Abstract

A simple method of measuring the losses of a ruby laser resonant cavity has been developed in which the thresholds for R 1 line and R 2 line operation are compared. A quartz birefringent filter is placed in the cavity with quartz disk cut to allow Brewster-angle operation and of such a thickness that the separation between pass bands of the filter analyzer combination is 28 A. The analyzer, placed between the filter and the output mirror, consists of a stack of fused quartz plates at the Brewster-angle. A known loss is introduced into the cavity by means of a plate inclined to the laser beam at a known angle. With the filter set for R 2 operation the threshold is adjusted to a suitable value by rotating the loss plate to give an attenuation L 2 /pass. The filter is then reset for R 1 operation and a different (larger) attenuation L 1 must be introduced by the loss plate to raise the R 1 threshold to the same level. An analysis of the threshold populations of the2 E levels shows that the losses of the cavity due to aU sources of loss other than the loss plate may be obtained from a plot of \log L_{1} , against \log L_{2} .

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