Chinese Optics Letters, Volume. 22, Issue 8, 082601(2024)

Wide-color-gamut, high-purity, and high-brightness thin film structural colors based on modified Fano resonant structure

Weijie Chen1,2, Zexiang He1,2, Zhenzhen Duan1,2, Jian Yang1,2, Ning Wang1,2, Dan Wang1,2, Zexiong Hu1,2, Nan Chen1,2, Zhengqian Luo1,2, and Yikun Bu1,2、*
Author Affiliations
  • 1School of Electronic Science and Engineering (National Model Microelectronics College), Xiamen University, Xiamen 361005, China
  • 2Fujian Key Laboratory of Ultrafast Laser Technology and Applications, Xiamen University, Xiamen 361005, China
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    Figures & Tables(7)
    (a) Schematic graph of film stack based on Fano resonance Sub/Ag/LaTiO3/Ag/MgF2/GST/air (MD2MD1A); (b) calculated (left, ‘-desi’) and measured (right, ‘-expt’) reflectance of film stacks using LaTiO3 (bottom) or TiO2 (top) as D2 layer (the optical thickness was kept the same); (c) effective interface method.
    (a) Phase shift and reflectance of MDM structure (data from: Ag/LaTiO3/Ag); (b) phase shift and reflectance of MA (data from: Ag/GST); (c) coupling of different damping rate oscillators or structures (MDM + MA); (d) phase shift and reflectance of coupled structure, MDMA (data from: Ag/LaTiO3/Ag/GST).
    Four different Fano structures with varied continuum states and the same bound state. (a) MDMD (data from: Ag/LaTiO3/Ag/MgF2); (b) MDMA (data from: Ag/LaTiO3/Ag/GST); (c) MDMAD (data from: Ag/LaTiO3/Ag/GST/MgF2); (d) MDMDA structure (data from: Ag/LaTiO3/Ag/MgF2/GST); color blocks beside are the calculated colors for (a), (b), (c), and (d) from top to bottom.
    (a) Phase curves and (b) reflectance spectra of these two states: Ag/LaTiO3/Ag and Ag/MgF2/GST, and their coupling unit Ag/LaTiO3/Ag/MgF2/GST (three graphs from top to bottom); (c) change in the thickness of LaTiO3 to tune the abrupt phase change created by Ag/LaTiO3/Ag.
    Total structure: Ag (100 nm)/LaTiO3/Ag (14 nm)/MgF2 (42 nm)/GST (7.5 nm). (a) Color palette calculated by varying the thickness of the dielectric LaTiO3 from 45 to 120 nm when the gap is fixed at 5 nm; (b) reflectance spectra calculated by varying the LaTiO3 from 45 to 125 nm at an interval of 10 nm; (c) color gamut in CIE 1931 chromaticity diagram to compare our structure with F–P cavities, sRGB gamut, and Adobe RGB gamut. The incidence angle is 0 deg. “Fano (single layer)” and “Fano (two layers)” mean the color range gotten by altering the thickness of one single layer (LaTiO3) and two layers (LaTiO3, MgF2).
    Calculated and measured optical spectra of the structure proposed here. (a) Red sample; (b) green sample; (c) blue sample; (d) picture of three samples taken at an angle of less than 5 deg.
    • Table 1. Thickness of Each Layer for Red, Green, and Blue Colors (in nm)

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      Table 1. Thickness of Each Layer for Red, Green, and Blue Colors (in nm)

       RedGreenBlue
      Ag100100100
      LaTiO36085100
      Ag141414
      MgF2424242
      Ge2Sb2Te57.57.57.5
      Total thickness223.5248.5263.5
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    Weijie Chen, Zexiang He, Zhenzhen Duan, Jian Yang, Ning Wang, Dan Wang, Zexiong Hu, Nan Chen, Zhengqian Luo, Yikun Bu, "Wide-color-gamut, high-purity, and high-brightness thin film structural colors based on modified Fano resonant structure," Chin. Opt. Lett. 22, 082601 (2024)

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    Paper Information

    Category: Physical Optics

    Received: Mar. 7, 2024

    Accepted: Apr. 24, 2024

    Published Online: Aug. 22, 2024

    The Author Email: Yikun Bu (buyikun0522@xmu.edu.cn)

    DOI:10.3788/COL202422.082601

    CSTR:32184.14.COL202422.082601

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