• Chinese Optics Letters
  • Vol. 18, Issue 12, 121402 (2020)
Yaoxiang Liu1、2、3, Tie-Jun Wang2、3、*, Na Chen2、3, Hao Guo2、3, Haiyi Sun2、3, Lu Zhang4, Zheng Qi4, Yuxin Leng2、3, Zhanshan Wang1, and Ruxin Li2、3
Author Affiliations
  • 1MOE Key Laboratory of Advanced Micro-structured Materials, Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 2State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-intense Laser Science, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 3Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 4Science and Technology on Space Physics Laboratory, Beijing 100076, China
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    DOI: 10.3788/COL202018.121402 Cite this Article Set citation alerts
    Yaoxiang Liu, Tie-Jun Wang, Na Chen, Hao Guo, Haiyi Sun, Lu Zhang, Zheng Qi, Yuxin Leng, Zhanshan Wang, Ruxin Li. Simultaneous generation of controllable double white light lasers by focusing an intense femtosecond laser pulse in air[J]. Chinese Optics Letters, 2020, 18(12): 121402 Copy Citation Text show less
    (a) Schematic of experimental setup. QWP is a zero-order quarter waveplate. ND filter is neutral density filter. (b) Input beam spatial profile and (c) typical forward beam pattern after filamentation (about 1.3 m away) on the screen taken by a digital camera (Nikon D7200). The laser pulse energy was 7.43 mJ.
    Fig. 1. (a) Schematic of experimental setup. QWP is a zero-order quarter waveplate. ND filter is neutral density filter. (b) Input beam spatial profile and (c) typical forward beam pattern after filamentation (about 1.3 m away) on the screen taken by a digital camera (Nikon D7200). The laser pulse energy was 7.43 mJ.
    (a) Real-color images of filaments in air with laser incident angle to the lens changing from 0 deg to 20 deg. Exposure time of the camera in (a) was 0.25 s. The energy of the linearly polarized laser pulse was 7.43 mJ. Corresponding forward white light beam patterns on the screen at different incident angles of (b) 0 deg, (c) 5 deg, (d) 10 deg, and (e) 20 deg. Exposure time of the camera in (b)–(e) was 0.02 s with an ND filter in front of the camera. There are 20 shots of white light beams accumulated in each image.
    Fig. 2. (a) Real-color images of filaments in air with laser incident angle to the lens changing from 0 deg to 20 deg. Exposure time of the camera in (a) was 0.25 s. The energy of the linearly polarized laser pulse was 7.43 mJ. Corresponding forward white light beam patterns on the screen at different incident angles of (b) 0 deg, (c) 5 deg, (d) 10 deg, and (e) 20 deg. Exposure time of the camera in (b)–(e) was 0.02 s with an ND filter in front of the camera. There are 20 shots of white light beams accumulated in each image.
    (a) Filament fluorescence images under different polarization states taken by a camera with the exposure time of 0.25 s. The laser energy was 7.43 mJ. The laser polarization is LP (CP) when the QWP angle was 0 deg or 90 deg (45 deg). (b) The effective filament length as a function of the QWP angle (the laser polarization state) under different laser energies. (c) The corresponding forward white light spots in (a) as the polarization states of the laser changed from LP to CP. The exposure time of the camera in (c) was 0.02 s without the ND filter.
    Fig. 3. (a) Filament fluorescence images under different polarization states taken by a camera with the exposure time of 0.25 s. The laser energy was 7.43 mJ. The laser polarization is LP (CP) when the QWP angle was 0 deg or 90 deg (45 deg). (b) The effective filament length as a function of the QWP angle (the laser polarization state) under different laser energies. (c) The corresponding forward white light spots in (a) as the polarization states of the laser changed from LP to CP. The exposure time of the camera in (c) was 0.02 s without the ND filter.
    (a) Normalized SC spectra of the upper and lower white light spots for LP filamenting pulses. The pulse energy was 7.43 mJ. (b) Spectra of white lights for LP, EP (the QWP angle was 30 deg), and CP. The spectral intensity is the integration of the spectral density of both the upper and lower white lights. (c) Spectral bandwidth of the SC versus different pump laser polarization states. The spectral bandwidth is defined by the full width of the spectral intensity curve at 3σ. σ is the standard deviation of the spectral noise. (d) Energy of each white light as a function of the pump laser polarization state under different pump laser energies.
    Fig. 4. (a) Normalized SC spectra of the upper and lower white light spots for LP filamenting pulses. The pulse energy was 7.43 mJ. (b) Spectra of white lights for LP, EP (the QWP angle was 30 deg), and CP. The spectral intensity is the integration of the spectral density of both the upper and lower white lights. (c) Spectral bandwidth of the SC versus different pump laser polarization states. The spectral bandwidth is defined by the full width of the spectral intensity curve at 3σ. σ is the standard deviation of the spectral noise. (d) Energy of each white light as a function of the pump laser polarization state under different pump laser energies.
    Yaoxiang Liu, Tie-Jun Wang, Na Chen, Hao Guo, Haiyi Sun, Lu Zhang, Zheng Qi, Yuxin Leng, Zhanshan Wang, Ruxin Li. Simultaneous generation of controllable double white light lasers by focusing an intense femtosecond laser pulse in air[J]. Chinese Optics Letters, 2020, 18(12): 121402
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