The narrowband light from a scannable, single-mode dye laser influences the electrical properties of gas discharges. The variation in these properties as the laser wavelength λ is scanned yields the optogalvanic spectrum of the discharge (i.e., electrical conductivity vs. frequency). By connecting a
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The narrowband light from a scannable, single-mode dye laser influences the electrical properties of gas discharges. The variation in these properties as the laser wavelength λ is scanned yields the optogalvanic spectrum of the discharge (i.e., electrical conductivity vs. frequency). By connecting a neon lamp, capacitor, and power supply in parallel, an undriven relaxation oscillator is formed whose natural frequency
f0 is affected by neon-resonant laser light and this λ-dependence of the relaxation oscillator frequency
f0 yields a variant optogalvanic spectrum (i.e.,
f0 vs. frequency). In this paper, a driving force is effectively applied to an otherwise undriven oscillator when the incident light is chopped periodically at
fd. For
fd ≈
f0 and a sufficiently large driving force amplitude (laser intensity and the degree of neon resonance), the relaxation oscillator can be entrained so that
f0 is locked on
fd and is independent of λ. For the new chopped-light technique described here,
fd is adjusted to be the subthreshold of the entrainment range, where the λ-dependence of
f0 is advantageously exaggerated by periodic pulling, and the beat frequency |
fd −
f0| vs. λ provides an optogalvanic spectrum with appealingly amplified signal-to-noise qualities. Beat frequency neon spectra are reported for the cases
fd <
f0 and
fd >
f0 and are compared with spectra obtained using the unchopped-light (i.e., undriven) method.
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