Devices and methods for coherent detection using chirped laser pulses

• US 10,067,055 B1
• Filed: 05/11/2017
• Issued: 09/04/2018
• Est. Priority Date: 05/11/2016
• Status: Active Grant

• Current Assignee: Pendar Technologies, LLC
• Original Assignee: Pendar Technologies, LLC
• Inventors: Vakhshoori, Daryoosh, Blanchard, Romain, Mansuripur, Tobias
• Primary Examiner(s): Ayub, Hina F
• Application Number:
  US15/593,248
• Time in Patent Office: 481 Days
• Field of Search: 356 72
• CPC Class Codes: G01J 3/4338 Frequency modulated spectrometry
• CPC Class Codes: G01N 2021/451 for determining the optical absorption
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis
• CPC Class Codes: G01N 21/45 using interferometric methods; using Schlieren methods
• CPC Class Codes: G01N 2201/06113 Coherent sources; lasers
• CPC Class Codes: G01N 2201/0697 Pulsed lasers

Abstract

We present here systems and methods for generating a heterodyne signal using the naturally occurring chirp of a pulsed single-mode laser. The electrical square-wave pulse used to drive the laser heats the laser cavity, causing the laser frequency to change or chirp during the emission of the optical pulse. This chirped optical pulse can be split into a chirped signal pulse that interacts with a sample and a chirped reference pulse that interferes with the chirped signal pulse on a detector to produce a heterodyne modulation whose instantaneous phase and amplitude depend on the sample'"'"'s dispersion and absorption, respectively. The chirp is reproducible, so the heterodyne modulation, instantaneous phase, and/or instantaneous amplitude can be average over many measurements, either with multiple pulses from the same laser or multiple pulses from different lasers, each emitting at a different wavelength.

Claims

1. A method of making a spectroscopic measurement of a sample, the method comprising:

generating a chirped signal pulse with a single-mode laser in response to an electrical pulse;

illuminating the sample with the chirped signal pulse so as to cause the chirped signal pulse to interact with the sample;

detecting a heterodyne modulation caused by interference of the chirped signal pulse and a chirped reference pulse generated with the single-mode laser, the heterodyne modulation depending on a dispersion and/or an absorption of the sample; and

determining the dispersion and/or the absorption of the sample from the detected heterodyne modulation.

2. The method of claim 1, wherein the chirped signal pulse is chirped due to at least one of heating of the single-mode laser by the electrical pulse or a carrier density change of the single-mode laser by the electrical pulse.

3. The method of claim 1, wherein the single-mode laser is a distributed feedback (DFB) laser and generating the signal pulse comprises emitting a chirped optical pulse from the DFB laser having a pulse duration of about 10 nanoseconds to about 10 microseconds and a chirp rate ranging from about 0.2 wavenumbers per hundred nanoseconds to about 4 wavenumbers per hundred nanoseconds.

4. The method of claim 1, wherein generating the signal pulse comprises:

emitting a chirped optical pulse from the single-mode laser in response to the electrical pulse; and

splitting the chirped optical pulse into the chirped signal pulse and the chirped reference pulse.

5. The method of claim 1, wherein generating the chirped signal pulse comprises emitting the chirped signal pulse from the single-mode laser at a first time and the chirped reference pulse is emitted by the single-mode laser at a second time different than the first time.

6. The method of claim 1, further comprising:

estimating the dispersion of the sample based on the instantaneous phase.

7. The method of claim 1, further comprising:

estimating the absorption of the sample based on the instantaneous amplitude.

8. The method of claim 1, wherein the chirped signal pulse is a first chirped signal pulse, the electrical pulse is a first electrical pulse, the chirped reference pulse is a first chirped reference pulse, and the heterodyne modulation is a first heterodyne modulation, and further comprising:

generating a second chirped signal pulse with the single-mode laser in response to the second electrical pulse;

illuminating the sample with the second chirped signal pulse so as to cause the second chirped pulse to interact with the sample; and

detecting a second heterodyne modulation caused by interference of the second chirped signal pulse and a second chirped reference pulse generated with the single-mode laser, the second heterodyne modulation depending on the dispersion and/or the absorption of the sample.

