogelberg, R.Schuber, W.Kurcewicz, E.Werner-Malento, R.Orlandi, M.Sawicka
On the structure of the anomalously low-lying 5/2+ state of 135Sb
RADIOACTIVITY 135Sn(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, βγ-coin following decay of mass-separated sources. 135Sb deduced levels, J, π, T1/2, B(M1), configurations. Comparison with shell model calculations.
doi: 10.1140/epjad/i2005-06-040-2
Nucl.Phys. A752, 264c (2005)
D.C.Radford, C.Baktash, C.J.Barton, J.Batchelder, J.R.Beene, C.R.Bingham, M.A.Caprio, M.Danchev, B.Fuentes, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, D.J.Hartley, P.Hausladen, J.K.Hwang, W.Krolas, Y.Larochelle, J.F.Liang, P.E.Mueller, E.Padilla, J.Pavan, A.Piechaczek, D.Shapira, D.W.Stracener, R.L.Varner, A.Woehr, C.-H.Yu, N.V.Zamfir
Coulomb excitation and transfer reactions with rare neutron-rich isotopes
NUCLEAR REACTIONS C(126Sn, 126Sn'), (128Sn, 128Sn'), (130Sn, 130Sn'), (132Sn, 132Sn'), (134Sn, 134Sn'), (132Te, 132Te'), (134Te, 134Te'), (136Te, 136Te'), E not given; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 126,128,130,132,134Sn, 132,134,136Te deduced transitions B(E2). 9Be(134Te, 8Be), 13C(134Te, 12C), E not given; measured Eγ, Iγ, γγ-, (particle)γ-coin. 135Te deduced level. Clarion, Hyball arrays.
doi: 10.1016/j.nuclphysa.2005.02.040
Eur.Phys.J. A 25, Supplement 1, 383 (2005)
D.C.Radford, C.Baktash, C.J.Barton, J.Batchelder, J.R.Beene, C.R.Bingham, M.A.Caprio, M.Danchev, B.Fuentes, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, D.J.Hartley, P.Hausladen, J.K.Hwang, W.Krolas, Y.Larochelle, J.F.Liang, P.E.Mueller, E.Padilla, J.Pavan, A.Piechaczek, D.Shapira, D.W.Stracener, R.L.Varner, A.Woehr, C.-H.Yu, N.V.Zamfir
Coulomb excitation and transfer reactions with neutron-rich radioactive beams
NUCLEAR REACTIONS C(126Sn, 126Sn'), (128Sn, 128Sn'), (130Sn, 130Sn'), (132Te, 132Te'), (134Te, 134Te'), (136Te, 136Te'), E not given; measured Eγ, Iγ, γγ-, (particle)γ-coin following projectile Coulomb excitation. 132,134,136Te, 126,128,130Sn deduced excitation B(E2). 9Be(134Te, 8Be), 13C(134Te, 12C), E=4.3 MeV/nucleon; measured Eγ, Iγ, γγ-coin, (particle)γ-coin; deduced single-neutron transfer σ(E). 135Te deduced levels J, π.
doi: 10.1140/epjad/i2005-06-205-y
J.Phys.(London) G31, S1503 (2005)
D.Seweryniak, C.N.Davids, A.Robinson, P.J.Woods, B.Blank, M.P.Carpenter, T.Davinson, S.J.Freeman, N.Hammond, N.Hoteling, R.V.F.Janssens, T.L.Khoo, Z.Liu, G.Mukherjee, J.Shergur, S.Sinha, A.A.Sonzogni, W.B.Walters, A.Woehr
Proton decay: spectroscopic probe beyond the proton drip line
RADIOACTIVITY 130Eu, 135Tb, 145,146Tm(p); analyzed proton-decay data.
doi: 10.1088/0954-3899/31/10/021
Phys.Rev. C 71, 064321 (2005)
J.Shergur, A.Wohr, W.B.Walters, K.-L.Kratz, O.Arndt, B.A.Brown, J.Cederkall, I.Dillmann, L.M.Fraile, P.Hoff, A.Joinet, U.Koster, B.Pfeiffer
Level structure of odd-odd 134Sb populated in the β- decays of 134, 135Sn
RADIOACTIVITY 134Sn(β-); 135Sn(β-), (β-n); measured Eγ, Iγ, βγ-, γγ-coin. 134Sb deduced levels, J, π, β-decaying isomeric state. Mass separator, shell model calculations.
doi: 10.1103/PhysRevC.71.064321
Phys.Rev. C 72, 024305 (2005)
J.Shergur, A.Wohr, W.B.Walters, K.-L.Kratz, O.Arndt, B.A.Brown, J.Cederkall, I.Dillmann, L.M.Fraile, P.Hoff, A.Joinet, U.Koster, B.Pfeiffer
Identification of shell-model states in 135Sb populated via β- decay of 135Sn
RADIOACTIVITY 135Sn(β-) [from U(n, F)]; measured Eγ, Iγ, γγ-coin. 135Sb deduced levels, J, π. Resonance ionization, mass separator. Comparisons with shell-model predictions.
doi: 10.1103/PhysRevC.72.024305
Eur.Phys.J. A 25, Supplement 1, 121 (2005)
J.Shergur, N.Hoteling, A.Wohr, W.B.Walters, O.Arndt, B.A.Brown, C.N.Davids, D.J.Dean, K.-L.Kratz, B.Pfeiffer, D.Seweryniak, and the ISOLDE Collaboration
New level information on Z = 51 isotopes, 111Sb60 and 134, 135Sb83, 84
RADIOACTIVITY 111Te(β+) [from 58Ni(56Fe, 2pn)]; 135Sn(β-), (β-n) [from U(p, F), E=1.4 GeV]; measured Eγ, Iγ, γγ-coin following decay of mass-separated sources. 111,134,135Sb deduced levels, J, π. Comparison with model calculations.
doi: 10.1140/epjad/i2005-06-071-7
Phys.Rev. C 71, 045502 (2005)
T.Sil, M.Centelles, X.Vinas, J.Piekarewicz
Atomic parity nonconservation, neutron radii, and effective field theories of nuclei
NUCLEAR STRUCTURE 168,170,172,174,176Yb, 156,158,161,162,164Dy, 130,132,134,138Ba, 121,123,125,127,129,131,133,135,137,139,141,145Cs, 207,212,213,219,223,225Fr; calculated charge radii, isotope shifts, neutron skin thickness, atomic parity nonconservation observables. 207,212,213,219,223,225Fr; calculated binding energy, quadrupole deformation. Effective field theories, comparison with data.
doi: 10.1103/PhysRevC.71.045502
At.Data Nucl.Data Tables 90, 75 (2005)
N.J.Stone
Table of nuclear magnetic dipole and electric quadrupole moments
NUCLEAR MOMENTS Z=0-99; A=1-255; compiled μ, electric quadrupole moments.
COMPILATION Z=0-99; A=1-255; compiled μ, electric quadrupole moments.
doi: 10.1016/j.adt.2005.04.001
Int.J.Mod.Phys. E14, 775 (2005)
Unnati, M.K.Sharma, B.P.Singh, R.Prasad, S.Gupta, H.D.Bhardwaj, A.K.Sinha
A study of excitation functions for some residues produced in the system 14N + 128Te in the energy range ≈ 64-90 MeV
NUCLEAR REACTIONS 128Te(14N, 4n), (14N, 5n), (14N, 4np), (14N, 5nα), (14N, 6nα), (14N, n2pα), (14N, n2p2α), (14N, 3α), E ≈ 64-90; measured excitation functions; deduced reaction mechanism features. Activation technique, comparison with model predictions.
doi: 10.1142/S0218301305003545
Eur.Phys.J. A 24, 161 (2005)
W.Urban, T.Rzaca-Urban, J.L.Durell, A.G.Smith, I.Ahmad
First observation of excited states in the 111Tc nucleus -A new region of deformation at 40 ≤ Z ≤ 46, N ≥ 68?
RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 109,110,111Tc, 135I deduced transitions. 111Tc deduced levels, J, π, configurations. Eurogam2 array. Level systematics in neighboring nuclides discussed.
doi: 10.1140/epja/i2004-10140-7
Phys.Rev. C 71, 054318 (2005)
S.-W.Xu, Z.-K.Li, Y.-X.Xie, Q.-Y.Pan, W.-X.Huang, X.-D.Wang, Y.Yu, Y.-B.Xing, N.-C.Shu, Y.-S.Chen, F.-R.Xu, K.Wang
β-delayed proton decays near the proton drip line
RADIOACTIVITY 81Zr, 85Mo, 89Ru, 92Rh, 93Pd, 121Ce, 125Nd, 128Pm, 129Sm, 135,137Gd, 139Dy, 142Ho, 149Yb(β+p); measured β-delayed Eγ, Iγ, proton spectra, pγ-coin, T1/2. Comparison with model predictions.
NUCLEAR REACTIONS 92Mo, 106Cd(32S, 3n), E=151 MeV; 92Mo(36Ar, 3n), E=169 MeV; 96Ru(36Ar, 3n), (36Ar, 3np), E=165, 174 MeV; 106Cd(36Ar, 3n), (36Ar, nα), E=176 MeV; 106Cd(40Ca, 4n), E=202 MeV; 112Sn(40Ca, 3n), E=185 MeV; measured σ.
doi: 10.1103/PhysRevC.71.054318
Eur.Phys.J. A 30, 347 (2006)
X.L.Che, S.J.Zhu, M.L.Li, Y.J.Chen, Y.N.U, H.B.Ding, L.H.Zhu, X.G.Wu, G.S.Li, C.Y.He, Y.Liu
High-spin levels based on the 11/2- isomer in 135Ba
NUCLEAR REACTIONS 130Te(9Be, 4n), E=45 MeV; measured Eγ, Iγ, γγ-coin. 135Ba deduced high-spin levels, J, π, configurations.
doi: 10.1140/epja/i2006-10142-1
Phys.Rev.Lett. 96, 072501 (2006)
D.S.Delion, R.J.Liotta, R.Wyss
Systematics of Proton Emission
RADIOACTIVITY 105Sb, 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141Ho, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,167Ir, 171Au, 177Tl, 185Bi(p); analyzed proton decay T1/2, Q; deduced systematic trends.
doi: 10.1103/PhysRevLett.96.072501
Phys.Rev. C 73, 051301 (2006)
M.S.Fetea, R.B.Cakirli, R.F.Casten, D.D.Warner, E.A.McCutchan, D.A.Meyer, A.Heinz, H.Ai, G.Gurdal, J.Qian, R.Winkler
First test of the E(5/4) Bose-Fermi symmetry: The structure of 135Ba
RADIOACTIVITY 135La(EC) [from 136Ba(p, 2n)]; measured Eγ, Iγ, γγ-coin. 135Ba deduced levels, J, π, B(E2), symmetry features. Comparison with interacting boson-fermion approximation and shell model predictions.
doi: 10.1103/PhysRevC.73.051301
Hyperfine Interactions 171, 203 (2006)
Yu.Gangrsky
Laser spectroscopy of high spin isomers - a review
NUCLEAR MOMENTS 97Y, 130Ba, 135Cs, 158,160Ho, 176Yb, 172,174,176,177,178Lu, 178Hf, 184Au, 202Pb; compiled, analyzed charge radii, quadrupole moments for ground states and high-spin isomeric states.
doi: 10.1007/s10751-006-9502-3
GSI 2006-1, p.154 (2006)
R.Kessler, K.-L.Kratz, J.Pereira Conca, H.Schatz, for the E040 Collaboration
β-decay properties of nuclei in the region around 132Sn
RADIOACTIVITY 133,135Sn, 137,138Sb, 138,139,140Te, 142,143I(β-) [from Pb(238U, X)]; measured T1/2.
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.
Hyperfine Interactions 171, 173 (2006)
R.Sifi, F.Le Blanc, N.Barre, L.Cabaret, J.Crawford, M.Ducourtieux, S.Essabaa, J.Genevey, G.Huber, M.Kowalska, C.Lau, J.K.P.Lee, G.Le Scornet, J.Oms, J.Pinard, B.Roussiere, J.Sauvage, M.Seliverstov, H.Stroke, and the ISOLDE Collaboration
Laser spectroscopy measurements of neutron-rich tellurium isotopes by COMPLIS
NUCLEAR MOMENTS 120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136Te; measured hfs, isotope shifts; deduced μ, quadrupole moments, radii. Laser spectroscopy, comparison with model predictions.
doi: 10.1007/s10751-006-9505-0
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.
