1980
DOI: 10.1364/ao.19.002926
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Elimination of drift in a single-mode optical fiber interferometer using a piezoelectrically stretched coiled fiber

Abstract: The feasibility of maintaining a single-mode optical fiber interferometer in quadrature is demonstrated using a servo driven piezoelectrically stretched coiled fiber. The controller has a range of ~10(-5)-1000 rad with a stress voltage coefficient of ~27pi rad/V.

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Cited by 384 publications
(106 citation statements)
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“…Differently from conventional interferometric approaches, the key element of the proposed approach is represented by a new polarization and phase diversity coherent demodulation scheme ( Figure 1) where the signal S, back-reflected from the sensing fiber end, and a local oscillator (LO) are combined in a 90° optical hybrid [21][22][23] enabling the extraction of both phase, amplitude and polarization of the optical field S. Indeed, the outputs of the 90° optical hybrid, used in combination with balanced photodetectors, provide the in-phase I and the quadrature Q signals for both polarization σ(t) components (// and ⊥) of S, where I ÷   (( )) and Q ÷   (( )). The four in-phase I and quadrature Q signals are then digitalized and post-processed with demodulation algorithms exploited in coherent optical communications [24,25], allowing the recovery of A(t), θ(t) and σ(t) in a completely passive way without the need of complex active feedbacks for quadrature point stabilization as in conventional fiber optic interferometric and polarimetric schemes [26,27].…”
Section: Sensing Principlementioning
confidence: 99%
“…Differently from conventional interferometric approaches, the key element of the proposed approach is represented by a new polarization and phase diversity coherent demodulation scheme ( Figure 1) where the signal S, back-reflected from the sensing fiber end, and a local oscillator (LO) are combined in a 90° optical hybrid [21][22][23] enabling the extraction of both phase, amplitude and polarization of the optical field S. Indeed, the outputs of the 90° optical hybrid, used in combination with balanced photodetectors, provide the in-phase I and the quadrature Q signals for both polarization σ(t) components (// and ⊥) of S, where I ÷   (( )) and Q ÷   (( )). The four in-phase I and quadrature Q signals are then digitalized and post-processed with demodulation algorithms exploited in coherent optical communications [24,25], allowing the recovery of A(t), θ(t) and σ(t) in a completely passive way without the need of complex active feedbacks for quadrature point stabilization as in conventional fiber optic interferometric and polarimetric schemes [26,27].…”
Section: Sensing Principlementioning
confidence: 99%
“…A frequency shift in one of the beams may be accomplished by acousto-optic frequency modulation (Culshaw & Giles, 1982), frequency ramping the optical source (Jackson et al, 1982), or piezoelectric-induced path length changes (Jackson et al, 1980;Cole et al, 1982). These heterodyne modulation approaches have been categorized as true-heterodyne, pseudo-heterodyne, and synthetic-heterodyne techniques.…”
Section: Modulation and Demodulation Techniquesmentioning
confidence: 99%
“…Drift in the fiber interferometer results from laser frequency fluctuations along with mechanical and temperature induced strains. An active homodyne technique has been demonstrated by Jackson et al [20] to compensate for drift in a Mach-Zender fiber interferometer. This technique used a piezoelectric fiber stretcher to control the reference fiber length such that quadrature was maintained.…”
Section: Principles Of Opera Nonmentioning
confidence: 99%