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NSR database version of April 26, 2024.

Search: Author = K.Dybdal

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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, T_1/2, configurations, B(λ), yrast sequence.

doi: 10.1103/PhysRevC.33.130
Citations: PlumX Metrics

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, T_1/2, δ, configurations, B(λ), yrast sequence. Enriched targets, Ge(Li), Ge detectors.

doi: 10.1103/PhysRevC.31.2087
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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, T_1/2, γ-branching, configurations.

doi: 10.1103/PhysRevC.28.1171
Citations: PlumX Metrics

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 T_1/2, g.

NUCLEAR REACTIONS ²³⁵U, ²³⁷Np(α, 2n), E=25 MeV; measured γ(θ, H, t). ²³⁹Am, ²³⁷Pu deduced fission isomer g, T_1/2.

doi: 10.1007/BF02159713
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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
Citations: PlumX Metrics

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, T_1/2, B(λ).

doi: 10.1016/0375-9474(81)90247-5
Citations: PlumX Metrics

1980EB01      Hyperfine Interactions 8, 387 (1980)

J.L.Eberhardt, K.Dybdal

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics