• Laser & Optoelectronics Progress
  • Vol. 57, Issue 21, 210001 (2020)
Liu Kefei1、2, Zhong Kai1、2、*, and Yao Jianquan1、2
Author Affiliations
  • 1天津大学精密仪器与光电子工程学院激光与光电子研究所, 天津 300072
  • 2天津大学光电信息技术教育部重点实验室, 天津 300072
  • show less
    DOI: 10.3788/LOP57.210001 Cite this Article Set citation alerts
    Liu Kefei, Zhong Kai, Yao Jianquan. Research Progress on Random Quasi-Phase Matching in Polycrystalline Materials[J]. Laser & Optoelectronics Progress, 2020, 57(21): 210001 Copy Citation Text show less
    Schematic of one-dimensional aperiodic materials. (a) Chirped crystal; (b) quasi-periodic crystal
    Fig. 1. Schematic of one-dimensional aperiodic materials. (a) Chirped crystal; (b) quasi-periodic crystal
    SHG in two-dimensional random SBN material. (a) Schematic; (b) experimental photograph (arrow indicates direction of fundamental beam)[20]
    Fig. 2. SHG in two-dimensional random SBN material. (a) Schematic; (b) experimental photograph (arrow indicates direction of fundamental beam)[20]
    Spectral broadening of incident femtosecond pulse at 2.4 μm central wavelength in 5-mm-long polycrystalline ZnSe via RQPM frequency mixing[26]
    Fig. 3. Spectral broadening of incident femtosecond pulse at 2.4 μm central wavelength in 5-mm-long polycrystalline ZnSe via RQPM frequency mixing[26]
    Harmonic and supercontinuum generation in polycrystalline Cr∶ZnS femtosecond laser. (a) 1st to 4th harmonic of fundamental beam; (b) supercontinuum spanning from 1.8 μm to 4.5 μm[28]
    Fig. 4. Harmonic and supercontinuum generation in polycrystalline Cr∶ZnS femtosecond laser. (a) 1st to 4th harmonic of fundamental beam; (b) supercontinuum spanning from 1.8 μm to 4.5 μm[28]
    OPO based on polycrystalline ZnSe. (a)Schematic of device with photo of ZnSe placed at the Brewster angle shown in bottom right; (b) broadband output spectrum spanning from 3 μm to 7.5 μm; (c) cavity length detuning[10]
    Fig. 5. OPO based on polycrystalline ZnSe. (a)Schematic of device with photo of ZnSe placed at the Brewster angle shown in bottom right; (b) broadband output spectrum spanning from 3 μm to 7.5 μm; (c) cavity length detuning[10]
    Schematic of laser beam with certain cross section passing through polycrystalline material. (a) Main view; (b) side view
    Fig. 6. Schematic of laser beam with certain cross section passing through polycrystalline material. (a) Main view; (b) side view
    Schematic of random rotation transformation between reference coordinate and crystal coordinate[38]
    Fig. 7. Schematic of random rotation transformation between reference coordinate and crystal coordinate[38]
    Effective nonlinear coefficient distribution of crystal grains after random rotation of one million times. (a) SHG with polarization parallel to that of fundamental beam; (b) SHG with polarization perpendicular to that of fundamental beam[10]
    Fig. 8. Effective nonlinear coefficient distribution of crystal grains after random rotation of one million times. (a) SHG with polarization parallel to that of fundamental beam; (b) SHG with polarization perpendicular to that of fundamental beam[10]
    Statistical result of SHG power of polycrystalline nSe with different lengths[10]
    Fig. 9. Statistical result of SHG power of polycrystalline nSe with different lengths[10]
    Grain-size distributions of ZnSe under different treatment methods. (a) Original CVD ZnSe; (b) treatment in 850 ℃ Se vapor for 12 h; (c) treatment in 850 ℃ Zn vapor for 168 h; (c) treatment in 850 ℃ vacuum for 168 h[42]
    Fig. 10. Grain-size distributions of ZnSe under different treatment methods. (a) Original CVD ZnSe; (b) treatment in 850 ℃ Se vapor for 12 h; (c) treatment in 850 ℃ Zn vapor for 168 h; (c) treatment in 850 ℃ vacuum for 168 h[42]
    (Left) Polycrystalline material generated by Neper and (right) its meshed morphology
    Fig. 11. (Left) Polycrystalline material generated by Neper and (right) its meshed morphology
    Statistical properties of grains generated by Neper software. (a) Grain size; (b) sphericity
    Fig. 12. Statistical properties of grains generated by Neper software. (a) Grain size; (b) sphericity
    Liu Kefei, Zhong Kai, Yao Jianquan. Research Progress on Random Quasi-Phase Matching in Polycrystalline Materials[J]. Laser & Optoelectronics Progress, 2020, 57(21): 210001
    Download Citation