3d fdtd simulation code Search Results


3d finite-difference time-domain (fdtd) simulations  (Lumerical Solutions)
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3d Finite Difference Time Domain (Fdtd) Simulations, supplied by Lumerical Solutions, 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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finite-difference time-domain (fdtd) simulations  (Rsoft Inc)
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Rsoft Inc finite-difference time-domain (fdtd) simulations
Finite Difference Time Domain (Fdtd) Simulations, 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
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3d fdtd fullwave 6.1  (Rsoft Inc)
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software lumerical solutions v8.17.1157  (Lumerical Solutions)
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3d fdtd method  (ANSYS inc)
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3d finite-differencetime-domain (fdtd) simulation  (ANSYS inc)
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ANSYS inc 3d finite-differencetime-domain (fdtd) simulation
3d Finite Differencetime Domain (Fdtd) Simulation, 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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3-d finite-difference timedomain method  (Time Domain Corporation)
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Time Domain Corporation 3-d finite-difference timedomain method
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finite-difference time-domain simulations  (Lumerical Solutions)
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Lumerical Solutions finite-difference time-domain simulations
Finite Difference Time Domain Simulations, supplied by Lumerical Solutions, 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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3d electromagnetic simulator fdtd solver 2023 r1  (Lumerical Solutions)
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Lumerical Solutions 3d electromagnetic simulator fdtd solver 2023 r1
3d Electromagnetic Simulator Fdtd Solver 2023 R1, supplied by Lumerical Solutions, 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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fdtd 3d electromagnetic simulator  (ANSYS inc)
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ANSYS inc fdtd 3d electromagnetic simulator
a AFM measurement performed on the surface of the DBR/DBR Schlieren cavity showing an average roughness R a = 2.6 nm. Scale bar, 2 μm. b TMCs of the reflectivity of DBR/DBR cavities with aligned 15% β-phase PFO at the design thickness for a resonance at 2.65 eV (red line) and assuming a 3 nm thickness increase over the design thickness (blue line). The calculation was performed for light polarized parallel to the alignment of the PFO transition dipole moment. c Calculated LP energy profile for a randomly generated film topography with a correlation length and amplitude matching the Schlieren cavity measured in ( a ). d <t>FDTD</t> simulation of the normalized squared electric field 1443 fs after excitation for the LP energy profile shown in ( c ). e Superposition of data from ( c and d ) illustrating how the electric field is confined to regions of lower LP energy, i.e., to thicker parts of the film.
Fdtd 3d Electromagnetic Simulator, 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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3d finite-difference time-domain (fdtd) simulation  (ANSYS inc)
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ANSYS inc 3d finite-difference time-domain (fdtd) simulation
Lumerical finite-difference time-domain <t>(FDTD)</t> computation for the optical characteristics of the spectra of ( A ) reflection, ( B ) transmission, ( C ) absorption, and ( D ) light absorption enhancement of optical sensing devices based on rippled graphite nanofilm under different stretch:release ratios (0%, 10%, 30%, and 50%).
3d Finite Difference Time Domain (Fdtd) Simulation, 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/result/3d finite-difference time-domain (fdtd) simulation/product/ANSYS inc
Average 90 stars, based on 1 article reviews
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Image Search Results


a AFM measurement performed on the surface of the DBR/DBR Schlieren cavity showing an average roughness R a = 2.6 nm. Scale bar, 2 μm. b TMCs of the reflectivity of DBR/DBR cavities with aligned 15% β-phase PFO at the design thickness for a resonance at 2.65 eV (red line) and assuming a 3 nm thickness increase over the design thickness (blue line). The calculation was performed for light polarized parallel to the alignment of the PFO transition dipole moment. c Calculated LP energy profile for a randomly generated film topography with a correlation length and amplitude matching the Schlieren cavity measured in ( a ). d FDTD simulation of the normalized squared electric field 1443 fs after excitation for the LP energy profile shown in ( c ). e Superposition of data from ( c and d ) illustrating how the electric field is confined to regions of lower LP energy, i.e., to thicker parts of the film.

Journal: Nature Communications

Article Title: Schlieren texture and topography induced confinement in an organic exciton-polariton laser

doi: 10.1038/s41467-025-55875-1

Figure Lengend Snippet: a AFM measurement performed on the surface of the DBR/DBR Schlieren cavity showing an average roughness R a = 2.6 nm. Scale bar, 2 μm. b TMCs of the reflectivity of DBR/DBR cavities with aligned 15% β-phase PFO at the design thickness for a resonance at 2.65 eV (red line) and assuming a 3 nm thickness increase over the design thickness (blue line). The calculation was performed for light polarized parallel to the alignment of the PFO transition dipole moment. c Calculated LP energy profile for a randomly generated film topography with a correlation length and amplitude matching the Schlieren cavity measured in ( a ). d FDTD simulation of the normalized squared electric field 1443 fs after excitation for the LP energy profile shown in ( c ). e Superposition of data from ( c and d ) illustrating how the electric field is confined to regions of lower LP energy, i.e., to thicker parts of the film.

Article Snippet: The simulations were performed using the FDTD 3D Electromagnetic Simulator from Lumerical-Ansys.

Techniques: Generated

Lumerical finite-difference time-domain (FDTD) computation for the optical characteristics of the spectra of ( A ) reflection, ( B ) transmission, ( C ) absorption, and ( D ) light absorption enhancement of optical sensing devices based on rippled graphite nanofilm under different stretch:release ratios (0%, 10%, 30%, and 50%).

Journal: Nanomaterials

Article Title: The Ripple Effect of Graphite Nanofilm on Stretchable Polydimethylsiloxane for Optical Sensing

doi: 10.3390/nano11112934

Figure Lengend Snippet: Lumerical finite-difference time-domain (FDTD) computation for the optical characteristics of the spectra of ( A ) reflection, ( B ) transmission, ( C ) absorption, and ( D ) light absorption enhancement of optical sensing devices based on rippled graphite nanofilm under different stretch:release ratios (0%, 10%, 30%, and 50%).

Article Snippet: To confirm our experimental results, a 3D finite-difference time-domain (FDTD) simulation was conducted using Lumerical FDTD Solutions (Release 2018a, Ansys Ltd., Suite, Montreal, QC, Canada) tools.

Techniques: Transmission Assay

FDTD-simulated electric field intensity distribution of the stretched PDMS/rippled graphite/Si (30%) at 532 nm laser illumination. ( A ) intensity profile at the cross-section through x − z plane, ( B ) intensity profile at the cross-section through x − y plane.

Journal: Nanomaterials

Article Title: The Ripple Effect of Graphite Nanofilm on Stretchable Polydimethylsiloxane for Optical Sensing

doi: 10.3390/nano11112934

Figure Lengend Snippet: FDTD-simulated electric field intensity distribution of the stretched PDMS/rippled graphite/Si (30%) at 532 nm laser illumination. ( A ) intensity profile at the cross-section through x − z plane, ( B ) intensity profile at the cross-section through x − y plane.

Article Snippet: To confirm our experimental results, a 3D finite-difference time-domain (FDTD) simulation was conducted using Lumerical FDTD Solutions (Release 2018a, Ansys Ltd., Suite, Montreal, QC, Canada) tools.

Techniques: