CPC H01S 3/0092 (2013.01) [H01S 3/0057 (2013.01); H01S 3/0085 (2013.01); H01S 3/107 (2013.01); H01S 3/108 (2013.01); H01S 3/1106 (2013.01); H01S 3/1121 (2013.01); H01S 5/0085 (2013.01); A61B 6/484 (2013.01); G02F 1/3528 (2021.01); G21K 7/00 (2013.01); G21K 2207/005 (2013.01)] | 22 Claims |
1. Method of generating broad spectra ultra-high frequency spread spanning from Extreme UV (EUV) to far infrared (FIR) comprising the step of introducing high intensity I pump laser pulses 25 fs to 200 fs from 100 μJ to 50 mJ into a medium having third and fifth order components of electric susceptibility χ3 and χ5, respectively, and an average Kerr nonlinear index of refraction
≤n(t)>=n0+n2I+n4I2,
said pulses including ps varying approximation (SVA) following the envelope of a light field and n2I is a first order non-linear Kerr index of refraction related to χ3 and n4I2 is a second order non-linear Kerr index of refraction related to χ5 at laser pulse within the range of 1014˜1020 W/m2, where n2 is a non-linear Kerr index of refraction representing molecular movements that arises from ps response χ3 and n4 is a non-linear Kerr index of refraction representing electric field that arises from χ5 to produce ultra-supercontinuum (USC) light.
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