References quoted in the XUNDL dataset: 86KR 86BR B- DECAY:55.1 S:XUNDL-4

2 references found.

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2012WA38

Chin.Phys.C 36, 1603 (2012)

M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer

The AME2012 atomic mass evaluation (II). Tables, graphs and references

COMPILATION A=1-295; compiled, evaluated atomic mass data.

2016UR04

Phys.Rev. C 94, 044328 (2016)

W.Urban, K.Sieja, T.Materna, M.Czerwinski, T.Rzaca-Urban, A.Blanc, M.Jentschel, P.Mutti, U.Koster, T.Soldner, G.de France, G.S.Simpson, C.A.Ur, C.Bernards, C.Fransen, J.Jolie, J.-M.Regis, T.Thomas, N.Warr

Low-spin structure of ⁸⁶₃₅Br₅₁ and ⁸⁶₃₆Kr₅₀ nuclei: The role of the g_7/2 neutron orbital

RADIOACTIVITY ⁸⁶Se, ⁸⁶Br(β^-)[from ²³⁵U(n, γ), E=thermal neutrons from PF1B-ILL-Grenoble facility using Lohengrin fission-fragment separator]; measured Eγ, Iγ, γγ-coin for both decays, γγ(θ) and γγ(linear polarization) for ⁸⁶Br decay using EXILL array of Ge detectors. ⁸⁶Br, ⁸⁶Kr; deduced levels, J, π, conversion coefficients, multipolarities, β feedings, logft. Comparison with large-scale shell-model calculations with refined interactions.

NUCLEAR REACTIONS ²³⁵U(n, γ), E=thermal neutrons from PF1B-ILL-Grenoble facility; measured Eγ, Iγ, γγ-coin using EXILL array of Ge detectors, level half-life by γγ(t). ⁸⁶Br; deduced levels, J, π, B(M2), B(E3).

doi: 10.1103/PhysRevC.94.044328