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COMSOL Inc 2d comsol simulations
2d Comsol Simulations, 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/2d+comsol+simulations/comsol+multiphysics/10__1016_slash_j__snr__2024__100273-170-3-4
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2d comsol simulations - by Bioz Stars, 2026-10
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Article Title: Design and optimization of a fluid flow splitting device for low-flow applications.
Article Snippet: Microfluidic devices are defined by the application of fluid flow to micron-scale features.. Inherent to most experiments involving microfluidic devices is the need to precisely and reproducibly control fluid flow at the microliter scale, often through multiple inlet ports on a single device.. While the number of fluid channels per device varies, perfusing multiple inputs requires either the use of multiple flow controllers (often syringe or peristaltic pumps) or the ability to evenly divide fluid across outlets.

Article Title: Planarized THz quantum cascade lasers for broadband coherent photonics.
Article Snippet: We performed 2D COMSOL simulations to evaluate the passive waveguide propagation losses.

Virus:

Article Title: Fast and Sensitive Virus Detection using a Plasmonic Sensor that Integrates Electrokinetically Assisted Sampling and Surface-enhanced Raman Scattering
Article Snippet: We present a novel plasmonic biosensing method for on-chip detection on viral particles featuring a microelectrode platform that integrates accelerated sampling of virus with surface-enhanced Raman scattering (SERS).. We show experimentally that our approach can produce spectacular results owing to the unique incorporation of two key features: (1) Concentration amplification of virus on the SERS-active substrate; (2) Local plasmonic activity enhancement due to the targeted superimposition of silver nanoparticles on the captured virus sites.. When tested for the detection of the M13 bacteriophage our “sandwich” assay yielded excellent reproducibility (signal variation <6 %) and a very low limit of detection (1.13 × 102 pfu/ml).

Sampling:

Article Title: Fast and Sensitive Virus Detection using a Plasmonic Sensor that Integrates Electrokinetically Assisted Sampling and Surface-enhanced Raman Scattering
Article Snippet: We present a novel plasmonic biosensing method for on-chip detection on viral particles featuring a microelectrode platform that integrates accelerated sampling of virus with surface-enhanced Raman scattering (SERS).. We show experimentally that our approach can produce spectacular results owing to the unique incorporation of two key features: (1) Concentration amplification of virus on the SERS-active substrate; (2) Local plasmonic activity enhancement due to the targeted superimposition of silver nanoparticles on the captured virus sites.. When tested for the detection of the M13 bacteriophage our “sandwich” assay yielded excellent reproducibility (signal variation <6 %) and a very low limit of detection (1.13 × 102 pfu/ml).

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Article Title: Planarized THz quantum cascade lasers for broadband coherent photonics.
Article Snippet: .. Here, we performed 2D COMSOL simulations of the waveguide cross-section, where the refractive index of the active region was fixed to 3.6, while the metals were approximated as a perfect electric conductor (PEC). ..

Article Title: Planarized THz quantum cascade lasers for broadband coherent photonics
Article Snippet: .. Here, we performed 2D COMSOL simulations of the waveguide cross-section, where the refractive index of the active region was fixed to 3.6, while the metals were approximated as a perfect electric conductor (PEC). ..



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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 <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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COMSOL Inc 2d flow velocity and 3d electrical field simulations comsol multiphysics v5.4
(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.
2d Flow Velocity And 3d Electrical Field Simulations Comsol Multiphysics V5.4, 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
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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: