References quoted in the ENSDF dataset: 120 REFERENCES
251 references found.
Clicking on a keynumber will list datasets that reference the given article.
Helv.Phys.Acta 23, 623 (1950)
J.P.Blaser, F.Boehm, P.Marmier
Decay of Sb120
Phys.Rev. 80, 1062 (1950)
H.E.Johns, L.Katz, R.A.Douglas, R.N.H.Haslam
Gamma-Neutron Cross Sections
Phys.Rev. 104, 967 (1956)
G.M.Temmer, N.P.Heydenburg
Coulomb Excitation of Medium-Weight Nuclei
Phys.Rev. 109, 888 (1958)
C.L.McGinnis
Radioactivity of In120 and Sb120
Phys.Rev. 120, 2185 (1960)
H.Ikegami
Nuclear Structure of Sn120
NUCLEAR STRUCTURE 120Sn; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 13, 196 (1960)
A.Poularikas, J.Cunningham, W.McMillan, J.McMillan, R.W.Fink
New Isomers of Scandium-50 and Indium-120; γ-Rays in Lutecium-178 Decay
NUCLEAR STRUCTURE 50Sc, 175Lu, 120In; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(60)80294-1
Phys.Rev. 124, 213 (1961)
H.H.Bolotin, A.C.Li, A.Schwarzschild
Level Structure of Sn118 and Sn120 from the Decay of Sb Isotopes
NUCLEAR STRUCTURE 120Sb, 118Sb; measured not abstracted; deduced nuclear properties.
Phys.Rev. 124, 1518 (1961)
H.Ikegami, T.Udagawa
Structure of Sn120 and the Effect of the Pairing Correlation on the Reduction of E2 Transition in Sn118 and Sn120
NUCLEAR STRUCTURE 118Te, 118Sb, 120Sb; measured not abstracted; deduced nuclear properties.
Phys.Rev. 122, 168 (1961)
L.A.Rayburn
14.4 MeV (n, 2n) Cross Sections
NUCLEAR STRUCTURE 95Ru, 89Zr, 91Mo, 68Ga, 73Se, 69Ge, 106Ag, 111Sn, 105Cd, 80Br, 78Br, 18F, 120Sb, 143Sm, 141Nd, 140Pr, 30P, 34Cl, 53Fe, 44Sc, 38K, 45Ti, 49Cr, 57Ni, 63Zn, 64Cu, 13N; measured not abstracted; deduced nuclear properties.
Z.Physik 168, 370 (1962)
E.Bodenstedt, H.J.Korner, E.Gerdau, J.Radeloff, K.Auerbach, L.Mayer, A.Roggenbuck
Die magnetischen Momente der 5--Niveaus von Sn118 und Sn120
NUCLEAR STRUCTURE 118Sn, 120Sn; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 48, 561 (1963)
W.M.Currie
Lifetimes in Sb120, Ba138 and Ce140
NUCLEAR STRUCTURE 120Sb, 138Cs; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90223-2
J.Phys.Soc.Japan 18, 1563 (1963)
K.Okano, K.Nishimura
(p, n) Threshold Measurements on Na, Al, Cu, Ga, Ge, Se, Y, and Sn
NUCLEAR STRUCTURE 27Si, 23Mg, 77Br, 78Br, 80Br, 89Zr, 74As, 69Ge, 63Zn, 65Zn, 118Sb, 120Sb; measured not abstracted; deduced nuclear properties.
Izv. Akad. Nauk SSSR, Ser. Fiz. 28, 232 (1964); Bull. Acad. Sci. USSR, Phys. Ser. 28, 149 (1965)
D.G.Alkhazov, Y.P.Gangrskii, I.K.Lemberg, Y.I.Udralov
Coulomb Excitation of Electric Octupole Transitions in Even-Even Tin Isotopes
NUCLEAR STRUCTURE 124Sn, 122Sn, 120Sn, 114Sn, 118Sn, 116Sn; measured not abstracted; deduced nuclear properties.
Perturbed Angular Correlations, E.Karlsson, E.Matthias, K.Siegbahn, Ed., North-Holland Publishing Co., Amsterdam, p.186 (1964)
M.Deutsch, A.Buyrn, L.Grodzins
Magnetic Moments of 5- States in Sn118 and Sn120
RADIOACTIVITY 118,120Sb; measured γγ(θ, H). 118,120Sn levels deduced g.
Phys.Rev. 135, B9 (1964)
J.Kantele, M.Karras
Nuclear Levels of Even Sn Isotopes Populated in the Decay of In Isomers
NUCLEAR STRUCTURE 120In, 122In, 118Sb, 118In; measured not abstracted; deduced nuclear properties.
Phys.Rev. 136, B40 (1964)
L.R.Norris, C.F.Moore
Energy Levels from (d, p) Reactions on Sn117 and Sn119
NUCLEAR STRUCTURE 120Sn, 118Sn; measured not abstracted; deduced nuclear properties.
Nucl.Phys. 66, 481 (1965)
D.L.Allan, B.H.Armitage, B.A.Doran
Energy Levels in Even Tin Isotopes from 11 MeV Proton Inelastic Scattering
NUCLEAR REACTIONS 116,118,120,122,124Sn(p, p'), E = 11 MeV; measured σ(Ep', θ). 116,118,120,122,124Sn deduced levels.
doi: 10.1016/0029-5582(65)90779-0
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.
J.Inorg.Nucl.Chem. 27, 907 (1965)
F.D.S.Butement, S.M.Qaim
Radioisotopes of Iodine and Xenon of Masses 120 and 121
NUCLEAR STRUCTURE 120I, 120Xe, 121Te, 121I, 121Xe, 126I, 123Xe, 122I; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(65)80400-6
Nucl.Phys. 61, 479 (1965)
T.G.Ebrey, P.R.Gray
Precision Half-Life Measurements of Fourteen Positon-Emitting Nuclei
RADIOACTIVITY 13N, 18F, 30P, 34Cl, 38K, 53Fe, 57Ni, 62Cu, 68Ga, 91Mo, 106Ag, 108Ag, 120Sb, 140Pr[from (z, a+1)(n, 2n) except 13N, 108Ag]; measured T1/2. Natural targets except 39K, 63Cu.
doi: 10.1016/0029-5582(65)90107-0
Phys.Rev. 139, B318 (1965)
R.K.Jolly
Analysis of Single Excitations in Inelastic Deuteron Scattering from Ni60, Zr92, and Sn120 Nuclei
NUCLEAR STRUCTURE 120Sn, 60Ni, 41Ca, 48Sc, 92Zr; measured not abstracted; deduced nuclear properties.
Physica 31, 1774 (1965)
P.Meyers, K.E.G.Lobner
Decay of the 4.7 minute Isomer of 118In and of the 48 second Isomer of 120In
NUCLEAR STRUCTURE 120In, 118In; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-8914(65)90097-2
Nucl.Phys. 74, 281 (1965)
R.L.Robinson, P.H.Stelson, F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner
Gamma Ray Energies Determined with a Lithium-Drifted Germanium Detector
NUCLEAR REACTIONS 48Ti, 50Cr, 56Fe, 64,66,68,70Zn, 70,72,74,76Ge, 75As, 76,78,80,82Se(α, α'γ), 79Br, 94,96,98,100Mo, 96,100,104Ru, 104,106,108,110Pd, 106,108,110,112,114,116Cd, 116,117,118,120,122,124Sn, 121,123Sb, 122,124,126,128,130Te, 195Pt(α, α'γ), E=6-9 MeV; measured Eγ. 77Se, 119Sn(α, α'γ), E=6-9 MeV; measured Eγ, Iγ. 18O(α, nγ), E=6-9 MeV; measured Eγ. 21Ne deduced level. Enriched targets.
RADIOACTIVITY 7Be, 22Na, 51Cr, 54Mn, 60Co, 65Zn, 88Y, 137Cs, 198Au, 203Hg, 207Bi; measured Eγ. 102,106Rh; measured Eγ, Iγ.
doi: 10.1016/0029-5582(65)90082-9
Nucl.Phys. 71, 529 (1965)
R.M.Wood, R.R.Borchers, H.H.Barschall
Neutrons from Protons on Isotopes of Tin
NUCLEAR REACTIONS 112,116,117,118,119,120,122,124Sn(p, n), E = 7-14 MeV; measured σ(E;En, θ n). 116,117,118,120Sb deduced levels, level densities. Enriched targets.
doi: 10.1016/0029-5582(65)90763-7
Nucl.Phys. 87, 1 (1966)
H.L.Acker, G.Backenstoss, C.Daum, J.C.Sens, S.A.De Wit
Measurement and Analysis of Muonic X-Ray Spectra in Spherical Nuclei
NUCLEAR REACTIONS 121Sb(μ-, νnγ), 123Sb(μ-, νnγ), 139La(μ-, νnγ), E > 100 MeV; measured Eγ. 120Sn, 122Sn, 138Ba deduced levels. 66Ga [from zn(p, γ)]; measured Eγ. Cl, Ca, Fe, Sn, Sb, Te, I, Cs, Ba, La, Ce, Pr, Nd, Au, Hg, Tl, 206Pb, Pb, Bi; measured E(X-ray), I(X-ray), deduced nuclear charge distribution parameters.
doi: 10.1016/0029-5582(66)90355-5
Phys.Rev. 146, 861 (1966)
N.Baron, R.F.Leonard, J.L.Need, W.M.Stewart, V.A.Madsen
Inelastic Alpha-Particle Excitation in the Even Tin Isotopes
NUCLEAR STRUCTURE 118Sn, 116Sn, 120Sn, 122Sn; measured not abstracted; deduced nuclear properties.
J.Phys.Soc.Japan 21, 1021 (1966)
H.Ejiri, M.Ishihara, M.Sakai, T.Inamura, K.Katori
Conversion Electrons from (p, 2n) and (α, 3n) Reactions on Vibrational Nuclei
NUCLEAR STRUCTURE 138Ce, 122Te, 120Te, 118Te, 186Os, 106Cd, 108Cd; measured not abstracted; deduced nuclear properties.
INSJ-98 (1966)
H.Ejiri, M.Ishihara, T.Inamura, K.Katori
Measurement of Gamma Rays from (p, 2n) Reactions on Vibrational Nuclei
NUCLEAR REACTIONS 103Rh, 109Ag, 121Sb, 139La, 197Au(p, 2nγ), E=14.3 MeV; measured Eγ, Iγ, γ(θ). 102Pd, 108Cd, 120Te, 138Ce, 196Hg deduced levels, ICC, J, π.
Nucl.Phys. 79, 165 (1966)
M.Harchol, S.Cochavi, A.A.Jaffe, C.Drory
Excitation of Isobaric Analogue States by (p, n) Reactions
NUCLEAR REACTIONS 65Cu, 76Ge, 93Nb, 116,118,119,122,124Sn, 121,123Sb, 125,126,130Te, 197Au(p, n), E = 2.3-11.0 MeV; measured σ(E). 66Zn, 77As, 94Mo, 117,119,120,123,125Sb, 122,124Te, 126,127,131I, 198Bi deduced IAR, , Coulomb displacement energies.
doi: 10.1016/0029-5582(66)90399-3
Nucl.Phys. 89, 412 (1966)
B.Hrastnik, V.Knapp, M.Vlatkovic
Lifetimes of the First Excited States in 118Sn and 120Sn by the Nuclear Gamma-Ray Resonance Method
NUCLEAR REACTIONS 118,120Sn(γ, γ), E = 1.18, 1.22 MeV; measured σ. 118,120Sn levels deduced T1/2. Natural targets.
Phys.Rev. 145, 971 (1966)
P.Richard, C.F.Moore, J.A.Becker, J.D.Fox
Isobaric Analogue States in Heavy Nuclei. III. Tin Isotopes
NUCLEAR STRUCTURE 117Sb, 113Sb, 115Sb, 119Sb, 118Sb, 123Sb, 121Sb, 120Sb, 125Sb; measured not abstracted; deduced nuclear properties.
Phys.Rev.Letters 19, 1444 (1967)
P.Barreau, J.B.Bellicard
Study of Collective Levels in Tin-116, Tin-120, and Tin-124 by Inelastic Electron Scattering
NUCLEAR REACTIONS 116,120,124Sn(e, e'), E=150 MeV; measured σ(Ee'); deduced form factors. 116,120,124Sn levels deduced transition probabilities, deformation parameters.
doi: 10.1103/PhysRevLett.19.1444
Nucl.Phys. A95, 176 (1967)
M.G.Betigeri, H.Morinaga
(3He, 3nγ) Reactions on Te, Sn and Cd Isotopes
NUCLEAR REACTIONS 126,128,130Te, 116,118,120,122,124Sn, 112,114,116Cd(3He, 3nγ), E = 19.3 MeV; measured Eγ, Iγ. 126,128,130Xe, 116,118,120,122,124Te, 112,114,116Sn deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(67)90158-3
Nucl.Phys. A93, 272 (1967)
J.E.Clarkson, R.M.Diamond, F.S.Stephens, I.Perlman
Collective Excitations in Neutron-Deficient Barium, Xenon and Cerium Isotopes
NUCLEAR REACTIONS 115In(10B, xnγ), (11B, 4nγ), (14N, xnγ), 116Sn(12C, 4nγ), 127I(11B, 4nγ), E = 3.7-7.5 MeV/nucleon; measured Eγ, Iγ, ce-decay. 120,122Xe, 124,126Ba, 134Ce deduced levels, J, π. 126Ba level deduced T1/2. 134Pr[from 127I(12C, 5n)]; measured T1/2.
doi: 10.1016/0375-9474(67)90271-0
J.Inorg.Nucl.Chem. 29, 2515 (1967)
E.Hagebo
Yields and Isomeric Yield Ratios of Antimony Isotopes from the Interaction of 159 MeV to 18.2 GeV Protons with Uranium
NUCLEAR STRUCTURE 117Sb, 116Sb, 119Sb, 118Sb, 115Sb, 126Sb, 120Sb, 124Sb, 127Sb, 122Sb, 130Sb, 131Sb, 129Sb, 128Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(67)80177-5
Arkiv Fysik 33, 183 (1967)
S.A.Hjorth
Analysis of Some Deuteron-Induced Reactions in the Sb Isotopes
NUCLEAR STRUCTURE 123Sb, 122Sb, 121Sb, 124Sb, 120Sb; measured not abstracted; deduced nuclear properties.
Ann.Phys.(Paris) 2, 141 (1967)
J.-M.Lagrange, G.Albouy, L.Marcus, M.Pautrat, H.Sergolle, O.Rahmouni
Contribution a l'Etude du Schema de Niveaux des Isotopes Pairs-Pairs du Tellure de Nombre de Masse: 126, 124, 122, 120, 118
NUCLEAR STRUCTURE 118I, 122Sb, 122I, 120I, 124Sb, 126I; measured not abstracted; deduced nuclear properties.
J.Phys.(Paris) 28, 857 (1967)
O.Rahmouni, H.Abou-Leila
Nature des Premiers Etats 4+ des Etains Pairs
RADIOACTIVITY 118,120Sb(EC); measured decay products, Eγ, Iγ; deduced level energies, T1/2. Comparison with theoretical calculations.
Phys.Rev. 156, 1316 (1967)
E.J.Schneid, A.Prakash, B.L.Cohen
(d, p) and (d, t) Reactions on the Isotopes of Tin
NUCLEAR REACTIONS 112,114,115,116,117,118,120,119,122,124Sn(d, p), E=15 MeV; measured σ(Ep, θ). 114,116,117,118,119,120,121,122,124Sn(d, t), E=15 MeV; measured σ(Et, θ). 113,115,116,117,118,119,120,121,123,125Sn deduced levels, L(n), J, π, S.
Nucl.Phys. A110, 1 (1968)
J.H.Bjerregaard, O.Hansen, O.Nathan, L.Vistisen, R.Chapman, S.Hinds
The Reactions 116,118Sn(t, p)118,120Sn
NUCLEAR REACTIONS 116,118Sn(t, p), E=12-13 MeV; measured Q, σ(θ, Ep). 118,120Sn deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(68)90678-7
Nucl.Phys. A115, 309 (1968)
M.Bormann, A.Behrend, I.Riehle, O.Vogel
Untersuchung von (n, 2n) Anregungsfunktionen
NUCLEAR REACTIONS 52Cr, 75As, 85Rb, 106Cd, 112Sn, 121Sb, 140,142Ce, 141Pr, 144Sm, 165Ho, 181Ta(n, 2n), E = 12.6-19.6 MeV; 123Sb, 144Sm(n, 2n), E = 14.1 MeV; measured σ(E), isomeric cross-section ratios.
