As an atomic beam propagates across a magnetic field, an electric field is
generated, E = V X B. This results in a spectral splitting and polarization
of the emitted radiation, known as the Stark effect. The direction of pola
rization of the emitted radiation provides a measure of the local magnetic
field direction or pitch angle. In addition to the electric field generated
by the neutral beam, intrinsic electric fields present in the plasma affec
t the direction of polarization. This has been exploited to measure both th
e plasma electric field and the magnetic field. Future development of the m
otional Stark effect utilizing laser induced fluorescence to access much lo
wer magnetic fields will be discussed. (C) 1999 American Institute of Physi
cs. [S0034-6748(99)50901-5].