2021
DOI: 10.1016/j.optcom.2020.126690
|View full text |Cite
|
Sign up to set email alerts
|

Mid-infrared full-Stokes polarization detection based on dielectric metasurfaces

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2

Citation Types

0
4
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 10 publications
(4 citation statements)
references
References 36 publications
0
4
0
Order By: Relevance
“…Subsequently, we obtained the measurement results for different polarization component at the focal plane separately using the standard algorithm. The function employed to reconstruct the full‐Stokes parameter matrix S = [ S 0 , S 1 , S 2 , S 3 ] T at the target pixel spots is modified to that [ 20,44 ] S0badbreak=Ax2goodbreak+Ay2$$\begin{equation}{S_0} = A_x^2 + A_y^2\end{equation}$$ S1badbreak=Ax2goodbreak−Ay2$$\begin{equation}{S_1} = A_x^2 - A_y^2\end{equation}$$ S2badbreak=2AxAycos()δ1δ2goodbreak=A452goodbreak−A1352$$\begin{equation}{S_2} = 2{A_x}{A_y}\cos \left( {{\delta _1} - {\delta _2}} \right) = A_{{{45}^ \circ }}^2 - A_{{{135}^ \circ }}^2\end{equation}$$ S3badbreak=2AxAysin()δ1δ2goodbreak=AR2goodbreak−AL2$$\begin{equation}{S_3} = 2{A_x}{A_y}\sin \left( {{\delta _1} - {\delta _2}} \right) = A_{\mathrm{R}}^2 - A_{\mathrm{L}}^2\end{equation}$$where A 45° and A 135° represent the amplitude projection along linearly diagonal and antidiagonal polarized, and A R , A L indicate the amplitude projection over RCP and LCP states. As can be seen in Figure 3d, the parameter matrix calculated by combining the E x ‐ and E y ‐components indicates that the measurement results are in good agreement with the simulation results.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Subsequently, we obtained the measurement results for different polarization component at the focal plane separately using the standard algorithm. The function employed to reconstruct the full‐Stokes parameter matrix S = [ S 0 , S 1 , S 2 , S 3 ] T at the target pixel spots is modified to that [ 20,44 ] S0badbreak=Ax2goodbreak+Ay2$$\begin{equation}{S_0} = A_x^2 + A_y^2\end{equation}$$ S1badbreak=Ax2goodbreak−Ay2$$\begin{equation}{S_1} = A_x^2 - A_y^2\end{equation}$$ S2badbreak=2AxAycos()δ1δ2goodbreak=A452goodbreak−A1352$$\begin{equation}{S_2} = 2{A_x}{A_y}\cos \left( {{\delta _1} - {\delta _2}} \right) = A_{{{45}^ \circ }}^2 - A_{{{135}^ \circ }}^2\end{equation}$$ S3badbreak=2AxAysin()δ1δ2goodbreak=AR2goodbreak−AL2$$\begin{equation}{S_3} = 2{A_x}{A_y}\sin \left( {{\delta _1} - {\delta _2}} \right) = A_{\mathrm{R}}^2 - A_{\mathrm{L}}^2\end{equation}$$where A 45° and A 135° represent the amplitude projection along linearly diagonal and antidiagonal polarized, and A R , A L indicate the amplitude projection over RCP and LCP states. As can be seen in Figure 3d, the parameter matrix calculated by combining the E x ‐ and E y ‐components indicates that the measurement results are in good agreement with the simulation results.…”
Section: Resultsmentioning
confidence: 99%
“…Subsequently, we obtained the measurement results for different polarization component at the focal plane separately using the standard algorithm. The function employed to reconstruct the full-Stokes parameter matrix S = [S 0 , S 1 , S 2 , S 3 ] T at the target pixel spots is modified to that [20,44]…”
Section: Resultsmentioning
confidence: 99%
“…Polarimetry can also be demonstrated with the design of plasmonic meta-gratings 15,16 , yet the reflection/diffraction mode makes it challenging for direct integration on sensors. Similar to the division of focal plane, researchers design a metalens array (usually consisting three to six metalenses) to split and focus light in different polarization bases for estimating the full Stokes vectors [17][18][19][20][21] .…”
Section: Introductionmentioning
confidence: 99%
“…[19][20][21][22][23][24][25][26] To overcome the limitations associated with the 50% energy efficiency constraint imposed by traditional methods, polarization-sensitive metalenses based on birefringence elements have been proposed to split and focus the orthogonal polarization states at different positions on the imaging sensor. [27][28][29] Sun et al demonstrated a maximum energy efficiency of 81.8% using an all-dielectric spatial multiplexing metalens design. [30] In 2019, Rubin et al introduced a compact full-Stokes polarization metasurface utilizing diffraction gratings that can efficiently diffract distinct polarization states onto separate diffraction orders exceeding 50% efficiencies.…”
Section: Introductionmentioning
confidence: 99%