RADIOACTIVITY 51Cr, 74As, 105Cd, 120,122Sb, 140Pr, 143Sm, 164Ho, 180Ta; measured T1/2.
doi: 10.1016/0375-9474(68)90006-7
Nucl.Phys. A115, 273 (1968)
R.A.Broglia, C.Riedel, B.Sorensen, T.Udagawa
The Pairing Vibrational Model and the Analysis of the 116,118Sn(t, p) Reactions
doi: 10.1016/0375-9474(68)90004-3
Nucl.Phys. A111, 81 (1968)
S.A.Fulling, G.R.Satchler
Theoretical Analysis of 30 MeV Proton Inelastic Scattering
NUCLEAR REACTIONS 28Si, 40Ca, 56Fe, 58,60Ni, 120Sn, 208Pb(p, p'), E=30.3 MeV; measured nothing; analyzed σ(θ). 28Si, 40Ca, 56Fe, 58,60Ni, 120Sn, 208Pb deduced deformation parameters.
doi: 10.1016/S0375-9474(68)90388-6
Nucl.Data A4, 1 (1968)
R.S.Hager, E.C.Seltzer
Internal Conversion Tables. Part 1: K-, L-, M-Shell Conversion Coefficients for Z = 30 to Z = 103
IPCR Cyclotron Progr.Rept. 2, p.98 (1968)
A.Hashizume, T.Inamura, T.Kato, Y.Tendow, H.Kamitsubo, T.Yamazaki, T.Nomura
The Excited States in Xe Isotopes Studied by (H. I., xnγ) and (α, xnγ) Reactions
NUCLEAR REACTIONS 107,109Ag(n, xn), E=58-87 MeV; 128,130Te(α, xn), E not given; measured σ(E;Eγ), Iγ, αγ-delay. 116,118,120,128,130,132Xe deduced levels.
Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 677 (1968); Bull.Acad.Sci.USSR, Phys.Ser. 32, 623 (1969)
B.G.Kiselev, V.R.Burmistrov, V.A.Didorenko
Gamma-Ray Spectra of the Long-Lived Isomers of 118Sb and 120Sb
RADIOACTIVITY 118mSb, 120mSb [from 118Sn(p, n), 120Sn(d, 2n)]; measured T1/2, Eγ, Iγ. 118,120Sn deduced levels. Enriched 118Sn target, Ge(Li)detector.
J.Phys.Soc.Japan 25, 14 (1968)
I.Kumabe, H.Ogata, T.-H.Kim, M.Inoue, Y.Okuma, M.Matoba
Scattering of 34.4-MeV Alpha Particles by the Tin Isotopes
NUCLEAR REACTIONS 116,117,118,119,120Sn(α, α'), E=34.4 MeV; measured σ(Eα', θ). 116,117,118,119,120Sn deduced levels, L, deformation parameters.
Phys.Rev. 175, 1507 (1968)
I.-M.Ladenbauer-Bellis, H.Bakhru
Decay Studies of Iodine-118 and -120
NUCLEAR STRUCTURE 120I, 118I; measured not abstracted; deduced nuclear properties.
Phys.Rev. 174, 1429 (1968)
W.Makofske, W.Savin, H.Ogata, T.H.Kruse
Elastic and Inelastic Proton Scattering from Even Isotopes of Cd, Sn, and Te
NUCLEAR REACTIONS 110,112,114,116Cd, 112,116,118,120,122,124Sn, 126,128,130Te(p, p'), E=16 MeV; measured σ(θ).
J.Phys.(Paris) 29, 550 (1968)
O.Rahmouni
Nouvelles Transitions des Etains Pairs 120, 118, 116, 114 et de l'Antimoine Impair-Impair 116
RADIOACTIVITY 116Te, 116,118,120Sb; measured Eγ, Iγ. 116Sb, 116,118,120Sn deduced levels, J, π.
Nucl.Phys. A123, 99 (1969)
I.Bergstrom, C.J.Herrlander, A.Kerek, A.Luukko
Excited Nuclear Levels in Doubly Even Xe Isotopes Populated in (α, 2n) Reactions
NUCLEAR REACTIONS Sn, Te(α, 2nγ), E=28 MeV; measured σ(Eγ, θ). 118,120,122,124,126Te, 124,126,128,130,132Xe deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90892-6
Phys.Letters 29B, 652 (1969)
J.Chaumont, E.Roeckl, Y.Nir-El, C.Thibault-Philippe, R.Klapisch, R.Bernas
Identification of New Neutron-Deficient Nuclides 76Rb and 118Cs. Half-Lives of 78Rb, 119-124Cs, 126Cs
RADIOACTIVITY 78Rb, 119,120,121,122,123,124,126Cs [from Ta, Th, U(p, X)]; measured T1/2. Mass spectrometer.
doi: 10.1016/0370-2693(69)90100-2
CEA-N 1232, p.42 (1969)
M.L.Chatterjee, N.Cindro, M.Conjeaud, B.Fernandez, S.Harar, E.Thuriere, M.Turk
Reactions 121,123Sb(t, α)120,122Sn
NUCLEAR REACTIONS 121,123Sb(t, α), E=11.8 MeV; measured σ(Eα, θ). 120,122Sn deduced levels, J, π.
Phys.Rev. 184, 1162 (1969)
T.H.Curtis, R.A.Eisenstein, D.W.Madsen, C.K.Bockelman
Quadrupole and Octupole Excitations of the Even Tin Isotopes by Electron Scattering
NUCLEAR REACTIONS 116,118,120Sn(e, e') , E = 60 MeV; measured σ(Ee'); deduced elastic, inelastic form factors. 116,118,120Sn deduced B(EL).
Contrib.Intern.Conf.Properties Nucl.States, Montreal, Canada, p.120(1969)
B.Cujec, R.Dayras
Spins of the L=1 States in 55Co
NUCLEAR REACTIONS 54Fe(3He, dγ), E = 10 MeV; measured σ(Ed, Eγ). 55Co levels deduced J, π, γ-branching. Ge(Li) detector.
Nucl.Phys. A133, 310 (1969); R.R.Borchers - Priv.Comm. (May 1972)
G.M.Heestand, R.R.Borchers, B.Herskind, L.Grodzins, R.Kalish, D.E.Murnick
g-Factors for 2+ States of Doubly Even Nuclei (Ge, Se, Mo, Ru, Pd, Cd and Te)
NUCLEAR REACTIONS 70,72,74,76Ge, 76,78,80,82Se, 98,100Mo, 99,100,102,104Ru, 104,106,108,110Pd, 110,112,114,116Cd, 120,122,124,126,128,130Te(16O, 16O'γ); measured γγ(θ, H) from recoil implantation. 70,72,74,76Ge, 76,78,80,82Se, 98,100Mo, 99,100,102,104Ru, 104,106,108,110Pd, 110,112,114,116Cd, 120,122,124,126,128,130Te deduced g for first 2+ state.
doi: 10.1016/0375-9474(69)90633-2
Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 1340 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 1238 (1970)
B.G.Kiselev, V.R.Burmistrov
The Decay of 120Sb
RADIOACTIVITY 120Sb[from 120Sn(p n)]; measured Eβ, Eγ, Iγ; deduced Qβ. 120Sn deduced levels. Ge(Li) detector, enriched target.
Phys.Rev. 186, 1270 (1969); Supersedes PPAR-13
E.H.Spejewski, P.K.Hopke, F.W.Loeser, Jr.
Level Structure of Te116,118,120,122
RADIOACTIVITY 116,118,120,122I; measured Eγ, Iγ, γγ-coin. 116,118,120Te deduced levels. 122Te deduced levels, J, π. Ge(Li) detectors.
Nucl.Phys. A147, 326 (1970)
O.Beer, A.El Behay, P.Lopato, Y.Terrien, G.Vallois, K.K.Seth
Spectroscopy of Even Tin Isotopes by Inelastic Scattering of 24.5 MeV Protons
NUCLEAR REACTIONS 116,118,120,122,124Sn(p, p'), Ep=24.5 MeV; measured σ(Ep', θ). 116,118,120,122,124Sn deduced J, π, β(L). Enriched targets.
doi: 10.1016/0375-9474(70)90271-X
Nucl.Phys. A146, 597 (1970)
G.Bruge, J.C.Faivre, H.Faraggi, A.Bussiere
44 MeV α-Particle Scattering on Doubly Even Spherical Nuclei Near Closed Shells and Nuclear Structure of Collective States
NUCLEAR REACTIONS 40Ca, 46,48,50Ti, 52Cr, 54,56,58Fe, 58,60,62,64Ni, 64Zn, 112,114,116,118,120,122,124Sn, 208Pb(α, α'), Eα=44 MeV; measured σ(Eα', θ). 40Ca, 46,48,50Ti, 52Cr, 54,56,58Fe, 58,60,62,64Ni, 64Zn, 112,114,116,118,120,122,124Sn, 208Pb deduced levels, deformation lengths, B(E2), B(E3). Enriched targets.
doi: 10.1016/0375-9474(70)90747-5
Thesis, Univ.Paris (1970); NP-18461 (1970)
V.Comparat
Etude de la Diffusion Elastique des Protons de 156 MeV par les Isotopes Pairs de l'Etain
NUCLEAR REACTIONS 116,118,120Sn(p, p), (p, p'), E=156 MeV; measured σ(θ); deduced optical model parameters. 116, 118, 120sn deduced deformation parameters.
Nucl.Phys. A157, 1 (1970)
D.G.Fleming, M.Blann, H.W.Fulbright, J.A.Robbins
(p, t) Reactions on the Even Tin Isotopes
NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(p, t), E=20 MeV; measured σ(Et, θ). 112Sn(p, t) deduced Q. 110Sn deduced mass excess. 110,112,114,116,118,120,122Sn deduced levels. 122Sn levels deduced J, π.
doi: 10.1016/0375-9474(70)90094-1
Izv.Akad.Nauk SSSR, Ser.Fiz. 34, 2048 (1970); Bull.Acad.Sci.USSR, Phys.Ser. 34, 1825 (1971)
S.Gabrakov, Z.Zhelev, N.G.Zaitseva, I.Penev, S.S.Sabirov
The Radiation from 120I, 120*I, 122I, and 126I, and the Nature of the Levels in Even-Even Tellurium Isotopes (A = 120, 122, 124, 126)
RADIOACTIVITY 120,122,126I[from Ta(660-MeV p, X)]; measured T1/2, Eγ, Iγ, I(ce), Eβ, Iβ, βγ-, γγ-coin. 120,122,126Te, 126Xe deduced levels, J, π.
Phys.Rev. C2, 639 (1970)
C.H.Johnson, R.L.Kernell
(p, n) Cross Sections and the Strength Functions for 3- to 5.5-MeV Protons on In and Sn Isotopes
NUCLEAR REACTIONS In, Sn, 117,119,120,122,124Sn(p, n), E=3-5.5 MeV; measured σ(E); deduced Q for 120Sn(p, n).
Nucl.Phys. A147, 461 (1970)
O.Karban, P.D.Greaves, V.Hnizdo, J.Lowe, G.W.Greenlees
Inelastic Scattering of Polarized Protons at 30.3 MeV by 54,56Fe, 58Ni, 120Sn and 208Pb
NUCLEAR REACTIONS 54,56Fe, 58Ni, 120Sn, 208Pb(polarized p, p'), E=30.3 MeV; measured σ(θ), asymmetry (θ). 54,56Fe, 58Ni, 120Sn, 208Pb deduced nuclear deformations β(L). Enriched targets.
doi: 10.1016/0375-9474(70)90592-0
Thesis, Univ.Paris (1970); NP-18447 (1970)
J.-M.Lagrange
Contribution a l'Etude des Isotopes Pairs de Tellure
RADIOACTIVITY 118I, 120gI, 120mI, 124I, 122Xe, 122Sb, 124Sb; measured Eγ, Iγ, γγ-coin; deduced log ft. 118,120,122,124Te deduced levels, J, π, γ-branching.
J.Phys.Soc.Jap. 29, 789 (1970)
K.Okano, T.Takeuchi
The Decay of 15.9 min 120Sb
RADIOACTIVITY 120Sb; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced log ft. 120Sn deduced levels, J, π.
Proc.Int.Conf.Prop.Nuclei Far from Region of Beta-Stability, Leysin, Switzerland, Vol.2, p.1093 (1970); CERN-70-30 (1970)
The OSIRIS Collaboration
Neutron-Rich Nuclides Obtained Using the OSIRIS Facility
RADIOACTIVITY 75,76,77Zn, 76,77,78,79Ga, 77,79,80Ge, 79,81,82,83As, 83,85Se, 85,87,88,89Br, 91Kr, 91,92Rb, 113,114,115,116,117,118,119,121Ag, 119,121,122Cd, 119,120,121,122,123,124,125,126,127,128,129,130,131In, 123,125,127,130,133Sn, 133,137,138,139I, 135Te, 137,139Xe, 139,141Cs, 143,145Ba, 145,146,147La, 145,146,147Ce; measured T1/2.
Can.J.Phys. 48, 1687 (1970)
R.J.Pan, D.W.Hetherington, D.B.McConnell, H.W.Taylor
Decay of 17.7 min 120gSb and 5.8 Day 120mSb
RADIOACTIVITY 120gSb, 120mSb; measured Eγ, Iγ, γγ-coin, T1/2; deduced (EC+β+) branching. 120Sn deduced levels. Ge(Li), NaI(Tl)-Ge(Li) detectors.
Phys.Rev. C2, 2001 (1970)
Y.Schlesinger, H.Szichman, G.Ben-David, M.Hass
Radiation Widths of Bound Nuclear Levels in the Vicinity of the Neutron Threshold
NUCLEAR REACTIONS 66Zn, 80Se, 86Sr, 120Sn, 130Te, 139La(γ, γ'), E=6-9 MeV; measured σ(Eγ'). 66Zn, 80Se, 86Sr, 120Sn, 130Te, 139La deduced levels, level-width.
Phys.Rev. C2, 2015 (1970)
P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner
Static Quadrupole Moment of the First 2+ States of the Even Tin Nuclei
NUCLEAR REACTIONS 112,116,118,120,122,124Sn(α, α'γ), E=10 MeV; 112,114,116,118,120,122,124Sn(16O, 16O'γ), E=46 MeV; measured σ(Eα', Eγ), σ(E(16O'), Eγ). 112,116,118,120,122,124Sn levels deduced quadrupole moment, B(E2).
Phys.Rev. C1, 1069 (1970)
R.A.Warner, J.E.Draper
Ground-State Quasirotational Bands to 8+ in 114-126Te Produced by (α, xn)
NUCLEAR REACTIONS 112,114,115,116,117,118,119,120,122,124Sn(α, xnγ), E=25-75 MeV; measured σ(E;Eγ, θ(γ)), αγ-delay. 112,114,116,118,120,122,124,126Te deduced transitions.
Z.Phys. 232, 256 (1970)
H.J.Wolf, P.Steiner, E.Gerdau, W.K.Muller, U.Lewandowski, A.Roggenbuck
Das Quadrupolmoment des 2, 3 Mev-Zustandes in 120Sn
NUCLEAR REACTIONS 119Sn(γ, γ), E=23.8 keV; measured Mossbauer effect.
RADIOACTIVITY 120Sb; measured γγ(θ, t). 120Sn level deduced quadrupole moment.
Bull.Amer.Phys.Soc. 16, No.10, 1170, DB11 (1971)
T.S.Bhatia
Level Structure of Sb120 and Sb122
NUCLEAR REACTIONS 121,123Sb(d, t), E=17 MeV; measured σ(θ). 120,122Sb deduced levels, J, π, L, S.
