• Chinese Optics Letters
  • Vol. 17, Issue 10, 101402 (2019)
Yangliang Li1, Chao Shen2,*, Li Shao1, and Yujun Zhang1,**
Author Affiliations
  • 1State Key Laboratory of Pulsed Power Laser Technology, National University of Defense Technology, Hefei 230037, China
  • 2Key Laboratory of Environmental Optics & Technology, Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei 230031, China
  • show less
    DOI: 10.3788/COL201917.101402 Cite this Article Set citation alerts
    Yangliang Li, Chao Shen, Li Shao, Yujun Zhang, "Dynamic image acquisition and particle recognition of laser-induced exit surface particle ejection in fused silica," Chin. Opt. Lett. 17, 101402 (2019) Copy Citation Text show less

    Abstract

    Particle ejection is an important process during laser-induced exit surface damage in fused silica. Huge quantities of ejected particles, large ejection velocity, and long ejection duration make this phenomenon difficult to be directly observed. An in situ two-frame shadowgraphy system combined with a digital particle recognition algorithm was employed to capture the transient ejecting images and obtain the particle parameters. The experimental system is based on the principle of polarization splitting and can capture two images at each damage event. By combining multiple similar damage events at different time delays, the timeline of ejecting evolution can be obtained. Particle recognition is achieved by an adaptively regularized kernel-based fuzzy C-means algorithm based on a grey wolf optimizer. This algorithm overcomes the shortcoming of the adaptively regularized kernel-based fuzzy C-means algorithm easily falling into the local optimum and can resist strong image noises, including diffraction pattern, laser speckle, and motion artifact. This system is able to capture particles ejected after 600 ns with a time resolution of 6 ns and spatial resolution better than 5 μm under the particle recognition accuracy of 100%.
    Vn,est=(Sn,t0+ΔtSn,t0)/Δt,(1)

    View in Article

    JFCM=i=1cj=1nuijmdij2,(2)

    View in Article

    dij=xjci,(3)

    View in Article

    i=1cuij=1,uij[0,1],(4)

    View in Article

    φj={2+ωjx¯j<xj2ωjx¯j>xj0x¯j=xj,(5)

    View in Article

    JARKFCM=i=1cj=1nuijm[1K(xj,ci)]+i=1cj=1nφjuijm[1K(x¯j,ci)],(6)

    View in Article

    X(t+1)=Xp(t)A·|C·Xp(t)X(t)|,(7)

    View in Article

    A=2a·r1a,(8)

    View in Article

    X=2r2,(9)

    View in Article

    X1=XαA1·|C1·XαX|,(10)

    View in Article

    X2=XβA2·|C2·XβX|,(11)

    View in Article

    X3=XδA3·|C3·XδX|,(12)

    View in Article

    X(t+1)=X1(t)+X2(t)+X3(t)3,(13)

    View in Article

    fitness=1/JFCM=1/(1+i=1cj=1nuijmdij2).(14)

    View in Article

    Yangliang Li, Chao Shen, Li Shao, Yujun Zhang, "Dynamic image acquisition and particle recognition of laser-induced exit surface particle ejection in fused silica," Chin. Opt. Lett. 17, 101402 (2019)
    Download Citation