“…These studies evidence the importance of selecting proper PCF excitation conditions (i.e., laser beam power, wavelength, and chirp) to achieve optimal SC spectral distribution and minimal noise , [14,[18][19][20][21] and therefore better performances for CARS measurements. [17,22] Numerical modelling [13,18,23] can be of help to this aim and has been actually used to simulate the SC generation, proving successful in reproducing the gross features of the experimental SC spectra and to evaluate optical noise, [24,25] even though detailed agreement with experimental data can be obtained at the expense of purposely introduced adjustments of the input parameters. [22] As far as noise and instabilities are concerned, it has been reported that noise in the SC spectra has two components [14,25] : the first, at high frequency, is related to the shot noise and has been widely investigated both theoretically and experimentally, [13,14,16,24,25] and a second, at low frequency, referred to as technical noise, which is due to amplification of the fluctuations of the input pulse characteristics.…”