9. The method of claim 8, further comprising:

averaging the first heterodyne modulation and the second heterodyne modulation.

10. The method of claim 8, further comprising:

dithering a phase of the second chirped reference pulse with respect to a phase of the first chirped reference pulse.

11. The method of claim 8, wherein the instantaneous frequency is a first instantaneous frequency and further comprising:

determining a second instantaneous phase of the second heterodyne modulation; and

averaging the first instantaneous phase and the second instantaneous phase.

12. The method of claim 8, wherein the instantaneous amplitude is a first instantaneous amplitude and further comprising:

determining a second instantaneous amplitude of the second heterodyne modulation; and

averaging the first instantaneous amplitude and the second instantaneous amplitude.

13. A system for making a spectroscopic measurement of a sample, the system comprising:

a single-mode laser, in optical communication with the sample, to generate a chirped signal pulse in response to an electrical pulse, the chirped signal pulse interacting with the sample; and

a photodetector, in optical communication with the sample, to detect a heterodyne modulation caused by interference of the chirped signal pulse and a chirped reference pulse generated with the single-mode laser, the heterodyne modulation being related to a dispersion and/or an absorption of the sample.

14. The system of claim 13, wherein the chirped signal pulse is chirped due to at least one of heating of the single-mode laser by the electrical pulse or a carrier density change of the single-mode laser by the electrical pulse.

15. The system of claim 13, wherein the single-mode laser is a distributed feedback (DFB) laser and the chirped signal pulse has a pulse duration of about 10 nanoseconds to about 10 microseconds and a chirp rate ranging from about 0.2 wavenumbers per hundred nanoseconds to about 4 wavenumbers per hundred nanoseconds.

16. The system of claim 13, wherein the signal-mode laser is configured to generate the chirped signal pulse at a first time and the chirped reference pulse at a second time different than the first time.

17. The system of claim 13, further comprising:

a beam splitter, in optical communication with the single-mode laser, to split a chirped optical pulse emitted by the single-mode laser into the chirped signal pulse and the chirped reference pulse.

18. The system of claim 13, further comprising:

circuitry, operably coupled to the photodetector, to determine an instantaneous phase and/or an instantaneous amplitude of the beat frequency.

19. The system of claim 18, wherein the circuitry is further configured to estimate a dispersion of the sample based on the instantaneous phase.

20. The system of claim 18, wherein the circuitry is further configured to estimate an absorption of the sample based on the instantaneous amplitude.

21. The system of claim 18, wherein:

the chirped signal pulse is a first chirped signal pulse,

the electrical pulse is a first electrical pulse,

the chirped reference pulse is a first chirped reference pulse,

the heterodyne modulation is a first heterodyne modulation,

the single-mode laser is configured to generate a second chirped signal pulse with the single-mode laser in response to the second electrical pulse, the second chirped signal pulse interacting with the sample; and

the photodetector is configured to detect a second heterodyne modulation caused by interference of the second chirped signal pulse and a second chirped reference pulse generated with the single-mode laser, the second heterodyne modulation depending on the dispersion and/or absorption of the sample.

22. The system of claim 21, wherein the circuitry is configured to average the first heterodyne modulation and the second heterodyne modulation.

23. The system of claim 21, wherein:

the instantaneous phase is a first instantaneous phase, and

the circuitry is configured to determine a second instantaneous phase of the second heterodyne modulation and to average the first instantaneous phase and the second instantaneous phase.

24. The system of claim 21, wherein:

the instantaneous amplitude is a first instantaneous amplitude, and

the circuitry is configured to determine a second instantaneous amplitude of the second heterodyne modulation and to average the first instantaneous amplitude and the second instantaneous amplitude.