| 摘要 |
1, 195,839. Photo-electric interferometer. BARRINGER RESEARCH Ltd. Nov.20, 1967 [Nov. 22, 1966], No.52134/66. Heading G1A. In a photo-electric interferometer the path difference between interfering portions of radiation is cyclically varied so as to produce a modulated interference pattern which is viewed by a photo-electric device; by comparing the photoelectric signals derived from modulated interference pattern of unknown radiation with signals characteristic of a modulated interference pattern using known radiation the spectral content of the unknown radiation can be determined. The radiation may be monochromatic or of several wavelengths such as from a gas absorption or emission spectrum. In one embodiment using a Michaelson interferometer a half-silvered mirror creates two beams which after reflection off mirrors 12 and 14 respectively, recombine at mirror 11. A small part of the resulting interference pattern is received through a slit 13a upon a photo-detector 21 such as a photo-electric transistor, diode, resistor or voltaic cell. An angularly oscillating plate 15 cyclically and linearly varies the path difference between the beams so modulating the interference pattern. The resulting photo-electric alternating signals, after removal of the D. C. in a H.P. filter 23, is fed to a gate which is opened by signals stored photographically as lines 17 open a disc 16 and reproduced by a photo-cell 19. The disc is fixed to the oscillating plate 15 and the resulting intermittant signals from photo-cell 19 will, if the wavelengths to which they relate are present in the light S incident upon the interferometer, correspond with particular portions of the signal from photo-cell 21, which portions are of the same polarity and pass through the gate to integrator 29 and readout 30. If the wavelengths to which the stored signals relate are not present in the incident light the gate passes signals of random polarity and the integrator readout is zero. In another embodiment Fig.5 (not shown) using different analysing circuitry the path difference is not linearly varied as before but varies sinusoidally or at a constant acceleration by appropriately oscillating the plate 15 so that the frequency of the photo-electric signals derived from the interference pattern varies sinusoidally or linearly. A crystal filter passes signals only in a narrow band in the middle of the frequency range, which signals, after rectification and passage through a L.P. filter to remove the high frequency and to pass only the envelope of the signals, appear as pulses at a gate. For a particular angle of oscillation of the plate 15 four pulses appear at the gate for different wavelengths, but occurring at different times, A particular wavelength can be looked for by recording signals to open the gate at the appropriate time. The apparatus may be used to record the characteristic of the modulated interference pattern of known radiation by recording the signals supplied to gate 24 from photo-cell 21 when the incident radiation is of known composition. Instead of the oscillating plate 15, useful for visible and ultraviolet light, two mirrors mounted parallel to one another upon a rotating disc Fig.6 (not shown) may be used, particularly for infrared radiation. |
