Abstract
To date, the most sensitive and accurate passive optical gyroscopes have been phase reading interferometers with optical outputs of the form I = I0 (1 + cos ϕtot), where ϕtot is the non-reciprocal phase shift due to all sources. Ideally, the phase shift has only two components: 2ϕs, the Sagnac phase shift (proportional to the rotation rate), and ϕdither, which is introduced by a transducer to facilitate the measurement. In the gyroscope we report here, ϕdither is applied to a "minimum configuration" gyroscope and creates an ac output of the form
© 1988 Optical Society of America
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