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finite- difference time- domain (fdtd) method using ansys lumerical fdtd  (ANSYS inc)

 
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    ANSYS inc finite- difference time- domain (fdtd) method using ansys lumerical fdtd
    Finite Difference Time Domain (Fdtd) Method Using Ansys Lumerical Fdtd, supplied by ANSYS 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/fdtd+method/finite+difference+time+domain++fdtd++simulations/pm40397752-142-18-18
    Average 90 stars, based on 1 article reviews
    finite- difference time- domain (fdtd) method using ansys lumerical fdtd - by Bioz Stars, 2026-09
    90/100 stars

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    Article Snippet: MATERIALS AND METHODS Simulation of PhC band structure We use the finite- difference time- domain (FDTD) method using Ansys Lumerical FDTD to calculate the photonic band structure of a 2D PhC (37, 39, 52, 53).

    Article Title: Microsphere-assisted generation of localized optical emitters in 2D hexagonal boron nitride
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    Article Title: On-Chip Array Fluorescent Sensor for High-Sensitivity Multi-Gas Detection.
    Article Snippet: Fluorescence array sensors provide an effective strategy to mitigate the cross-reactivity of single fluorescence materials by exploiting their high dimensionality and exceptional sensitivity.. However, conventional fluorescent sensing arrays are often hindered by complex and bulky designs, resulting in low costeffectiveness and severely restricting their potential for integration into compact sensing devices.. Benefiting from its high integration advantage, photonic integration technology offers a promising solution for developing low-cost and miniaturized fluorescent gas sensor arrays.

    Article Title: Roughness-dependent scaling of the contact area and separation gap with pressure for glassy polymers.
    Article Snippet: To determine the average absorbance for a 1- μm × 1- μm area, we have used the finite difference time domain (FDTD) solver (Ansys Lumerical FDTD) for the three PMMA rough surfaces as a function of gap thickness for a known angle of incidence and the complex refractive indices of Ge and PMMA.

    Article Title: Supporting Information: Postfabrication Tuning of Circular Bragg Resonators for Enhanced Emitter-Cavity Coupling
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    Schematic diagram of microsphere-assisted fs-laser fabrication of hBN emitters and simulations. (a) Experimental design of the MPM with spacer over the hBN flake surface on the SiO 2 /Si substrate. Bottom: Side view of microsphere enhancement of the fs-laser focus. (b)–(e) <t>FDTD</t> simulation of the light field distribution of the MPM focus: (b) light distribution in the xz -plane and intensity distribution along the z -axis with direct contact between the MPM and the substrate. (c) Light distribution in the xy -plane and intensity distribution along the y -axis at the maximum intensity position with direct contact. (d) Light distribution in the xz -plane and intensity distribution along the z -axis with a 6 µm distance between hBN and microsphere. (e) Light distribution in the xy -plane and intensity distribution along the y -axis at the maximum intensity position with a 6 µm distance.
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    Schematic diagram of microsphere-assisted fs-laser fabrication of hBN emitters and simulations. (a) Experimental design of the MPM with spacer over the hBN flake surface on the SiO 2 /Si substrate. Bottom: Side view of microsphere enhancement of the fs-laser focus. (b)–(e) FDTD simulation of the light field distribution of the MPM focus: (b) light distribution in the xz -plane and intensity distribution along the z -axis with direct contact between the MPM and the substrate. (c) Light distribution in the xy -plane and intensity distribution along the y -axis at the maximum intensity position with direct contact. (d) Light distribution in the xz -plane and intensity distribution along the z -axis with a 6 µm distance between hBN and microsphere. (e) Light distribution in the xy -plane and intensity distribution along the y -axis at the maximum intensity position with a 6 µm distance.

    Journal: Nanophotonics

    Article Title: Microsphere-assisted generation of localized optical emitters in 2D hexagonal boron nitride

    doi: 10.1515/nanoph-2024-0625

    Figure Lengend Snippet: Schematic diagram of microsphere-assisted fs-laser fabrication of hBN emitters and simulations. (a) Experimental design of the MPM with spacer over the hBN flake surface on the SiO 2 /Si substrate. Bottom: Side view of microsphere enhancement of the fs-laser focus. (b)–(e) FDTD simulation of the light field distribution of the MPM focus: (b) light distribution in the xz -plane and intensity distribution along the z -axis with direct contact between the MPM and the substrate. (c) Light distribution in the xy -plane and intensity distribution along the y -axis at the maximum intensity position with direct contact. (d) Light distribution in the xz -plane and intensity distribution along the z -axis with a 6 µm distance between hBN and microsphere. (e) Light distribution in the xy -plane and intensity distribution along the y -axis at the maximum intensity position with a 6 µm distance.

    Article Snippet: Numerical simulations of the electromagnetic field were conducted using a finite-difference time-domain (FDTD) method in Ansys Lumerical FDTD for focusing analysis, and a finite element method (FEM) in COMSOL Multiphysics for optical WGMs.

    Techniques: