NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = T.Weckstrom Found 15 matches. 1993BL02 Nucl.Phys. A554, 45 (1993) J.Blomqvist, R.Liotta, L.O.Norlin, U.Rosengard, B.Fant, T.Weckstrom, H.C.Jain, T.Lonnroth High-Spin States in 206Pb NUCLEAR REACTIONS 204Hg(α, 2n), E=35 MeV; measured Eγ, Iγ, γ(t), γ(θ), γγ-coin. 206Pb deduced levels, decay features, J, π. Metallic 204Hg target, Ge detectors. Shell-model calculations.
doi: 10.1016/0375-9474(93)90356-3
1990FA03 Phys.Scr. 41, 652 (1990) B.Fant, T.Weckstrom, A.Kallberg The High-Spin Structure of 202Po and 204Po and Systematical Features of the Even Polonium Isotopes NUCLEAR REACTIONS 196,198Pt(12C, 6n), E=100 MeV; 204Pb(α, 4n), E=52-54 MeV; measured γγ-coin, γ(θ), Eγ, Iγ, I(ce), σ(Eγ, E). 202,204Po deduced levels, J, π, T1/2, γ-multipolarity.
doi: 10.1088/0031-8949/41/5/005
1988RO08 Nucl.Phys. A482, 573 (1988) U.Rosengard, P.Carle, A.Kallberg, L.O.Norlin, K.-G.Rensfelt, H.C.Jain, B.Fant, T.Weckstrom Yrast Spectroscopy and g-Factor Measurements in 199Pb, 201Pb and 203Pb NUCLEAR REACTIONS 198,200Hg(α, 2n), (α, 3n), E=41 MeV; 200,202Hg(α, 3n), (α, 4n), E=53 MeV; measured Eγ, Iγ, γ(θ), γ(θ, H, t), γγ(t). 199,201,203Pb deduced levels, J, π, T1/2, g, B(E2), configurations. Enriched thick targets, Ge, Ge(Li) detectors. Shell model. NUCLEAR STRUCTURE 199,201,203Pb; calculated levels; deduced configurations. Shell model.
doi: 10.1016/0375-9474(88)90171-6
1987FA15 Nucl.Phys. A475, 338 (1987) B.Fant, T.Weckstrom, H.C.Jain, L.O.Norlin, K.-G.Rensfelt, P.Carle, U.Rosengard Investigation of the High-Spin Structure of 200,202Pb NUCLEAR REACTIONS 198Hg(α, 2n), E=41 MeV; 200,202Hg(α, 4n), E=53 MeV; measured E(γ), I(γ), γ(θ), γ(t), γγ(t). 200,202Pb deduced levels, J, π, T1/2, g, B(λ), configurations. Enriched targets, Ge, Ge(Li) detectors. Shell model.
doi: 10.1016/0375-9474(87)90170-9
1987JA08 Hyperfine Interactions 34, 73 (1987) H.C.Jain, L.O.Norlin, K.-G.Rensfelt, U.Rosengard, P.Carle, B.Fant, T.Weckstrom The g-Factor of 19- Isomer in 202Pb NUCLEAR REACTIONS 202Hg(α, 4n), E=53 MeV; measured γ(θ, H, t). 202Pb deduced isomer g, configuration, T1/2.
doi: 10.1007/BF02072682
1986FA04 Nucl.Phys. A453, 77 (1986) B.Fant, T.Weckstrom, V.Rahkonen, C.J.Herrlander, A.Kallberg High-Spin and Isomeric States in 203Po NUCLEAR REACTIONS 204Pb(α, 5n), E=63 MeV; measured Eγ, Iγ, γ(θ), γ(t), γγ(t), I(ce). 203Po deduced levels, J, π, T1/2, B(λ), configurations. Enriched targets, Ge, Ge(Li), Si(Li) detectors. Shell model.
doi: 10.1016/0375-9474(86)90030-8
1985RA18 Nucl.Phys. A441, 11 (1985) V.Rahkonen, B.Fant, C.J.Herrlander, K.Honkanen, A.Kallberg, T.Weckstrom An Investigation of the Yrast States in 205,207Po NUCLEAR REACTIONS 204,206,207,208Pb(α, xn), E=40-63 MeV; 207Pb(3He, 3n), E=27 MeV; measured Eγ, Iγ, γ(θ), γ(t), γγ(t), I(ce). 205,207Po deduced levels J, π, T1/2, ICC, γ-multipolarity, B(λ), configurations. Ge, Ge(Li), Si-Li detectors, enriched targets. Shell-model.
doi: 10.1016/0375-9474(85)90165-4
1985WE05 Z.Phys. A321, 231 (1985) T.Weckstrom, B.Fant, T.Lonnroth, V.Rahkonen, A.Kallberg, C.-J.Herrlander In-Beam Study of High-Spin States in 199,200,201Po and Systematical Features of Z = 84 Polonium Isotopes NUCLEAR REACTIONS 194Pt(12C, 7n), (12C, 6n), (12C, 5n), 195Pt(12C, 6n), E=100, 102, 106 MeV; measured Eγ, Iγ, γγ-, γγ(nn)-, γ(nn)-coin, γ yields, γ(X-ray)-coin. 199,201Po deduced levels, J, π, γ-branching. 200Po deduced levels, isomer T1/2, J, π, γ-branching, γ-multipolarity, configuration. Self-consistent Hartree-Fock calculations.
1984FA10 Nucl.Phys. A429, 296 (1984) B.Fant, T.Weckstrom, T.Lonnroth, C.J.Herrlander, K.Honkanen, A.Kallberg Study of the Three-Proton Three Neutron-Hole Nucleus 208At NUCLEAR REACTIONS 209Bi(α, 5n), E=51-60 MeV; measured Eγ, Iγ, γ(θ), γ(t), γγ(t), I(ce). 208At deduced levels J, π, T1/2, ICC, γ-multipolarity, B(λ), transition rates, configurations. Shell model considerations.
doi: 10.1016/0375-9474(84)90209-4
1980WE01 Phys.Scr. 21, 137 (1980) Energy Levels in 55Mn. II. Mean Lifetimes and Spins of Bound States NUCLEAR REACTIONS 54Cr(p, γ), E=1666-1879 keV; measured DSA, γ(θ), Eγ. 55Mn levels deduced T1/2, δ, J, π, B(λ). Shell model.
1978WE12 Phys.Scr. 18, 275 (1978) Energy Levels in 55Mn I. Excitation Curves, Gamma-Decay of Resonances And of Bound States NUCLEAR REACTIONS 54Cr(p, γ), E=1.04-2.56 MeV; measured σ(E, Eγ); deduced Q. 55Mn deduced resonances, levels, γ-branching.
1975WE10 Phys.Scr. 11, 10 (1975) T.Weckstrom, B.Fant, I.Forsblom, M.Viitasalo Energy Levels of 54Mn NUCLEAR REACTIONS 53Cr(p, γ), E=1180-2100 keV; measured σ(E, Eγ); deduced Q. 54Mn deduced resonances, levels, γ-branching.
1975WE24 Phys.Fenn. 10, 167 (1975) T.Weckstrom, I.Forsblom, P.Holmberg The Gamma Decay of Some States in 65Ga and the Mass Excess of 65Ga NUCLEAR REACTIONS 64Zn(p, γ), E=1.8-2.1 MeV; measured σ(E, Eγ); deduced Q. 65Ga deduced mass excess, levels.
1973HO42 Commentat.Phys.-Math. 43, 203 (1973) P.Holmberg, T.Weckstrom, A.Kiuru Properties of Nuclear Levels and Transitions in Odd Copper Isotopes. IV. The 64Ni(p, γ)65Cu Reaction NUCLEAR REACTIONS 64Ni(p, γ), E=1-1.85 MeV; measured Eγ, γ(θ). 65Cu deduced resonances, J, π, γ-branching.
1972FO25 Phys.Scr. 6, 309 (1972) I.Forsblom, T.Weckstrom, T.Sundius, G.Bergstrom, S.Forss, G.Wansen A Study of Excited States in 51Mn NUCLEAR REACTIONS 50Cr(p, γ), E=1.0-1.7 MeV; measured σ(E, Eγ, θ), deduced Q. 51Mn deduced levels, J, π, mixing ratios.
doi: 10.1088/0031-8949/6/5-6/019
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