• High Power Laser Science and Engineering
  • Vol. 11, Issue 1, 01000e13 (2023)
Yuanzhi Dong1、2、3, Yunxia Jin1、3、4, Fanyu Kong1、3、*, Jingyin Zhao1、3, Jianwei Mo1、3, Dongbing He1、3, Jing Sun1、3, and Jianda Shao1、2、3、4、5
Author Affiliations
  • 1Thin Film Optics Laboratory, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
  • 2School of Physical Sciences, University of Science and Technology of China, Hefei, China
  • 3Key Laboratory of High Power Laser Materials, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
  • 4CAS Center for Excellence in Ultra-intense Laser Science, Chinese Academy of Sciences, Shanghai, China
  • 5Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou, China
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    DOI: 10.1017/hpl.2022.42 Cite this Article Set citation alerts
    Yuanzhi Dong, Yunxia Jin, Fanyu Kong, Jingyin Zhao, Jianwei Mo, Dongbing He, Jing Sun, Jianda Shao. Angle amplifier in a 2D beam scanning system based on peristrophic multiplexed volume Bragg gratings[J]. High Power Laser Science and Engineering, 2023, 11(1): 01000e13 Copy Citation Text show less
    Scheme of the 2D beam scanning system. The incident beam (outgoing from the first stage addressing LCOPA) into multiplexed VBGs is first deflected to each amplified angle, then the second LCOPA finely controls and fills the beam in each exit angle. The LCOPA is capable of achieving precise angular deflection of the beam within the cone-shaped range.
    Fig. 1. Scheme of the 2D beam scanning system. The incident beam (outgoing from the first stage addressing LCOPA) into multiplexed VBGs is first deflected to each amplified angle, then the second LCOPA finely controls and fills the beam in each exit angle. The LCOPA is capable of achieving precise angular deflection of the beam within the cone-shaped range.
    (a) Typical schematic of volume Bragg grating recording (purple line) as well as diffraction (red line), where the angle is positive when it is turned counterclockwise from the z-axis. (b) Schematic diagram of the beam emerging from the VBG, where the z-axis coincides with the front surface normal of the recording medium, channel-A corresponds to the channel with no rotation angle and channel-B corresponds to the channel with a rotation angle of .
    Fig. 2. (a) Typical schematic of volume Bragg grating recording (purple line) as well as diffraction (red line), where the angle is positive when it is turned counterclockwise from the z-axis. (b) Schematic diagram of the beam emerging from the VBG, where the z-axis coincides with the front surface normal of the recording medium, channel-A corresponds to the channel with no rotation angle and channel-B corresponds to the channel with a rotation angle of .
    Relationship between grating thickness and diffraction efficiency as well as that between refractive index modulation and diffraction efficiency, under and . The red line corresponds to Equation (11).
    Fig. 3. Relationship between grating thickness and diffraction efficiency as well as that between refractive index modulation and diffraction efficiency, under and . The red line corresponds to Equation (11).
    Schematic diagram of three VBGs working as an amplifier. The beam is deflected to point-M by VBG1 when the incident angle and rotation angle of the incident beam are 1.5° and 0°, respectively, and is deflected to point-N by VBG2 when the incident angle and rotation angle of the incident beam are 3° and 30°, respectively.
    Fig. 4. Schematic diagram of three VBGs working as an amplifier. The beam is deflected to point-M by VBG1 when the incident angle and rotation angle of the incident beam are 1.5° and 0°, respectively, and is deflected to point-N by VBG2 when the incident angle and rotation angle of the incident beam are 3° and 30°, respectively.
    Scheme of DE measurement of multiplexed VBGs. The sample is positioned on a motorized rotational stage and different grating channels are tested using a sample stage, which allows the sample to be rotated around the front surface normal.
    Fig. 5. Scheme of DE measurement of multiplexed VBGs. The sample is positioned on a motorized rotational stage and different grating channels are tested using a sample stage, which allows the sample to be rotated around the front surface normal.
    (a) DE and deviation angle of each channel. Experimental angle selectivity curves for the incident angle (b) and exit angle (c) of the first channel in each grating.
    Fig. 6. (a) DE and deviation angle of each channel. Experimental angle selectivity curves for the incident angle (b) and exit angle (c) of the first channel in each grating.
    The RIM fitting curve of the first channel of each monolithic VBG and the corresponding picture. The total RIM of a sample would be calculated by summing the RIM of each channel, which is 1.16 × 10–3 for VBG1 (a), 1.57 × 10–3 for VBG2 (b) and 1.37 × 10–3 for VBG3 (c).
    Fig. 7. The RIM fitting curve of the first channel of each monolithic VBG and the corresponding picture. The total RIM of a sample would be calculated by summing the RIM of each channel, which is 1.16 × 10–3 for VBG1 (a), 1.57 × 10–3 for VBG2 (b) and 1.37 × 10–3 for VBG3 (c).
    Rotation anglePeristrophicNumberIncidentExitGratingSlant
    Gratingbetweenangular selectivityofangle in theangle in theperiodangleThickness
    numberchannels $\theta$ (°) $\mathrm{d}\theta$ (°)channelsair ${\theta}_{\mathrm{i}}$ (°)air ${\theta}_{\mathrm{o}}$ (°) $\Lambda$ (nm) $\varphi$ (°) $d$ (mm)
    VBG16020.9461.5105318.192.843
    VBG23010.3123202685.195.623
    VBG3206.67184.5301820.298.284
    Table 1. Key parameters of the designed three VBGs.
    Yuanzhi Dong, Yunxia Jin, Fanyu Kong, Jingyin Zhao, Jianwei Mo, Dongbing He, Jing Sun, Jianda Shao. Angle amplifier in a 2D beam scanning system based on peristrophic multiplexed volume Bragg gratings[J]. High Power Laser Science and Engineering, 2023, 11(1): 01000e13
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