Computationally-assisted multi-heterodyne spectroscopy

US10126170B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10126170-B2
Application numberUS-201615259687-A
CountryUS
Kind codeB2
Filing dateSep 8, 2016
Priority dateSep 10, 2015
Publication dateNov 13, 2018
Grant dateNov 13, 2018

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  5. First independent claim

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Abstract

Official abstract text for this publication.

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.

First claim

Opening claim text (preview).

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

Assignees

Inventors

Classifications

  • by beating two waves of a same source but of different frequency and measuring the phase shift of the lower frequency obtained · CPC title

  • Devices without moving parts · CPC title

  • Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry (beam switching arrangements G01J3/08) · CPC title

  • G01J3/28Primary

    Investigating the spectrum (using colour filters G01J3/51) · CPC title

  • Arrangements of light sources specially adapted for spectrometry or colorimetry · CPC title

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What does patent US10126170B2 cover?
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 syst…
Who is the assignee on this patent?
Massachusetts Inst Technology
What technology area does this patent fall under?
Primary CPC classification G01J3/28. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Nov 13 2018 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 8 related publications on this page (citations in our corpus or others sharing the same primary CPC).