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The Broadband Fixed-Angle Source Technique (BFAST) LUMERICAL SOLUTIONS INC. © LUMERICAL SOLUTIONS INC 1

The Broadband Fixed-Angle Source Technique (BFAST) · 2015. 12. 9. · available in the next release of FDTD Solutions (2016A) Accurate broadband results can be obtained from a single

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  • The Broadband Fixed-Angle Source Technique (BFAST)

    LUMERICAL SOLUTIONS INC.

    © LUMERICAL SOLUTIONS INC1

  • OutlineIntroduction• Lumerical’s simulation products• Simulation of periodic structures

    The new Broadband Fixed-Angle Source Technique (BFAST)• Details on BFAST• Limitations• Basic example: transmission through a dielectric stack• Performance considerations

    Application Examples• Lamellar plasmonic grating (2D)• Plasmonic solar cell (3D)

    Summary

    © LUMERICAL SOLUTIONS INC2

  • Introduction

    © LUMERICAL SOLUTIONS INC3

  • Our Products

    FDTD SolutionsNANOPHOTONIC SOLVER (2D/3D)

    MODE SolutionsWAVEGUIDE DESIGN ENVIRONMENT

    spatial distribution of

    charge carriers optical generation rate of charge

    carriers

    INTERCONNECTPHOTONIC INTEGRATED CIRCUIT SIMULATOR

    DEVICECHARGE TRANSPORT

    SOLVER (2D/3D)

    System/Circuit Level

    Component Level: Optical Component Level: Electrical

    © LUMERICAL SOLUTIONS INC4

  • © LUMERICAL SOLUTIONS INC5

    Simulation of Periodic Structures with FDTD

    Large class of systems in photonics is periodic

    Gratings

    Photonics crystals

    Meta-materials

    CMOS sensor arrays and solar cells

  • Example of a basic grating, excited by a plane-wave Problem can be reduced to simulation of a single unit cell

    © LUMERICAL SOLUTIONS INC6

    … …

    Periodicboundaryconditions

    Reduction to a unit cell

  • Tilting the plane-wave source breaks the symmetry

    Bloch’s theorem: 𝐸 𝑥 = 𝐸 𝑥 + 𝑎 𝑒𝑖 𝑘∥ 𝑎

    © LUMERICAL SOLUTIONS INC7

    Blochboundaryconditions

    a

    𝑘

    𝑘∥

    Changing the angle of incidence

    https://en.wikipedia.org/wiki/Bloch_wave

  • Works well for narrow-band simulations around a given center frequency 𝒇𝟎:

    Then 𝑘∥ =2𝜋𝑓0

    𝑐sin(𝜃0) is constant

    Length of the 𝑘-vector is frequency dependent, i.e. 𝑘 = k f =2𝜋𝑓

    𝑐

    For a given frequency range 𝑓min, 𝑓max → 𝑘min, 𝑘max

    As a result, 𝜃 𝑓 = sin−1𝑘∥

    𝑘= sin−1

    𝑓0

    𝑓sin(𝜃0)

    In broadband simulations with Bloch boundary conditions, differentfrequency components are injected at different angles!

    Wavelength-dependence of the angle

    © LUMERICAL SOLUTIONS INC8

    𝑘∥

  • For one or a few fixed angle(s): Run separate narrow-band simulations for each wavelength/frequency

    100 frequency points 100x the computational time!

    To compute an angle-wavelength map Sweep the angle and re-interpolate the data

    Current solutions to obtain broadband results

    © LUMERICAL SOLUTIONS INC9

    https://kb.lumerical.com/en/ref_sim_obj_bloch_broadband_sweep.html

    https://kb.lumerical.com/en/ref_sim_obj_bloch_broadband_sweep.html

  • The Broadband Fixed-Angle Source Technique (BFAST)

    AVAILABLE IN RELEASE 2016A

    © LUMERICAL SOLUTIONS INC10

  • Details on BFASTBFAST allows to inject light at a fixed angle over a broad spectrum!

    BFAST is not just a new type of boundary condition. The core algorithm is different from standard FDTD!

    It is based on the split-field method, but was customized to ensure compatibility with most existing material models and monitors!

    © LUMERICAL SOLUTIONS INC11

  • Limitations of BFASTTwo fundamental limitations:

    1. Nonlinear and all flexible material plugin materials will not function using BFAST.

    2. Injection above the critical angles for total internal reflection (TIR) is not stable.

    © LUMERICAL SOLUTIONS INC12

  • Basic ExampleTransmission through a dielectric stack (4 layers)

    © LUMERICAL SOLUTIONS INC13

    𝑙1 = 2.5𝜇𝑚 𝑙2 = 2.5𝜇𝑚Broadband source(0.8𝜇𝑚 – 1.6𝜇𝑚)

    n=1.5 n=2.5 n=1.5n=1.0

    Frequency domainmonitor

  • Results

    © LUMERICAL SOLUTIONS INC14

  • Results (20 deg)

    © LUMERICAL SOLUTIONS INC15

  • Results (40 deg)

    © LUMERICAL SOLUTIONS INC16

  • Results (60 deg)

    © LUMERICAL SOLUTIONS INC17

  • Performance ConsiderationsBFAST simulations take more time than identical simulations with Bloch boundary conditions.

