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finite-element method (fem) numerical simulations in the wavelength domain comsol multiphysics  (COMSOL Inc)

 
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    COMSOL Inc finite-element method (fem) numerical simulations in the wavelength domain comsol multiphysics
    Example of FEM simulations of a metaunit ( P x = P y = 600 nm) made of silicon nanopillars ( L x = 150 nm, L y = 300 nm, and H = 850 nm, i.e., pillar #9 in Fig. ) over a silicon substrate. ( a ) Boundary conditions imposed to properly simulate the nanostructure. PBC periodic boundary conditions. PML perfectly matched layers. ( b – d ) Electric field under TE polarization in input impinging from the air side. Lateral cross-sections at y = 0 ( b ), x = 0 ( c ), and top-view cross-section at z = H /4 ( d ). Input <t>wavelength</t> λ = 1310 nm. Colors refer to the intensity of the electric field (a.u.).
    Finite Element Method (Fem) Numerical Simulations In The Wavelength Domain Comsol Multiphysics, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/multiphysics+simulation+domain/comsol+multiphysics/pmc10293257-151-11-14
    Average 90 stars, based on 1 article reviews
    finite-element method (fem) numerical simulations in the wavelength domain comsol multiphysics - by Bioz Stars, 2026-09
    90/100 stars

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    1) Product Images from "Dual-functional metalenses for the polarization-controlled generation of focalized vector beams in the telecom infrared"

    Article Title: Dual-functional metalenses for the polarization-controlled generation of focalized vector beams in the telecom infrared

    Journal: Scientific Reports

    doi: 10.1038/s41598-023-36865-z

    Example of FEM simulations of a metaunit ( P x = P y = 600 nm) made of silicon nanopillars ( L x = 150 nm, L y = 300 nm, and H = 850 nm, i.e., pillar #9 in Fig. ) over a silicon substrate. ( a ) Boundary conditions imposed to properly simulate the nanostructure. PBC periodic boundary conditions. PML perfectly matched layers. ( b – d ) Electric field under TE polarization in input impinging from the air side. Lateral cross-sections at y = 0 ( b ), x = 0 ( c ), and top-view cross-section at z = H /4 ( d ). Input wavelength λ = 1310 nm. Colors refer to the intensity of the electric field (a.u.).
    Figure Legend Snippet: Example of FEM simulations of a metaunit ( P x = P y = 600 nm) made of silicon nanopillars ( L x = 150 nm, L y = 300 nm, and H = 850 nm, i.e., pillar #9 in Fig. ) over a silicon substrate. ( a ) Boundary conditions imposed to properly simulate the nanostructure. PBC periodic boundary conditions. PML perfectly matched layers. ( b – d ) Electric field under TE polarization in input impinging from the air side. Lateral cross-sections at y = 0 ( b ), x = 0 ( c ), and top-view cross-section at z = H /4 ( d ). Input wavelength λ = 1310 nm. Colors refer to the intensity of the electric field (a.u.).

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    Example of FEM simulations of a metaunit ( P x = P y = 600 nm) made of silicon nanopillars ( L x = 150 nm, L y = 300 nm, and H = 850 nm, i.e., pillar #9 in Fig. ) over a silicon substrate. ( a ) Boundary conditions imposed to properly simulate the nanostructure. PBC periodic boundary conditions. PML perfectly matched layers. ( b – d ) Electric field under TE polarization in input impinging from the air side. Lateral cross-sections at y = 0 ( b ), x = 0 ( c ), and top-view cross-section at z = H /4 ( d ). Input wavelength λ = 1310 nm. Colors refer to the intensity of the electric field (a.u.).

    Journal: Scientific Reports

    Article Title: Dual-functional metalenses for the polarization-controlled generation of focalized vector beams in the telecom infrared

    doi: 10.1038/s41598-023-36865-z

    Figure Lengend Snippet: Example of FEM simulations of a metaunit ( P x = P y = 600 nm) made of silicon nanopillars ( L x = 150 nm, L y = 300 nm, and H = 850 nm, i.e., pillar #9 in Fig. ) over a silicon substrate. ( a ) Boundary conditions imposed to properly simulate the nanostructure. PBC periodic boundary conditions. PML perfectly matched layers. ( b – d ) Electric field under TE polarization in input impinging from the air side. Lateral cross-sections at y = 0 ( b ), x = 0 ( c ), and top-view cross-section at z = H /4 ( d ). Input wavelength λ = 1310 nm. Colors refer to the intensity of the electric field (a.u.).

    Article Snippet: We set up custom-made Finite-Element Method (FEM) numerical simulations in the wavelength domain (using COMSOL Multiphysics ® ) to find the best set of metaatoms satisfying the DFMLs requirements described above (Fig. ).

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