Fig. 1. The principle of OPA, OPCPA and DC-OPA
Fig. 2. Schematic of an optical parametric amplifier
Fig. 3. Collinear and non-collinear phase-matching geometries
Fig. 4. Calculated gain spectrum of a 3 mm BBO under the type-I phase-matching condition, and the calculated gain spectrum at the pump wavelength of 708 nm with different phase-matching angle
[19] Fig. 5. A typical seed generation scheme
Fig. 6. Spectral range of the supercontinuum generated in various material while driven by light of different wavelengths
[25] Fig. 7. Reflectance and GDD of the complementary chirped mirror pair in the wavelength of 2~4 μm
[26] Fig. 8. Measured reflectance, transmittance, absorption and GDD curves of the chirped mirror
[27]. Reprinted with permission from Ref.[
27] ©The Optical Society
Fig. 9. Transmittances and GVD of several typical materials for dispersion management
Fig. 10. Transmittance of the liquid-crystal in the SLM and the setup of the SLM based pulse shaper
[30] Fig. 11. Some typical reports on the performance of mid-infrared femtosecond sources based on optical parametrical amplification technique driven by pumps of different wavelength in recent years
Fig. 12. Schematic of DC-OPA with peak power of 0.3 TW
[40] Fig. 13. Schematic of the mid-infrared source with average power of 15.1 W
[46] Fig. 14. 9 μm femtosecond mid-infrared source based on LiGaS
2[52]. Reprinted with permission from Ref.[
52] ©The Optical Society
Fig. 15. 7 μm femtosecond mid-infrared source with pulse energy of millijoule level
[59]. Reprinted with permission from Ref.[
59] ©The Optical Society
Fig. 16. Proof-of-principle schematic setup of the 4~12 μm mid-Infrared source
[60] Fig. 17. Layout of the Ho:YAG thin-disk laser
Fig. 18. Thermal imaging of BBO crystal pumped with optical power of 120 W at 515 nm and the photograph of the BBO-sapphire sandwich structure
[63-64] Fig. 19. Schematic of the wavelength tunable optical vortex OPA system
[65]. Reprinted with permission from Ref.[
65] ©The Optical Society
Fig. 20. Schematic of the 4 μm optical vortex OPCPA system
[66] Fig. 21. Spectra of the optical vortex beam measured at four different quadrants
[66] Fig. 22. Schematic of the experimental setup for second harmonic generation of radially polarized beam with two nonlinear crystals
[67]. Reprinted with permission from Ref.[
67] ©The Optical Society
Nonlinear crystals | Transmission range/μm | Band gap/V | Effective nonlinear coefficient /(pm·V-1) | Damage threshold@ 10 ns/(GW·cm-2) |
---|
LiNbO3 | 0.42~5.2 [20] | / | d33=34.4, d31=d15=5.95, d22=3.07[20] | 0.2 (1.06 μm)[20] | KNbO3 | 0.40~5.5[21] | / | d31= -15.8, d32=-18.3[21] | 0.24 (1.06 μm)[21] | KTiOAsO4 | 0.35~5.5[22] | / | d31=2.76, d32=4.74, d33=18.5[22] | 0.5 (1.06 μm)[23] | KTiOPO4 | 0.35~4.5[22] | / | d31=2.0, d32=3.6[22] | 0.5 (1.06 μm)[23] | AgGaS2 | 0.47~13[22] | 2.73[22] | d36=12.6[22] | 0.014 (1.06 μm)[23] | AgGaSe2 | 0.76~18[22] | 1.8[22] | d36=39.5[22] | 0.056 (2.05 μm)[23] | LiGaS2 | 0.32~11.6[22] | 4.1[22] | d31=5.8, d24=5.1, d33=-10.7[22] | 1.0 (1.06 μm)[22] | ZnGeP2 | 0.74~12[22] | 2.1[22] | d36=75±8[22] | 0.18 (10.6 μm)[23] |
|
Table 1. Parameters of the frequently employed nonlinear crystals in mid-infrared range
Materials | Band gap/eV | Transmission range/μm | n2/(×10-16cm2·W-1) | n0 | λ0/μm |
---|
LiF | 13.6 | 0.12~6.6 | 0.81 | 1.39 | 1.23 | CaF2 | 10 | 0.12~10 | 1.3 | 1.43 | 1.55 | Al2O3 | 9.9 | 0.19~5.2 | 3.1 | 1.76 | 1.31 | SiO2 | 9.0 | 0.18~3.5 | 2.4 | 1.45 | 1.27 | YAG | 6.5 | 0.21~5.2 | 6.2 | 1.82 | 1.60 |
|
Table 2. Parameters of frequently used materials for supercontinuum generation
[25]