| 摘要 |
1,127,238. Television; light deflectors. UNITED AIRCRAFT CORP. 8 Oct., 1965 [28 Oct., 1964], No. 42717/65. Heading H4F. A light beam 14, preferably a laser beam, is deflected by means of an ultrasonic deflection or scanning cell comprising a transducer 10 and a transparent medium 12, the transducer being actuated to establish a standing acoustical wave within the medium thereby producing a time varying density gradient and thus a time varying refractive index gradient within the medium normal to the direction of light propagation which causes the light beam to be deflected back and forth at the ultrasonic driving frequency. The curves T 1 -T 3 in Fig. 3, represent the acoustical pressure gradient within the cell, the portions of the curve to the right of the centre-line illustrating regions of higher density and those to the left regions of lower density. The magnitude of the angle of deflection of the light or laser beam is primarily determined by the wavelength of the sound wave, the index of refraction of the cell medium which is preferably a liquid, i.e. tetrachloroethylene, and the peak pressures. The cell medium may alternatively comprise crystalline quartz, water or luuite. As the light beam diameter is smaller than the sonic wavelength, the divergence or distortion of the light beam is not significantly affected and if it is directed through a pressure nodal plane of a sinusoidal standing wave the light beam deflection is sinusoidal. To obtain a more linear pressure gradient a triangular instead of a sinusoidal wave may be used, and to improve the performance of the cell a mosaic or segmented transducer is used. Cavitation of the cell liquid is inhibited by operating the cell under pressure, and fine tuning for adjusting the resonant frequency of the cell is achieved by increasing or decreasing this pressure, major tuning adjustments being accomplished by means of spacers and screws. By employing two deflection cells, one horizontal and the other vertical, Fig. 1, not shown, the cells being driven from the same ultrasonic power oscillator with a 90 degrees phase shift between them, a circular scan is generated. This scan may be made to spiral by amplitude modulating the driving power at a lower frequency than the ultrasonic frequency to provide a two-dimensional area coverage. An optical imaging system using this arrangement is described with reference to Fig. 5, not shown, in which the scattered radiation from a target area is received and used to modulate a cathoderay tube electron beam in accordance with the reflectivity of the target area. |
