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

 
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    ANSYS inc finite-difference time-domain (fdtd) algorithm ansys lumerical fdtd
    Experimental and computational optical characteristics around left-handed Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from <t>FDTD</t> simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with a wavelength of 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.
    Finite Difference Time Domain (Fdtd) Algorithm 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+algorithm/pmc11487658-31-18-22?v=ANSYS+inc
    Average 90 stars, based on 1 article reviews
    finite-difference time-domain (fdtd) algorithm ansys lumerical fdtd - by Bioz Stars, 2026-07
    90/100 stars

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    1) Product Images from "Achiral Plasmonic Antennas Enhance Differential Absorption To Increase Preferential Detection of Chiral Single Molecules"

    Article Title: Achiral Plasmonic Antennas Enhance Differential Absorption To Increase Preferential Detection of Chiral Single Molecules

    Journal: ACS Measurement Science Au

    doi: 10.1021/acsmeasuresciau.4c00026

    Experimental and computational optical characteristics around left-handed Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with a wavelength of 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.
    Figure Legend Snippet: Experimental and computational optical characteristics around left-handed Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with a wavelength of 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.

    Techniques Used:

    Experimental and computational optical characteristics around achiral Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with wavelength 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.
    Figure Legend Snippet: Experimental and computational optical characteristics around achiral Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with wavelength 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.

    Techniques Used:



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    Image Search Results


    Experimental and computational optical characteristics around left-handed Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with a wavelength of 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.

    Journal: ACS Measurement Science Au

    Article Title: Achiral Plasmonic Antennas Enhance Differential Absorption To Increase Preferential Detection of Chiral Single Molecules

    doi: 10.1021/acsmeasuresciau.4c00026

    Figure Lengend Snippet: Experimental and computational optical characteristics around left-handed Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with a wavelength of 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.

    Article Snippet: Full-field electromagnetic simulations of Au NP dimer antennas excited by an incident plane wave were performed with a finite-difference time-domain (FDTD) algorithm (Ansys Lumerical FDTD) as described previously.

    Techniques:

    Experimental and computational optical characteristics around achiral Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with wavelength 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.

    Journal: ACS Measurement Science Au

    Article Title: Achiral Plasmonic Antennas Enhance Differential Absorption To Increase Preferential Detection of Chiral Single Molecules

    doi: 10.1021/acsmeasuresciau.4c00026

    Figure Lengend Snippet: Experimental and computational optical characteristics around achiral Au NP dimer antennas under left and right circularly polarized light (LCP and RCP, respectively). (a) Distributions of the intensities of molecules detected at the center of the Au NP dimer antenna (apparent position within the red circle; radius = 12.5 nm). (b–e) Profiles in the sample plane calculated from FDTD simulations of Au NP dimer antennas excited by a circularly polarized plane wave incident along the z -axis with wavelength 635 nm. (b, c) Electric field enhancement profiles under (b) left and (c) right circularly polarized excitation. (d, e) Optical chirality enhancement profiles under (d) left and (e) right circularly polarized excitation.

    Article Snippet: Full-field electromagnetic simulations of Au NP dimer antennas excited by an incident plane wave were performed with a finite-difference time-domain (FDTD) algorithm (Ansys Lumerical FDTD) as described previously.

    Techniques: