Abstract: A correlation spectrometer permanently incorporates a reference cell (12) and an electro-optical phase modulator (EOPM) (50) in the light path between a sample cell (30) and a detector (20). The effect of the EOPM is such that its frequency modulates all of the monochromatic component of the incoherent radiation passing through it. The EOPM is adjusted so that when it is ON all of the energy in the monochromatic components is thrown into sidebands (55) differing from the original frequencies by integral multiples of the modulation frequency, with the total amount of energy absorbed from the original radiation remaining constant. When there is no coincidence between the constituents in the two cells, the detector's output is the same when the EOPM is ON and when it is OFF. However, when there is coincidence the detector's output changes when the EOPM is switched between its two states. The change in the detector's output is related to the quantity of the constituents in the sample cell.

Abstract: An electronically controllable apparatus is described which modulates a continuous wave laser beam 22 so as to produce an output beam 42 consisting of coherent "pulses" that are electronically controllable as to both pulse repetition rate and pulse width. The apparatus includes two acoustic devices 24, 26 positioned so that the laser beam passes through them in sequence, and apparatus 32 or 34 for passing sound waves through the devices to frequency shift the laser radiation as well as to diffract it. Each acoustic device such as 24 generates sound waves containing a group of frequencies which result in spaced pulses. The spreading of a laser beam at 40 which emanates from the first acoustic device 24 is countered by the second acoustic device 26 to produce a collimated, coherently pulsed, laser beam 42.

Abstract: An optoacoustic detector for gas analysis is implemented with Stark-effect cell modulation for switching a beam in and out of coincidence with a spectral line of a constituent gas in order to eliminate the heating effect of laser energy in the cell as a source of background noise. By using a multiline laser, and linearly sweeping the DC bias voltage while exciting the cell with a multiline laser, it is possible to obtain a spectrum from which to determine the combination of excited constituents and determine their concentrations in parts per million.

Abstract: A method and apparatus for frequency modulating radiation, such as from a laser, for optoacoustic detectors, interferometers, heterodyne spectrometers, and similar devices using two oppositely reciprocating cat's-eye retroreflectors to Doppler modulate the radiation. By reciprocally moving both retroreflectors, the center of mass is maintained constant to permit smooth operation at many Hertz. By slightly offsetting the axis of one retroreflector relative to the other, multiple passes of a light beam may be achieved for greater Doppler shifts with the same reciprocating motion of the retroreflectors. A Doppler shift of 2(v/c).nu. occurs for each pass where v is the velocity of each retroreflector, c is the speed of light, and .nu. is the frequency of radiation.