| 摘要 |
1,031,224. Masers. WESTERN ELECTRIC CO. Inc. Feb. 7, 1963 [Feb. 23, 1962], No. 4971/63. Heading H3B. In an optical or microwave maser amplifier, a quartz piezo-electric element 13 transmits a mechanical wave, frequency fac, along a ruby rod 10 and a signal wave 17, frequency f 1 , is reflected to and fro between a wave peak of the mechanical wave and the interface between the ruby rod 10 and the element 13. There is a Doppler shift of frequency on reflection and there results a series of wave trains of frequencies f 1 , f 2 , f 3 , f 4 &c. where f 2 , = f 1 - fac, f 3 = f 1 -f 2 fac, f 4 = f 1 -f 3 fac &c- A pumping wave 19 is applied to the ruby either laterally in known manner or endwise as described in Specification 1,012,835. The change of frequency on reflection permits amplification without self-oscillation. The piezo-electric element is driven by electromagnetic wave energy from a source 12, the cavity 11 being resonant at the same frequency. The opposite end of the rod 10 is terminated optically and acoustically by a first portion 14 of optically absorptive material such as black sapphire and a second portion 15 of acoustically absorptive material such as ruby with rough surfaces. The mechanical wave and the signal may be transmitted in opposite directions as shown in Fig. 4. The transducer 43 is coupled to the rod by light-absorbing material 42. The cavity 41 in which the transducer 43 is mounted is placed on a Dewar flask 44 maintained at the temperature of liquid nitrogen (77‹K). The signal wave may be transmitted at an angle to the mechanical wave, Fig. 5 (not shown) . The end of the rod through which the signal wave is introduced has a totally reflecting portion 50 which may be perpendicular to the rod axis, as shown, or may be tilted. The input and output channels for signals 17, 18 may be coupled to the rod by a circulator comprising optical polarizers and polarization separators. |