Nucl.Phys. A174, 485 (1971)
G.Duhamel, L.Marcus, H.Langevin-Joliot, J.P.Didelez, P.Narboni, C.Stephan
Diffusion Elastique et Inelastique de Deutons de 80 MeV
NUCLEAR REACTIONS 12C, 24Mg, 27Al, 58Ni, 68Zn, 89Y, 120Sn, 208Pb(d, d), (d, d'); 12C(d, p)13C, Eα=80 MeV; measured σ(θ); deduced optical potentials. 12C, 58Ni, 68Zn, 120Sn deduced deformation parameters. 13C deduced S. Enriched targets.
doi: 10.1016/0375-9474(71)90398-8
Phys.Lett. 36B, 334 (1971)
B.Fogelberg, A.Backlin, T.Nagarajan
Energy Levels in 114,116,118,120,122Cd as Observed in the Beta Decay of Ag Isotopes
RADIOACTIVITY 114,116,118,120,122Ag; measured Eγ, Iγ, γγ-coin, T1/2, I(ce), Iβ; deduced log ft. 114,116,118Ag, 120,122Ag deduced levels, J, π.
doi: 10.1016/0370-2693(71)90718-0
Phys.Lett. 35B, 35 (1971)
V.Hnizdo, J.Lowe
Collective-Model Analysis of Inelastic Proton Scattering Using Potentials Derived from Nuclear Matter Distributions
NUCLEAR REACTIONS 56Fe, 58Ni, 120Sn, 208Pb(polarized p, p), E=30.3 MeV; measured nothing; analyzed σ(θ), asymmetry(θ). Collective model analysis.
doi: 10.1016/0370-2693(71)90433-3
Z.Phys. 241, 150 (1971)
E.Liukkonen, J.Hattula
Level Structure of 120Sn from the Decay of 120In and 120Sb Isomers
RADIOACTIVITY 120mIn, 120mSb; measured Eγ, Iγ, γγ-coin; deduced log ft. 120mIn; measured T1/2, γγ-delay. 120Sn deduced levels, J, π.
Phys.Rev. C6, 595 (1972)
I.Brissaud, B.Tatischeff, L.Bimbot, V.Comparat, A.Willis, M.K.Brussel
Study of Some Properties of Tin Isotopes Through High-Energy Alpha-Particle Scattering
NUCLEAR REACTIONS 116,118,120,124Sn(α, α), (α, α'), E=166 MeV; measured σ(θ); deduced optical model parameters. 116,118,120,124Sn deduced B(E2), B(E3), nuclear radii.
Nucl.Phys. A192, 595 (1972)
C.Droste, W.Neubert, S.Chojnacki, T.Morek, K.F.Alexander, Z.Wilhelmi
Investigation of Neutron-Deficient Cs Nuclei
RADIOACTIVITY 124Ba[from 116Sn(12C, 4n)]; measured Eγ, Iγ, T1/2. 124Cs deduced levels, ground state J, π. 122Cs[from 109Ag(16O, 3n)]; measured Eγ, Iγ, T1/2, γγ-coin. 122Cs deduced isomeric state, J. 120Cs[from 107Ag(18O, 5n), 107Ag(16O, 3n)]; measured Eγ, T1/2.
NUCLEAR REACTIONS 115In(12C, xn), E=50-80 MeV; 109Ag(18O, xn), E=50-110 MeV; measured relative σ(E), Eγ, Iγ, E(ce), I(ce), (HI)γ-delay, (HI)ce- delay . 123Cs deduced levels, T1/2. 124Cs deduced ground state T1/2, J, π.
doi: 10.1016/0375-9474(72)90092-9
Phys.Rev. C5, 561 (1972)
R.H.Howell, A.I.Galonsky
Proton Spin-Flip Probability in Inelastic Scattering on 120Sn and 124Sn at 30 MeV
NUCLEAR REACTIONS 120,124Sn(p, p'γ), E=30 MeV; measured spin-flip probability(θ). DWBA.
Nucl.Phys. A192, 651 (1972)
R.H.Howell, G.R.Hammerstein
Effect of Complex Coupling in Inelastic Cross Sections, Asymmetries and Spin Flip in the DWA
NUCLEAR REACTIONS 58Ni, 120Sn, 208Pb(p, p'), calculated σ(θ), spin-flip probability, asymmetry(θ); analyzed complex coupling effects.
doi: 10.1016/0375-9474(72)90096-6
Proc.Int.Conf.Nucl.Struct.Studies Using Electron Scattering and Photoreaction, Sendai, Japan, K.Shoda, H.Ui, Eds., Res.Rep.Lab.Nucl.Sci.Tohoku Univ. 5, Suppl. p.139 (1972)
K.Hosoyama, Y.Torizuka, Y.Kawazoe, H.Ui
Transition Charge Density of Vibrational Nuclei
NUCLEAR REACTIONS 106Pd, 114Cd, 116,120Sn(e, e'), E=183, 250 MeV; measured σ(Ee'). 106Pd, 114Cd, 116,120Sn deduced B(E2), charge density.
Proc.Int.Conf.Nucl.Struct.Studies Using Electron Scattering and Photoreaction, Sendai, Japan, K.Shoda, H.Ui, Eds., Res.Rep.Lab.Nucl.Sci.Tohoku Univ. 5, Suppl. p.125 (1972)
Phan Xuan Ho, J.B.Bellicard, P.Leconte, I.Sick
Inelastic Electron Scattering on Single Closed Shell Nuclei
NUCLEAR REACTIONS 50Ti, 52Cr, 54Fe, 90Zr, 92Mo, 116,120,124Sn(e, e'), E=209 MeV; measured σ(Ee', θ).
Sci.Pap.Inst.Phys.Chem.Res. 66, 141 (1972)
T.Inamura
Search for Shape Isomers in Neutron Deficient Even Xe and Ba Isotopes in the Nanosecond Time Range
NUCLEAR REACTIONS 107,109Ag, 115In(14N, xnγ), E=65, 85 MeV; measured 14Nγ(t). 116,118,120Xe, 124,126Ba deduced no isomers.
Nucl.Phys. A183, 105 (1972)
H.Iwe, R.Reif, C.Riedel
Reaction Spectroscopy with Even Tin Isotopes
NUCLEAR REACTIONS 116,118Sn(t, p), E=12 MeV; 116Sn(p, p'), E=55 MeV; 116,118,120Sn(p, p'), E=16 MeV; calculated σ(θ). DWBA.
doi: 10.1016/0375-9474(72)90933-5
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, 127,129,131,132Sn, 128,133Sb, 132,135,136,137I, 133,135Te, 139,140Cs, 141Ba; measured Eβ, deduced Q.
Phys.Rev. C5, 1658 (1972)
W.Kutschera, W.Dehnhardt, O.C.Kistner, P.Kump, B.Povh, H.J.Sann
Lifetime Measurements in 120,122Xe and 126,128Ba
NUCLEAR REACTIONS 108,110Pd, 114,116Cd(16O, 4nγ), E=75, 80 MeV; measured recoil distance. 120,122Xe, 126,128Ba levels deduced T1/2, B(E2), deformation parameters.
Nucl.Phys. A196, 337 (1972)
M.B.Lewis, F.E.Bertrand
Evidence from Inelastic Proton Scattering for a Giant Quadrupole Vibration in Spherical Nuclei
NUCLEAR REACTIONS 27Al, 54Fe, 120Sn, 209Bi(p, p'), Ep=61.7 MeV; measured σ(θ). 27Al, 54Fe, 120Sn, 209Bi deduced giant quadrupole excitation from systematics of σ.
doi: 10.1016/0375-9474(72)90968-2
N72-18705 (1972)
R.F.Leonard
Particle Hole States in Sn120
NUCLEAR REACTIONS 121Sb(d, 3He), E=45 MeV; measured σ(θ). 120Sn deduced levels, L(p), J, π, S.
Part.Nucl. 4, 209 (1972)
A.Osman
Short-Range Correlations in One- and Two-Nucleon Transfer Reactions
NUCLEAR REACTIONS 31P(t, p), E=12.1 MeV; 40,48Ca, 50,52,54Cr(d, p), E=10 MeV; 70Ge(p, d), 96Zr, 116,118Sn, 206Pb(t, p), 210Pb(p, t), E=20 MeV; measured nothing, calculated σ(θ). 33P, 41,49Ca, 51,53,55Cr, 69Ge, 98Zr, 118,120Sn, 208Pb deduced L, S.
J.Inorg.Nucl.Chem. 34, 1485 (1972)
J.A.Panontin, N.Sugarman
Mass Yield Distribution and Charge Dispersion in 450 MeV Proton Fission of 238U
RADIOACTIVITY 109In, 115mIn, 116mIn, 116mSb, 117mCd, 117gCd, 117gIn, 117mIn, 117mSn, 117Sb, 118mSb, 120mSb, 122Sb, 126gSb, 126mSb, 127Sb, 128mSb, 128gSb; measured T1/2.
NUCLEAR REACTIONS, Fission 238U(p, F), E=450 MeV; measured charge, mass distributions, σ for Ag, Cd, In, Sn, Sb isotope formation.
doi: 10.1016/0022-1902(72)80268-9
Phys.Lett. 39B, 337 (1972)
H.L.Ravn, S.Sundell, L.Westgaard
Very Neutron-Deficient Isotopes of Cs Studied by on-Line Isotope Separator Techniques
RADIOACTIVITY 117,118,119,120Cs; measured T1/2.
doi: 10.1016/0370-2693(72)90132-3
COO-1265-126, p.88 (1972)
R.Seltz, N.M.Hintz
(p, t) Strength to Excited 0+ States in Even Te Isotopes
NUCLEAR REACTIONS 122,124,126,128,130Te(p, t); measured σ(θ). 120,122,124,126,128Te deduced levels, J, π, 0+ state strengths.
AECL-4205, p.12 (1972)
S.H.Sie, R.L.Graham, J.S.Geiger, H.R.Andrews, D.Ward
Search for the Transient Field Effect in 120Sn by DSAM
NUCLEAR REACTIONS 120Sn(35Cl, 35Cl'), E=100 MeV; measured unspecified. 120Sn level deduced g.
Phys.Rev. C5, 1705 (1972)
M.Sugawara, K.Shoda, T.Saito, H.Miyase, A.Suzuki, S.Oikawa, R.Bergere
Photoproton Reaction on Sn Isotopes
NUCLEAR REACTIONS 116,117,118,120,122,124Sn(γ, p), (e, e'p), E < 24 MeV; measured σ(E;Ep). 116,117,118,120,122,124Sn deduced resonances, isobaric analogs.
Yad.Fiz. 16, 677 (1972); Sov.J.Nucl.Phys. 16, 380 (1973)
A.V.Yushkov
Shapes of Heavy Nuclei
NUCLEAR REACTIONS 92,100Mo, 116,118,120,122Sn, 122,124,126,128,130Te, 148,152,154Sm, 166Er, 176Yb(α, α), (α, α'); calculated signs for equlibrium deformation.
INR-1464, p.14 (1973)
J.Araminowicz, J.Dresler
Investigation of the (n, 2n) Reaction with 14.6 MeV Neutrons
RADIOACTIVITY 13N, 18F, 30P, 34Cl, 38K, 45Ti, 49,51Cr, 53Fe, 58Co, 57Ni, 64Cu, 63Zn, 68Ga, 69,75Ge, 74As, 78Br, 84,86Rb, 85Sr, 89,95Zr, 91,99Mo, 101Pd, 106Ag, 112In, 111Sn, 120,122Sb, 129Te, 126I, 132Cs, 140Pr, 180Ta, 208Tl, 203Pb; measured T1/2.
NUCLEAR REACTIONS 14N, 19F, 23Na, 31P, 35Cl, 39K, 46Ti, 50,52Cr, 55Mn, 54Fe, 59Co, 58Ni, 65Cu, 64,66Zn, 69Ga, 70,76Ge, 75As, 79Br, 85,87Rb, 86Sr, 89Y, 90,96Zr, 92,100Mo, 102Pd, 107Ag, 113In, 112Sn, 121,123Sb, 130Te, 127I, 133Cs, 141Pr, 181Ta, 203Tl, 204Pb(n, 2n); measured σ.
Nucl.Phys. A210, 397 (1973)
L.Bimbot, B.Tatischeff, I.Brissaud, Y.Le Bornec, N.Frascaria, A.Willis
Study of Microscopic Wave Functions of Nuclear Levels Through Inelastic Scattering of 166 MeV α-Particles
NUCLEAR REACTIONS 12C, 24Mg, 28Si, 32S, 40,44,48Ca, 48Ti, 56Fe, 58,60,62Ni, 68Zn, 88Sr, 90Zr, 92Mo, 116,118,120,124Sn, 140Ce, 208Pb(α, α'), Eα=166 MeV; measured σ(Eα, θ); α-n interaction, phenomenological, calculated optical potentials used with DWBA; microscopic wave functions tested.
doi: 10.1016/0375-9474(73)90310-2
Nucl.Instrum.Methods 113, 157 (1973)
K.Fransson, M.Af Ugglas, A.Engstrom
An Isotope Separator on-Line System at a Cyclotron for Heavy Ions (PINGIS)
RADIOACTIVITY 120,120mAg, 120In; measured Eγ.
Nucl.Phys. A213, 45 (1973)
G.R.Hammerstein, R.H.Howell, F.Petrovich
Electron and Proton Inelastic Scattering from 40Ca, 120Sn, and 208Pb
NUCLEAR REACTIONS 40Ca, 120Sn, 208Pb(e, e'), (p, p'); calculated σ(θ).
doi: 10.1016/0375-9474(73)90181-4
Proc.Int.Conf.Nucl.Phys., Munich, J.de Boer, H.J.Mang, Eds., North-Holland Publ.Co., Amsterdam, Vol.1, p.59 (1973)
M.Matoba, M.Hyakutake, J.Nidome, K.Yagi, Y.Aoki, C.Rangacharyulu
Excitation of Two Quasi-Particle States in Even-Mass Te Nuclei
NUCLEAR REACTIONS 122,124,126,128,130Te(p, t); measured σ(Et). 120,122,124,126,128Te deduced levels.
Ann.Rept.Mich.State Univ.Cyclotron Lab., 1972-1973, p.101 (1973)
D.M.Patterson, R.R.Doering, A.I.Galonsky
(p, n) Reactions to the Isobaric Analog States of 48Ca, 90Zr, 120Sn, and 208Pb at 25 MeV
NUCLEAR REACTIONS 48Ca, 90Zr, 120Sn, 208Pb(p, n); measured σ(Et, θ). 48Sc, 90Nb, 120Sb, 208Bi deduced levels.
Nucl.Phys. A206, 623 (1973)
G.Perrin, Nguyen Van Sen, J.Arvieux, C.Perrin, R.Darves-Blanc, J.L.Durand, A.Fiore, J.C.Gondrand, F.Merchez
Elastic and Inelastic Scattering of Polarized Deuterons by 120Sn at 28.6 MeV
NUCLEAR REACTIONS 120Sn(polarized d, d), E=28.6 MeV; measured σ(θ), iT11(θ), T20(θ), T22(θ)-square root(3/2)T20(θ); 120Sn(polarized d, d'), E=28.6 MeV; measured σ(θ), iT11(θ); deduced optical-model parameters. 120Sn deduced deformations β2, β3. Enriched target.
doi: 10.1016/0375-9474(73)90091-2
INS-J-140 (1973)
M.Sakai
3+ State in Even-Even Medium Soft Nuclei
NUCLEAR REACTIONS 75As, 79Br, 81Br, 85Rb, 121Sb, 127I, 133Cs(p, 2nγ), 121Sb, 127I, 139La, 141Pr(p, 4nγ); 74Se, 78,80Kr, 84Sr, 118,120Te, 124,126Xe, 132Ba, 136Ce, 138Nd deduced levels, J, π.
J.Inorg.Nucl.Chem. 35, 3055 (1973)
O.Scheidemann, E.Hagebo
120Cd and 122Cd
RADIOACTIVITY 120,122Cd, 120,122In; measured Eγ, Iγ, T1/2. Deduced log ft. 120,122Sn deduced levels, γ-branching.
doi: 10.1016/0022-1902(73)80002-8
Z.Phys. 259, 217 (1973)
H.Szichman
Studies on the Level Schemes of 66Zn, 144Sm and 120Sn Using the (γ, γ') Reaction
NUCLEAR REACTIONS 66Zn, 120Sn, 144Sm(γ, γ'), E=Ni(n, γ) source; measured σ(Eγ', θ). 66Zn, 120Sn, 144Sm deduced levels, J, π, γ-multipolarity, level-width.
Nucl.Phys. A199, 65 (1973)
Y.Terrien
Microscopic Calculation for Proton Inelastic Scattering from Collective Levels in the Tin Isotopes
NUCLEAR REACTIONS 116,118,120,122,124Sn(p, p'), E=16, 24.5 MeV; analyzed σ(θ); deduced transition densities.
doi: 10.1016/0375-9474(73)90334-5
Phys.Lett. 45B, 235 (1973)
Y.Terrien, J.L.Escudie, M.Buenerd, J.M.Loiseaux, P.Martin, J.B.Viano
The Role of the Imaginary Part in the Microscopic Description of (p, p') Scattering
NUCLEAR REACTIONS 92Mo, 116,120,124Sn(p, p'), E=40 MeV; measured σ(θ).
doi: 10.1016/0370-2693(73)90191-3
Nucl.Phys. A215, 29 (1973)
Y.Terrien
The Role of the Imaginary Form Factor in the Microscopic Description of (p, p') Scattering from Nuclei with One Closed Shell
NUCLEAR REACTIONS 40Ca, 58,60,62,64Ni, 88Sr, 90Zr, 92Mo, 116,118,120,124Sn(p, p'), E=20-62 MeV; calculated σ(Ep', θ).
doi: 10.1016/0375-9474(73)90098-5
Phys.Rev. C8, 796 (1973)
W.G.Wyckoff, J.E.Draper
In-Beam Electron Conversion from Yrast Levels of 72,74,76,78Se, 78,80,82,84Kr, 114,116,118,120,122,124,126Te, and 130,132,134,136,138Ce Excited by (α, xn)
NUCLEAR REACTIONS 70,72,74,76Ge, 76Se(α, 2n), E=27.5 MeV; 78,80,82Se(α, 2n), E=25 MeV; 112,116Sn(α, 2n), E=33 MeV; 114,118,120,122Sn(α, 2n), E=27.5 MeV; 124Sn(α, 2n), E=25 MeV; 130,134,136Ba(α, 4n), E=62 MeV; 130,136Ba(α, 2n), E=27.5, 33 MeV; measured E(ce), I(ce). 72,74,76,78Se, 78,80,82,84Kr, 114,116,118,120,122,124,126Te, 130,132,134,136,138Ce transitions deduced ICC.
Priv.Comm. (October 1974)
M.R.Ahmed, S.Al-Najjar, M.A.Al-Amili, N.Rammo, Y.S.Al-Shiraida, A.M.Demidov, L.I.Govor, Y.K.Cherepantsev
De-Excitation of the 116,118,120,122,124Sn Levels from the Inelastic Scattering of Reactor Fast Neutrons
NUCLEAR REACTIONS 116,118,120,122,124Sn(n, n'γ), E=fast; measured Eγ, Iγ. 116,118,120,122,124Sn deduced levels, J, π.
Bull.Amer.Phys.Soc. 19, No.9, 995, AE4 (1974)
F.D.Bechetti, W.S.Gray, R.Tickle, J.Janecke
The Sn(3He, t) Reaction to Isobaric Analog States in the Sb Isotopes
NUCLEAR REACTIONS 112,116,118,120,122,124Sn(3He, t), E=47 MeV; measured σ(Et); deduced Q. 112,116,118,120,122,124Sb resonances deduced level-width.
Nucl.Phys. A221, 1 (1974)
P.T.Callaghan, M.Shott, N.J.Stone
The Magnetic Dipole Moments of Doubly Odd Antimony Isotopes with (h11/2)n Neutron Configuration
RADIOACTIVITY 118mSb; measured T1/2, γ(θ, t), NMR; 120mSb; measured γ(θ, t); 122Sb; measured NMR; 124,125Sb; measured nothing. 118m,120mSb deduced J, μ. 122Sb deduced hyperfine field in Fe. 124,125Sb deduced μ.
doi: 10.1016/0375-9474(74)90094-3
Nucl.Phys. A234, 157 (1974)
J.Conrad, R.Repnow, E.Grosse, H.Homeyer, E.Jaeschke, J.P.Wurm
Quasi-Rotational Bands in Neutron Deficient Doubly Even Ba Isotopes
NUCLEAR REACTIONS 106,108,110Cd(16O, 2nγ), E=52.5-66 MeV; measured Eγ, Iγ, γγ, nγ, pγ, αγ-coincidences. 120,122,124Ba deduced levels, J, π. 120Ba deduced ground-state T1/2 upper limit. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(74)90384-4
Nucl.Phys. A226, 219 (1974)
C.Ekstrom, W.Hogervorst, S.Ingelman, G.Wannberg
Atomic-Beam Investigations of Some Antimony Nucleides
NUCLEAR MOMENTS 116,116m,118m,120m,128Sb; measured J. 117Sb; measured a, b; deduced μ, quadrupole moment. 116Sb; measured T1/2.
doi: 10.1016/0375-9474(74)90403-5
Z.Phys. 267, 209 (1974)
W.Fischer, M.Hartmann, H.Huhnermann, H.Vogg
Isotopieverschiebung der Bariumnuklide 140Ba, 138Ba, 136Ba und 134Ba in der Ba II-Resonanzlinie 6 p 2P1/2 - 6 s 2S1/2
ATOMIC PHYSICS 132,134,136,138,140Ba; measured isotope shift, deduced nuclear charge radius.
COO-535-710, p.73 (1974)
H.W.Fielding, R.E.Anderson, D.A.Lind, C.D.Zafiratos, W.P.Alford
Studies of the (3He, n) Reaction on Sn, Cd, Zn, and Sr Isotopes
NUCLEAR REACTIONS 112,114Cd, 112,116,118,120,124Sn, 88Sr, 90,92,94Zr(3He, n); measured σ(En, θ). 114,116Sn, 114,118,120,122,126Te transitions deduced L.
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
Phys.Rev. C9, 1954 (1974)
G.K.Hubler, H.W.Kugel, D.E.Murnick
Nuclear Magnetic Moments of Very Short-Lived States via the Transient-Field Implantation Perturbed-Angular-Correlation Technique
NUCLEAR REACTIONS 54Fe(α, α'γ), E=2.1, 2.75 MeV; 54Fe(16O, 16O'γ), E=25.5 MeV; 104,106,108,110Pd(16O, 16O'γ), E=36 MeV; measured γ(θ, H). 54Fe, 104,106,108,110Pd levels deduced g. 70,72,74,76Ge, 98,100,102,104Ru, 104,106,108,110Pd, 110,112,114,116Cd, 120,122,124,126,128,130Te levels deduced g from reanalysis of IMPAC data.
Nucl.Phys. A223, 1 (1974)
S.Kikuchi, Y.Sugiyama
Study of Energy Levels of 120Sn Through the (n, n'γ) Reaction
NUCLEAR REACTIONS 120Sn(n, n'γ), E=2.0-3.1 MeV; measured Eγ, σ(E;Eγ, θ). 120Sn deduced levels, J, π, branching ratios, γ-mixing ratios. Enriched target.
doi: 10.1016/0375-9474(74)90275-9
Nucl.Phys. A225, 137 (1974)
H.G.Miller, R.M.Dreizler
A Microscopic Calculation of Inelastic Electron Scattering to the First 2+ State in Some Even Tin Isotopes
NUCLEAR REACTIONS 116,120,124Sn(e, e'), E=150, 250 MeV; calculated σ(θ), deduced form factor.
doi: 10.1016/0375-9474(74)90370-4
Nucl.Phys. A224, 437 (1974)
F.Munnich, D.Lode, H.Schrader, A.Hoglund, W.Pessara
The Decay of 120Xe
RADIOACTIVITY 120Xe [from Ce(p, 5pxn), mass separated]; measured T1/2, Eγ, Iγ, E(ce), I(ce), γγ coin, γγ delay, ce-γ delay; deduced log ft, Q. 120I deduced levels, ICC, γ-multipolarity, J, π, T1/2.
doi: 10.1016/0375-9474(74)90548-X
Phys.Lett. 51B, 45 (1974)
C.A.Whitten, Jr., J.Chai, N.Chirapatpimol, W.H.Dunlop, G.J.Igo
Study of the (p, np) Reaction on the Isotopes of Tin
NUCLEAR REACTIONS 112,114,115,116,117,118,119,120,122,124Sn(p, np), E=23, 38.5 MeV; measured σ(En, Ep). 112,114,115,116,117,118,119,120,122,124Sb IAS deduced level-width.
doi: 10.1016/0370-2693(74)90147-6
Nucl.Phys. A249, 349 (1975)
M.Campbell, K.W.D.Ledingham, A.D.Baillie, M.L.Fitzpatrick, J.Y.Gourlay, J.G.Lynch
The Ratio of K-Capture to Positon Emission in the Decay of 120Sb: Experiment and Theory Disagree
RADIOACTIVITY 120Sb [from 121Sb(γ, n)]; measured I(K X-ray)/Iβ+, T1/2, Iγ; deduced K-capture probability P(K)/P(β+), log ft.
doi: 10.1016/0375-9474(75)90192-X
MSUCL-162 (1975)
R.R.Doering, D.M.Patterson, A.Galonsky
A Microscopic Description of Isobaric-Analog-State Transitions Induced By 25-, 35-, and 45-MeV Protons
NUCLEAR REACTIONS 48Ca, 90Zr, 120Sn, 208Pb(p, n), E=25, 35, 45 MeV; measured σ(En, Eγ, θ). 48Sc, 90Nb, 120Sb, 208Bi deduced IAS.
Phys.Rev. C12, 1462 (1975)
R.Graetzer, S.M.Cohick, J.X.Saladin
Quadrupole Moments of 2+ States of Even Tin Isotopes
NUCLEAR REACTIONS 112,116,118,120,122,124Sn(α, α'), E=10.0, 10.5, 10.6 MeV; 112,116,118,120,122,124Sn(16O, 16O'), E=42.0, 46.0 MeV; measured σ(θ). 112,116,118,120,122,124Sn levels deduced quadrupole moment, B(E2).
Nucl.Phys. A239, 15 (1975)
P.Hornshoj, B.R.Erdal, P.G.Hansen, B.Jonson, K.Aleklett, G.Nyman
Beta-Strength Functions of Neutron-Deficient Isotopes in the Xenon and Mercury Regions
RADIOACTIVITY 182,183,184,185,186,187,189,191Hg, 182,183,184,185,186,187,188,190Au, 182,183,184,185Pt, 182,183Ir, 117,118,119,120,121,123Xe, 117,118,119,120,121I; measured total-absorption γ-spectra, deduced β-strength functions sβ(E). Mass separated samples, natural targets.
doi: 10.1016/0375-9474(75)91130-6
Phys.Lett. 57B, 147 (1975)
P.Hornshoj, P.Tidemand-Petersson, R.Bethoux, A.A.Caretto, J.W.Gruter, P.G.Hansen, B.Jonson, E.Hagberg, S.Mattsson
Beta-Delayed Alpha-Particle Emission from 118,120Cs
RADIOACTIVITY 118,119,120,122Cs; measured β delayed α, p emission; deduced α-branching.
doi: 10.1016/0370-2693(75)90010-6
Nucl.Phys. A252, 381 (1975)
D.C.Kocher, W.Haeberli
Vector Analyzing Power and Cross Section for (d, p) Reactions on 53Cr, 57Fe, 117Sn and 119Sn
NUCLEAR REACTIONS 53Cr, 57Fe(polarized d, d), (polarized d, p), E=10 MeV; 117,119Sn(polarized d, d), (polarized d, p), E=12 MeV; measured σ(θ), polarization parameters iT11(θ); deduced deuteron optical-model parameters, angular momentum transfer. 54Cr, 58Fe, 118,120Sn levels deduced J, π, S. Enriched targets.
doi: 10.1016/0375-9474(75)90507-2
Z.Phys. A 275, 127 (1975)
L.Westgaard, K.Aleklett, G.Nyman, E.Roeckl
Beta-Decay Energies and Masses of Short-Lived Isotopes of Rubidium, Caesium, Francium, and Radium
RADIOACTIVITY 106Rh(β-), 66Ga, 79Rb, 130,128,127,125Cs(EC), 223Fr, 227Ra(β-); measured decay products, Eβ; deduced Q. 76,77,78,80Rb, 126,124,123,122,121,120,119Cs(EC), 222,224,225,226,227Fr, 229Ra, 229Ac(β-); measured decay products, Eβ, βγ-coin; deduced Q, Q limits.
doi: 10.1007/bf01409588
Proc.Int.Conf.Nuclei Far from Stability, Cargese, Corsica, p.106 (1976); CERN-76-13 (1976)
T.Batsch, M.Nowicki, J.Zylicz, D.D.Bogdanov, V.A.Karnaukhov, L.A.Pietrov, A.Plochocki
Studies of the Decay of 120Cs, 118Cs and 116Cs
RADIOACTIVITY 118,120,116Cs; measured Eγ, Iγ, βγ-coin; deduced Q. 116,118,120Xe deduced levels.
Nucl.Phys. A271, 77 (1976)
F.D.Becchetti, W.S.Gray, J.Janecke, E.R.Sugarbaker, R.S.Tickle
Isobaric Analog States of the Tin and Tellurium Isotopes Studied with the (3He, t) Reaction at θ(L) = 0°
NUCLEAR REACTIONS 112,114,116,117,118,119,120,122,124Sn, 124,125,126,128,130Te(3He, t), E=45.9 MeV; measured σ(Et, θ), θ=0°. 112,114,116,117,118,119,120,122,124Sb, 124,125,126,128,130I deduced IAS, Coulomb displacement energies, Γ. Enriched targets, magnetic spectrometer.
doi: 10.1016/0375-9474(76)90269-4
Z.Phys. A276, 403 (1976)
J.Conrad, R.Repnow
Investigation of Neutron-Deficient Isotopes in the Barium-Region
NUCLEAR REACTIONS 106,108,110Cd(16O, xnypzαγ), E=52.5-66.0 MeV; measured σ(E, Eγ), γγ-, particle γ-coin. 119,120Xe, 119,120Cs, 119,120Ba deduced transitions. 121,122,123,124Ba, 120,122,124Ba deduced levels, K, J, π.
Proc.Int.Conf.Nuclei Far from Stability, 3rd, Cargese, France, R.Klapisch, Ed., CERN-76-13, p.193 (1976)
C.Ekstrom, W.Ingelman, G.Wannberg, M.Skarestad
Atomic-Beam Measurements of Nuclear Spins at ISOLDE, CERN
NUCLEAR MOMENTS 77,78,78m,79,84mRb, 120,121,122,122m,123,124,126,128,130mCs, 135mCs, 185Au; measured I.
J.Phys.Chem.Ref.Data 5, 835 (1976)
G.H.Fuller
Nuclear Spins and Moments
COMPILATION A=1-253; compiled μ, quadrupole moment, I.
Phys.Lett. 64B, 151 (1976)
A.Iordachescu, E.A.Ivanov, D.Plostinaru, O.Echt, G.Pascovici, S.Vajda, B.Constantinescu, P.Racoltea
Spin, Lifetime and Magnetic Moment of a New Isomeric State in 120Sb
NUCLEAR REACTIONS 120Sn(p, n), E=11 MeV; measured γ(θ, H, t), X-rays. 120Sb deduced level, J, π, g.
doi: 10.1016/0370-2693(76)90317-8
Nucl.Data Sheets 17, 39 (1976)
D.C.Kocher
Nuclear Data Sheets for A = 120
COMPILATION 120Ag, 120Cd, 120In, 120Sn, 120Sb, 120Te, 120I, 120Xe, 120Cs, 120Ba; compiled, evaluated structure data.
Nucl.Phys. A261, 223 (1976)
M.Matoba, M.Hyakutake, K.Yagi, Y.Aoki, C.Rangacharyulu
Excitation of 3-, 5- and 7- States in Te Isotopes A = 120, 122, 124, 126, 128 with (p, t) Reactions
NUCLEAR REACTIONS 122,124,126,128Te(p, t), E=51.9 MeV; measured σ(Et, θ). 120,122,124,126,128Te deduced levels, J, π, L. Enriched targets.
doi: 10.1016/0375-9474(76)90566-2
Z.Phys. A278, 241 (1976)
H.Spieler, H.J.Korner, K.E.Rehm, M.Richter, H.P.Rother
16,18O Induced Transfer Reactions on 122,120Sn
NUCLEAR REACTIONS 120Sn(18O, 16O), (18O, 20O), E=72 MeV; 122Sn(16O, 18O), E=74 MeV; measured σ(θ). 120Sn(18O, 12C), (18O, 13C), (18O, 14C), (18O, 15C), (18O, 16C), (18O, 15N), (18O, 16N), (18O, 17N), (18O, 18O), E=72 MeV; 122Sn(16O, 11B), (16O, 12C), (16O, 13C), (16O, 14C), (16O, 15C), (16O, 14N), (16O, 16O), E=74 MeV; measured σ. 120,122Sn levels deduced S.
