Direct light differential measurement system
US-2024423517-A1 · Dec 26, 2024 · US
US10126170B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10126170-B2 |
| Application number | US-201615259687-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 8, 2016 |
| Priority date | Sep 10, 2015 |
| Publication date | Nov 13, 2018 |
| Grant date | Nov 13, 2018 |
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According to one aspect, a multi-heterodyne system is disclosed, which comprises a first laser source for generating multi-mode radiation having a frequency spectrum characterized by a first plurality of phase coherent frequencies, and a second laser source for generating multi-mode radiation having a frequency spectrum characterized by a second plurality of phase coherent frequencies. The system further comprises at least one detector for detecting a combination of the multi-mode radiation generated by the first and second laser sources so as to provide a multi-heterodyne signal having a frequency spectrum characterized by a plurality of beat frequencies, each beat frequency corresponding to a pairwise difference in the first and second plurality of phase coherent frequencies. The system further comprises an analyzer for receiving said multi-heterodyne signal and configured to employ a predictive model of the multi-heterodyne signal to provide estimates of any of phase error and timing error associated with the beat frequencies.
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What is claimed is: 1. A multi-heterodyne system, comprising: a first laser source for generating multi-mode radiation having a frequency spectrum characterized by a first plurality of phase coherent frequencies, a second laser source for generating multi-mode radiation having a frequency spectrum characterized by a second plurality of phase coherent frequencies, at least one detector for detecting a combination of said multi-mode radiation generated by said first and second laser sources so as to provide a multi-heterodyne signal having a frequency spectrum characterized by a plurality of beat frequencies each beat frequency corresponding to a pairwise difference in said first and second plurality of phase coherent frequencies, an analyzer for receiving said multi-heterodyne signal and configured to employ a predictive model of said multi-heterodyne signal to provide estimates of any of phase error and timing error associated with said beat frequencies. 2. The system of claim 1 , wherein said analyzer corrects any of said phase error and timing error of said detected multi-heterodyne signal based on said estimates so as to generate a corrected multi-heterodyne signal. 3. The multi-heterodyne system of claim 2 , wherein said predictive model of said multi-heterodyne signal (y(t)) is defined as: y ( t ) = ∑ n A n e i 2 π ∫ f n d t = ∑ n r n e i φ n e i 2 π ∫ f n dt wherein, A n denotes a complex amplitude associated with n th beat frequency characterized by a real amplitude r n and a phase φ n , ƒ n denotes the frequency of the n th beat frequency. 4. The multi-heterodyne system of claim 3 , wherein said analyzer minimizes an error function defined as: J ( x ) = ∑ k y k - h ( x k ) R - 1 2 + x k - f ( x k - 1 ) Q - 1 2 wherein, x k denotes a state of the system at time k, y k denotes measurement of the multi-heterodyne signal at time k, h(x k ) denotes the measurement function h evaluated at state x k and defined as follows: h(x k )=Σ n A nk e i2πϕ nk =Σ n r nk e iφ nk e iϕ nk , wherein A nk , r nk , φ nk , ϕ nk denote, respectively, A n , r n , φ n and ϕ n evaluated at time k, ƒ(x k ) denotes the time evolution function ƒ evaluated at state x k such that: r n(k+1) =r nk φ n(k+1) =φ nk ϕ n(k+1) =ϕ nk +2πΔ t ƒ nk wherein r n(k+1) , φ n(k+1) , ϕ n(k+1) , denote, respectively, r n , φ n , and ϕ n evaluated at time k+1, R is said measurement noise covariance, and Q is said process noise covariance. 5. The multi-heterodyne system of claim 1 , wherein said analyzer is further configured to minimize an error function associated with a difference between said detected and sa
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