“…By applying a current ramp (10-100 Hz sawtooth) to a narrowwavelength laser, an optical beam is repeatedly wavelength-scanned across a previously measured absorption feature [2,3,29,30]. For WMS, a secondary 10-500 kHz sinusoidal dither is applied [31] allowing phase sensitive detection [32] and digital lock-in amplification (DLIA) [19,20,21,22]. The gas parameters [2,3,11,29,30,33] and ultimately the path concentration integral (PCI) of the target gas along the beam [3,7,8,25], can be inferred by using a spectroscopic curve-fitting model based upon the Beer-Lambert law and the known properties of the gas.…”