• Chinese Optics Letters
  • Vol. 14, Issue 5, 051402 (2016)
Qiang Zhou*, Rong Qiu, Yong Jiang, Xiang Gao, Yongjia Yang, Huili Wang, and Huan Ren
Author Affiliations
  • Joint Laboratory for Extreme Conditions Matter Properties, Southwest University of Science and Technology, Mianyang 621010, China
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    DOI: 10.3788/COL201614.051402 Cite this Article Set citation alerts
    Qiang Zhou, Rong Qiu, Yong Jiang, Xiang Gao, Yongjia Yang, Huili Wang, Huan Ren. Ultra-fast diagnosis of shock waves and plasma at front and rear surfaces in the bulk of fused silica induced by an Nd:YAG pulse laser[J]. Chinese Optics Letters, 2016, 14(5): 051402 Copy Citation Text show less
    Experimental setup.
    Fig. 1. Experimental setup.
    Time-resolved images of shock waves generated by 1064 and 532 nm pulse lasers at fused silica’s front surface with fluences of 27.6 and 15.7 J/cm2, respectively.
    Fig. 2. Time-resolved images of shock waves generated by 1064 and 532 nm pulse lasers at fused silica’s front surface with fluences of 27.6 and 15.7J/cm2, respectively.
    Time-resolved images of 532 nm pulse laser ablation in the bulk of fused silica with fluence of 12.8 J/cm2.
    Fig. 3. Time-resolved images of 532 nm pulse laser ablation in the bulk of fused silica with fluence of 12.8J/cm2.
    Shock wave expansion distance as a function of delay time.
    Fig. 4. Shock wave expansion distance as a function of delay time.
    Time-resolved images of plasma and shock waves induced by 532 and 1064 nm pulse laser ablation fused silica at rear surface with fluences of 12.4 and 20 J/cm2.
    Fig. 5. Time-resolved images of plasma and shock waves induced by 532 and 1064 nm pulse laser ablation fused silica at rear surface with fluences of 12.4 and 20J/cm2.
    Shock wave expansion distance as a function of delay time.
    Fig. 6. Shock wave expansion distance as a function of delay time.
    Time-resolved images of laser ablation fused silica rear surface by using 532 nm laser with fluence of 16.8 J/cm2. The features labeled in the figures are shock wave front S, the ionization area I, contact front D, ejected material E, thermal elastic wave A, and mechanical shock wave B.
    Fig. 7. Time-resolved images of laser ablation fused silica rear surface by using 532 nm laser with fluence of 16.8J/cm2. The features labeled in the figures are shock wave front S, the ionization area I, contact front D, ejected material E, thermal elastic wave A, and mechanical shock wave B.
    Calculated shock wave properties in fused silica as a function of the shock wave velocity D.
    Fig. 8. Calculated shock wave properties in fused silica as a function of the shock wave velocity D.
     cv(Jkg1K1)c0 (kms1)Density ρ (gcm3)Gruneisen parameter γ0λ
    Fused silica4151.892.2040.021.392
    Table 1. Hugoniot Parameters of Fused Silica Used Here
    Qiang Zhou, Rong Qiu, Yong Jiang, Xiang Gao, Yongjia Yang, Huili Wang, Huan Ren. Ultra-fast diagnosis of shock waves and plasma at front and rear surfaces in the bulk of fused silica induced by an Nd:YAG pulse laser[J]. Chinese Optics Letters, 2016, 14(5): 051402
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