Abstract
The theory of NMR in perturbed angular correlations is extended to include the effects of two rotating magnetic fields, and their superposition to give an oscillatory field. If both radiations are parallel to the static field, the counter-rotating field gives a second-order shift of the resonance (Bloch-Siegert effect). For other directions, there is a first-order change in the line shape which depends on the azimuthal orientation of the counters.
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