Laser swept source with controlled mode locking for OCT medical imaging
View Patent ↗An optical coherence analysis system uses a laser swept source that is constrained to operate in a mode locked condition. This is accomplished by synchronously changing the laser cavity's gain and/or phase based on the round trip travel time of light in the cavity. Many high-speed wavelength swept laser sources emit pulses synchronized with the round trip time of the cavity as part of a nonlinear optical frequency red shifting process. Stable pulsation is associated with smooth tuning and low relative intensity noise. Addition of mode-locking methods to this class of lasers can control and stabilize these lasers to a low clock jitter and RIN state, and in specific cases allow long-to-short wavelength tuning in addition to the usual short-to-long (red shifting). The laser may comprise a SOA ( 410 ), a tunable Fabry-Perot-Filter ( 412 ) as one reflector and an Output coupler ( 405 ) in an optical fiber ( 406 ) to adjust the cavity length.
1. An optical coherence imaging method, comprising:
providing a laser swept source having a laser cavity that is less than a meter long and defined between a Fabry-Perot tunable filter and an output coupler at one end of a fiber;
controlling a swept mode-locked operation of the laser swept source by actively modulating cavity gain by applying a bias current to a gain element in the laser cavity, synchronized with a round trip time of the laser cavity to produce one laser pulse per round trip, and generating a swept optical signal by tuning the Fabry-Perot tunable filter with a tunable filter sweep rate that is several orders of magnitude smaller than a laser cavity round trip rate and the tunable filter sweep rate is greater than 20 kHz, and the laser cavity round trip rate is greater than 1 GHz;
transmitting the swept optical signal to an interferometer having a reference arm and a sample arm, in which a sample is located;
combining the swept optical signal returning from the sample arm and the reference arm to generate an interference signal;
detecting the interference signal; and
generating image information of the sample from the detected interference signal.
2. A method as claimed in claim 1 , wherein the laser swept source further comprises an intracavity phase modulator configured to be driven at a rate related to the round trip time of the laser cavity.
3. The method as claimed in claim 1 , wherein the bias current has one of: a square or a sinusoidal waveform.
4. An optical coherence imaging method, comprising:
providing a laser swept source having a laser cavity that is less than a meter long and defined between a Fabry-Perot tunable filter and an output coupler at one end of a fiber, the laser swept source further comprising a semiconductor optical amplifier (SOA) chip having a gain section, and an intracavity phase modulator configured to be driven at a rate related to the round trip time of the laser cavity, wherein the phase modulator is integral with the SOA chip and configured to be driven at a harmonic of the round trip frequency of the laser cavity by a bias source different from a bias source for the gain section;
controlling a swept mode-locked operation of the laser swept source by actively modulating cavity gain by applying a bias current to the gain section synchronized with a round trip time of the laser cavity to produce one laser pulse per round trip, and generating a swept optical signal;
transmitting the swept optical signal to an interferometer having a reference arm and a sample arm, in which a sample is located;
combining the swept optical signal returning from the sample arm and the reference arm to generate an interference signal;
detecting the interference signal; and
generating image information of the sample from the detected interference signal.