“…Numerically we have investigated the properties of the combination components 3ω ± 2∆ω, the results are shown on Figure 3 (the spectral density near the third harmonic for pulses with two different values of ∆ω) and Figure 4 (the dependence of intensities of 3ω ± 2∆ω on the intensity of one of the components with fixed intensities of two other in a three-color pulse and ∆ω = 0.07ω). Expression (15) does not correctly describe the entire form of the dependence of dj 3ω+2∆ω /dt on µ 1,2 , since to do this, it is necessary to take into account all the significant higher orders of the IMWM. However, already from it one can see some properties of the generation of a given combination frequency, such as linearity in both amplitudes at low values, and a slight asymmetry: if we put µ 1 = µ 2 and change the sign of ∆ω, we see that when the intensities of both additional components are equal, the low-frequency satellite of the third harmonic should have a slightly larger amplitude, which is confirmed by both semiclassical and quantum mechanical calculations.…”