Acta Optica Sinica, Volume. 41, Issue 24, 2422001(2021)

Active Deformation Mirror with Variable Thickness

Hao Zhou1,2, Xin Wang1,2、*, Qiang Liu1, Jianjun Jia1,2, and Rong Shu1,2
Author Affiliations
  • 1Key Laboratory of Space Active Opto-Electronics technology, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
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    Figures & Tables(22)
    Diagram of internal bending moment, torque and stress of plate under equilibrium state
    Relationship between thickness distribution and normalized radius
    Finite element division of deformable mirror
    Face shape cloud view of deformable mirror
    Relationship between third-order spherical aberration coefficient A40 and linear forces
    Astigmatic shape with force of ±1 N applied to ends of orthogonal diameters
    Relationship between Zernike term coefficient of astigmatic plane and external force
    Surface shape cloud image of uniform thickness deformable mirror with 5 N load applied to edge
    57 region positions loaded on deformable mirror with constant thickness
    Displacement cloud image of deformable mirror with constant thickness produced by movement of 57 nodes
    Structure of deformable mirror with variable thickness. (a) Deformable mirror; (b) overall structure
    Actual machined deformable mirror test piece. (a) Deformable mirror; (b) overall structure
    Experimental optical path of deformable mirror
    Initial surfaces of deformable mirror under different conditions. (a) Spherical aberration and astigmatism are existed; (b) defocus, spherical aberration, and astigmatism are removed
    Mirror surface of helical micrometer head relative to initial position at different displacement s. (a) s=0; (b) s=0.12 mm; (c) s=0.18 mm; (d) s=0.23 mm; (e) s=0.28 mm; (f) s=0.32 mm
    Relationship between Z9 term in Zernike polynomial and displacement of mirror edge
    Astigmatic surfaces at different clearance. (a) t'=0; (b) t'=0.05 mm; (c) t'=0.10 mm; (d) t'=0.15 mm;(e) t'=0.20 mm; (f) t'=0.25 mm
    Relationship between astigmatic Zernike coefficients Z5 and Z6 and gap distance of rigid beams
    Experimental optical path of spherical aberration compensation for off-axis dual reflection optical system
    Spherical aberration wave surface change diagram compensated by deformable mirror. (a) s=0; (b) s=0.02 mm; (c) s=0.03 mm; (d) s=0.04 mm
    • Table 1. Aberration comparison between deformable mirror with constant thickness and deformable mirror with variable thickness under the same applied force

      View table

      Table 1. Aberration comparison between deformable mirror with constant thickness and deformable mirror with variable thickness under the same applied force

      Seidel aberrationCoefficient of deformable mirror with constant thickness /mmCoefficient of deformable mirror with variable thickness /mm
      Piston(A00)0.19763270.0000421
      Tilt(A11)0.05408130.0000008
      Focus(A20)13.7429771-34.7315700
      Astigmatism(A22)0.00001120.0000001
      Coma(A31)0.00128570.0000009
      Spherical(A40)-9.4068757-424.8320600
    • Table 2. Parameters of off-axis dual reflection optical system

      View table

      Table 2. Parameters of off-axis dual reflection optical system

      SurfaceRadius /mmConicTypeAperture /mmOff-axis /mm
      1-480-1Mirror6096
      2-80-1Mirror1016
      3Deformable mirror10
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    Hao Zhou, Xin Wang, Qiang Liu, Jianjun Jia, Rong Shu. Active Deformation Mirror with Variable Thickness[J]. Acta Optica Sinica, 2021, 41(24): 2422001

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    Paper Information

    Category: Optical Design and Fabrication

    Received: Apr. 29, 2021

    Accepted: Jun. 22, 2021

    Published Online: Dec. 10, 2021

    The Author Email: Wang Xin (wangxin@mail.sitp.ac.cn)

    DOI:10.3788/AOS202141.2422001

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