Mode hopping swept frequency laser for FD OCT and method of operation
View Patent ↗A frequency swept laser source that generates an optical signal that is tuned over a spectral scan band at single discrete wavelengths associated with longitudinal modes of the swept laser source. Laser hopping over discrete single cavity modes allows long laser coherence length even under dynamic very high speed tuning conditions. A ramp drive to the laser is used to linearize laser frequency tuning. A beam splitter is used to divide the optical signal between a reference arm leading to a reference reflector and a sample arm leading to a sample. A detector system detects the optical signal from the reference arm and the sample arm for generating depth profiles and images of the sample.
1. An optical coherence analysis system comprising:
a swept laser source that generates an optical signal that is tuned over a spectral scan band, the laser emitting one wavelength mode at a time and tuning discretely over wavelengths associated with longitudinal modes of the swept laser source;
a beam splitter for dividing the optical signal between a reference arm leading to a reference reflector and a sample arm leading to a sample; and
a detector system for detecting the optical signal from the reference arm and the sample arm.
2. An optical coherence analysis system as claimed in claim 1 , wherein the swept laser source comprises:
a laser cavity having at least two reflectors, which define the longitudinal cavity modes;
a semiconductor gain medium in the laser cavity; and
a tuning element for the laser cavity.
3. An optical coherence analysis system as claimed in claim 2 , wherein the tuning element provides a tunable pass band that restricts the swept laser source to lasing at the single discrete ones of the longitudinal modes.
4. An optical coherence analysis system as claimed in claim 3 , wherein the tuning element comprises a Fabry-Perot tunable filter.
5. An optical coherence analysis system as claimed in claim 3 , wherein the tuning element comprises an angled reflective Fabry-Perot tunable filter.
6. An optical coherence analysis system as claimed in claim 3 , wherein the tuning element comprises a MEMS Fabry-Perot tunable filter.
7. An optical coherence analysis system as claimed in claim 3 , wherein the tuning element comprises a MEMS angled reflective Fabry-Perot tunable filter.
8. An optical coherence analysis system as claimed in claim 2 , further comprising a phase compensation medium in the laser cavity for compensating for dispersion effects over the spectral scan band.
9. An optical coherence analysis system as claimed in claim 8 , wherein phase compensation medium is semiconductor medium.
10. An optical coherence analysis system as claimed in claim 8 , wherein phase compensation medium is an electro-optic medium.
11. An optical coherence analysis system as claimed in claim 8 , wherein phase compensation semiconductor medium is integral with the semiconductor gain medium.
12. An optical coherence analysis system as claimed in claim 2 , wherein one of the reflectors is integral with the semiconductor gain medium.
13. An optical coherence analysis system as claimed in claim 2 , wherein one of the reflectors is integral with tuning element.
14. An optical coherence analysis system as claimed in claim 2 , wherein a bandwidth of the tuning element and spacing between the longitudinal modes enables only individual ones of the longitudinal modes to lase as the optical signal is tuned over the spectral scan band.
15. An optical coherence analysis system as claimed in claim 2 , wherein the optical signal is taken from the laser cavity through the tuning element.
16. An optical coherence analysis system as claimed in claim 2 , wherein the optical signal is taken from the laser cavity through the semiconductor gain medium.
17. An optical coherence analysis system as claimed in claim 1 , wherein longitudinal mode spacing of the longitudinal modes is greater than 4 GHz.
18. An optical coherence analysis system as claimed in claim 1 , wherein longitudinal mode spacing of the longitudinal modes is between 5 GHz and 15 GHz.
19. An optical coherence analysis system as claimed in claim 1 , wherein a coherence length of the optical signal is greater than 10 mm at a tuning rate of greater than 25 kHz.
20. An optical coherence analysis system as claimed in claim 1 , further comprising:
an image processing system for controlling the swept laser source and constructing an image from a response of the detector system; and
a trigger system for monitoring a magnitude of the optical signal detected by the detector system and signaling the image processing system to sample the response of the detector system.
21. An optical coherence analysis system as claimed in claim 1 , further comprising an image processing system for resampling data from the detector system for the discrete wavelengths to equally spaced optical frequencies.
22. An optical coherence analysis system as claimed in claim 1 , wherein the beam splitter is a fiber coupler.
23. An optical coherence analysis system as claimed in claim 1 , wherein the beam splitter combines the optical signal from the reference arm and optical signal from the signal arm prior to detection by the detector system.
24. An optical coherence analysis method comprising generating an optical signal that is tuned over a spectral scan band at discrete wavelengths by generating the discrete wavelengths at longitudinal modes of a laser cavity comprising a semiconductor gain medium and a tuning element for the laser cavity that restricts lasing of the laser cavity to only discrete ones of the longitudinal modes;
dividing the optical signal between a reference arm leading to a reference reflector and a sample arm leading to a sample; and
detecting the optical signal from the reference arm and the sample arm.
25. An optical coherence analysis method as claimed in claim 24 , further compensating for dispersion effects over the spectral scan band.
26. An optical coherence analysis method as claimed in claim 24 , wherein the tuning element comprises a Fabry-Perot tunable filter.
27. An optical coherence analysis method as claimed in claim 24 , wherein the tuning element comprises a MEMS Fabry-Perot tunable filter.
28. An optical coherence analysis method as claimed in claim 24 , further comprising configuring a bandwidth of the tuning element and spacing between longitudinal modes to enable only individual ones of the longitudinal modes to lase as the optical signal is tuned over the spectral scan band.
29. An optical coherence analysis method as claimed in claim 24 , further comprising taking the optical signal from the laser cavity through the tuning element.
30. An optical coherence analysis method as claimed in claim 24 , further comprising taking the optical signal from the laser cavity through the semiconductor gain medium.
31. An optical coherence analysis method as claimed in claim 24 , wherein longitudinal mode spacing is greater than 4 GHz.
32. An optical coherence analysis method as claimed in claim 24 , wherein longitudinal mode spacing is between 5 GHz and 15 GHz.
33. An optical coherence analysis method as claimed in claim 24 , wherein a coherence length of the optical signal is greater than 10 mm at a tuning rate of greater than 25 kHz.
34. An optical coherence analysis method as claimed in claim 24 , further comprising:
controlling the tuning of the optical signal and constructing an image from a detection of the optical signal; and
monitoring a magnitude of the optical signal and controlling sampling of the optical signal in response to the monitored magnitude.
35. An optical coherence analysis method as claimed in claim 24 , further comprising resampling data from detection of the optical signal for the discrete wavelengths to equally spaced optical frequencies.