| 摘要 |
1,144,585. Lasers. PHILCO-FORD CORP. 23 June, 1966 [23 June, 1965], No. 28053/66. Heading H1C. A ring laser produces outputs of two distinct frequencies, one output being a reference frequency and the other a carrier frequency which may be frequency modulated. As shown, reflectors 10, 12, 14 together define a closed optical path which includes two active media 16, 18, each active medium comprising a helium-neon tube which is pumped by radiofrequency and has polarizing Brewster angle windows. The optical path includes a Kerr cell 26 and two 45 degree Faraday rotators which together cause the polarizations of the clockwise and anticlockwise light beams 40, 42, where they pass through the Kerr cell, to be rotated and then restored. The rotated polarization of beam 40 is parallel to the direction of a field applied to the Kerr cell by electrodes 28, 30, while the rotated polarization of beam 42 is orthogonal to this field. Consequently a bias voltage applied between the electrodes has little effect on the anticlockwise beam, so that its frequency remains substantially the same, but changes the frequency of the clockwise beam by effectively increasing its path length. The clockwise beam constitutes the carrier frequency which may be modulated by superimposing an A.C. signal from source 32 on the bias. The two. output frequencies are extracted by using a reflector 34 in association with reflector 14 which is partially transmitting, the reference (anticlockwise beam) frequency enabling demodulation by heterodyning and frequency discrimination to take place at a receiver 48. The difference in frequency between the two beams 40, 42 may be stabilized by sampling in the output path 36 and using the D.C. output of a discriminator to control the bias potential. Modulation may also be effected by cells employing stress induced or magnetic field birefringence. |
