IP Library Granted Patent US 9,207,121
Granted Patent B2
US 9,207,121 · App. 14/482,469 · Granted Dec 8, 2015

Cavity-enhanced frequency comb spectroscopy system employing a prism cavity

Inventor: Florian Adler (Lafayette Hill, PA)
Assignee: TIGER OPTICS, LLC
G01J3/42G01J3/021G01J3/10G01J3/4338
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Quick Facts
Patent No.
US 9,207,121
App. No.
14/482,469
Granted
Dec 8, 2015
Kind
B2
Abstract

Spectroscopy systems and methods of comb-based spectroscopy are provided. A light source generates light corresponding to a frequency comb. A prism cavity is optically coupled to the light source. The prism cavity receives the generated light and produces first and second output light. The first output light is associated with reflection of the received light within the prism cavity. The second output light is associated with transmission of the received light through a prism of the prism cavity. A coupling system is coupled to the light source and the prism cavity. The coupling system adjusts a characteristic of at least one of the light source or the prism cavity, based on at least one of the first output light and the second output light. The characteristic is adjusted to increase optical coupling between the light source and the prism cavity and to compensate for a dispersion of the prism cavity.

Claims (36)

1. A spectroscopy system comprising:

a light source configured to generate light corresponding to a frequency comb;

a prism cavity optically coupled to the light source, the prism cavity configured to receive the generated light and to produce first output light and second output light, the first output light associated with reflection of the received light within the prism cavity, the second output light associated with transmission of the received light through a prism of the prism cavity; and

a coupling system coupled to the light source and the prism cavity, the coupling system configured to adjust a characteristic of at least one of the light source or the prism cavity, based on at least one of the first output light and the second output light, the characteristic adjusted to increase optical coupling between the light source and the prism cavity and compensate for a dispersion of the prism cavity.

2. The system of claim 1 , further including a detector optically coupled to the prism cavity, the detector configured to measure a cavity transmission of the first output light from the prism cavity.

3. The system of claim 2 , wherein the detector includes at least one of a non-dispersive detector, a dispersive detector or a Fourier transform detector.

4. The system of claim 3 , wherein the dispersive detector includes at least one of a monochromator, a diffraction grating, a virtually imaged phased array spectrometer or an Echelle spectrograph.

5. The system of claim 1 , further comprising a polarizer having a predetermined polarization characteristic disposed between the light source and the prism cavity.

6. The system of claim 1 , wherein the characteristic includes at least one of a comb cavity length of the frequency comb, a pump power of the light source or a cavity length of the prism cavity.

7. The system of claim 1 , wherein the coupling system is configured to statically couple a comb frequency mode of the frequency comb to a prism cavity mode of the prism cavity based on the second output light from the prism cavity.

8. The system of claim 7 , wherein the coupling system is configured to statically couple the comb frequency mode to the prism cavity mode based on at least one of phase modulation locking or polarization locking.

9. The system of claim 7 , wherein the coupling system includes:

a first detector configured to monitor a first frequency of the second output light, the first frequency associated with an offset of the frequency comb; and

a second detector configured to monitor a second frequency of the second output light, the second frequency associated with a repetition rate of the frequency comb,

the monitored first frequency and the monitored second frequency used to adjust the characteristic of the light source.

10. The a system of claim 1 , wherein the coupling system is configured to:

dynamically couple comb frequencies of the frequency comb to prism cavity modes of the prism cavity, by sequentially sweeping the comb frequencies over a predetermined period of time, and

adjust the characteristic of at least one of the light source or the prism cavity, for each comb frequency in the predetermined period of time, based on at least one of the first output light or the second output light.

11. The system of claim 1 , wherein the prism cavity includes the prism and a further prism spaced apart by a cavity length, the prism and the further prism configured to form a ring cavity.

12. The system of claim 11 , wherein the prism and the further prism each includes a Brewster angle retro-reflecting prism.

13. The system of claim 1 , wherein the spectroscopy system is a cavity-enhanced direct frequency comb spectroscopy (CE-DFCS) system.

14. A method of comb-based spectroscopy, the method comprising:

generating, by a light source, light corresponding to a frequency comb;

directing the generated light to a prism cavity, such that the prism cavity produces first output light and second output light, the first output light associated with reflection of the generated light within the prism cavity, the second output light associated with transmission of the generated light through a prism of the prism cavity; and

adjusting a characteristic of at least one of the light source or the prism cavity, based on at least one of the first output light and the second output light, the characteristic adjusted to increase optical coupling between the light source and the prism cavity and compensate for a dispersion of the prism cavity.

15. The method of claim 14 , wherein the characteristic includes at least one of a comb cavity length of the frequency comb, a pump power of the light source or a cavity length of the prism cavity.

16. The method of claim 14 , wherein the adjusting of the characteristic includes:

dynamically coupling comb frequencies of the frequency comb to prism cavity modes of the prism cavity, by sequentially sweeping the comb frequencies over a predetermined period of time; and

adjusting the characteristic of at least one of the light source or the prism cavity, for each comb frequency in the predetermined period of time, based on at least one of the first output light or the second output light.

17. The method of claim 14 , wherein the adjusting of the characteristic includes statically maintaining a match between a comb frequency mode of the frequency comb and a prism cavity mode of the prism cavity based on the second output light from the prism cavity.

18. The method of claim 17 , wherein the adjusting of the characteristic includes:

monitoring a first frequency of the second output light, the first frequency associated with an offset of the frequency comb;

monitoring a second frequency of the second output light, the second frequency associated with a repetition rate of the frequency comb; and

adjusting the characteristic of the light source based on the monitored first frequency and the monitored second frequency.

19. The method of claim 14 , the method further comprising measuring a cavity transmission of the first output light from the prism cavity.

20. The method of claim 14 , wherein the prism cavity includes the prism and a further prism spaced apart by a cavity length, the prism and the further prism configured to form a ring cavity.

Assignments (8)
TERMINATION AND RELEASE OF SECURITY INTEREST IN PATENTS Recorded Aug 3, 2023
From: KAYNE SENIOR CREDIT IV LOANCO, LLC
To: COSA XENTAUR CORPORATION; TIGER OPTICS, LLC; PROCESS INSIGHTS AG (FORMERLY KNOWN AS LAR PROCESS ANALYSERS AG)
Reel/Frame 064483/0194 →
RELEASE OF SECURITY INTERESTS IN PATENTS Recorded Jul 21, 2023
From: JPMORGAN CHASE BANK, N.A.
To: TIGER OPTICS, LLC
Reel/Frame 064356/0544 →
SECURITY INTEREST Recorded Jul 19, 2023
From: COSA XENTAUR CORPORATION; TIGER OPTICS, LLC
To: ANTARES CAPITAL LP, AS AGENT
Reel/Frame 064342/0908 →
RELEASE OF SECURITY INTEREST RECORDED AT REEL/FRAME 048357/0732 Recorded Nov 2, 2020
From: CRYSTAL FINANCIAL LLC
To: COSA XENTAUR CORPORATION; LAR PROCESS ANALYSERS AG; TIGER OPTICS, LLC
Reel/Frame 054271/0013 →
SECURITY INTEREST Recorded Oct 30, 2020
From: COSA XENTAUR CORPORATION; TIGER OPTICS, LLC; LAR PROCESS ANALYSERS AG
To: KAYNE SENIOR CREDIT IV LOANCO, LLC, AS ADMINISTRATIVE AGENT AND COLLATERAL AGENT
Reel/Frame 054226/0982 →
SECURITY INTEREST Recorded Jul 3, 2019
From: TIGER OPTICS, LLC
To: JPMORGAN CHASE BANK, N.A., AS ADMINISTRATIVE AGENT
Reel/Frame 049666/0071 →
SECURITY INTEREST Recorded Feb 16, 2019
From: COSA XENTAUR CORPORATION; TIGER OPTICS, LLC; LAR PROCESS ANALYSERS AG
To: CRYSTAL FINANCIAL LLC, AS ADMINISTRATIVE AGENT
Reel/Frame 048357/0732 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 11, 2014
From: ADLER, FLORIAN, DR.
To: TIGER OPTICS, LLC
Reel/Frame 033719/0633 →
Continuity (2)
Provisional Application 61876266 · Sep 11, 2013
Related Publication 20150070692A1 · Mar 12, 2015