Abstract
It is shown that unlike the σ·ϱ single-particle, velocity-dependent potential, a static parity non-conserving (PNC) potential can lead to both electric as well as magnetic irregular transitions even for a spin-independent nuclear Hamiltonian. Specific calculations are made of the circular polarization P to be expected in the case of the 480 keV γ-transition in 181Ta due to a static PNC potential. It is found that P ≈ −0.7 · 10 −4.
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