• Opto-Electronic Advances
  • Vol. 4, Issue 12, 210027-1 (2021)
Yonglei Liu, Yahong Chen, Fei Wang*, Yangjian Cai*, Chunhao Liang*, and Olga Korotkova
DOI: 10.29026/oea.2021.210027 Cite this Article
Yonglei Liu, Yahong Chen, Fei Wang, Yangjian Cai, Chunhao Liang, Olga Korotkova. Robust far-field imaging by spatial coherence engineering[J]. Opto-Electronic Advances, 2021, 4(12): 210027-1 Copy Citation Text show less

Abstract

The degree of coherence (DOC) function that characterizes the second-order correlations at any two points in a light field is shown to provide a new degree of freedom for carrying information. As a rule, the DOC varies along the beam propagation path, preventing from the efficient information recovery. In this paper, we report that when a partially coherent beam carrying a cross phase propagates in free space, in a paraxial optical system or in a turbulent medium, the modulus of the far-field (focal plane) DOC acquires the same value as it has in the source plane. This unique propagation feature is employed in a novel protocol for far-field imaging via the DOC, applicable to transmission in both free-space and turbulence. The advantages of the proposed approach are the confidentiality and resistance to turbulence, as well as the weaker requirement for the beam alignment accuracy. We demonstrate the feasibility and the robustness of the far-field imaging via the DOC in the turbulent media through both the experiment and the numerical simulations. Our findings have potential applications in optical imaging and remote sensing in natural environments, in the presence of optical turbulence.
${W_0}\left( {{{\boldsymbol{r}}_1},{{\boldsymbol{r}}_2}} \right) = \tau \left( {{{\boldsymbol{r}}_1}} \right){\tau ^*}\left( {{{\boldsymbol{r}}_2}} \right){\mu _0}\left( {\Delta {\boldsymbol{r}}} \right){\rm{exp}} \left[ {{\rm{i}}u\left( {{x_1}{y_1} - {x_2}{y_2}} \right)} \right]\;,$(1)

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$\;{\mu _0}\left( {\rm{\Delta}}{ {\boldsymbol{r}}} \right) = \cos \left( {\frac{{n\sqrt {2\pi } \Delta x}}{{{{i\text{δ}} _0}}}} \right)\cos \left( {\frac{{n\sqrt {2\pi } \Delta y}}{{{{i\text{δ}}_0}}}} \right)\exp \left({ - \frac{{\Delta {{\boldsymbol{r}}^2}}}{{2{i\text{δ}}_0^2}}} \right)\;,$(2)

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$\begin{split} &W\left( {{{{{\boldsymbol{\textit{ρ}}} }}_1},{{\boldsymbol{\textit{ρ}}}_2}} \right) = \frac{{{k^2}}}{{4{{\rm{\pi}} ^2}{{\boldsymbol{B}}^2}}}{\rm{exp}} \left[ { - \frac{{{\rm{i}}k{\boldsymbol{D}}}}{{2{\boldsymbol{B}}}}\left( {{{{\boldsymbol{\textit{ρ}}} }}_1^2 - {\boldsymbol{\textit{ρ}}}_2^2} \right)} \right]\\ &\times \int_{ - \infty }^\infty {\int_{ - \infty }^\infty{{W_0}\left( {{{\boldsymbol{r}}_1},{{\boldsymbol{r}}_2}} \right)} } {\rm{exp}} \left[ { - \frac{{{\rm{i}}k{\boldsymbol{A}}}}{{2{\boldsymbol{B}}}}\left( {{\boldsymbol{r}}_1^2 - {\boldsymbol{r}}_2^2} \right)} \right]\\ &\times{\rm{exp}} \left[ {\frac{{{\rm{i}}k}}{{\boldsymbol{B}}}\left( {{{\boldsymbol{r}}_1} \cdot {{\boldsymbol{\textit{ρ}}}_1} - {{\boldsymbol{r}}_2} \cdot {{\boldsymbol{\textit{ρ}}}_{\bf{2}}}} \right)} \right]{\rm{d}}^2{{\boldsymbol{r}}_1}{\rm{d}}^2{{\boldsymbol{r}}_2}\;, \end{split}$(3)

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$\left( {\begin{array}{*{20}{c}} {\boldsymbol{A}}&{\boldsymbol{B}} \\ {\boldsymbol{C}}&{\boldsymbol{D}} \end{array}} \right) = \left( {\begin{array}{*{20}{c}} 1&z \\ 0&1 \end{array}} \right)\left( {\begin{array}{*{20}{c}} 1&0 \\ {{{ - 1} / f}}&1 \end{array}} \right) = \left( {\begin{array}{*{20}{c}} {1 - z/f}&z \\ {{{ - 1} / f}}&1 \end{array}} \right)\;.$(4)

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$\left| {{\mu _f}\left( {{\rm{\Delta}} {\boldsymbol{\textit{ρ}}} } \right)} \right| = \left| {\cos \left( {\frac{{n\sqrt {2\pi } \Delta {ρ _x}}}{{{{i\text{δ}} _f}}}} \right)\cos \left( {\frac{{n\sqrt {2\pi } \Delta {{ρ} _y}}}{{{{i\text{δ}} _f}}}} \right)\exp \left( { - \frac{{\Delta {\boldsymbol{\textit{ρ}}} _{}^2}}{{2{i\text{δ}} _f^2}}} \right)}\right|\;,$(5)

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$ u>{\rm{max}}\left\{\sqrt{\rm{400}\pi {n}^{\rm{2}}/{{i\text{δ}} }_{0}^{2}-{\Omega }^{2}}/{\omega }_{0}, \sqrt{10}\Omega /\omega_{0}\right\}\;,$(6)

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$\mu ({\rm{\Delta}} {\boldsymbol{r}}) \propto \int {P({\boldsymbol{v}}){\rm{exp}} ( - {\rm{i}}2{\rm{\pi}} {\boldsymbol{v}} \cdot {\rm{\Delta}} {\boldsymbol{r}}/\lambda f){{\rm{d}}^2}{\boldsymbol{v}}}\; ,$(7)

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$ {\left|\mu (x-{x}_{0},y-{y}_{0})\right|}^{2}=\frac{{\displaystyle \sum _{n=1}^{N}I({x}_{0},{y}_{0},{t}_{n})I(x,y,{t}_{n})}}{N\overline{I}({x}_{0},{y}_{0})\overline{I}(x,y)}-1\;, $(8)

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${\Phi _n}\left( \kappa \right){\rm{ = }}0.33{\rm C}_n^2{\left( {{\kappa ^2} + \kappa _0^2} \right)^{ - 11/6}}{\rm{exp}} ( - {\kappa ^2} + \kappa _m^2)\;,$(9)

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Yonglei Liu, Yahong Chen, Fei Wang, Yangjian Cai, Chunhao Liang, Olga Korotkova. Robust far-field imaging by spatial coherence engineering[J]. Opto-Electronic Advances, 2021, 4(12): 210027-1
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