• Infrared and Laser Engineering
  • Vol. 51, Issue 3, 20220007 (2022)
Yushi Zhao, Wenjun He, Zhiying Liu, and Yuegang Fu
Author Affiliations
  • School of Opto-electronic Engineering, Changchun University of Science and Technology, Changchun 130022, China
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    DOI: 10.3788/IRLA20220007 Cite this Article
    Yushi Zhao, Wenjun He, Zhiying Liu, Yuegang Fu. Development of convex blazed grating in coded aperture spectral imager[J]. Infrared and Laser Engineering, 2022, 51(3): 20220007 Copy Citation Text show less

    Abstract

    Aiming at the performance requirements of a DMD-based Offner spectral imager encoding in spectral dimension for a convex blazed grating, a macro-micro integrated optimization design method for convex blazed gratings was proposed. The three-dimensional polarization ray tracing algorithm was used to organically integrate the optical design of the Offner system in macro-level and the groove design of the convex blazed grating in micro-level. The composition and working principle of the coded aperture Offner spectral imaging system were introduced, and a MWIR convex blazed grating with an average diffraction efficiency of 85.47% was designed according to the requirements of the system. On this basis, a convex blazed grating with curvature radius of 120 mm, grating period of 99.945 μm, blazed angle of 1.1783°, groove depth of 1.834 μm was successfully fabricated by using an ultra-precision single-point diamond lathe. The test results show that in the spectral range of 3-5 μm, the maximum diffraction efficiency is 93.46% and the average diffraction efficiency is 84.29%, which is in good agreement with the theoretical design value. Thus, the proposed design method of the convex blazed grating is verified to be effective and valuable.
    $ {R_{\rm{M}}} = 2{R_{\rm{G}}} $(1)

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    $ {R_{\rm{G}}} = \frac{{d\delta }}{{m\left( {{\lambda _2} - {\lambda _1}} \right)}} $(2)

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    $ {{\boldsymbol{E}}_{out}} = {{\boldsymbol{P}}_{{\text{total}}}} \cdot {{\boldsymbol{E}}_{in}} $(3)

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    $ {{\boldsymbol{P}}_{total}} = \prod\limits_{q = N, - 1}^1 {{{\boldsymbol{P}}_q}} $(4)

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    $ {{\boldsymbol{P}}_q} = {O_{out,q}} \cdot {J_q} \cdot O_{in,q}^{ - 1} $(5)

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    $ {O_{out,q}} = \left( {s^x,qp^x,qk^x,qs^y,qp^y,qk^y,qs^z,qp^z,qk^z,q} \right) $(6)

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    $ {J_q} = \left( {αs,q000αp,q0001} \right) $(7)

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    $ O_{in,q}^{ - 1} = \left( {s^x,qs^y,qs^z,qp^x,qp^y,qp^z,qk^x,q1k^y,q1k^z,q1} \right) $(8)

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    $ {\hat s_q} = \dfrac{{{{\hat k}_{q - 1}} \times {{\hat k}_q}}}{{\left| {{{\hat k}_{q - 1}} \times {{\hat k}_q}} \right|}}\text{,}{\hat p_q} = {\hat k_{q - 1}} \times {\hat s_q}\text{,}\hat p_q' = {\hat k_q} \times {\hat s_q}\text{,} $(9)

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    $ d\left( {\sin i - sin\theta } \right) = m{\lambda _B} $(10)

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    $ 2\gamma = \theta - i $(11)

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    $ h\left( {\tan \gamma + \dfrac{1}{{\tan \gamma }}} \right) = d $(12)

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    $ {{\boldsymbol{\eta}} _G} = \dfrac{{\displaystyle\sum\limits_{\kappa = 1}^K {\displaystyle\sum\limits_{\lambda = {\lambda _1}}^{{\lambda _2}} {\displaystyle\sum\limits_{m = 1}^M {\displaystyle\sum\limits_{n = 1}^N {{\boldsymbol{\eta}} _{m,n}^{\lambda ,\kappa }} } } } }}{{K \times Y \times m \times n}} $(13)

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    $ \left\{ {\boldsymbolP=[\boldsymbolXt],\boldsymbolXt=[γt,ht]\boldsymbolηg=F([\boldsymbolXgt])=[\boldsymbolηgt]\boldsymbolηt=F([\boldsymbolXtg])=[\boldsymbolηtg]} \right. $(14)

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    $ \left\{\boldsymbolηgbest=max(\boldsymbolηg)=F(\boldsymbolXgbest)\boldsymbolηtbest=max(\boldsymbolηt)=F(\boldsymbolXtbest)\right. $(15)

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    $ \left\{ {Δgt=\boldsymbolXg1t\boldsymbolXgtΔgbest=\boldsymbolXgt\boldsymbolXgbestΔtbest=\boldsymbolXgt\boldsymbolXtbest} \right. $(16)

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    $ \left\{ {Δg+1t=k1Δgt+k2Δgbest+k3Δtbest\boldsymbolXg+1t=\boldsymbolXgt+Δgt\boldsymbolPg+1=[\boldsymbolXg+1t]} \right. $(17)

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    $ {{\boldsymbol{\eta}} _\lambda } = \dfrac{{{P_{G,\lambda }}}}{{r_\lambda ^2 \cdot {P_{0,\lambda }}}} $(18)

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    Yushi Zhao, Wenjun He, Zhiying Liu, Yuegang Fu. Development of convex blazed grating in coded aperture spectral imager[J]. Infrared and Laser Engineering, 2022, 51(3): 20220007
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