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Interferometers
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Interferometer optical - COH24
COH24 enables to extract phase and amplitude from a single polarization signal by performing...
Interferometer optical - COH24
COH24 enables to extract phase and amplitude from a single polarization signal by performing...
Interferometer optical - COH28
Based on two single polarization 90° optical hybrid coh24, COH28 achieves...
Interferometer optical - COH28
Based on two single polarization 90° optical hybrid coh24, COH28 achieves...
Interferometer optical - MINT
MINT is a Delay Line Interferometer (DLI) performing the interference between the signal and itself 1-bit delayed. MINT is tunable to perfectly match the carrier frequency.
Interferometer optical - WTMINT
WTMINT is the tunable version of the MINT. WTMINT tunes the FSR from 0.33 GHz to...
Interferometer optical - WTMINT
WTMINT is the tunable version of the MINT. WTMINT tunes the FSR from 0.33 GHz to infinity. A micrometer head allows the FSR tuning. The phase tuning is performed with an external voltage. A piloted version is available.
Our products can be all customized at any wavelength (808 nm, 1064 nm, 1310 nm...).
Our products can be all customized at any wavelength (808 nm, 1064 nm, 1310 nm...).
Interferometer - FFP-SI
The Micron Optics FFP-SI Fiber Fabry-Perot Scanning Interferometer is a lensless, plane Fabry-Perot interferometer with a single-mode fiber waveguide between two highly reflective multi-layer mirrors that are deposited...
Interferometer - FFP-SI
The Micron Optics FFP-SI Fiber Fabry-Perot Scanning Interferometer is a lensless, plane Fabry-Perot interferometer with a single-mode fiber waveguide between two highly reflective multi-layer mirrors that are deposited directly onto optical fibers. The cavity consists entirely of fiber waveguide, permitting an extremely wide range of possible Free Spectral Ranges (FSRs), and no alignment or mode-matching is required.
Wavelength scanning is achieved by axially straining a short section of fiber inside the cavity using a stacked piezoelectric actuator. Scanning frequencies to 100 Hz and higher can provide direct measurement of transient optical phenomenon such as laser chirp and jitter. Stable and repeatable scanning over longer periods of time can provide direct measurement of slowly varying optical phenomenon such as laser drift.
Wavelength scanning is achieved by axially straining a short section of fiber inside the cavity using a stacked piezoelectric actuator. Scanning frequencies to 100 Hz and higher can provide direct measurement of transient optical phenomenon such as laser chirp and jitter. Stable and repeatable scanning over longer periods of time can provide direct measurement of slowly varying optical phenomenon such as laser drift.
Interferometer - FFP-I, picoWave®
The Micron Optics FFP-I, Fiber Fabry-Perot Interferometer family of products is based on a fixed interferometer design with smooth, uniformly spaced transmission peaks. The FFP-I consists of a lensless plane Fabry-Perot Interferometer with a single-mode optical fiber...
Interferometer - FFP-I, picoWave®
The Micron Optics FFP-I, Fiber Fabry-Perot Interferometer family of products is based on a fixed interferometer design with smooth, uniformly spaced transmission peaks. The FFP-I consists of a lensless plane Fabry-Perot Interferometer with a single-mode optical fiber...
Interferometer white light - max. 1 550 nm
The Distributed Polarization Crosstalk (X-Talk) Analyzer (PXA-1000) is an enhanced version of a white light interferometer designed to obtain space-resolved stress information by analyzing stress-induced polarization cross-coupling along a length of polarization maintaining (PM) fiber. Its patent-pending optical design eliminates the strong zero-order...
Interferometer white light - max. 1 550 nm
The Distributed Polarization Crosstalk (X-Talk) Analyzer (PXA-1000) is an enhanced version of a white light interferometer designed to obtain space-resolved stress information by analyzing stress-induced polarization cross-coupling along a length of polarization maintaining (PM) fiber. Its patent-pending optical design eliminates the strong zero-order interference and reduces the multi-coupling interference common in traditional white light interferometers, both of which can cause ghost peaks in the measured signal. The removal of the ghost peaks enables the PXA-1000 to unambiguously identify the magnitudes and locations of actual x-talk peaks, resulting in higher measurement sensitivity, higher dynamic range, and higher spatial measurement accuracy than traditional white light interferometers. The PXA-1000 also enables the use of the PM fiber itself as the sensing medium, eliminating the need to place multiple fiber gratings along the fiber. It can therefore obtain higher spatial resolution of the stress distribution than grating-based systems. Because no discrete sensing elements are required, the system is easy to install and calibrate, making it ideal for monitoring space-resolved structural changes along bridges, tunnels, dams, oil pipes, or buildings. It can also be used as an intrusion detection system, because any mechanical disturbances to the PM fiber will cause polarization coupling.
Interferometer - max. 1 550 nm | MZI-001
The MZI-001 is a fiber pigtailed compact Mach-Zehnder interferometer, based on freespace optics, for detecting changes in optical frequency. The device comes with two fast photodetectors for the balanced detection of the two complementary outputs of the interferometer....
Interferometer - max. 1 550 nm | MZI-001
The MZI-001 is a fiber pigtailed compact Mach-Zehnder interferometer, based on freespace optics, for detecting changes in optical frequency. The device comes with two fast photodetectors for the balanced detection of the two complementary outputs of the interferometer....