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Frequency measuring system using mirror gap stabilized Fabry-Perot interferometer

机译:使用镜隙稳定的法布里-珀罗干涉仪的频率测量系统

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The mirror gap of a Fabry-Perot interferometer was stabilized with two laser diodes; one locked to the line frequency 385 243 555.14445 MHz of the F=3<--1 in 5D(3/2)<--5S(1/2) (Rb-87) and the other to the 385 284 566.3663 MHz of the F=4<--2 in 5D(5/2)<--5S(1/2) (Rb-87) [Opt. Commun. 102 (1993) 432]. The length of the mirror gap was adjusted to generate the zero-cross points simultaneously at both of the two line positions. The fringe signals obtained from an interferometer thus stabilized can be used as frequency markers having accuracies of the order of 10(10) depending on the finesse of the interferometer used. Based on measurement using Cs D-1 hyperfine lines reported by Udem et al. [Phys. Rev. Lett. 82 (1999) 3568], the uncertainty of markers in the region 50 THz apart from the reference lines is +/-5 MHz. (C) 2003 Elsevier B.V All rights reserved. [References: 16]
机译:Fabry-Perot干涉仪的镜间隙由两个激光二极管稳定;一个锁定到5D(3/2)<-5S(1/2)(Rb-87)中F = 3 <-1的线路频率385243555.14445 MHz,另一个锁定到3852842846.36.3663 MHz在5D(5/2)<-5S(1/2)(Rb-87)中F = 4 <-2社区102(1993)432]。调整镜面间隙的长度,以在两条线的两个位置同时生成零交叉点。从这样稳定的干涉仪获得的条纹信号可以用作频率标记,其精度取决于所使用的干涉仪的精度为10(10)。基于使用Udem等人报道的Cs D-1超细品系进行的测量。 [物理牧师82(1999)3568],在距参考线50 THz的区域内标记的不确定度为+/- 5 MHz。 (C)2003 Elsevier B.V保留所有权利。 [参考:16]

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