• Laser & Optoelectronics Progress
  • Vol. 55, Issue 6, 061903 (2018)
Dan Jin1; , Linghui Jin1; , and Cheng Gong2*; *;
Author Affiliations
  • City College, Wuhan University of Science and Technology, Wuhan, Hubei 430083, China
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    DOI: 10.3788/LOP55.061903 Cite this Article Set citation alerts
    Dan Jin, Linghui Jin, Cheng Gong. Influence of Material Dispersion on Output Characteristics of Cross-Polarized Wave[J]. Laser & Optoelectronics Progress, 2018, 55(6): 061903 Copy Citation Text show less
    XPW conversion efficiency versus peak intensity of laser pulses. (a) τ=100 fs, β=22.5°; (b) τ=30 fs, β=22.5°
    Fig. 1. XPW conversion efficiency versus peak intensity of laser pulses. (a) τ=100 fs, β=22.5°; (b) τ=30 fs, β=22.5°
    XPW conversion efficiency versus angle β. (a) τ=100 fs, I=0.2×1012 W·cm-2; (b) τ=100 fs, I=0.8×1012 W·cm-2; (c) τ=30 fs, I=0.2×1012 W·cm-2; (d) τ=30 fs, I=0.8×1012 W·cm-2
    Fig. 2. XPW conversion efficiency versus angle β. (a) τ=100 fs, I=0.2×1012 W·cm-2; (b) τ=100 fs, I=0.8×1012 W·cm-2; (c) τ=30 fs, I=0.2×1012 W·cm-2; (d) τ=30 fs, I=0.8×1012 W·cm-2
    Pulse widths of XPW generated from input pulses with different widths. (a) τ=100 fs; (b) corresponding spectra shown in Fig.3 (a); (c) τ=30 fs; (d) corresponding spectra shown in Fig.3 (c)
    Fig. 3. Pulse widths of XPW generated from input pulses with different widths. (a) τ=100 fs; (b) corresponding spectra shown in Fig.3 (a); (c) τ=30 fs; (d) corresponding spectra shown in Fig.3 (c)
    Dan Jin, Linghui Jin, Cheng Gong. Influence of Material Dispersion on Output Characteristics of Cross-Polarized Wave[J]. Laser & Optoelectronics Progress, 2018, 55(6): 061903
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