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finite-element method (fem) based commercial software comsol multiphysics  (COMSOL Inc)

 
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    Structured Review

    COMSOL Inc finite-element method (fem) based commercial software comsol multiphysics
    ( a ) the cross-sectional structure of the proposed tubular hollow-core fiber (THCF); ( b ) fundamental mode field distribution inside the hollow core (Produced by COMSOL <t>Multiphysics</t> 3.5).
    Finite Element Method (Fem) Based Commercial Software 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/finite-element+method+(fem)+based+commercial+software+comsol+multiphysics/comsol+multiphysics/pmc11682127-94-20-20
    Average 90 stars, based on 1 article reviews
    finite-element method (fem) based commercial software comsol multiphysics - by Bioz Stars, 2026-10
    90/100 stars

    Images

    1) Product Images from "Numerical optimization of anti resonant hollow core fiber for high sensitivity methane detection"

    Article Title: Numerical optimization of anti resonant hollow core fiber for high sensitivity methane detection

    Journal: Scientific Reports

    doi: 10.1038/s41598-024-83051-w

    ( a ) the cross-sectional structure of the proposed tubular hollow-core fiber (THCF); ( b ) fundamental mode field distribution inside the hollow core (Produced by COMSOL Multiphysics 3.5).
    Figure Legend Snippet: ( a ) the cross-sectional structure of the proposed tubular hollow-core fiber (THCF); ( b ) fundamental mode field distribution inside the hollow core (Produced by COMSOL Multiphysics 3.5).

    Techniques Used: Produced

    Cross-sectional geometries and fundamental mode field distributions of the modified AR-HCF designs. (a), (b): the nested structure; (c), (d): the nested-in-nested structure. All mode field distributions are calculated at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\:3.3\:{\upmu\:}\text{m}$$\end{document} wavelength (Produced by COMSOL Multiphysics 3.5).
    Figure Legend Snippet: Cross-sectional geometries and fundamental mode field distributions of the modified AR-HCF designs. (a), (b): the nested structure; (c), (d): the nested-in-nested structure. All mode field distributions are calculated at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\:3.3\:{\upmu\:}\text{m}$$\end{document} wavelength (Produced by COMSOL Multiphysics 3.5).

    Techniques Used: Modification, Produced

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    Image Search Results


    ( a ) the cross-sectional structure of the proposed tubular hollow-core fiber (THCF); ( b ) fundamental mode field distribution inside the hollow core (Produced by COMSOL Multiphysics 3.5).

    Journal: Scientific Reports

    Article Title: Numerical optimization of anti resonant hollow core fiber for high sensitivity methane detection

    doi: 10.1038/s41598-024-83051-w

    Figure Lengend Snippet: ( a ) the cross-sectional structure of the proposed tubular hollow-core fiber (THCF); ( b ) fundamental mode field distribution inside the hollow core (Produced by COMSOL Multiphysics 3.5).

    Article Snippet: For more accurate results considering the complex geometry and specific conditions, we utilized the finite-element method (FEM) based commercial software COMSOL Multiphysics for our numerical simulations .

    Techniques: Produced

    Cross-sectional geometries and fundamental mode field distributions of the modified AR-HCF designs. (a), (b): the nested structure; (c), (d): the nested-in-nested structure. All mode field distributions are calculated at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\:3.3\:{\upmu\:}\text{m}$$\end{document} wavelength (Produced by COMSOL Multiphysics 3.5).

    Journal: Scientific Reports

    Article Title: Numerical optimization of anti resonant hollow core fiber for high sensitivity methane detection

    doi: 10.1038/s41598-024-83051-w

    Figure Lengend Snippet: Cross-sectional geometries and fundamental mode field distributions of the modified AR-HCF designs. (a), (b): the nested structure; (c), (d): the nested-in-nested structure. All mode field distributions are calculated at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\:3.3\:{\upmu\:}\text{m}$$\end{document} wavelength (Produced by COMSOL Multiphysics 3.5).

    Article Snippet: For more accurate results considering the complex geometry and specific conditions, we utilized the finite-element method (FEM) based commercial software COMSOL Multiphysics for our numerical simulations .

    Techniques: Modification, Produced

    Numerical model created in the COMSOL Multiphysics software with lens parameters \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$a = 1.0{\text{ mm}},{ }\Lambda = 1.5{\text{ mm}},{\text{ and h}} = 40.0{\text{ mm}}$$\end{document} a = 1.0 mm , Λ = 1.5 mm , and h = 40.0 mm .

    Journal: Scientific Reports

    Article Title: A novel approach to Fabry–Pérot-resonance-based lens and demonstrating deep-subwavelength imaging

    doi: 10.1038/s41598-020-67409-4

    Figure Lengend Snippet: Numerical model created in the COMSOL Multiphysics software with lens parameters \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$a = 1.0{\text{ mm}},{ }\Lambda = 1.5{\text{ mm}},{\text{ and h}} = 40.0{\text{ mm}}$$\end{document} a = 1.0 mm , Λ = 1.5 mm , and h = 40.0 mm .

    Article Snippet: For numerical analysis, the finite element method (FEM)-based commercial software COMSOL Multiphysics was employed.

    Techniques: Software

    Numerical results from the COMSOL Multiphysics simulation. Distance between the two monopole point sources = d. ( a ) Results obtained with lens thickness h = 40 mm; without the lens, the data were scaled by adding 22 dB to the original data. ( b ) Results obtained with lens thickness h = 80 mm; without the lens, the data were scaled by adding 67 dB to the original data. ( c ) Results obtained with lens thickness h = 212 mm; without the lens, the data were scaled by adding 125 dB to the original data. ( d ) Data obtained with a single monopole source using metalenses with thicknesses h = 40, 80, and 212 mm. Data with lens thicknesses h = 80 and 212 mm were scaled by adding 8 and 15 dB, respectively. R1, R2, and R3 are the ranges for the full width at half maximum (FWHM) 3 dB below the peak.

    Journal: Scientific Reports

    Article Title: A novel approach to Fabry–Pérot-resonance-based lens and demonstrating deep-subwavelength imaging

    doi: 10.1038/s41598-020-67409-4

    Figure Lengend Snippet: Numerical results from the COMSOL Multiphysics simulation. Distance between the two monopole point sources = d. ( a ) Results obtained with lens thickness h = 40 mm; without the lens, the data were scaled by adding 22 dB to the original data. ( b ) Results obtained with lens thickness h = 80 mm; without the lens, the data were scaled by adding 67 dB to the original data. ( c ) Results obtained with lens thickness h = 212 mm; without the lens, the data were scaled by adding 125 dB to the original data. ( d ) Data obtained with a single monopole source using metalenses with thicknesses h = 40, 80, and 212 mm. Data with lens thicknesses h = 80 and 212 mm were scaled by adding 8 and 15 dB, respectively. R1, R2, and R3 are the ranges for the full width at half maximum (FWHM) 3 dB below the peak.

    Article Snippet: For numerical analysis, the finite element method (FEM)-based commercial software COMSOL Multiphysics was employed.

    Techniques: