> You basically have a very fast laser that
> can do volumetric scans at a high framerate,
> did I get this right?
Now the challenge is to get the wavelength spectrum. You can either use a broadband CW light source and a spectrometer. But these are slow, so you can't generate depth scans at more than about 30kHz (which is too slow for 3D but suffices for 2D imaging). Or you can encode the wavelength in time and use a very fast photodetector (those go up to well over 4GHz bandwidth).
This is what we do: Have a laser that sweeps over 100nm at a rate >1.5MHz and use a very fast digitizer (1.8GS/s) to obtain a interference spectrum with over 1k sampling points. Then apply a little bit of DSP (mapping time to wavelength, resampling, windowing, iFFT, dynamic range compression) and you get a volume dataset.
BTW, all the GPU OCT processing and visualization code I wrote, too.
> What do people typically use it for?
Frequency-sweeping... How are you doing that? Is the laser itself able to frequency sweep? Or are you chirping pulses?
> Frequency-sweeping... How are you doing that?
A much more thorough description is found in the paper that introduced FDML for the first time:
> Is the laser itself able to frequency sweep?
> Or are you chirping pulses?
What you're doing sounds a lot like time-domain spectroscopy in an odd sort of way.
What are the advantages of this versus just chirping a pulsed supercontinuum source?
> What you're doing sounds a lot like time-domain
> spectroscopy in an odd sort of way.
> What are the advantages of this versus just
> chirping a pulsed supercontinuum source?
Sweep uniformity: The phase evolution of the sweeps is very stable; the mean deviation in phase differences between sweeps is in the order of millirad. Which means that for the time→k-space mapping the phase evolution has to be determined only one time and can then be used for hours of operation; in fact the system operates to repeatable that even after being powered off over the night, the next morning you can often reuse the phase calibration of the previous day. Without that, you'd have to use a second interferometer and sample a k-space reference signal for each and every sweep in parallel and use that for k-space remapping.
Ease of synchronization: Trigger signals have very small jitter. Also the jitter between electrical and optical synchronization is in the order of few ps, which is important for things like Doppler-OCT.
Coherence: Supercontinuum Sources have issues with coherence stability, which degrades the imaging range.
Sentisivity issued: Chirping Pulsed Supercontinuum Sources (which are actually used for OCT) is challenging. It requires a lot of dispersion. High dispersion means a lot of loss, which in turn means it requires another output amplification stage, which in turn will also produce significant optical noise. And optical noise is the bane of OCT, since that reduces the sensitivity. In contrast to that if properly dispersion compensated an FDML laser will exhibit very little noise.
Price: Pulsed Supercontinuum Sources suitable for chirping and OCT applications are quite expensive. Our laser is not cheap as well, but it's still more price effective.