A Perspective on the 40-Year History of FDTD … Number 1: Kane Yee IEEE AP-S Transactions, ......
Transcript of A Perspective on the 40-Year History of FDTD … Number 1: Kane Yee IEEE AP-S Transactions, ......
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A Perspective on the 40-Year History ofFDTD Computational Electrodynamics
Allen Taflove, ProfessorDepartment of Electrical Engineering and Computer Science
Northwestern University, Evanston, IL 60208
Presented at:
Applied Computational Electromagnetics Society (ACES) ConferenceMiami, Florida
March 15, 2006
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Paper Number 1: Kane YeeIEEE AP-S Transactions, May 1966
Numerical Solution of Initial Boundary ValueProblems Involving Maxwell’s Equations
In Isotropic Media
KANE S. YEE
Abstract—Maxwell’s equations are replaced by a set of finitedifference equations. It is shown that if one chooses the field pointsappropriately, the set of finite difference equations is applicable fora boundary condition involving perfectly conducting surfaces. Anexample is given of the scattering of an electromagnetic pulse by aperfectly conducting cylinder.
obstacle is moderately large compared to that of an in-coming wave.
A set of finite difference equations for the system ofpartial differential equations will be introduced in theearly part of this paper. We shall then show that with anx
2441 citations as of March 7, 2006 (Source: ISI Web of Science)
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Yearly FDTD-Related Publications
Source: Shlager & Schneider, 1998.
2005
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ased
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1000
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1965 1970 1975 1980 1985 1990 1995
Year
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My First Paper: IEEE MTT, Aug. 1975
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My Second Paper: IEEE MTT, Nov. 1975
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Coining of “FDTD”: IEEE EMC, Aug. 1980
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Timeline:1966 to 1980 1965
1970
1975
Yee (IEEE AP)
Taflove & Brodwin (IEEE MTT)
Holland (IEEE NS)Kunz and Lee (IEEE EMC)
Taflove (IEEE EMC)
Engquist-Majda ABC
Bayliss-Turkel ABC 1980
Wexler (IEEE MTT)Taylor & Shumpert (IEEE AP)
Merewether (IEEE EMC)
Lopez & Rich (IEEE NS)Merewether & Radasky (IEEE NS) Merewether & Ezell (IEEE NS)
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Timeline:1981 to 1990 1980
1985
Mur ABC
Waveguides (Choi & Hoefer)
Contour path subcell models(Umashankar et al.)
NTFF/RCS (Umashankar & Taflove)
L-C formulation (Gwarek)
ABCs in IEEE AP-S Trans.
Liao ABC
Unstructured grids (Cangellaris;Shankar; Madsen & Ziolkowski)
Entire human body (Sullivan et al.)
Microstrips (Zhang et al.)
FDTD at IEEE AP-S Symp.
Dispersive dielectrics(Kashiwa & Fukai)
1990
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Timeline:1991 to 1995 1990
1995
Recursive convolution andauxiliary differential equations(Luebbers et al., Joseph et al.)
Antennas (Maloney et al., Katzet al., Tirkas and Balanis)
Linear and nonlinear circuit elements(Sui, Piket-May & Taflove)
Nonlinear media; solitons(Ziolkowski, Taflove et al.)
Berenger PML ABCSPICE interface (Thomas et al.)
Tunnel and Gunn diodes(Toland et al.)Entire jet fighter for RCS (Taflove)
UPML ABC (Sacks et al.)
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Timeline:1996 to 2000 1995
Periodic structures(Maloney & Kesler)
COM ABC (Ramahi)
MRTD (Krumpholz & Katehi)
Fourier-based PSTD (Q. Liu)
Exact grid dispersion analysis(Schneider & Wagner)
Stable subcells (Dey & Mittra)
UPML ABC (Gedney)
ADI (Namiki; Zheng et al.)CPML ABC (Roden & Gedney) 2000
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Timeline:2000 to 2005 2000
4-quantum-level laser model(Huang; Chang & Taflove)
Stable FDTD/FETD hybrid(Rylander & Bondeson)
Entire Earth-ionosphere models(Hayakawa; Simpson & Taflove)
Matrix-exponential “one-steptechnique” (De Raedt et al.)
Higher-order PML ABC (J. Jin)2005
Many emerging applications inphotonics, nanoplasmonics,
and biophotonicsChebyshev-based PSTD (Q. Liu)
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Some Major Technical Paths Since Yee
• Absorbing boundary conditions
• Numerical dispersion
• Numerical stability
• Conforming grids
• Digital signal processing
• Dispersive and nonlinear materials
• Multiphysics
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Some Major Technical Paths Since Yee
• Absorbing boundary conditions
— Engquist-Majda, Math. Comp., 1977
— Bayliss-Turkel, Com. Pure Appl. Math., 1980
— Liao et al., Scientia Sinica A, 1984
— Berenger PML, 1994 JCP
UPML, CPML, higher-order PML
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Some Major Technical Paths Since Yee
• Numerical dispersion
— Schneider and Wagner, IEEE MGWL, 1999
— High-order space differences
— MRTD (Krumpholz and Katehi, IEEE MTT,1996)
— PSTD (Q. H. Liu, 1997 IEEE AP-S Symp.)
