• Photonics Research
  • Vol. 1, Issue 4, 154 (2013)
Mehrdad Irannejad*, Mustafa Yavuz, and Bo Cui
Author Affiliations
  • Waterloo Institute for Nanotechnology, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada
  • show less
    DOI: 10.1364/PRJ.1.000154 Cite this Article Set citation alerts
    Mehrdad Irannejad, Mustafa Yavuz, Bo Cui. Finite difference time domain study of light transmission through multihole nanostructures in metallic film[J]. Photonics Research, 2013, 1(4): 154 Copy Citation Text show less
    Schematic diagram of the studied unit cells of infinite periodic arrays of (a) a single subwavelength hole and (b) dissimilar vertical chain holes with hole depths of 100 nm, structural period of P, and hole radii of R.
    Fig. 1. Schematic diagram of the studied unit cells of infinite periodic arrays of (a) a single subwavelength hole and (b) dissimilar vertical chain holes with hole depths of 100 nm, structural period of P, and hole radii of R.
    FDTD calculated transmission spectrum of single-hole array of fixed hole depth of 100 nm, different hole radii in the range of 50–80 nm, and structural periodicity of (a) P=400 nm, (b) P=450 nm, (c) P=500 nm, and (d) P=550 nm. The incident EM field was polarized along y axis.
    Fig. 2. FDTD calculated transmission spectrum of single-hole array of fixed hole depth of 100 nm, different hole radii in the range of 50–80 nm, and structural periodicity of (a) P=400nm, (b) P=450nm, (c) P=500nm, and (d) P=550nm. The incident EM field was polarized along y axis.
    Transmittance spectra of three similar hole chain array of fixed hole depth of 100 nm, hole radius of 50 nm, and different structural periodicities. The incident EM field was linearly polarized along the y axis.
    Fig. 3. Transmittance spectra of three similar hole chain array of fixed hole depth of 100 nm, hole radius of 50 nm, and different structural periodicities. The incident EM field was linearly polarized along the y axis.
    Transmittance spectra of three-hole chain arrays of fixed hole depth of 100 nm, different side-hole radii, and structural periodicities of (a) P=400 nm, (b) P=450 nm, (c) P=500 nm, and (d) P=550 nm. The incident EM field was linearly polarized along the y axis.
    Fig. 4. Transmittance spectra of three-hole chain arrays of fixed hole depth of 100 nm, different side-hole radii, and structural periodicities of (a) P=400nm, (b) P=450nm, (c) P=500nm, and (d) P=550nm. The incident EM field was linearly polarized along the y axis.
    Transmittance spectra of three-hole chain arrays of fixed hole depth of 100 nm, different side-hole radii, Rs, and structural periodicities of (a) P=400 nm, (b) P=450 nm, (c) P=500 nm, and (d) P=550 nm. The incident EM field was linearly polarized along the x axis.
    Fig. 5. Transmittance spectra of three-hole chain arrays of fixed hole depth of 100 nm, different side-hole radii, Rs, and structural periodicities of (a) P=400nm, (b) P=450nm, (c) P=500nm, and (d) P=550nm. The incident EM field was linearly polarized along the x axis.
    FDTD calculated electric profile of the (1,0) resonance mode of three-hole chain arrays at different incident light polarization and structural periodicities. The top row shows the electric profile of the three-hole chain array of periods of (a) 400 nm, (b) 450 nm, (c) 500 nm, and (d) 550 nm under illumination of an x-polarized EM field. The bottom row is for a y-polarized incident EM field and periods of (e) 400 nm, (f) 450 nm, (g) 500 nm, and (h) 550 nm.
    Fig. 6. FDTD calculated electric profile of the (1,0) resonance mode of three-hole chain arrays at different incident light polarization and structural periodicities. The top row shows the electric profile of the three-hole chain array of periods of (a) 400 nm, (b) 450 nm, (c) 500 nm, and (d) 550 nm under illumination of an x-polarized EM field. The bottom row is for a y-polarized incident EM field and periods of (e) 400 nm, (f) 450 nm, (g) 500 nm, and (h) 550 nm.
     Resonance Wavelength (nm)
      FDTDTheory (Eq. 2)
      Air/FilmFilm/SubAir/FilmFilm/Sub
    PeriodGold Transmission0,11,10,11,10,11,10,11,1
    400480370690593417295662468
    450480363746611469332745527
    500480581810638521368827585
    550480615371877669573405910643
    Table 1. Resonance Wavelength Position of a Square Single-Hole Array Perforated on the Silica-Supported Gold Film with Hole Radius of 50 nm, Hole Depth of 100 nm, and Different Structural Periodicitiesa
      TchainEnhancement TchainEnhancement
    PeriodTsingley-axis polarizedy-axis polarizedTsinglex-axis polarizedx-axis polarized
    4000.0830.121.440.0830.192.29
    4500.0580.0851.460.0580.132.24
    5000.0340.0521.530.0340.0772.26
    5500.0170.0251.470.0170.0412.41
    Table 2. Optical Transmission and Transmittance Enhancement of the (1,0) Peak of the Three-Hole Chain Array Relative to the Single-Hole Array at Different Structural Periods, Rs=25nm, R=Rc=80nm, and Different Incident EM Field Polarization
    PeriodRb(nm)y(nm)FWHM (nm)Rb(nm)y(nm)FWHM (nm)
    4002523.3355506.67175
    4502531.67365511.6792
    501575608.33152
    655273
    5002540306513.3385
    5023.33417010121
    552048756.67195
    6016.676280
    5502548.33296521.6740
    5031.67337018.3350
    5528.3335751572
    6025378011.67101
    Table 3. FWHM of the (1,0) Resonance Mode of Three-Hole Chain Arrays as a Function of Vertical Distance between Holes (y) at Different Structural Periodsa
    Mehrdad Irannejad, Mustafa Yavuz, Bo Cui. Finite difference time domain study of light transmission through multihole nanostructures in metallic film[J]. Photonics Research, 2013, 1(4): 154
    Download Citation