Tunable Michelson and Mach-Zehnder interferometers modified with Gires-Tournois interferometers
AssigneeLockheed Martin Corporation
InventorsChristopher W. Tischhauser, James E. Mason
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AssigneeLockheed Martin Corporation
InventorsChristopher W. Tischhauser, James E. Mason
Estimating the term…
Optical filters tunable for both center wavelength and bandwidth, having applications such as in astronomy, remote sensing, laser spectroscopy, and other laser-based sensing applications, using Michelson interferometers or Mach-Zehnder interferometers modified with Gires-Tournois interferometers (“GTIs”) are disclosed. A GTI nominally has unity magnitude reflectance as a function of wavelength and has a phase response based on its resonator characteristics. Replacing the end mirrors of a Michelson interferometer or the fold mirrors of a Mach-Zehnder interferometer with GTIs results in both high visibility throughput as well as the ability to tune the phase response characteristics to change the width of the bandpass/notch filters. A range of bandpass/bandreject optical filter modes, including a Fabry-Perot (“FP”) mode, a wideband, low-ripple FP mode, a narrowband notch/bandpass mode, and a wideband notch/bandpass mode, are all tunable and wavelength addressable.
An optical filter comprising a Michelson interferometer or a Mach-Zehnder interferometer having a first optical path length L1 and a second optical path length L2, the Michelson interferometer or the Mach-Zehnder interferometer further having a plurality of Gires-Tournois interferometers (“GTIs”) replacing a plurality of mirrors of the Michelson interferometer or the Mach-Zehnder interferometer, a first one of the plurality of GTIs having a first GTI physical spacing d1, a second one of the plurality of GTIs having a second GTI physical spacing d2,
An optical filter comprising a Michelson interferometer or a Mach-Zehnder interferometer having a first optical path length L1 and a second optical path length L2, the Michelson interferometer or the Mach-Zehnder interferometer further having a plurality of Gires-Tournois interferometers (“GTIs”) replacing a plurality of mirrors of the Michelson interferometer or the Mach-Zehnder interferometer, a first one of the plurality of GTIs having a first GTI physical spacing d1, a second one of the plurality of GTIs having a second GTI physical spacing d2,
Dependencies are inferred from the claim text.