    Two contributions:

    1. Angle-independent overhead: 1.5x - 4x

    2. Angle-dependent factor: Δ𝑡~(1 − sin𝜃)

    Rule of thumb: For angles > 𝟔𝟎∘, it mightstill be faster to use Bloch BCs instead of BFAST.

    © LUMERICAL SOLUTIONS INC19

    Angle 𝜽[degrees]

    Simulationtime

    0 1.0x

    10 1.2x

    20 1.5x

    30 2.0x

    40 2.8x

    50 4.3x

    60 7.5x

    70 16.6x

    80 65.8x

  • Application Examples

    © LUMERICAL SOLUTIONS INC21

  • Gold surface with narrow but deep trenches

    Acts as a “perfect absorber” around 𝜆 ≈ 3.2𝜇𝑚

    Study angular dependence of reflectance spectrum

    Lamellar Plasmonic Grating

    © LUMERICAL SOLUTIONS INC22

    2µm

    ……Gold

    80nm

    50

    0n

    m

    F. J. Garcia-Vidal et al., "Localized Surface Plasmons in Lamellar Metallic Gratings," J. Lightwave Technol. 17, 2191-2195 (1999)

    Nicolas Bonod et al., "Total absorption of light by lamellar metallic gratings," Opt. Express 16, 15431-15438 (2008)

  • FDTD Setup for the Lamellar GratingNarrow spectral features require high

    frequency resolution

    Also: a longer simulation time (20ps) and lower auto-shutoff tolerance (10−7)

    Strong field gradients in the slot requirelocal mesh refinement

    © LUMERICAL SOLUTIONS INC23

    Broadband source(2.2μm – 4.2μm)

    Frequency domainmonitor (1001 pts)

    Mesh refinementregion (10nm)

  • Lamellar Plasmonic GratingReflection spectrum under normal incidence

    © LUMERICAL SOLUTIONS INC24

  • Lamellar Plasmonic GratingComparison of Bloch BCs and BFAST (10 deg)

    © LUMERICAL SOLUTIONS INC25

    Broadband simulation withBloch BCs fails to accuratelysimulate this resonance(even at only 10 degrees).

  • Lamellar Plasmonic GratingComparison of Bloch BCs and BFAST (20 deg)

    © LUMERICAL SOLUTIONS INC26

  • Lamellar Plasmonic GratingComparison of Bloch BCs and BFAST (30 deg)

    © LUMERICAL SOLUTIONS INC27

  • Lamellar Plasmonic GratingBFAST allows convenient and accurate sweeps

    © LUMERICAL SOLUTIONS INC28

  • For BFAST, computational time increases with angle:

    Comparison with Bloch-sweep difficult due to varying auto-shutoff.

    A broad-band Bloch simulation takes about 15s (at 10∘)!

    Performance

    Angle BFAST

    0∘ 3s

    10∘ 20s

    20∘ 25s

    30∘ 31s

    40∘ 56s

    © LUMERICAL SOLUTIONS INC29

    Computer: Intel® Core™ i5-4460 (4 cores @ 3.2GHz)

  • Plasmonic enhanced solar cell

    © LUMERICAL SOLUTIONS INC30

    kb.lumerical.com/en/index.html?solar_cells_plasmonic_at_normal_and_oblique_incidence.html

    Broadband simulation (400nm – 1100nm)

    Contains highly dispersive media (silver and silicon)

    Symmetries can be exploited to accelerate the simulations

    https://kb.lumerical.com/en/index.html?solar_cells_plasmonic_at_normal_and_oblique_incidence.html

  • Plasmonic enhanced solar cell

    © LUMERICAL SOLUTIONS INC31

    Symmetries 4 x reduction

    Materials Silicon, Silver

    Wavelength 400 – 1100 nm (351 points)

    Simulation time 90 seconds

    Symmetries 2 x reduction

    Simulation time 1800s

  • © LUMERICAL SOLUTIONS INC32

    Summary

    The new Broadband Fixed-Angle Source Technique (BFAST) will be available in the next release of FDTD Solutions (2016A)

    Accurate broadband results can be obtained from a single simulation

    Faster simulations for a fixed angle of incidence More convenient and/or accurate for angle-wavelength sweeps

    Significant performance gains for broad spectra and moderate angles (below 45 degrees)

  • Questions? [email protected]

    Sales Inquiries: [email protected]

    Contact your local Lumerical representative

    Start your free 30 day trial today www.lumerical.com

    Contact Us

    Connect with Lumerical

    www.lumerical.com

    © LUMERICAL SOLUTIONS INC33

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