• Chinese Optics Letters
  • Vol. 15, Issue 5, 051401 (2017)
Mincheng Zhong1、*, Ziqiang Wang2, and Yinmei Li2
Author Affiliations
  • 1School of Instrument Science and Opto-electronic Engineering, Hefei University of Technology, Hefei 230009, China
  • 2Department of Optics and Optical Engineering, University of Science and Technology of China, Hefei 230026, China
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    DOI: 10.3788/COL201715.051401 Cite this Article Set citation alerts
    Mincheng Zhong, Ziqiang Wang, Yinmei Li. Laser-accelerated self-assembly of colloidal particles at the water–air interface[J]. Chinese Optics Letters, 2017, 15(5): 051401 Copy Citation Text show less
    Schematic of the experimental setup. L1, lens; M1-M2, mirrors; DM, dichroic mirror; Ltube, tube lens; MO, microscope objective; CMOS, CMOS camera. Inset: top view of the circular trough. ‘+’ indicates the optical trap center.
    Fig. 1. Schematic of the experimental setup. L1, lens; M1-M2, mirrors; DM, dichroic mirror; Ltube, tube lens; MO, microscope objective; CMOS, CMOS camera. Inset: top view of the circular trough. ‘+’ indicates the optical trap center.
    Two-dimensional self-assembly accelerated at the water–air interface by optical tweezers. The NA of the objective is 1.25. The white lines mark the water–air interface at the upper left. The black arrow indicates the direction of the particles’ movement. Scale bar, 10 μm; ‘+’ indicates the optical trap center.
    Fig. 2. Two-dimensional self-assembly accelerated at the water–air interface by optical tweezers. The NA of the objective is 1.25. The white lines mark the water–air interface at the upper left. The black arrow indicates the direction of the particles’ movement. Scale bar, 10 μm; ‘+’ indicates the optical trap center.
    Particles’ velocities dependence of laser power at the pupil of the objective lens. Error bars are the standard deviations of velocity. NA=1.25. The line is a linear fit to the whole data.
    Fig. 3. Particles’ velocities dependence of laser power at the pupil of the objective lens. Error bars are the standard deviations of velocity. NA=1.25. The line is a linear fit to the whole data.
    Gap at the growing front is filled up by the incoming particles. The steep peak is created by optical tweezers. Scale bar, 10 μm; ‘+’ indicates the optical trap center.
    Fig. 4. Gap at the growing front is filled up by the incoming particles. The steep peak is created by optical tweezers. Scale bar, 10 μm; ‘+’ indicates the optical trap center.
    Smoothing process for a steep peak at the growing front. The particles at the peak are pulled down by the Marangoni flow, resulting in a reduction of the local roughness. Scale bar, 10 μm; ‘+’ indicates the optical trap center. The black arrows indicate the direction of the particles’ movement.
    Fig. 5. Smoothing process for a steep peak at the growing front. The particles at the peak are pulled down by the Marangoni flow, resulting in a reduction of the local roughness. Scale bar, 10 μm; ‘+’ indicates the optical trap center. The black arrows indicate the direction of the particles’ movement.
    Integration of particle aggregation into the crystal. (a) and (b) The aggregation is created by the optical tweezers. (c) and (d) The wide peak growing. Black lines mark the shape of the peak. Scale bar, 10 μm; ‘+’ indicates the optical trap center.
    Fig. 6. Integration of particle aggregation into the crystal. (a) and (b) The aggregation is created by the optical tweezers. (c) and (d) The wide peak growing. Black lines mark the shape of the peak. Scale bar, 10 μm; ‘+’ indicates the optical trap center.
    NAVelocity (μm/s)
    0.45.08±0.62
    0.78.27±0.47
    1.2520.87±2.05
    Table 1. Particles’ Velocities Dependence of NAs of Objectives with Error Barsa
    Mincheng Zhong, Ziqiang Wang, Yinmei Li. Laser-accelerated self-assembly of colloidal particles at the water–air interface[J]. Chinese Optics Letters, 2017, 15(5): 051401
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