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numerical simulations using finite element method comsol multiphysics v. 6.2  (COMSOL Inc)

 
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    COMSOL Inc numerical simulations using finite element method comsol multiphysics v. 6.2
    Numerical Simulations Using Finite Element Method Comsol Multiphysics V. 6.2, 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/result/numerical simulations using finite element method comsol multiphysics v. 6.2/product/COMSOL Inc
    Average 90 stars, based on 1 article reviews
    numerical simulations using finite element method comsol multiphysics v. 6.2 - by Bioz Stars, 2026-04
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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.).
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    COMSOL Inc numerical finite-element simulations comsol multiphysics
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    Average 90 stars, based on 1 article reviews
    numerical finite-element simulations comsol multiphysics - by Bioz Stars, 2026-04
    90/100 stars
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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. ).

    Techniques: