We have observed normally forbidden two-quantum transitions in the optical spectrum of a helium plasma. We induced these transitions by applying a microwave field to a separately generated steady-state helium discharge. Measurements of the relative intensity and wave-length of the optical photons emitted in the two-quantum transition 5¹F⁰→2¹P⁰ in He I determined both the frequency and the strength of the microwave field in the plasma. The field strength was also measured by observation of the Stark shift of a spectral line and by measurement of the microwave power input and the Q of the microwave cavity. All measurements of the field strength are in satisfactory agreement and indicate an rms microwave field strength in the plasma of about 215 V/cm. The spectroscopic measurement of the frequency of the microwave field is within 3% of the actual value, and the measured polarization of the radiation agrees with theory.
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Cooper et al. (1969) studied this question.
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