Methods and apparatus for swept-source optical coherence tomography
In one embodiment of the invention, a semiconductor optical amplifier (SOA) in a laser ring is chosen to provide low polarization-dependent gain (PDG) and a booster semiconductor optical amplifier, outside of the ring, is chosen to provide high polarization-dependent gain. The use of a semiconductor optical amplifier with low polarization-dependent gain nearly eliminates variations in the polarization state of the light at the output of the laser, but does not eliminate the intra-sweep variations in the polarization state at the output of the laser, which can degrade the performance of the SS-OCT system.
1. A clock generator for generating a clock signal from laser light, the clock generator comprising:
an interferometer having a dual optical output and an input, the interferometer receiving laser light at the input and the interferometer having an optical imbalance;
a first photodetector and a second photodetector, each photodetector in optical communication with a respective one of the dual optical outputs of the interferometer, and each photodetector having an output;
a multiplier having an output and having a first input in electrical communication with the output of the first photodetector and second input in electrical communication with the output of the second photodetector;
a zero-crossing detector having an electrical input in electrical communication with the output of the multiplier, the output of the zero-crossing detector being the generated clock signal.
2. The clock generator of claim 1 further comprising a first bandpass filter in electrical communication between the output of one photodetector and the first input of the multiplier and a second bandpass filter in electrical communication between the output the other photodetector and the second input of the multiplier.
3. The clock generator of claim 2 further comprising a frequency multiplier having an input in electrical communication with the output of the bandpass filter and having an output in electrical communication with the input of the zero-crossing detector.
4. The clock generator of claim 1 wherein the interferometer is a phase splitting interferometer and the optical outputs of the interferometer have equal intensity but are shifted by 90 degrees.
5. A method for generating a clock signal from laser light comprising the steps of:
receiving the laser light with an interferometer having a dual optical output, the interferometer having an optical imbalance;
detecting the received laser light with a pair of photodetectors, each photodetector in optical communication with a respective one of the dual optical outputs of the interferometer, and each photodetector having an output;
multiplying the output of the first photodetector and the output of second photodetector; and
detecting the zero-crossing of the result of multiplying the output of the first photodetector and the second photodetector, the result of the detection being the generated clock signal.
6. The clock generator of claim 1 wherein the multiplier multiplies a signal received from the first input by a signal received from the second input.
7. A clock generator for generating a clock signal from laser light, the clock generator comprising:
an interferometer having a dual optical output and an input, the interferometer receiving laser light at the input and the interferometer having an optical imbalance;
a first photodetector and a second photodetector, each photodetector in optical communication with a respective one of the dual optical outputs of the interferometer, and each photodetector having an output;
a multiplier having an output and having a first input in electrical communication with the output of the first photodetector and second input in electrical communication with the output of the second photodetector;
a zero-crossing detector having an electrical input in electrical communication with the output of the multiplier, the output of the zero-crossing detector being the generated clock signal;
a first bandpass filter in electrical communication between the output one photodetector and the first input of the multiplier; and
a second bandpass filter in electrical communication between the output the other photodetector and the second input of the multiplier.