Priv.Comm. (2007)
X.-L.Che
Phys.Rev. C 75, 054308 (2007)
B.Fogelberg, K.A.Mezilev, V.I.Isakov, K.I.Erokhina, H.Mach, E.Ramstrom, H.Gausemel
Neutron separation energies at N = 83 and the isomer position in 136I
RADIOACTIVITY 135,136Te(β-); measured Eβ, Eγ, βγ-coinc. Deduced β endpoint energies and mass excess.
doi: 10.1103/PhysRevC.75.054308
Phys.Rev. C 75, 054322 (2007)
N.Fotiades, R.O.Nelson, M.Devlin, J.A.Cizewski, J.A.Becker, W.Younes, R.Krucken, R.M.Clark, P.Fallon, I.Y.Lee, A.O.Macchiavelli, T.Ethvignot, T.Granier
High-spin states in 135Xe
RADIOACTIVITY 135Xe; measured Eγ, Iγ, γγ-coinc. Deduced high spin level structure, J, π.
NUCLEAR REACTIONS 136Xe(n, 2nγ), E not given; measured excitation functions.
doi: 10.1103/PhysRevC.75.054322
Phys.Rev. C 76, 024313 (2007)
M.P.Kartamyshev, T.Engeland, M.Hjorth-Jensen, E.Osnes
Effective interactions and shell model studies of heavy tin isotopes
NUCLEAR STRUCTURE 134,135,136,137,138,139,140,141,142Sn; calculated binding energies, single and two neutron separation energies, level energies, J, π, B(E2) using the single particle model.
doi: 10.1103/PhysRevC.76.024313
Eur.Phys.J. A 32, 25 (2007)
A.Korgul, H.Mach, B.A.Brown, A.Covello, A.Gargano, B.Fogelberg, W.Kurcewicz, E.Werner-Malento, R.Orlandi, M.Sawicka
On the unusual properties of the 282 keV state in 135Sb
RADIOACTIVITY 135Sn(β-) [from 235U(n, X), E=thermal]; measured Eγ, Iγ, βγ, γγ-coinc. 135Sb deduced T1/2, B(M1), B(E2).
doi: 10.1140/epja/i2007-10363-0
Acta Phys.Pol. B38, 1213 (2007)
H.Mach, L.M.Fraile, O.Arndt, A.Blazhev, N.Boelaert, M.J.G.Borge, R.Boutami, H.Bradley, N.Braun, B.A.Brown, P.A.Butler, A.Covello, Z.Dlouhy, C.Fransen, H.O.U.Fynbo, A.Gargano, Ch.Hinke, P.Hoff, A.Joinet, A.Jokinen, J.Jolie, U.Koster, A.Korgul, K.-L.Kratz, T.Kroll, W.Kurcewicz, J.Nyberg, E.-M.Reillo, E.Ruchowska, W.Schwerdtfeger, G.S.Simpson, M.Stanoiu, O.Tengblad, P.G.Thirolf, W.B.Walters
The Single-Particle and Collective Features in the Nuclei Just Above 132Sn
RADIOACTIVITY 136Sn(β-); measured Eγ, Iγ, γγ-coinc. 135Sb deduced levels, B(E2).
Phys.Rev.Lett. 99, 172501 (2007)
S.Mukhopadhyay, D.Almehed, U.Garg, S.Frauendorf, T.Li, P.V.Madhusudhana Rao, X.Wang, S.S.Ghugre, M.P.Carpenter, S.Gros, A.Hecht, R.V.F.Janssens, F.G.Kondev, T.Lauritsen, D.Seweryniak, S.Zhu
From Chiral Vibration to Static Chirality in 135Nd
NUCLEAR REACTIONS 100Mo(40Ar, 5n), E=175 MeV; measured Eγ, Iγ, lifetimes. 135Nd deduced B(M1), B(E2).
doi: 10.1103/PhysRevLett.99.172501
Priv.Comm. (2007)
S.Mukhopadhyay