RING LASER

摘要

1,203,628. Lasers. SPERRY RAND CORP. 21 Nov., 1967 [29 Nov., 1966], No. 52814/67. Heading H1C. In a ring laser rotation rate sensor in which plane polarized light beams from a gas laser source 1 are propagated in opposite directions in a closed loop optical cavity comprising mirrors 4, 5 and a Faraday cell 11, the frequency locking threshold is reduced by applying an alternating signal from an adjustable voltage source 13 to the Faraday cell so as to frequency modulate the two beams, and by simultaneously frequency modulating from the same signal source one of the two beams 18, 19 extracted from the optical cavity. The Faraday cell 11 forms part of a composite structure 6 comprising Brewster angle prisms 7, 8 and quarter wave plates 9, 10, the prisms producing the output beams 18, 19 by partial reflection and the quarter wave plates converting the plane polarized closed loop beams into circular polarization. The Faraday cell, when energized by current in coil 12, introduces an optical delay which is different for the two directions of closed loop propagation. The extracted beams are collimated by mirror 20 and beam splitter 22, and detected by photo detector 23, mirror 20 being variably positioned by energization of a piezo electric element 24 from A.C. source 13 and constituting the modulator for beam 18. The alternating signal has a frequency substantially higher, e.g. five times, than the minimum beat frequency obtainable from the laser in the absence of both modulators. The beat frequency output may be biased by using a D.C. source 16. In a modification only one of the two beams in the closed loop is internally modulated.