| D. Herriott, H. Kogelnik, and R. Kompfner, "O#-axis paths in spherical mirror interferometers," Appl. Opt., vol. 3, pp. 523-- 526, April 1964. |
....[99 101] which has since become of great importance as a tunable filter and optical spectrum analyzer. A small flurry of interest in passive multibounce stable resonators as optical delay lines and longpath length spectroscopic absorption cells also led to some particularly clever experiments [102, 103]. C. The Unstable Resonator In 1965 I introduced the so called unstable optical resonator which has very di#erent physical and mathematical properties as compared to gaussian stable resonators [104] Earlier papers by Fox and Li [44, 45] had calculated a few unstable resonator cases as an aside, ....
.... in Kogelnik and Li s classic review [10] and in the revised (1965) edition of Ramo, Whinnery and van Duzer s classic text [172] Real ray matrices, already known in standard optics texts [173] had been applied to optical resonators [70, 174 179] and converted to the now standard ABCD notation [102, 180 182]. Kogelnik in particular [180] had identified the bilinear transformation of the complex q parameter through any paraxial optical system using the ABCD matrix. The historical connection between the di#erential phase shifts of gaussian modes and the Gouy phase shift of the 19th century [4 6, 183, ....
D. Herriott, H. Kogelnik, and R. Kompfner, "O#-axis paths in spherical mirror interferometers," Appl. Opt., vol. 3, pp. 523-- 526, April 1964.
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