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3d finite-difference time-domain (fdtd) simulations  (ANSYS inc)

 
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    ANSYS inc 3d finite-difference time-domain (fdtd) simulations
    3d Finite Difference Time Domain (Fdtd) Simulations, 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
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    Average 90 stars, based on 1 article reviews
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    Article Title: Deterministic Fabrication of Plasmonic Nanostructures on Optical Nanofibers via Blurred Electron Beam Deposition.
    Article Snippet: Numerical Simulations: A Finite Difference Time Domain model (FDTD, Ansys Lumerical Solutions) was developed to simulate the nanostructure and assess both scattering spectra and electromagnetic field polarization under the influence of the TNF’s fundamental mode propagation.

    Article Title: Numerical Analysis of a SiN Digital Fourier Transform Spectrometer for a Non-Invasive Skin Cancer Biosensor
    Article Snippet: Additionally, wherever waveguides of different widths are connected, optimized linear tapers are used, each with a length of 10 μ m. These tapers were designed and simulated using the Finite-Difference Time-Domain (FDTD) tool from Ansys Lumerical 2024 to obtain the S-parameters while adhering to the NanoSOI design constraints.

    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
    Article Snippet: The 3D finite-difference time-domain (FDTD) simulations are performed using the commercial solution ANSYS Lumerical.

    Article Title: Phase and amplitude gradient waveguide coupled metasurfaces.
    Article Snippet: Numerical simulations were carried out using a commercially available 3D finite-difference time-domain (FDTD) solver (Ansys Lumerical FDTD simulation suite).

    Article Title: Numerical Analysis of a SiN Digital Fourier Transform Spectrometer for a Non-Invasive Skin Cancer Biosensor.
    Article Snippet: These tapers were designed and simulated using the Finite-Difference Time-Domain (FDTD) tool from Ansys Lumerical 2024 to obtain the S-parameters while adhering to the NanoSOI design constraints.



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    a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. <t>FDTD</t> simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.
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    a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. <t>FDTD</t> simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.
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    a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. <t>FDTD</t> simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.
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    a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. <t>FDTD</t> simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.
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    a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. <t>FDTD</t> simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.
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    a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. <t>FDTD</t> simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.
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    a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. FDTD simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.

    Journal: bioRxiv

    Article Title: Intracellular photonic crystals in photosynthetic sea slugs form via a kidney-mediated biomineralisation pathway

    doi: 10.64898/2026.05.07.723475

    Figure Lengend Snippet: a) Bright-field upright optical microscope (Zeiss axioscope, 63X WI objective) of calcophores on the dorsal surface of E. viridis , showing both homogenous ‘glassy’ colour (right), and striped, opalescent ‘crystalline’ optical texture (left). Exposure time for ‘glassy’ images is 2.5X that of ‘crystalline’ ones. Scale bar, 20 µ m. b) Reciprocal space (K-space) images for calcophores showing both ‘glassy’ (bottom) and ‘crystalline’ (top) type optical appearance corresponding to real space images in a , glassy K-space images show homogenous colouring, with a very slight blue shift at high angles. Crystalline K-space images show a strong blue shift at higher scattering angles, and a highly textured, hexagonal colour distribution corresponding to the angular response of the photonic crystals. The edge of the circle in the K-space images corresponds to NA = 0.9 (scattering at 42 ° ). Images taken with Zeiss axioscope, 63X WI objective. c) Dark-field upright optical microscope images of a cluster of calcophores before and after 20 minutes exposure to air. Dark orange carotenoid volumes (top and bottom left) can be used as markers to correlate the calcophores in the two images. Of the 7 calcophores in the cluster 4 of them show a blue-shift. Scale bar, 50 µ m. FDTD simulations of 5 µ m diameter spherical photonic structures found in E. viridis . A gaussian beam of radius 1.25 µ m was used for all simulations. The particles have been simplified to perfect spheres. d) Simulated spectra for a correlated structure (photonic glass), with particle sizes varying from 140 - 200 nm. e) Simulated spectra for expanded FCC photonic crystal with particle-to-particle distances varying from 1 d to 2 d (where d is the diameter of one particle, in this case 160 ± 5 nm). The (111) plane is perpendicular to the detector for simulations. f) Simulated spectra for close packed spheres with polycrystallinity i.e. the simulated structure is composed of multiple crystallographic volumes for d = 140 - 200 nm. g) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic glass-like response. Spectra are normalised to a silver mirror. h) Experimental bright field spectra (Zeiss axioscope, 63X WI objective, 50 µ m fibre) spectra of E. viridis photonic calcophores, showing photonic crystal-like response. Spectra are normalised to a silver mirror.

    Article Snippet: To match the optical properties of the photonic structures described here to those observed by electron microscopy and to demonstrate an expanded-FCC lattice that captures the measured optical response, we used finite-difference time-domain (FDTD) calculations on structures generated by molecular dynamics ( ).

    Techniques: Microscopy