NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = K.Dybdal Found 10 matches. 1986CH01 Phys.Rev. C33, 130 (1986) T.Chapuran, K.Dybdal, D.B.Fossan, T.Lonnroth, W.F.Piel, Jr., D.Horn, E.K.Warburton High-Spin γ-Ray Spectroscopy in 197Bi NUCLEAR REACTIONS, ICPND 192Pt(10B, 5n), E=50-80 MeV; measured σ(Eγ, E), γγ-coin, γ(θ), γγ(t), gamma-ray yields. 197Bi deduced levels, J, π, isomers, T1/2, configurations, B(λ), yrast sequence.
doi: 10.1103/PhysRevC.33.130
1985PI05 Phys.Rev. C31, 2087 (1985) W.F.Piel, Jr., T.Chapuran, K.Dybdal, D.B.Fossan, T.Lonnroth, D.Horn, E.K.Warburton High-Spin γ-Ray Spectroscopy in Z = 83 Isotopes: 199,201Bi NUCLEAR REACTIONS 194,196Pt(10B, 5n), E=57-72 MeV; measured Eγ, Iγ, γγ-coin, Iγ(t), Iγ(θ), γγ(θ). 199,201Bi deduced levels, J, π, T1/2, δ, configurations, B(λ), yrast sequence. Enriched targets, Ge(Li), Ge detectors.
doi: 10.1103/PhysRevC.31.2087
1984NI14 Phys.Scr. 30, 297 (1984) P.T.Nielsen, K.Dybdal, K.Bonde Nielsen, N.Rud K-Shell Cross-Sections Extracted from Measured Charge-State Distributions for F and Si Ions Penetrating C ATOMIC PHYSICS C(19F, X), E=10-38 MeV; C(28Si, X), E=25-56 MeV; measured charge state distributions; deduced K-shell σ.
doi: 10.1088/0031-8949/30/5/003
1983DY02 Phys.Rev. C28, 1171 (1983) K.Dybdal, T.Chapuran, D.B.Fossan, W.F.Piel, Jr., D.Horn, E.K.Warburton High-Spin States in 201,203At and the Systematic Behavior of Z = 85 Isotopes NUCLEAR REACTIONS, ICPND 192,194Pt(14N, 5n), E=58-100 MeV; measured γγ-coin, σ(Eγ, E), γ(θ), γ(t), Eγ, Iγ, γ yields. 201,203At deduced levels, J, π, T1/2, γ-branching, configurations.
doi: 10.1103/PhysRevC.28.1171
1983RA36 Hyperfine Interactions 15/16, 43 (1983) M.H.Rafailovich, E.Dafni, G.Schatz, S.Y.Zhu, K.Dybdal, S.Vajda, C.Alonso-Arias, S.Rolston, G.D.Sprouse g-Factor Measurements of Fission Isomers RADIOACTIVITY 239mAm, 237Pu(SF) [from 235U, 237Np(α, 2n), E=25 MeV]; measured fission fragment anisotropy, isomer T1/2, g. NUCLEAR REACTIONS 235U, 237Np(α, 2n), E=25 MeV; measured γ(θ, H, t). 239Am, 237Pu deduced fission isomer g, T1/2.
doi: 10.1007/BF02159713
1982RA04 Phys.Rev.Lett. 48, 982 (1982); Erattum Phys.Rev.Lett. 49, 244 (1982) M.H.Rafailovich, E.Dafni, G.Schatz, S.Y.Zhu, K.Dybdal, S.Vajda, C.Alonso-Arias, G.D.Sprouse Measurement of the g Factor of the 237Pu Short-Lived Fission Isomer NUCLEAR REACTIONS 235U(α, 2n), E=25.2 MeV; measured γ(θ, H, T). 237Pu deduced fission isomer g, Nilsson configuration.
doi: 10.1103/PhysRevLett.48.982
1981DY01 Nucl.Phys. A359, 431 (1981) K.Dybdal, J.S.Forster, P.Hornshoj, N.Rud, C.A.Straede DSAM Lifetime Measurements in 26Mg with High-Velocity Recoils NUCLEAR REACTIONS 4He(23Na, p), E=43.3 MeV; measured pγ-coin, DSA. 26Mg levels deduced γ-branching ratios, T1/2, B(λ).
doi: 10.1016/0375-9474(81)90247-5
1980EB01 Hyperfine Interactions 8, 387 (1980) The Velocity and Z Dependence of the Transient Magnetic Field in Iron NUCLEAR REACTIONS 134Ba(12C, 12C'), E=30 MeV; 134Ba(16O, 16O'), E=45 MeV; 134Ba(32S, 32S'), E=80 MeV; measured γ(θ, H) in Fe, Coulomb excitation. 134Ba level deduced g.
1979DY05 Hyperfine Interactions 7, 29 (1979) K.Dybdal, J.L.Eberhardt, N.Rud The Transient Magnetic Field for 12C in Iron NUCLEAR REACTIONS 2H(12C, pγ), E=15.5, 33 MeV; measured γ(θ, H), Eγ, Iγ. 12C level deduced time-integral transient field precision in magnetized Fe.
doi: 10.1007/BF01021490
1976DY05 Phys.Lett. 64B, 414 (1976) K.Dybdal, J.L.Eberhardt, N.Rud The Transient Field in Iron for 13C NUCLEAR REACTIONS 2H(12C, pγ), E=15.5 MeV; measured γ yields of 13C recoiling into Fe. 13C deduced transient field in Fe.
doi: 10.1016/0370-2693(76)90109-X
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