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three-dimensional finite difference time domain simulation fdtd rsoft 9.0 fullwave  (Rsoft Inc)

 
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    Rsoft Inc three-dimensional finite difference time domain simulation fdtd rsoft 9.0 fullwave
    Three Dimensional Finite Difference Time Domain Simulation Fdtd Rsoft 9.0 Fullwave, supplied by Rsoft 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/finite+difference/finite+difference+time+domain+fdtd+method+using+rsoft+fullwave+version+6+0/us09640777-106-30-36
    Average 90 stars, based on 1 article reviews
    three-dimensional finite difference time domain simulation fdtd rsoft 9.0 fullwave - by Bioz Stars, 2026-11
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    Article Title: Integrated optic/nanofluidic fluorescent detection device with plasmonic excitation
    Article Snippet: Integrated optic/microfluidic devices have proven to be useful tools in many sensing applications.. However, the resolution and sensitivity of existing devices is limited by the processes and materials chosen for their fabrication.. A procedure for the production of a new family of low-noise, high-resolution integrated microfluidic optical detection devices is presented, along with results from a prototype device.

    Article Title: Surface Enhanced Raman Scattering on a Single Nanometric Aperture
    Article Snippet: Arrays of nanoapertures have been demonstrated to realize efficient, robust, and reproducible substrates for surface-enhanced Raman scattering SERS spectroscopy.. However, little attention has been devoted to single nanoapertures, although a thorough understanding of the SERS phenomenon in a single aperture is essential for the rationale optimization of nanoaperture arrays SERS.. In this study, single nanoapertures milled in optically thick gold films are quantitatively evaluated for the first time to determine the SERS enhancement factors using para-mercaptoaniline as nonresonant analyte.

    Article Title: Multi-focus parallel detection of fluorescent molecules at picomolar concentration with photonic nanojets arrays
    Article Snippet: The electromagnetic field distribution in the vicinity of microspheres was computed using a 3D finite-difference time-domain method (FDTD) (Rsoft Fullwave 6.0 commercial software) when illuminated with a Gaussian beam with a full width at half maximum of 10.0 lm corresponding to the experimental conditions (Fig. 2).

    Article Title: Heterogeneous laser with high efficiency and method for manufacturing the laser
    Article Snippet: To calculate the nanostructured elements, like the reflectivity of first and second reflectors 14a, 14b, the trenches of array 15 for the coupling with an optical fiber 16, the finite-difference time-domain FDTD method of RSOFT® module Fullwave may be used.

    Article Title: Colloidal quantum dots as probes of excitation field enhancement in photonic antennas.
    Article Snippet: Heykel Aouani, Stella Itzhakov, David Gachet, Eloı̈se Devaux, Thomas W. Ebbesen, Hervé Rigneault, Dan Oron, and Jérôme Wenger* Institut Fresnel, Aix-Marseille Université, CNRS, Ecole Centrale Marseille, Campus de St Jérôme, 13397 Marseille, France, Department of Physics of Complex Systems, Weizmann Institute of Science, Rehovot 76100, Israel, and Institut de Science et d’Ingénierie Supramoléculaires, Université de Strasbourg, CNRS, 8 allée G. Monge, 67000 Strasbourg, France

    Generated:

    Article Title: Electroluminescent devices with improved optical out-coupling and external quantum efficiencies
    Article Snippet: .. To get more insights of how the ITO nanomesh device configuration enhances coupling of internally generated light into the substrate and air, optical simulation was conducted by combining the three-dimensional finite difference time domain simulation (FDTD, Rsoft 9.0 FullWave, Synosys Inc.) for near-field behaviors near the active region and the ray-tracing simulation (LightTools 8.2, Synosys Inc.) for far-field behaviors in the substrate and air. ..

    Software:

    Article Title: Optically stitched arbitrary fan-sectors with selective polarization states for dynamic manipulation of surface plasmon polaritons
    Article Snippet: .. We employ a commercial three-dimensional FDTD software (Rsoft 8.01) to simulate the SPPs intensity distribution. ..



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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