“…Nevertheless, it can be shown, that the length scales on which specific orders act can be estimated by |L P (3) /L P (5) | ≃ |P (5) /P (3) | ≃ |E/E at | 2 where E is the laser field and E at = 5×10 10 V/m [16]. We used field strengths E ≃ 0.4 × 10 9 V/m, giving |L P (3) /L P (5) | ≃ 2 × 10 −4 , so P (5) is negligible. Furthermore, the pulses launched at ω 00 do have a spectral width, thus experiencing, e.g., a n 2 ≈ 2.7 × 10 −23 m 2 /W at the halfmaximum frequency due to dispersion of the nonlinearity, which is already comparable to usual values of n 2 ∼ 1.0 × 10 −23 m 2 /W.…”