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2d finite-element method simulation package rf module of comsol multiphysics  (COMSOL Inc)

 
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    COMSOL Inc 2d finite-element method simulation package rf module of comsol multiphysics
    2d Finite Element Method Simulation Package Rf Module Of 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+2d+simulations/rf+module+of+comsol+multiphysics/pm39434490-602-27-27
    Average 90 stars, based on 1 article reviews
    2d finite-element method simulation package rf module of comsol multiphysics - by Bioz Stars, 2026-11
    90/100 stars

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    Software:

    Article Title: The Pre-Polarization and Concentration of Cells near Micro-Electrodes Using AC Electric Fields Enhances the Electrical Cell Lysis in a Sessile Drop
    Article Snippet: The AC/DC module of COMSOL Multiphysics (COMSOL Inc., Burlington MA, USA) was utilized to calculate electric fields and their gradients (∇E2).

    Article Title: The Pre-Polarization and Concentration of Cells near Micro-Electrodes Using AC Electric Fields Enhances the Electrical Cell Lysis in a Sessile Drop
    Article Snippet: The AC/DC module of COMSOL Multiphysics (COMSOL Inc., Burlington MA, USA) was utilized to calculate electric fields and their gradients (∇ E 2 ).

    Article Title: Chiral lasing enabled by strong coupling
    Article Snippet: The complex numbered eigenfrequencies (ω) of photonics crystal structure are directly calculated with the radio-frequency module of a commercial software for the finite element method (COMSOL Multiphysics).

    Article Title: Three-dimensional nonreciprocal transport in photonic topological heterostructure of arbitrary shape.
    Article Snippet: All theoretical simulations were performed using the radio- frequency module of COMSOL Multiphysics.

    Article Title: Chiral lasing enabled by strong coupling.
    Article Snippet: The complex numbered eigenfrequencies (ω) of photonics crystal structure are directly calculated with the radio- frequency module of a commercial software for the finite element method (COMSOL Multiphysics).

    Article Title: Observation of cavity-tunable topological phases of polaritons
    Article Snippet: In this work, all numerical simulations are performed using the finite element method (FEM) with the radio frequency module of COMSOL Multiphysics.



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    (a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL <t>Multiphysics,</t> this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.
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    (a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL <t>Multiphysics,</t> this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.
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    (a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL Multiphysics, this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.

    Journal: Scientific Reports

    Article Title: Inverse designed aperiodic multilayer perfect absorbers for mid infrared enable tunability switchability and angular robustness

    doi: 10.1038/s41598-025-99995-6

    Figure Lengend Snippet: (a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL Multiphysics, this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.

    Article Snippet: To further validate these findings, Fig. (b) presents 2D electric field maps simulated using COMSOL Multiphysics for two representative chemical potentials: μc = 0 eV (top) and μc = 1 eV (bottom).

    Techniques: