• Chinese Optics Letters
  • Vol. 16, Issue 6, 061403 (2018)
Haiyi Sun1, Yonghong Liu1、2, Jiansheng Liu1、3、*, Jingjing Ju1, Cheng Wang1, Xingkai Hu1, Zhongbin Zhu1, Yaoxiang Liu1, Tiejun Wang1, See Leang Chin4, Ruxin Li1, and Zhizhan Xu1
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2MOE Key Laboratory of Advanced Micro-structured Materials, Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 3IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
  • 4Center for Optics, Photonics and Laser (COPL), Laval University, Quebec City, Quebec G1V 0A6, Canada
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    DOI: 10.3788/COL201816.061403 Cite this Article Set citation alerts
    Haiyi Sun, Yonghong Liu, Jiansheng Liu, Jingjing Ju, Cheng Wang, Xingkai Hu, Zhongbin Zhu, Yaoxiang Liu, Tiejun Wang, See Leang Chin, Ruxin Li, Zhizhan Xu. Sub-picosecond chirped laser pulse-induced airflow and water condensation in a cloud chamber[J]. Chinese Optics Letters, 2018, 16(6): 061403 Copy Citation Text show less
    Plasma columns and their corresponding grey values generated by (a) positively and (b) negatively chirped sub-picosecond laser pulses with a pulse duration of (a) ∼0.92 ps and (b) 0.97 ps at a laser power of 6.5 W, respectively. The images of the plasma columns were captured by a camera (Nikon D7000: shutter speed S=1/40 s, f number F=5, light sensitivity ISO=1600).
    Fig. 1. Plasma columns and their corresponding grey values generated by (a) positively and (b) negatively chirped sub-picosecond laser pulses with a pulse duration of (a) 0.92ps and (b) 0.97 ps at a laser power of 6.5 W, respectively. The images of the plasma columns were captured by a camera (Nikon D7000: shutter speed S=1/40s, f number F=5, light sensitivity ISO=1600).
    Airflow generated by (a) positively and (b) negatively chirped sub-picosecond laser pulses with a pulse duration of (a) ∼0.92 ps and (b) 0.97 ps at a laser power of 6.5 W, respectively. The images were captured by a Nikon D7000 camera (S=1/50 s, F=3.2, ISO=1600).
    Fig. 2. Airflow generated by (a) positively and (b) negatively chirped sub-picosecond laser pulses with a pulse duration of (a) 0.92ps and (b) 0.97 ps at a laser power of 6.5 W, respectively. The images were captured by a Nikon D7000 camera (S=1/50s, F=3.2, ISO=1600).
    (a) Snow on the cold plate without laser shooting. (b) Close-up view of part of the snow in (a). The shooting conditions of the camera are S=1/40 s, F=3.2, and ISO=1600 for (a), S=1/40 s, F=5.0, and ISO=1600 for (b).
    Fig. 3. (a) Snow on the cold plate without laser shooting. (b) Close-up view of part of the snow in (a). The shooting conditions of the camera are S=1/40s, F=3.2, and ISO=1600 for (a), S=1/40s, F=5.0, and ISO=1600 for (b).
    Snow piles on the cold plate with (a), (b) positively and (c), (d) negatively chirped sub-picosecond laser pulses at a laser power of 6.5 W with a pulse duration of (a), (b) ∼0.92 ps and (c), (d) 0.97 ps, respectively; (b) and (d) are close-up views of (a) and (c). Panels (a), (c) and (b), (d) are in the same scale. The shooting conditions of the camera are S=1/50 s, F=3.2, and ISO=1600 for (a), S=1/50 s, F=5.0, and ISO=1600 for (b), and S=1/40 s, F=5.0, and ISO=1600 for (c) and (d).
    Fig. 4. Snow piles on the cold plate with (a), (b) positively and (c), (d) negatively chirped sub-picosecond laser pulses at a laser power of 6.5 W with a pulse duration of (a), (b) 0.92ps and (c), (d) 0.97 ps, respectively; (b) and (d) are close-up views of (a) and (c). Panels (a), (c) and (b), (d) are in the same scale. The shooting conditions of the camera are S=1/50s, F=3.2, and ISO=1600 for (a), S=1/50s, F=5.0, and ISO=1600 for (b), and S=1/40s, F=5.0, and ISO=1600 for (c) and (d).
    Dependence of the amount of small snow piles below the plasma columns (black circles and red squares, left scale) and concentration of NO3− in the melted water (green triangles and blue stars, right scale) in the pulse duration of positively (black circles and green triangles) and negatively chirped pulses (red squares and blue stars), respectively. There is no chirp for the 27 fs pulse duration. The pulse duration was measured at the laser exit.
    Fig. 5. Dependence of the amount of small snow piles below the plasma columns (black circles and red squares, left scale) and concentration of NO3 in the melted water (green triangles and blue stars, right scale) in the pulse duration of positively (black circles and green triangles) and negatively chirped pulses (red squares and blue stars), respectively. There is no chirp for the 27 fs pulse duration. The pulse duration was measured at the laser exit.
    Haiyi Sun, Yonghong Liu, Jiansheng Liu, Jingjing Ju, Cheng Wang, Xingkai Hu, Zhongbin Zhu, Yaoxiang Liu, Tiejun Wang, See Leang Chin, Ruxin Li, Zhizhan Xu. Sub-picosecond chirped laser pulse-induced airflow and water condensation in a cloud chamber[J]. Chinese Optics Letters, 2018, 16(6): 061403
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