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    ANSYS inc commercial implementation of the finite-difference time-domain method
    Commercial Implementation Of The Finite Difference Time Domain Method, 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: Orientation Sensitive SEIRA Sensors Based on Single-Walled Carbon Nanotube Near Fields.
    Article Snippet: Numerical simulations of plasmon resonances in SWCNTs: Plasmon resonances in SWCNTs were simulated using the finite-difference time-domain method (Ansys).

    Article Title: Electrochemical Control of Strong Coupling of CdSe Exciton-Polaritons in Plasmonic Cavities.
    Article Snippet: To identify the modes measured in the dispersion diagram of the uncoupled Al nanoparticle lattice cavity, we performed finite-difference time-domain (FDTD) simulations (Lumerical Package, Ansys).

    Article Title: Highly efficient coupling of single photons using a pair of nanostructures
    Article Snippet: The finite difference time domain (FDTD) method (FDTD package, Ansys) is used to perform numerical simulations (Garcia et al. 2005).

    Article Title: Modeling and Design of GeSn Avalanche Photodiodes With High Tin Content for Applications at 3.3 μm
    Article Snippet: Finite-Difference Time Domain (FDTD) simulations were carried out by a commercial software (Ansys Lumerical) and a valid combination could be found: h = 2.25 μm, P = 1.75 μm and r ∼ 250 ÷ 525 nm.

    Article Title: Surface Lattice Resonance Lasers with Epitaxial InP Gain Medium
    Article Snippet: Moreover, we performed finite-difference time-domain simulations with ANSYS Lumerical to obtain the dispersion of the modes of the system and explain additional emission modes.

    Article Title: Strong Chiro-Optical Activity of Plasmonic Metasurfaces with Inverted Pyramid Arrays
    Article Snippet: To validate our experimental results, we performed numerical simulations using the finite-difference time-domain (FDTD) method (Ansys FDTD-Solutions, Lumerical).

    Article Title: Chirality conferral enables the observation of hyper-Raman optical activity
    Article Snippet: Simulations of the nanohelices were performed using finite-difference time-domain simulations in ANSYS-Lumerical.

    Article Title: Plasmon-Enhanced Multiphoton Polymer Crosslinking for Selective Modification of Plasmonic Hotspots
    Article Snippet: The geometry, which enables matching of the LSPR wavelength λ LSPR with that of NIR fs laser λ L , was identified by using finite-difference time-domain (Ansys Lumerical FDTD) simulations.



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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