Nucl.Phys. A266, 424 (1976)
W.F.Steele, P.A.Smith, J.E.Finck, G.M.Crawley
A Survey of the (3He, 7Be) Reaction at 70 MeV
NUCLEAR REACTIONS 12,13C, 16O, 24,26Mg, 40,42,44Ca, 58,60,62,64Ni, 90Zr, 120,124Sn, 144Sm, 206Pb(3He, 7Be), E=70 MeV; measured σ(θ); deduced S α. 60Fe, 120Cd deduced mass excess. 8,9Be, 12C, 20,22Ne, 36,38,40Ar, 54,56,58,60Fe, 86Sr, 116,120Cd deduced levels.
doi: 10.1016/0375-9474(76)90368-7
Nucl.Phys. A287, 280 (1977)
R.Bangert, B.Gonsior, M.Roth, B.Steinmetz, A.Stromich
The (p, n) Reaction between Analog States in Isotopes of Sn and Sb
NUCLEAR REACTIONS 115,116,117,118,119,120Sn(p, p), E ≈ 14.25-17.65 MeV; measured σ(Ep, θ); deduced optical model parameters. 115,116,117,118,119,120Sn(p, np), E ≈ 14.25-17.65 MeV; measured σ(Ep); deduced Q. 115,116,117,118,119,120Sb IAS deduced proton branching ratios, Coulomb displacement energies. Enriched targets, Lane-model nucleon-nucleus potential, DWBA analysis.
doi: 10.1016/0375-9474(77)90497-3
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
C.R.Acad.Sci., Ser.B 284, 65 (1977)
Y.Cauchois, H.ben Abdelaziz, Y.Heno, R.Kherouf, C.Schloesing-Moller
Determination des Vies Moyennes de Niveaux Nucleaires par Resonance de Fluorescence avec Rayonnement de Freinage
NUCLEAR REACTIONS 24Mg, 27Al, 48Ti, 59Co, 61Ni, 62Ni, 63,65Cu, 64,66,68Zn, 103Rh, 113,115In, 116,118,120Sn(γ, γ); measured resonance fluorescence. 24Mg, 27Al, 48Ti, 59Co, 61,62Ni, 63,65Cu, 64,66,68Zn, 103Rh, 113,115In, 116,118,120Sn levels deduced T1/2.
Phys.Rev.Lett. 39, 1451 (1977)
G.M.Crawley, W.Benenson, D.Weber, B.Zwieglinski
Observation of Hole States at High Excitation in (p, t) Reactions
NUCLEAR REACTIONS 106Cd, 104Pd, 116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ). 114,116,118,120,122Sn deduced enhancements, widths.
doi: 10.1103/PhysRevLett.39.1451
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
Nucl.Phys. A283, 45 (1977)
J.Genevey-Rivier, A.Charvet, G.Marguier, C.Richard-Serre, J.D'Auria, A.Huck, G.Klotz, A.Knipper, G.Walter
Level Structure of Light Even Xenon Nuclei Populated in the Decays of Isomeric and Ground States of 118,120,122Cs
RADIOACTIVITY 118m,118,120m,120,122m,122Cs [from La(p, 3pxn)]; measured T1/2, Eγ, Iγ, E(ce), I(ce), γγce-coin; deduced ICC. 118,120,122Xe deduced levels, J, π. On-line mass separated sources, Ge(Li), Si(Li).
doi: 10.1016/0375-9474(77)90698-4
At.Data Nucl.Data Tables 19, 175 (1977); 20, 1 (1977)
A.H.Wapstra, K.Bos
The 1977 Atomic Mass Evaluation (In Four Parts)
ATOMIC MASSES A > 0; compiled, evaluated atomic mass data, reaction Q-values for all nuclides.
RADIOACTIVITY A > 0; analyzed, compiled, evaluated Q, separation energies, systematics.
doi: 10.1016/0092-640X(77)90019-5
Nucl.Phys. A299, 381 (1978)
Z.Basrak, N.Cindro, M.Turk
The (t, α) Reaction on 121Sb and 123Sb
NUCLEAR REACTIONS 121,123Sb(t, α), E=12 MeV; measured σ(Eα, θ). 120,122Sn deduced levels, L(p), π, S. Enriched targets.
doi: 10.1016/0375-9474(78)90378-0
J.Phys.(London) G4, 1501 (1978)
H.C.Cheung, H.Huang, B.N.Subba Rao, L.Lessard, J.K.P.Lee
Decay of 120In
RADIOACTIVITY 120,120mIn [from 238U(p, F), separated isotope]; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 120Sn deduced levels, J, π.
doi: 10.1088/0305-4616/4/9/020
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.
Phys.Lett. 76B, 565 (1978)
C.Ekstrom, G.Wannberg, J.Heinemeier, The ISOLDE Collaboration
Nuclear Spin of a New Isomer in 119Cs and Magnetic Moment of 120Cs - Evidence for Strongly Deformed Nuclear Shapes of the Light Cesium Isotopes
NUCLEAR MOMENTS 119mCs; measured I. 120Cs; measured μ. ABMR.
doi: 10.1016/0370-2693(78)90855-9
J.Phys.Soc.Jpn. 45, 1076 (1978)
Y.Kawarasaki
Nuclear Resonant Scattering from the 6730-keV Level in 120Sn
NUCLEAR REACTIONS 120Sn(γ, γ'), E=6730 keV; measured resonance fluorescence, σ(Eγ', θ). 120Sn deduced levels, J, Γ. Natural target, Ge(Li) detector.
J.Phys.Soc.Jpn. 45, 1085 (1978)
Y.Kawarasaki
Photoexcitation of the 7310-keV Level in 120Sn and the 6517-keV Level In 117Sn
NUCLEAR REACTIONS 120Sn(γ, γ'), E=7310 keV; 117Sn(γ, γ'), E=6517 keV; measured resonant fluorescence, σ(Eγ', θ). 117,120Sn deduced levels, J, Γ. Natural target, Ge(Li) detector.
Nucl.Phys. A314, 80 (1979)
M.Adachi, T.Matsuzaki, H.Taketani
Low-Lying Levels in 120Sb Studied with the 120Sn(p, nγ) Reaction
NUCLEAR REACTIONS 120Sn(p, nγ), E=3.40-4.10 MeV; measured σ(E, Eγ, θγ), Eγ, Iγ, γγ-coin, γ(t), γ-linear plarization. 120Sb levels deduced J, π, γ-branching, T1/2, δ. Enriched target.
doi: 10.1016/0375-9474(79)90556-6
Nucl.Phys. A316, 40 (1979)
R.Chapman, M.Hyland, J.L.Durell, J.N.Mo, M.Macphail, H.Sharma, N.H.Merrill
Neutron Orbit Sizes in the Isotopes of Tin
NUCLEAR REACTIONS 112,114,116,117,118,119Sn(t, d), E=4.25-5.75 MeV; measured σ(θ). 113,115,117,118,119,120Sn levels deduced rms radii of neutron orbits, S. Enriched targets.
doi: 10.1016/0375-9474(79)90672-9
Nucl.Phys. A323, 205 (1979)
B.Fogelberg, P.Carle
Levels and Transition Probabilities in 120,122,124,126,128Sn Studied in the Decay of In Isotopes
RADIOACTIVITY 120,122,124,126,128In [from 235U(n, F)]; measured Eγ, Iγ, I(ce), γγ-coin, βγ(t), γγ(E); deduced levels, T1/2. 120,122,124,126,128Sn deduced levels, J, π. 122,124,126,128Sn deduced B(λ). Ge(Li), Si(Li), NaI, Ge(Li)-Ge(Li)-coin, plastic detectors.
doi: 10.1016/0375-9474(79)90108-8
Nucl.Phys. A325, 337 (1979)
J.Janecke, F.D.Becchetti, C.E.Thorn
Alpha-Cluster Pickup from Te and Sn Isotopes with the (d, 6Li) Reaction
NUCLEAR REACTIONS 122,124,126,128,130Te, 112,116,118,120,122,124Sn(d, 6Li), E=33 MeV; measured σ(E(6Li), θ). 118,120,122,124,126Sn, 108,112,114,116,118,120Cd deduced levels, J, π, S, α-reduced width. 124Sn(d, 6Li), E=33 MeV; measured Q. 120Cd deduced mass excess. DWBA analyses. Semi-microscopic analyses with shell model spectroscopic amplitudes.
doi: 10.1016/0375-9474(79)90021-6
Phys.Rev.Lett. 45, 982 (1980)
H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, M.B.Johnson, N.S.P.King, J.Piffaretti, E.R.Siciliano, J.Alster, A.Doron, S.Gilad, M.Moinester, P.R.Bevington, E.Winkelmann
Observation of Isobaric Analog States in Pion Single-Charge-Exchange Reactions
NUCLEAR REACTIONS 7Li, 13C, 27Al, 58Ni, 90Zr, 120Sn, 208Pb(π+, π0), E=98 MeV; measured σ(θ). 7Be, 13N, 27Si, 58Cu, 90Nb, 120Sb, 208Bi deduced IAS. Optical model.
doi: 10.1103/PhysRevLett.45.982
Phys.Rev. C22, 1832 (1980)
F.E.Bertrand, G.R.Satchler, D.J.Horen, J.R.Wu, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, A. van der Woude
Giant Multipole Resonances from Inelastic Scattering of 152-MeV Alpha Particles
NUCLEAR REACTIONS 208Pb, 120Sn, 90Zr, 58Ni, 46Ti(α, α), (α, α'), E=152 MeV; measured σ(Eα, θ). 46Ti, 58Ni, 90Zr, 120Sn, 208Pb deduced GQR, giant monopole resonances, Γ, L, T, β(L), B(λ), EWSR. Folding model analysis.
Phys.Rev. C22, 97 (1980)
M.Hass, C.Broude, Y.Niv, A.Zemel
Magnetic Moments of the 2+1 Levels in Even Sn Isotopes
NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(35Cl, 35Cl'), E=108 MeV; measured γ(θ, H), Coulomb excitation. 112,114,116,118,120,122,124Sn level deduced g. Shell model.
Proc.Int.Conf.on Nucl.Phys., Berkeley, p.751 (1980)
T.Katou, Y.Tendow, H.Kumagai, Y.Gono, A.Hashizume
Lifetimes of the Yrast States of 118,120Xe
NUCLEAR REACTIONS 107,109Ag(14N, 3n), E=60 MeV; measured Eγ, recoil. 118,120Xe deduced levels, T1/2, B(E2).
At.Data Nucl.Data Tables 25, 29 (1980)
K.S.Krane
E2, M1 Multipole Mixing Ratios, Supplement and Corrections through December 1979
COMPILATION A=28-223; compiled, evaluated data on γ(θ), Eγ; deduced consisent δ(E2/M1) values.
doi: 10.1016/0092-640X(80)90003-0
J.Phys.Soc.Jpn. 49, 444 (1980)
K.Miyano, Y.Kato
The 12.34-keV M1 Transition in 133mBa
RADIOACTIVITY 133mBa [from 133Cs(p, n)], 120Sb [from 120Sn(p, n)]; measured Eγ, Iγ, γγ(t), γ(X-ray)(t). 133Ba deduced ICC, M1 hindrance factor. 133Ba, 120Sn levels deduced T1/2.
Nucl.Phys. A351, 490 (1981)
A.Backlin, N.G.Jonsson, R.Julin, J.Kantele, M.Luontama, A.Passoja, T.Poikolainen
0+ States and E0 and E2 Transition Rates in Even Sn Nuclei
NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(16O, 16O'), E=48 MeV; measured Eγ, Iγ, γγ-coin, Coulomb excitation; 112,114,116,118,120,122,124Sn(p, p'γ), E not given; measured Iγ, Eγ, I(ce), γp'-, (ce)p'-coin, γp(t), (ce)p(t), Coulomb excitation; 124Sn(p, 2n), E not given; measured Eγ, Iγ, I(ce). 112,114,116,118,120,122,124Sn deduced levels, J, π, ICC, B(E0), B(E2), sign of matrix product.
RADIOACTIVITY 116,118,120Sb; measured Iγ, I(ce), γγ(θ); 116,118In; measured Iγ, I(ce), βγ-coin. 116,118Sn deduced levels, J, π, B(λ). Ge(Li), annular NaI detectors, magnetic spectrometers, enriched targets.
doi: 10.1016/0375-9474(81)90184-6
Phys.Lett. 103B, 326 (1981)
F.E.Bertrand, E.E.Gross, D.J.Horen, J.R.Wu, J.Tinsley, D.K.McDaniels, L.W.Swenson, R.Liljestrand
Excitation of Giant Resonance Modes in 90Zr and 120Sn by 200 MeV Protons
NUCLEAR REACTIONS 90Zr, 120Sn(p, p'), E=200 MeV; measured σ(Ep, θ). 90Zr deduced M1 transition strength. 90Zr, 120Sn deduced GDR, isoscalar GQR, giant octupole resonance, hexadecapole strength upper limit. Broad-range magnetic spectrograph.
doi: 10.1016/0370-2693(81)90235-5
J.Phys.(London) G7, 1539 (1981)
Y.Cauchois, H.Ben Abdelaziz, R.Kherouf, C.Schloesing-Moller
Etude de Niveaux Nucleaires d'Isotopes Naturels, par Resonance ou Fluorescence, avec Rayonnement X de Freinage
NUCLEAR REACTIONS 24Mg, 27Al, 48Ti, 58,61,62Ni, 63,65Cu, 64,66,68Zn, 75As, 103Rh, 59Co, 113,115In, 116,118,120Sn, 121,123Sb(γ, γ'), E ≈ 0.5-1.65 MeV bremsstrahlung; measured γ(θ), self absorption, absolute γ-transition strength. 24Mg, 27Al, 48Ti, 59Co, 58,61,62Ni, 63,65Cu, 64,66,68Zn, 75As, 103Rh, 113,115In, 116,118,120Sn, 121,123Sb levels deduced T1/2. Nuclear resonance fluorescence technique.
doi: 10.1088/0305-4616/7/11/013
Phys.Rev. C23, 589 (1981)
G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski
Hole States in the Tin Isotopes Observed by the (p, t) Reaction
NUCLEAR REACTIONS 112,116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ); 117,119Sn(p, d), E=42 MeV; measured σ(Ed). 110,114,116,118,120,122Sn deduced broad resonances, Γ. DWBA analysis. Enriched targets.
Nucl.Phys. A371, 333 (1981)
N.-G.Jonsson, A.Backlin, J.Kantele, R.Julin, M.Luontama, A.Passoja
Collective States in Even Sn Nuclei
NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(16O, 16O'γ), E=48 MeV; measured Eγ, Iγ, γγ-coin. 112,114,116,118,120,122,124Sn(p, p'γ), E=6-8 MeV; measured Eγ, Iγ. 112,114,116,118,120,122,124Sn deduced B(E2), B(E3), B(E1). Ge(Li), NaI detectors. Enriched targets.
RADIOACTIVITY 116Sb; measured Iγ. 116Sn deduced B(E2) ratio.
doi: 10.1016/0375-9474(81)90071-3
Phys.Rev. C24, 954 (1981)
N.K.B.Shu, R.Levy, N.Tsoupas, A.Lopez-Garcia, W.Andrejtscheff, N.Benczer-Koller
Magnetic Moments of the 21+ States of Even-Even Te Isotopes
NUCLEAR REACTIONS 120,122,124,126,128,130Te(32S, 32S'), E ≈ 80 MeV; measured γ(θ, H), Coulomb excitation, 32Sγ(θ). 120,122,124,126,128,130Te level deduced g. Enriched, triple layered targets, recoil in polarized Fe, NaI(Tl) detector.
Phys.Rev. C23, 937 (1981); Erratum Phys.Rev. C23, 2798 (1981)
T.Yamagata, S.Kishimoto, K.Yuasa, K.Iwamoto, B.Saeki, M.Tanaka, T.Fukuda, I.Miura, M.Inoue, H.Ogata
High Energy Component of Giant Octupole Resonance in Medium and Heavy Mass Nuclei
NUCLEAR REACTIONS 90,92Zr, 116,118,120Sn, 144Sm, 208Pb(3He, 3He'), E=110-140 MeV; measured σ(θ, E). 90,92Zr, 116,118,120Sn, 144Sm, 208Pb deduced giant octupole resonance, deformation β3, EWSR. Enriched target. DWBA analysis.
Phys.Rev. C26, 1157 (1982)
K.Aleklett, P.Hoff, E.Lund, G.Rudstam
Total β-Decay Energies and Mass Systematics of Neutron-Rich Silver and Cadmium Isotopes
RADIOACTIVITY 116,117,118,119,120,121Ag [from fission product mass separation]; 119,121Cd [from 119,121Ag(β-) decay]; measured βγ-coin; deduced Qβ, maximum Eβ, mass excess. Fission product mass separation, Ge(Li), Si-Li detectors.
Phys.Rev. C25, 813 (1982)
P.Chowdhury, W.F.Piel, Jr., D.B.Fossan
Collective Properties of 1g9/2 Proton-Hole Excitations: High-spin states in 116,118,120,122Te and 120Xe nuclei
NUCLEAR REACTIONS 117Sn(α, n), E=16, 18, 20 MeV; 119Sn(α, n), E=18 MeV; 114Sn(α, 2n), E=22, 24 MeV; 116Sn(α, 2n), E=22 MeV; 106Pd(12C, 2n), E=58 MeV; 110Pd(13C, 3n), E=40, 45, 49, 52 MeV; 110Cd(13C, 3n), E=52 MeV; measured γγ-coin, γ(θ), σ(Eγ). 116,118,120,122Te, 120Xe deduced levels, J, π. Enriched targets, Ge(Li) detectors.
Nucl.Phys. A388, 1 (1982)
C.Djalali, N.Marty, M.Morlet, A.Willis, J.C.Jourdain, N.Anantaraman, G.M.Crawley, A.Galonsky, P.Kitching
Systematics of the Excitation of M1 Resonances in Medium Heavy Nuclei by 200 MeV Proton Inelastic Scattering
NUCLEAR REACTIONS 51V, 58,60,62Ni, 68Zn, 90,92,94,96Zr, 92,94,96,98,100Mo, 120,124Sn, 140Ce(p, p'), E=200 MeV; measured σ(θ). 51V, 58,60,62Ni, 68Zn, 90,92,94,96Zr, 92,94,96,98,100Mo, 120,124Sn, 140Ce deduced resonances, Γ, T, M1 character.
doi: 10.1016/0375-9474(82)90505-X
Z.Phys. A308, 165 (1982)
R.A.Emigh, C.A.Fields, M.L.Gartner, L.E.Samuelson, P.A.Smith
A Study of the 121,123Sb(p, d) Reactions
NUCLEAR REACTIONS 121,123Sb(p, d), E=26.2 MeV; measured σ(Ed, θ). 120,122Sb deduced levels, L, J, π, C2S. Enriched targets, magnetic spectrometer. DWBA analysis.
Z.Phys. A308, 173 (1982)
R.A.Emigh, C.A.Fields, M.L.Gartner, L.E.Samuelson, P.A.Smith
A Study of the 120Sn(p, nγ)120Sb Reaction
NUCLEAR REACTIONS 120Sn(p, nγ), E=3.9-6.25 MeV; measured Eγ, Iγ(θ), γγ-coin. 120Sb deduced levels, J, π. Enriched targets, Ge(Li), hyperpure Ge detectors.
Nucl.Phys. A380, 125 (1982)
J.J.Van Ruyven, W.H.A.Hesselink, J.Akkermans, P.Van Nes, H.Verheul
Band Structures in 118,120Te
NUCLEAR REACTIONS 116,118Sn(α, 2n), E=22-33 MeV; measured Eγ, Iγ, γγ(θ), σ(Eγ, θ), I(ce), linear polarization. 118,120Te deduced levels, J, π, γ-branching, δ. Enriched targets, Ge(Li), Si-Li detectors. Interacting boson approximation, broken pair model.
doi: 10.1016/0375-9474(82)90586-3
Phys.Rev. C28, 280 (1983)
N.Auerbach, J.D.Bowman, M.A.Franey, W.G.Love
(p, n) and (n, p) Reactions as Probes of Isovector Giant Monopole Resonances
NUCLEAR REACTIONS 90Zr, 40Ca, 120Sn, 208Pb(p, n), E=120, 800 MeV; calculated σ(θ) for isovector giant monopole resonance excitation. DWIA, RPA based charge exchange transition densities.
Phys.Rev. C28, 1475 (1983)
M.Blann, H.K.Vonach
Global Test of Modified Precompound Decay Models
NUCLEAR REACTIONS, ICPND 202Hg(p, 2p), (p, n2p), E=30-90 MeV; calculated σ(E). 27Al, 58Ni, 90Zr, 120Sn, 208Pb(p, X), E ≈ 10-100 MeV; 208Pb, 27Al(n, X), E ≈ 0.3-100 MeV; Ni(n, X), E ≈ 1-15 MeV; Sn(n, X), E ≈ 0.5-30 MeV; calculated reaction σ(E). 52Cr, 56Fe, 93Nb(n, xn), E=14.5 MeV; calculated σ vs En. 52Cr, 56Fe, 93Nb(n, p), E=14.7 MeV; calculated σ(Ep). 51V(p, n), E=18-26 MeV; 107,109Ag, 108,110Pd(p, n), E=18, 22, 25 MeV; 208Pb(p, n), E=35, 45 MeV; 120Sn, 48Ca(p, n), E=25, 35, 45 MeV; 27Al, 58Ni, 90Zr, 209Bi(p, n), E=90 MeV; calculated σ(En). 90Zr, 209Bi, 27Al, 58Ni(p, p'), E=90 MeV; 54Fe, 209Bi(p, p'), E=39, 62 MeV; calculated σ(Ep'); deduced best-fit model, parameter set. Hybrid, geometry dependent hybrid precompound decay models.
Z.Phys. A310, 43 (1983)
E.Gadioli, E.Gadioli Erba, R.Gaggini, P.Guazzoni, P.Michelato, A.Moroni, L.Zetta
Evidence of the Spectator Role of Unpaired Nucleons of the Target Nucleus in (p, α) Reactions
NUCLEAR REACTIONS 90,91Zr, 122Sn, 123Sb, 142,143,144Nd, 208Pb, 209Bi(p, α), E ≈ 24 MeV; measured σ(θα, Eα); deduced reaction mechanism, structure effects.
Phys.Rev. C27, 3002 (1983)
P.L.Reeder, R.A.Warner, R.L.Gill
Half-Lives and Emission Probabilities of Delayed Neutron Precursors 121-124Ag
NUCLEAR REACTIONS 235U(n, F), E not given; measured β-delayed En, In, β-spectra; deduced evidence for 124Ag, 123Cd.
RADIOACTIVITY 120,121,122,123,124Ag(β-n) [from 235U(n, F)]; measured T1/2, β-delayed En, In, β-delayed neutron emission probabilities. 122,123,124Cd(β-) [from 235U(n, F)]; measured β-decay; deduced T1/2. On-line separation.
Phys.Rev. C28, 1527 (1983)
K.Sato, A.Iwamoto, K.Harada
Pre-Equilibrium Emission of Light Composite Particles in the Framework of the Exciton Model
NUCLEAR REACTIONS 89Y, 120Sn, 197Au, 54Fe(p, p), (p, d), (p, t), (p, 3He), (p, α), E=62 MeV; 58Ni(p, t), (p, α), (p, 3He), E=90 MeV; calculated σ(Ep), σ(Ed), σ(Et), σ(E(3He)), σ(Eα); deduced composite particle emission mechanism. Exciton model.
Phys.Rev. C27, 2995 (1983)
S.Vajda, W.F.Piel, Jr., M.A.Quader, W.A.Watson III, F.C.Yang, D.B.Fossan
Proton-Hole Induced Bands in Odd-Odd 118,120Sb
NUCLEAR REACTIONS 114,116Cd(7Li, 3n), E=29 MeV; 110Pd(11B, 3n), E=51 MeV; measured γγ(t). 118,120Sb deduced levels, J, π, T1/2, γ-multipolarity, band structure, configuration, isomer.
J.Nucl.Mater. 122/123, 972 (1984)
K.Abe, A.Iizuka, A.Hasegawa, S.Morozumi
Induced Radioactivity of Component Materials by 16-MeV Protons and 30-MeV Alpha Particles
NUCLEAR REACTIONS, ICPND 45Sc, 59Co, 58Ni, 65Cu, 66Zn, 91Zr, 93Nb, 181Ta, 197Au(p, np), 46,47Ti(p, α), 48Ti, 51V, 52Cr, 56Fe, 61Ni, 65Cu, 67Zn, 72,74,76Ge, 89Y, 90,92,96Zr, 93Nb, 94,95,96Mo, 107Ag, 116,117,118,120,122Sn, 181Ta, 182W, 194,196Pt, 197Au(p, n), 49Ti, 53Cr, 57Fe, 62Ni, 63Cu, 68Zn, 73Ge, 94,95,96,97,100Mo, 117,119Sn, 182W, 194,195Pt(p, 2n), E=16 MeV; 45Sc, 46,48Ti, 51V, 54Fe, 63Cu, 70Ge, 89Y, 90,96Zr, 93Nb, 92,94,100Mo, 103Rh, 107Ag, 181Ta, 182W, 194Pt(α, n), 45Sc(α, nα), 45Sc, 59Co(α, 2p), 46Ti, 50,52,54Cr, 54,56Fe, 70Ge, 92Mo(α, np), 46,49Ti, 50Cr, 59Co, 65Cu, 91Zr, 93Nb, 103Rh, 107,109Ag, 181Ta, 183W(α, 2n), 51V, 56Fe, 182W(α, 3n), 186W(α, 2np), E=30 MeV; measured residuals thick target yields. Activation technique.
J.Phys.(London) G10, 331 (1984)
K.Amos, I.Morrison, R.Smith
Interacting Boson-Fermion Models and Transition Densities
NUCLEAR REACTIONS 20Ne(p, p'), E=24.5 MeV; 112,114,116,118,120,122,124Sn(n, n'), E=24 MeV; calculated σ(θ). 20Ne(e, e'), E not given; calculated form factor. Interacting boson model spectroscopic amplitudes, B(E2) matching.
NUCLEAR STRUCTURE 20Ne, 112,114,116,118,120,122,124Sn; calculated BCS level occupancies, spectroscopic amplitudes. Interacting boson approximation.
doi: 10.1088/0305-4616/10/3/009
Bull.Am.Phys.Soc. 29, No.7, 1041, CC3 (1984)
A.Aprahamian, D.S.Brenner, D.M.Rehfield, J.Van Dyk, R.F.Casten, R.L.Gill, H.Mach, A.Piotrowski
Coexistence in the Cadmium Isotopes
RADIOACTIVITY 120Ag(β-); measured γγ(θ). 120Cd deduced levels, J, π.
Nucl.Instrum.Methods 219, 123 (1984)
Y.Iwata, M.Yasuhara, K.Maeda, Y.Yoshizawa
Precision Measurements of Gamma-Ray Intensities VI. 120Sb, 124Sb and 125Sb
RADIOACTIVITY 120Sb(EC) [from 120Sn(p, n)]; 124,125Sb(β-) [from neutron irradiation of Sb]; 152Eu(EC), (β+), (β-); 154Eu, 192Ir(EC), (β-); measured Eγ, Iγ, βγ-, (X-ray)γ-coin; deduced Iγ per decay. 192Os, 192Pt, 154,152Gd, 120Sn, 124,125Te levels deduced γ-branching.
doi: 10.1016/0167-5087(84)90143-1
Z.Phys. A316, 249 (1984)
J.M.Nitschke, P.A.Wilmarth, P.K.Lemmertz, W.-D.Zeitz, J.A.Honkanen
Beta-Delayed Proton Emission Observed in New Lanthanide Isotopes
RADIOACTIVITY 143,141Dy(β+p) [from 92Mo(56Fe, αn), (54Fe, αn), E=275, 274 MeV]; 141Gd(β+p) [from 92Mo(54Fe, n4p), E=274 MeV]; 123Ce(β+p) [from 92Mo(36Ar, nα), E=196 MeV]; 122La(β+p) [from 92Mo(36Ar, npα), E=205 MeV]; 120La(β+p) [from 58Ni(64Zn, np), E=253 MeV]; measured β-delayed Ep, Ip, γp-, X-ray p-coin; deduced T1/2.
Phys.Rev. C30, 1772 (1984)
M.A.Quader, W.F.Piel, Jr., S.Vajda, W.A.Watson III, F.C.Yang, D.B.Fossan
Proton-Hole-Induced Bands in Odd-Odd 116,118,120,122I Nuclides
NUCLEAR REACTIONS 106Cd(12C, np), E=58, 63 MeV; 112,114,116Cd(10B, 4n), E=51, 54 MeV; 114,116,118Sn(7Li, 3n), E=34 MeV; measured γγ-coin, γ(θ), σ(Eγ, E), γγ(θ). 116,118,120,122I deduced levels, J, π, band structure, configuration.
Thesis, State Univ of New York at Stony Brook (1984)
M.A.Quader
Collective Properties of Odd-dd Nuclei in Z Greater than 50 Transition Region
Phys.Rev. C29, 1710 (1984)
C.Wong, S.M.Grimes, R.W.Finlay
Analysis of (p, p), (p, n), and (n, n) Scattering on the Even Tin Isotopes using the Lane Coupled Equations
NUCLEAR REACTIONS 116,118,122,124Sn(p, n), E=24.5 MeV; measured σ(θ), σ(En); deduced isocalar, isovector strengths of potential. 116,120,124Sn(n, n), E=11 MeV; analyzed σ(θ); deduced potential parameters. Lane model, imaginary potential Coulomb correction.
Bull.Am.Phys.Soc. 30, No.4, 742, DE9 (1985)
A.Chaudhury, M.W.Drigert, E.G.Funk, J.W.Mihelich, U.Garg
RDM Measurements in 119-120Xe and 119I
NUCLEAR REACTIONS 104Pd(19F, 3np), (19F, 2np), (19F, 2n2p), E=81 MeV; measured recoil, Eγ, Iγ. 119,120Xe, 119I levels deduced T1/2.
Nucl.Phys. A436, 221 (1985)
K.Miura, Y.Hiratate, T.Shoji, T.Suehiro, H.Yamaguchi, Y.Ishizaki
Ground-State Transition Strengths of the (p, t) Reactions for Nuclei with A=23-238
NUCLEAR REACTIONS 23Na, 24,26Mg, 27Al, 28,30Si, 35,37Cl, 40,44Ca, 46,48,50Ti, 51V, 54,56Fe, 58,60,62Ni, 63,65Cu, 64,66,68Zn, 76,78,80,82Se, 90,92,94,96Zr, 92,96,98,100Mo, 102,104Ru, 104,106,108,110Pd, 112,114,116Cd, 115In, 118,120,122,124Sn, 122,124,126,128,130Te, 136,138Ba, 140,142Ce, 144,146,148,150Nd, 158,160Gd, 165Ho, 168,170Er, 172,174,176Yb, 181Ta, 184,186W, 188,190,192Os, 191,193Ir, 194,196,198Pt, 197Au, 202,204Hg, 208Pb, 209Bi, 232Th, 238U(p, t), E=51.9 MeV, measured σ(θ). 21Na, 22,24Mg, 25Al, 26,28Si, 33,35Cl, 38,42Ca, 44,46,48Ti, 49V, 52,54Fe, 56,58,60Ni, 61,63Cu, 62,64,66Zn, 74,76,78,80Se, 88,90,92,94Zr, 90,94,96,98Mo, 100,102Ru, 102,104,106,108Pd, 110,112,114Cd, 113In, 116,118,120,122Sn, 120,122,124,126,128Te, 134,136Ba, 138,140Ce, 142,144,146,148Nd, 156,158Gd, 163Ho, 166,168Er, 170,172,174Yb, 179Ta, 182,184W, 186,188,190Os, 189,191Ir, 192,194,196Pt, 195Au, 200,202Hg, 206Pb, 207Bi, 230Th, 236U deduced systematic g.s. transition strength. Natural, enriched targets.
doi: 10.1016/0375-9474(85)90197-6
Phys.Rev.Lett. 55, 681 (1985)
J.W.Norbury, F.A.Cucinotta, P.A.Deutchman, L.W.Townsend
Theoretical Spectral Distributions and Total Cross Sections for Neutral Subthreshold Pion Production in Carbon-Carbon Collisions
NUCLEAR REACTIONS 12C(12C, π0), E=20-100 MeV/nucleon; calculated pion production σ(E), spectral distribution. Particle-hole theory, coherent isobar formation, decay.
doi: 10.1103/PhysRevLett.55.681
Diss.Abst.Int. 46B, 1218 (1985)
M.A.Quader
Collective Properties of Odd-Odd Nuclei in Z > 50 Transition Region
NUCLEAR REACTIONS 106Cd(12C, npα), 103Rh(12C, 3n), 110Pd(11B, 3n), 114,116Cd(7Li, 3n), 106Cd(12C, np), 112,114,116Cd(10B, 4n), 114,116,118Sn(7Li, 3n), 112Sn(12C, 3np), 109Ag(18O, 5n), 103Rh(27Al, 3np), 112Sn(16O, 2np), 116Sn(14N, 2n), 139La(7Li, nα), (7Li, 3n), 130Te(18O, 5n), E not given; measured σ(Eγ, E), γ(θ), γγ(t). 112,118,120Sb, 116,118,120,122I, 120,122Cs, 126,128La deduced levels, J, π, δ, configurations.
Diss.Abst.Int. 46B, 1219 (1985)
J.L.Thornton
Simultaneous Measurement of Nuclear Magnetic Moments by the Transient Field Method
NUCLEAR STRUCTURE 102,104,106,108,110Pd, 120,122,124,126,128Te; measured not abstracted; deduced g.
Diss.Abst.Int. 46B, 561 (1985)
J.R.Tinsley
A Survey of Giant Resonance Excitations with 200 MeV Protons
NUCLEAR REACTIONS 60Ni, 90Zr, 120Sn, 208Pb(p, p'), E=200 MeV; measured σ(θ). 60Ni, 90Zr, 120Sn, 208Pb deduced giant multipole resonances.
Nucl.Phys. A460, 361 (1986)
K.Loewenich, K.O.Zell, A.Dewald, W.Gast, A.Gelberg, W.Lieberz, P.von Brentano, P.Van Isacker
In-Beam Spectroscopy of 120Xe
NUCLEAR REACTIONS 110Cd(13C, 3n), 111Cd(12C, 3n), E=46-58 MeV; measured Eγ, Iγ, γ(θ), σ(E, Eγ, θ), γγ-coin. 120Xe deduced levels, J, π, B(E2) ratios. IBA calculations. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(86)90132-6
Phys.Rev. C33, 1109 (1986)
M.A.Quader, C.W.Beausang, P.Chowdhury, U.Garg, D.B.Fossan
Band Structure Change in Z > 50 Region: Doubly odd 120,122Cs and 126,128La
NUCLEAR REACTIONS 112Sn(12C, 3np), E=86 MeV; 109Ag(18O, 5n), E=96 MeV; 112Sn(16O, np), E=72 MeV; 103Rh(27Al, 3np), E=137 MeV; 116Sn(14N, 2n), E=60 MeV; measured σ(Eγ), γγ(t), γ(θ). 120,122Cs, 126,128La deduced levels, J, π, γ-branching, band structure, configuration, δ.
Nucl.Phys. A467, 528 (1987)
S.Harissopulos, A.Dewald, A.Gelberg, P.von Brentano, K.Loewenich, K.Schiffer, K.O.Zell
Lifetime Measurements in 120Xe, using a Coincidence Plunger Technique
NUCLEAR REACTIONS 110Cd(13C, 3n), E=56 MeV; measured recoil-distance Doppler shift, γγ-coin. 120Xe levels deduced T1/2, side feeding times, B(E2) ratios. Enriched target, Ge detectors.
doi: 10.1016/0375-9474(87)90543-4
Nucl.Data Sheets 52, 641 (1987)
A.Hashizume, Y.Tendow, M.Ohshima
Nuclear Data Sheets for A = 120
COMPILATION 120Ag, 120Cd, 120In, 120Sn, 120Sb, 120Te, 120I, 120Xe, 120Cs, 120Ba, 120La; compiled, evaluated structure data.
Z.Phys. A328, 487 (1987)
S.Lunardi, P.J.Daly, F.Soramel, C.Signorini, B.Fornal, G.Fortuna, A.M.Stefanini, R.Broda, W.Meczynski, J.Blomqvist
Decay of (νh11/2(n))(+10)+ and (πd5/2νh11/2(n))(25/2)+ Isomers in Even-A Sn and Odd-A Sb Nuclei
NUCLEAR REACTIONS 116Cd(7Li, X), E=26-40 MeV; measured Eγ, Iγ. 120Sn deduced isomer T1/2, configuration, B(E2), decay characteristics. 116,118Sn, 119,120Sb deduced isomer decay characteristics, configuration.
Z.Phys. A328, 493 (1987)
M.S.Rouabah, Th.Byrski, F.A.Beck, D.Curien, B.Haas, J.C.Merdinger, J.P.Vivien, J.Gizon, B.Nyako
High Spin Bands in 120Xe
NUCLEAR REACTIONS 106Cd(18O, 4n), E=90 MeV; measured Eγ, Iγ, γ yield vs E, γγ-coin. 120Xe deduced levels, J, π, γ-branching, band structure.
J.Phys.(London) G13, L195 (1987)
P.M.Walker, C.J.Ashworth, I.S.Grant, V.R.Green, J.Rikovska, T.L.Shaw, N.J.Stone
E0 Transitions in the Light Tellurium Isotopes: Evidence for intruder states
RADIOACTIVITY 118,120,122I(β+), (EC) [from 93Nb(32S, X), (34S, X), E=160-175 MeV]; measured I(ce), γγ-coin, γ linear polarization. 118,120,122Te deduced levels, J, π, γ-branching, ICC, transition strength ratios.
doi: 10.1088/0305-4616/13/9/005
Hyperfine Interactions 43, 353 (1988)
D.E.Brown, L.Goettig, I.S.Grant, V.R.Green, K.S.Krane, J.Rikovska, T.L.Shaw, N.J.Stone, P.M.Walker
On-Line Nuclear Orientation of Odd - Odd 120I
RADIOACTIVITY 120I(β+) [from 93Nb(32S, X), (34S, X)]; measured γγ-, (ce)γ-coin, γ(θ), oriented nuclei. 120Te deduced levels, J, π, δ(M1/E2).
Phys.Rev. C38, 2514 (1988)
M.Buenerd, K.Bouhelal, Ph.Martin, J.Chauvin, D.Lebrun, G.Perrin, P.de Saintignon, G.Duhamel
Quadrupole Transitions at Very Small Momentum Transfer in Nuclei
NUCLEAR REACTIONS 58Ni, 92Mo, 120,124Sn, 140Ce, 208Pb(3He, 3He'), E=108.5 MeV; measured σ(θ). 58Ni, 92Mo, 120,124Sn, 140Ce, 208Pb deduced giant resonances excitation, deformation parameters, B(λ).
Phys.Rev. C37, 1203 (1988)
S.Raman, T.A.Walkiewicz, L.G.Multhauf, K.G.Tirsell, G.Bonsignori, K.Allaart
Decays of 118In, 120In, and 122In Isomers to Levels in 118Sn, 120Sn, and 122Sn
RADIOACTIVITY 118,120,122In(β-) [from 118,120,122Sn(n, p), E=14 MeV]; measured Eγ, Iγ. 118,120,122Sn deduced levels, γ transitions. Broken pair model.
NUCLEAR STRUCTURE 118,120,122Sn; calculated levels. Broken pair model.
Phys.Rev. C38, 2562 (1988)
M.M.Sharma, W.T.A.Borghols, S.Brandenburg, S.Crona, A.van der Woude, M.N.Harakeh
Giant Monopole Resonance in Sn and Sm Nuclei and the Compressibility of Nuclear Matter
NUCLEAR REACTIONS 112,114,116,120,124Sn, 144,148,150,152Sm(α, α'), E=120 MeV; measured σ(E, θ); deduced compressibility of nuclear matter. 112,114,116,120,124Sn, 144,148,150,152Sm deduced GQR, GMR, Γ, sum rule strength. DWBA analysis.
Hyperfine Interactions 43, 343 (1988)
W.B.Walters, J.Rikovska, N.J.Stone, T.L.Shaw, P.Walker, I.S.Grant
E0 Transitions in the Mid-Shell Even-Even Xe Nuclides: Decay of 31-s 124Cs to levels of 124Xe
RADIOACTIVITY 124Cs(EC), (β+) [from 92Mo(32S, X)]; measured E(γ), I(γ), I(ce), γγ-, γ(ce)-, (ce)(ce)-coin. 124Xe deduced levels, ICC, γ-multipolarity, B(E0)/B(E2).
Phys.Rev.Lett. 63, 143 (1989)
H.Mach, M.Moszynski, R.F.Casten, R.L.Gill, D.S.Brenner, J.A.Winger, W.Krips, C.Wesselborg, M.Buscher, F.K.Wohn, A.Aprahamian, D.Alburger, A.Gelberg, A.Piotrowski
Picosecond Lifetime Measurements in 116,118,120Cd and the Structure of Normal and Intruder States
RADIOACTIVITY 116,118,120Ag(β-); measured βγγ-coin. 116,118,120Cd deduced levels, J, π, T1/2, B(λ).
doi: 10.1103/PhysRevLett.63.143
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
Aust.J.Phys. 42, 41 (1989)
R.H.Spear, A.M.Baxter, S.M.Burnett, C.L.Miller
Measurement of Reduced Electric Octupole Transition Probabilities, B(E3;01+ → 31-), for 118,120,122Sn
NUCLEAR REACTIONS 118,120,122Sn(12C, 12C'), E=37, 38 MeV; measured projectile spectra following Coulomb excitation. 118,120,122Sn levels deduced B(λ). Shell model comparison.
Thesis, Oxford Univ. (1990)
D.E.Brown
Low Temperature Nuclear Orientation Studies of Nuclei Far from Stability
Proc.Int.Conf. on Spectroscopy of Heavy Nuclei, 1989, Crete, Greece, p.307 (1990)
J.L.Durell
Fission Fragment Spectroscopy
NUCLEAR STRUCTURE 98,100,102Zr, 100,102,104,106,108Mo, 104,106,108,110,112Ru, 108,110,112,114,116Pd, 114,116,118,120,122Cd, 146,148Nd, 150Sm, 144,146Ce, 142,144,146Ba; analyzed data; deduced levels. Nuclei produced in 252Cf(SF) and (HI, xn) reactions.
Thesis, Univ.Maryland (1990)
P.F.Mantica, Jr.
Shape Coexistence in Xenon and Tellurium: Nuclear structure studies on levels in 119,121Te and 120,126,127,136Xe
RADIOACTIVITY 136I(β-); 119,121I, 120,126,127,129Cs(β+), (EC); measured Eγ, Iγ, I(ce), γγ-, γ(ce)-coin; deduced log ft. 119,121Te, 120,126,127,136Xe deduced levels, J, π, ICC, β-feeding intensities. 120Xe deduced deformation features.
Z.Phys. A338, 461 (1991)
B.Cederwall, A.Johnson, R.Wyss, F.Liden, B.Fant, S.Juutinen, P.Ahonen, S.Mitarai, J.Mukai, J.Nyberg
High Spin States of 120Ba
NUCLEAR REACTIONS 92Mo(32S, 2n2p), E=145 MeV; measured γ-spectra. 120Ba deduced levels, J, π, band structure. NORDBALL detector system. Total Routhian Surface calculations.
Yad.Fiz. 54, 330 (1991); Sov.J.Nucl.Phys. 54, 196 (1991)
L.I.Govor, A.M.Demidov, O.K.Zhuravlev, I.V.Mikhailov, E.Yu.Shkuratova
Lifetime Measurements for Excited 116-124Sn States in the (n, n'γ) Reaction
NUCLEAR REACTIONS 116,118,122,124,120Sn(n, n'γ), E=fast; measured γ-spectra, DSA. 116,118,120,122,124Sn levels deduced T1/2.
J.Phys.(London) G18, 977 (1992)
A.Bhagwat, S.S.Al-Ghamdi, P.M.Walker, B.D.D.Singleton, C.G.Barham, I.S.Grant
Lifetime Measurements of Intruder States in 120Xe and the Shape Coexistence Picture
RADIOACTIVITY 120,120mCs(β+), (EC) [from 93Nb(32S, xnyp), E=165 MeV]; measured I(ce), (β)(ce)-coin, centroid shifts. 120Xe deduced levels, γ-multipolarity, K-electron branching ratio, T1/2, B(λ).
doi: 10.1088/0954-3899/18/5/025
Nucl.Phys. A542, 454 (1992)
B.Cederwall, F.Liden, A.Johnson, L.Hildingsson, R.Wyss, B.Fant, S.Juutinen, P.Ahonen, S.Mitarai, J.Mukai, J.Nyberg, I.Ragnarsson, P.B.Semmes
Signature Inversion in 120Cs: Evidence for a residual pn interaction
NUCLEAR REACTIONS 92Mo(32S, n3p), E=145 MeV; measured Eγ, Iγ, σ(Eγ, θ), (particle)γγ-coin. 120Cs deduced levels, J, π, routhians, aligned angular momenta. Enriched targets, array of Compton suppressed hyperpure Ge detectors, array of neutron detectors, 4π array of Si charged particle detectors. Total routhian surface, two-particle plus triaxial rotor calculations.
doi: 10.1016/0375-9474(92)90106-T
Yad.Fiz. 55, 865 (1992); Sov.J.Nucl.Phys. 55, 481 (1992)
A.M.Demidov, I.V.Mikhailov
Study of γ Transitions of 120Sn in the (n, n'γ) Reaction
NUCLEAR REACTIONS 120Sn(n, n'γ), E=fast; measured Eγ, Iγ, γ(θ), linear polarization. 120Sn deduced levels, J, π, δ.
Z.Phys. A344, 233 (1992)
J.Goswamy, A.Sharma, D.Mehta, B.Chand, N.Singh, P.N.Trehan, P.Singh, R.G.Pillay, H.G.Devare, R.K.Bhowmik, C.R.Praharaj
High Spin States in 120Xe
NUCLEAR REACTIONS 107Ag(16O, 2np), E=80 MeV; 108Pd(16O, 4n), E=84 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 120Xe deduced levels, J, π, band structure. Cranked shell model.
Phys.Rev. C46, 510 (1992); Erratum Phys.Rev. C46, 2644 (1992)
S.-W.Xu, J.-S.Guo, S.-G.Yuan, M.-Q.Liu, E.Hagberg, V.T.Koslowsky, J.C.Hardy, G.Dyck, H.Schmeing
Decay of 120Ba
RADIOACTIVITY 120Ba(β+), (EC) [from 106Cd(16O, 2n), E=78 MeV]; measured Eγ, Iγ, βγ(t), γγ(t), γ(X-ray)-coin, β-endpoint energy; deduced T1/2, Q(EC), log ft. 120Cs deduced levels, J, π.
Nucl.Phys. A552, 340 (1993)
Z.Janas, J.Aysto, K.Eskola, P.P.Jauho, A.Jokinen, J.Kownacki, M.Leino, J.M.Parmonen, H.Penttila, J.Szerypo, J.Zylicz
Gamow-Teller Decay of 118Pd and of the New Isotope 120Pd
RADIOACTIVITY 118,120Pd(β-) [from 238U(p, F), E=20 MeV, on-line mass separation]; measured β-decay T1/2, Iγ, I(ce), K X-rays, γγ-, β-γ-, (X-ray)γ-coin; deduced log ft. 118,120Ag deduced levels, ICC, γ-multipolarity, J, π, beta strength. Plastic, Ge detectors, Si(Li)+magnetic electron transporter. Deformed shell-model calculations with pairing.
doi: 10.1016/0375-9474(93)90497-L
Nucl.Phys. A553, 531c (1993)
S.Juutinen, S.Tormanen, P.Ahonen, B.Cederwall, B.Fant, A.Johnson, R.Julin, S.Mitarai, J.Mukai, J.Nyberg, M.Piiparinen, A.Virtanen, R.Wyss
Competing Proton and Neutron Alignments in 117-120Xe
NUCLEAR REACTIONS 92Mo(32S, X), E=145 MeV; measured γ-spectra. 106Pd(18O, 4n), E=75 MeV; measured total Eγ, γ-multiplicity, γγ-coin. 117,118,120Xe deduced levels, J, π, configuration.
doi: 10.1016/0375-9474(93)90654-G
Phys.Rev. C47, 1219 (1993)
M.A.Kagarlis, H.T.Fortune, P.Hui, S.Loe, D.A.Smith, A.L.Williams, J.Urbina
Double Charge Exchange in 93Nb(π+, π-)93Tc at T(π) = 164, 230, and 294 MeV
NUCLEAR REACTIONS 93Nb(π+, π-), E=164-294 MeV; measured spectra, σ(θ). 93Tc deduced levels, double IAS excitation.
Nucl.Phys. A560, 733 (1993)
R.Liguori Neto, P.Roussel-Chomaz, L.Rochais, N.Alamanos, F.Auger, B.Fernandez, J.Gastebois, A.Gillibert, R.Lacey, A.Miczaika, D.Pierroutsakou, J.Barrette, S.K.Mark, R.Turcotte, Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Roynette, J.A.Scarpaci, T.Suomijarvi, A.Van der Woude, A.M.Van den Berg
Excitation of Giant Resonances in 208Pb, 120Sn, 90Zr and 60Ni by 84 MeV/nucleon 17O Ions
NUCLEAR REACTIONS 60Ni, 90Zr, 120Sn, 208Pb(17O, 17O), (17O, 17O'), E=1435 MeV; measured σ(θ); deduced model parameters. 60Ni, 90Zr, 120Sn, 208Pb levels deduced B(λ), giant monopole, quadrupole reasonances.
doi: 10.1016/0375-9474(93)90043-W
Nucl.Phys. A572, 417 (1994)
S.Tormanen, S.Juutinen, R.Julin, B.Cederwall, A.Johnson, R.Wyss, P.Ahonen, B.Fant, M.Matsuzaki, J.Nyberg, M.Piiparinen, S.Mitarai, J.Mukai, A.Virtanen
Competing Proton and Neutron Alignments in Neutron-Deficient Xe-Nuclei
NUCLEAR REACTIONS 92Mo(32S, xn2pα), (32S, 4p), E=145 MeV; 106Pd(18O, 4n), E=75 MeV; measured Eγ, Iγ, DCO ratios, γγ-coin. 117,118,120Xe deduced levels, J, π, γ-branching, B(λ) ratios, experimental routhians, aligned angular momenta. Enriched targets, array of Compton-suppressed Ge-detectors, 4π array of Si charged-particle detectors, neutron detectors. Total routhian surface calculations, γS-band.
doi: 10.1016/0375-9474(94)90183-X
Nucl.Phys. A595, 409 (1995)
G.Audi, A.H.Wapstra
The 1995 Update to the Atomic Mass Evaluation
COMPILATION A=1-266; compiled, evaluated, updated mass excess, isomeric transition energies data. 1n, 1,2,3H, 3,4He, 13,14C, 14,15N, 16O, 20Ne, 28Si, 40Ar deduced precise masses.
doi: 10.1016/0375-9474(95)00445-9
Proc.Intern.Conf on Exotic Nuclei and Atomic Masses, Arles, France, June 19-23, 1995, p.553 (1995)
S.Czajkowski, F.Ameil, P.Armbruster, M.Bernas, P.Dessagne, C.Donzaud, C.Engelmann, H.-R.Faust, H.Geissel, E.Hanelt, A.Heinz, M.Hesse, C.Kozhuharov, C.Miehe, G.Munzenberg, M.Pfutzner, C.Rohl, K.-H.Schmidt, W.Schwab, C.Stephan, K.Summerer, L.Tassan-Got, B.Voss
Identification of New Neutron-Rich Isotopes Produced in Fission of Relativistic 238U Projectiles at the GSI Fragment Separator
NUCLEAR REACTIONS 9Be(238U, F), E=750 MeV/nucleon; measured projectile fission fragment mass, charge distribution; deduced for 62V, 120Ru, 78Ni. Other data considered, new limits of nuclide chart.
Z.Phys. A352, 11 (1995)
H.Kaur, J.Singh, A.Sharma, J.Goswamy, D.Mehta, N.Singh, R.K.Bhowmik, P.N.Trehan
Band Structures in Doubly-Odd 120I Nucleus
NUCLEAR REACTIONS 108Pd(16O, 3np), E=84 MeV; 114Cd(11B, 5n), E=60 MeV; measured γγ-coin. 120I deduced levels, J, π, B(λ) ratios, band structures, configuration.
Phys.Rev. C52, 1792 (1995)
J.C.Walpe, B.F.Davis, S.Naguleswaran, W.Reviol, U.Garg, X.-W.Pan, D.H.Feng, J.X.Saladin
Lifetime Measurements in 120Xe
NUCLEAR REACTIONS 106Pd(18O, 4n), E=70 MeV; measured Eγ, Iγ, recoil distance method spectra. 120Xe levels deduced T1/2, B(λ), quadrupole moments.
Phys.Rev. C53, R2586 (1996)
P.F.Mantica, W.B.Walters
Enhanced E0 and E2 Transition Rates in the Midshell Xe Isotopes
RADIOACTIVITY 120Cs(β+), (EC) [from 92Mo(32S, X), E=175 MeV]; measured βγγ-coin. 120Xe levels deduced T1/2, B(λ).
doi: 10.1103/PhysRevC.53.R2586
Proc.Intern.on Nuclear Data for Science and Technology, Trieste, Italy, 19-24 May, 1997, G.Reffo, A.Ventura, C.Grandi, Eds., Editrice Compositori, Italy, Pt.1, p.784 (1997)
Y.S.Abdelrahman
New Energy Levels in Cd Isotopes
NUCLEAR REACTIONS 197Au(19F, X), 232Th(18O, X), E=120 MeV; measured Eγ, Iγ, γγ-coin following compound nucleus fission. 112,114,116,118,120Cd deduced high-spin levels, J, π.
Nucl.Phys. A624, 1 (1997)
G.Audi, O.Bersillon, J.Blachot, A.H.Wapstra
The NUBASE Evaluation of Nuclear and Decay Properties
COMPILATION A=1-277; compiled, evaluated mass excess, J, π, T1/2, other ground-state properties.
doi: 10.1016/S0375-9474(97)00482-X
Phys.Rev. C55, 512 (1997)
H.Kaur, J.Singh, A.Sharma, J.Goswamy, D.Mehta, N.Singh, P.N.Trehan, E.S.Paul, R.K.Bhowmik
Collective Structures in Doubly Odd 120I
NUCLEAR REACTIONS 108Pd(16O, X), E=84 MeV; 114Cd(11B, X), E=60 MeV; measured γγ-coin, DCO ratios. 120I deduced high-spin levels, J, π, band structure, configuration, γ-multipolarity.
Phys.Rev. C56, 1157 (1997)
Z.Li, S.Xu, Y.Xie, R.Ma, Y.Ge, C.Wang, W.Huang, T.Zhang
New β-Delayed Proton Precursor 121Ce
RADIOACTIVITY 121Ce(β+p) [from 92Mo(32S, 3n), E=171 MeV]; measured β-delayed proton spectrum, Eγ, Iγ, γ(p)-, (X-ray)(p)-coin, T1/2. 120Ba deduced tentative partial level scheme, proton branching ratios.
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.
Nucl.Phys. A635, 428 (1998)
T.Baumann, E.Ramakrishnan, A.Azhari, J.R.Beene, R.J.Charity, J.F.Dempsey, M.L.Halbert, P.-F.Hua, R.A.Kryger, P.E.Mueller, R.Pfaff, D.G.Sarantites, L.G.Sobotka, D.W.Stracener, M.Thoennessen, G.Van Buren, R.L.Varner, S.Yokoyama
Evolution of the Giant Dipole Resonance in Excited 120Sn and 208Pb Nuclei Populated by Inelastic Alpha Scattering
NUCLEAR REACTIONS 120Sn(α, α'), E=40, 50 MeV/nucleon; 208Pb(α, α'), E=40 MeV/nucleon; measured Eγ, Iγ, Eα, Iα, αγ-coin. 120Sn, 208Pb deduced GDR width vs temperature, shape effects. Adiabatic coupling model.
doi: 10.1016/S0375-9474(98)00197-3
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
Phys.Rev. C59, 1930 (1999)
J.Bryssinck, L.Govor, D.Belic, F.Bauwens, O.Beck, P.von Brentano, D.De Frenne, T.Eckert, C.Fransen, K.Govaert, R.-D.Herzberg, E.Jacobs, U.Kneissl, H.Maser, A.Nord, N.Pietralla, H.H.Pitz, V.Yu.Ponomarev, V.Werner
Uniform Properties of Jπ = 1- Two-Phonon States in the Semimagic Even-Even Tin Isotopes 116, 118, 120, 122, 124Sn
NUCLEAR REACTIONS 116,118,120,122,124Sn(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ. 116,118,120,122,124Sn deduced levels, J, π, excitation B(M1), two-phonon excitations. Quasiparticle-phonon model calculations.
Phys.Rev. C60, 054603 (1999)
P.Guazzoni, M.Jaskola, L.Zetta, A.Covello, A.Gargano, Y.Eisermann, G.Graw, R.Hertenberger, A.Metz, F.Nuoffer, G.Staudt
Level Structure of 120Sn: High resolution (p, t) reaction and shell model description
NUCLEAR REACTIONS 122Sn(p, t), E=26 MeV; measured triton spectrum, σ(θ); deduced optical model parameters. 120Sn deduced levels, J, π.
NUCLEAR STRUCTURE 120Sn; calculated levels, J, π. Shell model.
doi: 10.1103/PhysRevC.60.054603
Phys.Rev. C60, 067304 (1999)
Z.Li, S.Xu, Y.Xie, R.Ma, Y.Ge, C.Wang, W.Huang, T.Zhang
Ground-State Spin of the β-Delayed Proton Precursor 121Ce
RADIOACTIVITY 121Ce(β+p) [from 92Mo(32S, 3n)]; measured β-delayed proton spectra, pγ-coin. 120Ba deduced final state proton branching ratios. 121Ce deduced ground-state J, π. Statistical model calculation.
doi: 10.1103/PhysRevC.60.067304
Phys.Rev. C61, 024309 (2000)
J.Bryssinck, L.Govor, V.Yu.Ponomarev, F.Bauwens, O.Beck, D.Belic, P.von Brentano, D.De Frenne, T.Eckert, C.Fransen, K.Govaert, R.-D.Herzberg, E.Jacobs, U.Kneissl, H.Maser, A.Nord, N.Pietralla, H.H.Pitz, V.Werner
Systematic Study of Electric Quadrupole Excitations in the Stable Even Mass Sn Nuclei
NUCLEAR REACTIONS 116,118,120,122,124Sn(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ. 116,118,120,122,124Sn deduced levels J, π, B(E1), B(E2).
doi: 10.1103/PhysRevC.61.024309
Phys.Scr. T88, 127 (2000)
N.Fotiades, J.A.Cizewski, K.Y.Ding, R.Krucken, J.A.Becker, L.A.Bernstein, K.Hauschild, D.P.McNabb, W.Younes, P.Fallon, I.Y.Lee, A.O.Macchiavelli
High-Spin Studies of Fission Products in Fusion-Evaporation Reactions
NUCLEAR REACTIONS 208Pb(18O, F), E=91 MeV; 176Yb(23Na, F), E=129 MeV; measured Eγ, Iγ, γγ-coin following compound nucleus fission. 173Yb(24Mg, F), E=134.5 MeV; measured Eγ, Iγ, γγ-coin following compound nucleus fission; deduced fission fragments charge and mass distributons. 88,90,91,92Sr, 101Tc, 107Ru, 113,114,115,116,117,118,119,120Cd deduced high-spin levels, J, π.
doi: 10.1238/Physica.Topical.088a00127
J.Korean Phys.Soc. 36, 199 (2000)
J.H.Ha, B.H.Choi, J.C.Kim, S.H.Park, C.S.Lee, J.H.Lee, Y.K.Kwon, J.H.Kim, J.S.Chai
In-Beam γ-Ray Coincidence Spectroscopy for Low-Lying States of Tellurium Isotopes by using a natSn(α, 2nγ) Reaction
NUCLEAR REACTIONS 116,118,120Sn(α, 2n), E=22 MeV; measured Eγ, Iγ, γγ-coin. 118,120,122Te deduced levels, J, π, deformation. Total Routhian surface and IBA calculations.
Radiochim.Acta 88, 139 (2000)
A.Hohn, H.H.Coenen, S.M.Qaim
Positron Emission Intensity in the Decay of 120gI
RADIOACTIVITY 120I(β+), (EC) [from 120Te(p, n)]; measured Eγ, Iγ, X-ray spectra, T1/2; deduced positron emission branching ratio.
Eur.Phys.J. A 9, 293 (2000)
A.A.Pasternak, Y.Sasaki, A.D.Efimov, V.M.Mikhailov, T.Hayakawa, Y.Toh, M.Oshima, Y.Hatsukawa, J.Katakura, N.Shinohara, Z.Liu, K.Furuno
DSA Lifetime Measurements and Structure of Positive-Parity Bands of 120Xe
NUCLEAR REACTIONS 111Cd(12C, 3n), E=56 MeV; measured Eγ, Iγ, γγ-coin, DSA. 120Xe deduced high-spin levels, J, π, T1/2, B(E2). Comparison with IBM calculations.
Phys.Lett. 483B, 7 (2000)
J.F.Smith, C.J.Chiara, D.B.Fossan, G.J.Lane, J.M.Sears, I.Thorslund, I.M.Hibbert, R.Wadsworth, I.Y.Lee, A.O.Macchiavelli
Multiple Shape-Driving ν(h11/2)2 and π(h11/2)2 Alignments in 120Ba
NUCLEAR REACTIONS 58Ni(64Zn, 2p), E=265 MeV; measured Eγ, Iγ(θ), γγ-coin. 120Ba deduced high-spin levels, J, π, band configuration and aligned angular momenta. Comparison with neighboring nuclei and with theoretical calculations. GAMMASPHERE array.
doi: 10.1016/S0370-2693(00)00557-8
Phys.Rev. C63, 024607 (2001)
E.Bauge, J.P.Delaroche, M.Girod
Lane-Consistent, Semimicroscopic Nucleon-Nucleus Optical Model
NUCLEAR REACTIONS 58Ni(polarized p, p), E=10-200 MeV; 208Pb(polarized n, n), E=2-155 MeV; 54,56Fe, 58,61,62,64Ni, 70Zn, 90,96Zr, 96Mo, 96Ru, 115In, 112,116,117,118,120,124Sn(polarized p, n), E=23 MeV; calculated σ(θ), Ay(θ). 40Ca, 90Zr, 120Sn, 208Pb(n, X), E < 200 MeV; calculated total σ. 54,56Fe, 60Ni, 92Mo, 93Nb, 104Pd, 112,116,120,124Sn, 138Ba, 142Nd, 144Sm, 208Pb(p, n), E=26, 30, 35 MeV; 48Ca, 90Zr, 120Sn, 208Pb(p, n), E=25, 35, 45, 120, 135, 160 MeV; calculated σ(θ). Lane-consistent, semimicroscopic optical model, comparisons with data.
doi: 10.1103/PhysRevC.63.024607
Nucl.Phys. A696, 45 (2001)
C.-B.Moon, S.J.Chae, J.H.Ha, T.Komatsubara, Y.Sasaki, T.Jumatsu, K.Yamada, K.Satou, K.Furuno
Level Structure of 120Cs
NUCLEAR REACTIONS 107Ag(16O, 3n), E=85 MeV; measured Eγ, Iγ, DCO ratios, γγ-coin. 120Cs deduced high-spin levels, J, π, ocnfigurations, Routhians. γ-dependent Routhian surface calculations, cranked shell model calculations. Array of Compton-suppressed HPGe and LEPS detectors.
doi: 10.1016/S0375-9474(01)01118-6
Nucl.Phys. A679, 287 (2001)
C.P.Silva, M.A.G.Alvarez, L.C.Chamon, D.Pereira, M.N.Rao, E.S.Rossi, Jr., L.R.Gasques, M.A.E.Santo, R.M.Anjos, J.Lubian, P.R.S.Gomes, C.Muri, B.V.Carlson, S.Kailas, A.Chatterjee, P.Singh, A.Shrivastava, K.Mahata, S.Santra
The Heavy-Ion Nuclear Potential: Determination of a systematic behavior at the region of surface interaction distances
NUCLEAR REACTIONS 120Sn(16O, 16O), E=53-55 MeV; 138Ba(16O, 16O), E=54-57 MeV; 208Pb(16O, 16O), E=74-78 MeV; measured σ(θ); deduced optical potentials. Double-folding calculations with microscopic densities.
doi: 10.1016/S0375-9474(00)00347-X