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

 
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    ANSYS inc finite-difference time-domain (fdtd) method in ansys lumerical fdtd
    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.
    Finite Difference Time Domain (Fdtd) Method In 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/pmc12273537-156-15-15
    Average 90 stars, based on 1 article reviews
    finite-difference time-domain (fdtd) method in ansys lumerical fdtd - by Bioz Stars, 2026-09
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    1) Product Images from "Microsphere-assisted generation of localized optical emitters in 2D hexagonal boron nitride"

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

    Journal: Nanophotonics

    doi: 10.1515/nanoph-2024-0625

    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.
    Figure Legend 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.

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    Article Title: Polarisation Control in Arrays of Microlenses and Gratings: Performance in Visible–IR Spectral Ranges
    Article Snippet: To investigate the performance of the GO polariser with different geometrical parameters in the IR region, the numerical modelling was simulated with the finite-difference time-domain (FDTD, Lumerical, Ansys) method with wavelengths from 3 to 10 μ m. The GO polariser was modelled as one GO ribbon and an adjacent air groove with the periodic boundary condition ( ). displays the main results of the parameter study as the simulated IR transmittance spectra of the GO polariser with different geometrical parameters P , w and d under both the TE and TM incident polarisations and the difference between them.

    Article Title: Photonic crystal enhanced light emitting diodes fabricated by single pulse laser interference lithography
    Article Snippet: Integration of photonic crystal (PhC) configurations onto the surfaces of light-emitting diodes (LEDs) can play an important role in enhancing light extraction efficiency.. While the literature is rich with various PhC fabrication approaches, there is a need for high throughput methods that are appropriate for low-cost devices.. In this paper, we report the use of single pulse laser interference lithography (LIL) for the fabrication of photonic crystal structures on LEDs.

    Article Title: Design and Modeling of a Fully Integrated Microring-Based Photonic Sensing System for Liquid Refractometry.
    Article Snippet: The frequency response of the MRR sensor was calculated using the FDTD (Finite Difference Time Domain) method in the Ansys Lumerical software as follows: a simulation time of 7000 fs, a mesh accuracy of 3, and a minimum mesh step of 0.25 nm.

    Article Title: Directive giant upconversion by supercritical bound states in the continuum.
    Article Snippet: The radiation properties of the PCNS were evaluated using the FDTD method in Ansys Lumerical.



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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) <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) <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.

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