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Performance of Transparent Metallic Thin Films
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    C: Physical Properties of Materials and Interfaces

    Performance of Transparent Metallic Thin Films
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    The Journal of Physical Chemistry C

    Cite this: J. Phys. Chem. C 2021, 125, 29, 16334–16342
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    https://doi.org/10.1021/acs.jpcc.1c04832
    Published July 19, 2021
    Copyright © 2021 American Chemical Society

    Abstract

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    The ability to maintain high electrical conductivity and optical transparency simultaneously under mechanical deformation has made transparent metallic films (TMFs) the best candidates among transparent conductive films (TCFs). However, there is a lack of suitable models to predict the overall performance of the TMFs. Here, empirical relationships for resistance Rs based on the network resistor model, Kirchoff’s rules, and the thickness-dependent resistivity and transmission T based on the effective medium theory, the geometric model, and the Beer–Lambert law are proposed. A systematic thickness t- and perforation area ratio PR-dependent study on the silver nanohole array TMF has been performed. Both models fit well with our experimental data as well as the data reported in the literature, regardless of the lattice structure of the TMFs. A general and comprehensive figure-of-merit (FOM) expression for TMFs, Φ = Tβ/Rs, is obtained. Both the experimental data and the theoretical predictions show that β = 5 is better to characterize the performance of nanohole array TMFs as compared to β = 10 for TCFs. The observed empirical models and the FOM expression not only can be used to assess the overall quality of any type of TMFs but also provide guidance for fabrication.

    Copyright © 2021 American Chemical Society

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    Supporting Information

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    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.jpcc.1c04832.

    • Schematic of the resistors R0 of the infinite two-dimensional hexagonal resistor lattice and tetragonal resistor lattice, T(λ) of the Ag thin film with different t, FDTD-calculated T(λ) of the Ag NH array with different t (L = 500 nm, D = 340 nm) and different η (L = 500 nm, t = 50 nm), SEM images of the Ag NH array with different L and different D, T(λ) of the Ag NH array with different t (L = 500 nm, D = 340 nm and L = 720 nm, D = 613 nm), T(λ) of the Ag NH array with different D (L = 500 nm, t = 50 nm), and fitting results in Figure 4 (PDF)

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    The Journal of Physical Chemistry C

    Cite this: J. Phys. Chem. C 2021, 125, 29, 16334–16342
    Click to copy citationCitation copied!
    https://doi.org/10.1021/acs.jpcc.1c04832
    Published July 19, 2021
    Copyright © 2021 American Chemical Society

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