• Acta Photonica Sinica
  • Vol. 49, Issue 11, 59 (2020)
Hua-bao CAO1, Hu-shan WANG1, Hao YUAN1、2, Xin LIU1、2, Pei HUANG1, Yi-shan WANG1、*, Wei ZHAO1, and Yu-xi FU1
Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Institute of Optics and Precision Mechanics of CAS, Xi'an709, China
  • 2University of Chinese Academy of Sciences, Beijing100049, China
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    DOI: 10.3788/gzxb20204911.1149005 Cite this Article
    Hua-bao CAO, Hu-shan WANG, Hao YUAN, Xin LIU, Pei HUANG, Yi-shan WANG, Wei ZHAO, Yu-xi FU. Research Progress of Mid-infrared Femtosecond Sources Based on Optical Parametric Amplification (Invited)[J]. Acta Photonica Sinica, 2020, 49(11): 59 Copy Citation Text show less
    The principle of OPA, OPCPA and DC-OPA
    Fig. 1. The principle of OPA, OPCPA and DC-OPA
    Schematic of an optical parametric amplifier
    Fig. 2. Schematic of an optical parametric amplifier
    Collinear and non-collinear phase-matching geometries
    Fig. 3. Collinear and non-collinear phase-matching geometries
    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. 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]
    A typical seed generation scheme
    Fig. 5. A typical seed generation scheme
    Spectral range of the supercontinuum generated in various material while driven by light of different wavelengths[25]
    Fig. 6. Spectral range of the supercontinuum generated in various material while driven by light of different wavelengths[25]
    Reflectance and GDD of the complementary chirped mirror pair in the wavelength of 2~4 μm[26]
    Fig. 7. Reflectance and GDD of the complementary chirped mirror pair in the wavelength of 2~4 μm[26]
    Measured reflectance, transmittance, absorption and GDD curves of the chirped mirror[27]. Reprinted with permission from Ref.[27] ©The Optical Society
    Fig. 8. Measured reflectance, transmittance, absorption and GDD curves of the chirped mirror[27]. Reprinted with permission from Ref.[27] ©The Optical Society
    Transmittances and GVD of several typical materials for dispersion management
    Fig. 9. Transmittances and GVD of several typical materials for dispersion management
    Transmittance of the liquid-crystal in the SLM and the setup of the SLM based pulse shaper[30]
    Fig. 10. Transmittance of the liquid-crystal in the SLM and the setup of the SLM based pulse shaper[30]
    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. 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
    Schematic of DC-OPA with peak power of 0.3 TW[40]
    Fig. 12. Schematic of DC-OPA with peak power of 0.3 TW[40]
    Schematic of the mid-infrared source with average power of 15.1 W[46]
    Fig. 13. Schematic of the mid-infrared source with average power of 15.1 W[46]
    9 μm femtosecond mid-infrared source based on LiGaS2[52]. Reprinted with permission from Ref.[52] ©The Optical Society
    Fig. 14. 9 μm femtosecond mid-infrared source based on LiGaS2[52]. Reprinted with permission from Ref.[52] ©The Optical Society
    7 μm femtosecond mid-infrared source with pulse energy of millijoule level[59]. Reprinted with permission from Ref.[59] ©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
    Proof-of-principle schematic setup of the 4~12 μm mid-Infrared source[60]
    Fig. 16. Proof-of-principle schematic setup of the 4~12 μm mid-Infrared source[60]
    Layout of the Ho:YAG thin-disk laser
    Fig. 17. Layout of the Ho:YAG thin-disk laser
    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. 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]
    Schematic of the wavelength tunable optical vortex OPA system[65]. Reprinted with permission from Ref.[65] ©The Optical Society
    Fig. 19. Schematic of the wavelength tunable optical vortex OPA system[65]. Reprinted with permission from Ref.[65] ©The Optical Society
    Schematic of the 4 μm optical vortex OPCPA system[66]
    Fig. 20. Schematic of the 4 μm optical vortex OPCPA system[66]
    Spectra of the optical vortex beam measured at four different quadrants[66]
    Fig. 21. Spectra of the optical vortex beam measured at four different quadrants[66]
    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
    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 crystalsTransmission range/μmBand gap/V

    Effective nonlinear coefficient

    /(pm·V-1

    Damage threshold@

    10 ns/(GW·cm-2

    LiNbO30.42~5.2 [20]/d33=34.4, d31=d15=5.95, d22=3.07[20]0.2 (1.06 μm)[20]
    KNbO30.40~5.5[21]/d31= -15.8, d32=-18.3[21]0.24 (1.06 μm)[21]
    KTiOAsO40.35~5.5[22]/d31=2.76, d32=4.74, d33=18.5[22]0.5 (1.06 μm)[23]
    KTiOPO40.35~4.5[22]/d31=2.0, d32=3.6[22]0.5 (1.06 μm)[23]
    AgGaS20.47~13[22]2.73[22]d36=12.6[22]0.014 (1.06 μm)[23]
    AgGaSe20.76~18[22]1.8[22]d36=39.5[22]0.056 (2.05 μm)[23]
    LiGaS20.32~11.6[22]4.1[22]d31=5.8, d24=5.1, d33=-10.7[22]1.0 (1.06 μm)[22]
    ZnGeP20.74~12[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
    MaterialsBand gap/eVTransmission range/μmn2/(×10-16cm2·W-1)n0λ0/μm
    LiF13.60.12~6.60.811.391.23
    CaF2100.12~101.31.431.55
    Al2O39.90.19~5.23.11.761.31
    SiO29.00.18~3.52.41.451.27
    YAG6.50.21~5.26.21.821.60
    Table 2. Parameters of frequently used materials for supercontinuum generation[25]
    Hua-bao CAO, Hu-shan WANG, Hao YUAN, Xin LIU, Pei HUANG, Yi-shan WANG, Wei ZHAO, Yu-xi FU. Research Progress of Mid-infrared Femtosecond Sources Based on Optical Parametric Amplification (Invited)[J]. Acta Photonica Sinica, 2020, 49(11): 59
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