“…Likewise, to calculate the response function of LPS (Figure 4b), we modeled the interaction of a VIS-UV few-cycle intense pulse and a NIR infrared drive pulse in GaP using the method described in ref. [36]. To this end, we solved the 3D time-dependent Schrödinger equation in the stationary basis of Kohn-Sham orbitals.…”
Section: Resultsmentioning
confidence: 99%
“…In order to derive the criteria for linear injection, the VIS-UV induced charge density was calculated in GaP as a function of peak field strengths of the laser using the method described in ref. [36]. The dependence of the computed charge density on the peak electric field was compared with a polynomial scaling characteristic of both single and multi-photon absorption.…”
Figure 4. a) EOS (in red) and b) LPS (in blue) spectral response functions calculated with different GDD values applied to the VIS-UV pulse. c) EOS response calculated for a compressed VIS-UV pulse and different crystal thicknesses.
“…Likewise, to calculate the response function of LPS (Figure 4b), we modeled the interaction of a VIS-UV few-cycle intense pulse and a NIR infrared drive pulse in GaP using the method described in ref. [36]. To this end, we solved the 3D time-dependent Schrödinger equation in the stationary basis of Kohn-Sham orbitals.…”
Section: Resultsmentioning
confidence: 99%
“…In order to derive the criteria for linear injection, the VIS-UV induced charge density was calculated in GaP as a function of peak field strengths of the laser using the method described in ref. [36]. The dependence of the computed charge density on the peak electric field was compared with a polynomial scaling characteristic of both single and multi-photon absorption.…”
Figure 4. a) EOS (in red) and b) LPS (in blue) spectral response functions calculated with different GDD values applied to the VIS-UV pulse. c) EOS response calculated for a compressed VIS-UV pulse and different crystal thicknesses.
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