Mid-infrared supercontinuum generation and its application on all-optical quantization with different input pulses
Spectra obtained with different pumping powers (T0 = 100 fs). The input pulses of panels (a), (d), (g), and (j) are parabolic pulses. The input pulses of panels (b), (e), (h), and (k) are hyperbolic-secant pulses. The input pulses of panels (c), (f), (i), and (l) are Gaussian pulses. L = 1.5 cm.
