Abstract
The one-pion-exchange contributions to the Lobashov experiment are carefully calculated and are shown to be relativistic corrections. Their contribution to the circular polarization, P γ , is 1.1 × 10 −9 A, where A measures the strength of the parity violating NNπ coupling. For A = 1 this is approximately 10% of the usual nonrelativistic result arising from heavy meson exchange.
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