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Some Major Technical Paths Since Yee
• Numerical stability
— Taflove & Brodwin, IEEE MTT, 1975
— ADI techniques (Namiki, IEEE MTT, 1999;Zheng, Chen, and Zhang, IEEE MTT, 2000)
— One-step Chebyshev method (De Raedt etal., IEEE AP, 2003)
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Some Major Technical Paths Since Yee
• Conforming grids
— Locally conforming (Taflove-Umashankarcontour path, Dey/Yu-Mittra)
— Globally conforming (Shankar et al., and Madsen and Ziolkowski, Electromagnetics,1990).
— Stable hybrid FETD/FDTD (Rylander andBondeson, Comput. Phys. Comm., 2000).
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Some Major Technical Paths Since Yee
• Digital signal processing
— Near-to-far-field transformation (Umashankarand Taflove, IEEE EMC, 1982, 1983; Luebbers et al., IEEE AP, 1991)
— Impulse response Fourier transformation andextrapolation
— Extraction of resonances, possibly degenerate
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Some Major Technical Paths Since Yee
• Dispersive and nonlinear materials
— Isotropic linear dispersions (Debye, Lorentz,Drude characteristics; multiple poles)
— Anisotropic linear dispersions (magnetizedplasmas, ferrites)
— Nonlinear dispersions, yielding temporal andspatial solitons
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Some Major Technical Paths Since Yee
• Multiphysics coupling to Maxwell’s equations
— Charge generation,recombination, andtransport in semiconductors
— Electron transitions between multiple energylevels of atoms, modeling pumping, emission,and stimulated emission processes
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Some Interesting Emerging Applications
• Earth / ionosphere models in geophysics
• Wireless personal communications devices
• Ultrawideband microwave detection of early-stagebreast cancer
• Ultrahigh-speed bandpass digital interconnects
• Micron / nanometer-scale photonic devices
• Biophotonics, especially optical detection of early stage epithelial cancers
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Earth / Ionosphere Modelsin Geophysics
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Earth / Ionosphere Models in Geophysics
• There is a rich history of investigationof ELF and VLF electromagnetic wavepropagation within the Earth-ionosphere waveguide.
• Applications:– Submarine communications– Remote-sensing of lightning and
sprites– Global temperature change– Subsurface structures– Potential earthquake precursors
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Geodesic Grid
Source: Simpson & Taflove, IEEE Trans. Antennas and Propagation, in press.
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Snapshots of FDTD-Computed Global Propagationof ELF Electromagnetic Pulse Generated by
Vertical Lightning Strike off South America Coast
All features of the lithosphere and atmosphere located within ±100 km of sea levelare modeled in 3-D with a resolution of approximately 40 × 40 × 5 km.
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LasVegas
Map of the percent increase in the peak vertical E-field power for 20-km deepbowl-shaped ionospheric depressions above downtown Los Angeles.
Detection of an Ionosphere Depression Above Los Angeles(Hypothesized Precursor of a Major Earthquake)
Via Illumination by a 76-Hz Pulse from the Former Navy WTF
LasVegas
Los Angeles Los Angeles
San Francisco San Francisco
Las VegasLas Vegas
200-km radius 380-km radius
Source: Simpson & Taflove, IEEE Geoscience & Remote Sensing Letters, submitted.
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Wireless Personal CommunicationsDevices
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Motorola T250 Cellphone
High-resolutionFDTD model. Thelattice-cell size is asfine as 0.1 mm toresolve individualcircuit board layersand the helicalantenna.
Source: Chavanneset al., IEEE Antennasand PropagationMagazine, Dec. 2003,pp. 52–66.
Physical phone
CAD model
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PhoneModelValidationat 1.8 GHz
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Phantom Head Validation at 1.8 GHz
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Final Head Model Results
The head model has 121 slices (1-mm thick in the ear region;3-mm thick elsewhere) having a transverse resolution of 0.2 mm.
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Ultrawideband Microwave Detectionof Early-Stage Breast Cancer
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Modeled Detection of a 2-mm Tumor
±10%
S/C=16 dB
Numerical breast phantom
Simulated 2-mmdiameter tumor
Calculated imageof tumor
FDTD simulation of UWBmicrowave detection of a2-mm-diameter malignanttumor embedded 3 cmwithin an MRI-derivednumerical breast model.The cancer’s signature is15 to 30 dB stronger thanthe clutter due to thesurrounding normaltissues. Source: Bond etal., IEEE Trans. Antennasand Propagation, 2003,pp. 1690–1705.
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Ultrahigh-Speed BandpassDigital Interconnects
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-140
-120
-100
-80
-60
-40
-20
0
Tra
nsm
issi
on
rat
io (
dB
)
Frequency (GHz)
0 10 20 30 40 50 60 70 80
Straight
90° bend
TE30 cutofffrequency
Both straight and bentSIW’s exhibit100%bandwidths.
In this example, thepassband is 27 to 81GHz with negligiblemultimoding (asconfirmed bymeasurements atIntel Corporation).
Source: Simpson et al,IEEE Trans. MTT, in press.
Substrate Integrated Waveguides (SIW’s)
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New Half-Width Folded SIW Has 115% BandwidthPredicted by FDTD: 27 to 100 GHz
27 — 100 GHz
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Micron / Nanometer ScalePhotonic Devices
Category 1: Linear
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Photonic Bandgap Defect Mode Cavities
Fabricated device:membrane microresonator
in InGaAsP
Images of degenerate microcavity modes in2-D thin-film photonic crystal defect cavities
Source: E. Yablonovitch, UCLA
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Photonic Bandgap Defect Mode Laser Cavities
Electrically driven, single-mode, low-threshold-current photonic crystal microlaser operating atroom temperature. Source: Park et al., Science,
Sept. 3, 2004, pp. 1444–1447.
Top view of fabricated sampleFDTD-calculated E-field intensity
of monopole mode (log scale)
Schematic view
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Laterally Coupled Photonic Disk Resonators
1st- and 2nd-order radial whisperinggallery mode resonances
= 1.55 m(off resonance)
Source: S. C. Hagness, D. Rafizadeh, S. T. Ho, and A. Taflove, IEEE J. Lightwave Tech., 1997.
fabricated device
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Vertically Coupled Photonic Racetrack(Fully 3-D Model)
Plan view
Verticalcross-section
Source: J. H. Greene and A. Taflove, Optics Letters, 2003.
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PulsePropagation inthe VerticallyCoupledRacetrack
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Vertical Cuts Showing Transient Multimoding
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Gold film thickness = 100 nmHole diameter = 200 nmIncident wavelength = 532 nmNormal incidence
Nanoplasmonics: Enhanced TransmissionThrough a Sub-Micron Hole in a Gold Film
Experiment FDTD
Source: L. Yin et al.,Applied PhysicsLetters 85, 467 (2004)
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Focusing Plasmonic Lens
SEMphoto
Experiment FDTD
Source (left and bottom left images): L. Yinet al., Nano Letters 5, 1399 (2005).
Source (bottom right image): S-H. Chang
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Micron / Nanometer ScalePhotonic Devices
Category 2: Macroscopic Nonlinearity
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“Braided” Spatial Solitons in Glass
Source: R. Joseph and A. Taflove, IEEE Photonics Technology Letters, 1994.
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Braiding Transitions to Divergence When the Width ofEach Laser Beam is Sufficiently Narrow
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All-Optical Photonic CrystalCross-Waveguide Switch
Source: Yanik et al., Optics Letters, 2003, pp. 2506–2508.
(a) control input is absent,yielding low signal output
(b) control input is present,yielding high signal output
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Micron / Nanometer ScalePhotonic Devices
Category 3: Semiclassical Models
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Four-Level, Two-Electron Model for ZnO
[ ]ENNkPdt
dP
dt
Pdaaa
aa
a03
22
2
−=++ ωγ
[ ]ENNkPdt
dP
dt
Pdbbb
bb
b12
22
2
−=++ ωγ
( ) ( )dt
dPE
NNNN
dt
dN a
a
?+−−−−=ωττ h111
30
03
32
233
( ) ( )dt
dPE
NNNN
dtdN b
b
?+−−−=ωττ h111
21
12
32
232
( ) ( )dt
dPE
NNNNdt
dN b
b
?−−−−=ωττ h111
10
01
21
121
( ) ( )dt
dPE
NNNN
dt
dN a
a
?−−+−=ωττ h111
10
01
30
030
EC
EV
N0
N3
N2
N1
N0
N3
N1
N2
32τ
21τ
10τ
30τ
PPaa
PPbb
.
.
.
.
Source: S.-H. Chang and A. Taflove, Optics Express, 2004.
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Pumping, Population Inversion, and Lasing
0.0 5.0x10-12 1.0x10-11 1.5x10-11
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
n
Time(sec)
n1 n2 n3 n0
8.0x10-121.0x10-111.2x10-111.4x10-111.6x10-11
0.4950.4960.4970.4980.4990.5000.5010.5020.5030.5040.5050.506
n
Time (sec)
n1 n2
0.0 5.0x10-12 1.0x10-11 1.5x10-11
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
n
Time(sec)
n1 n2 n3 n0
8.0x10-121.0x10-111.2x10-111.4x10-111.6x10-11
0.4950.4960.4970.4980.4990.5000.5010.5020.5030.5040.5050.506
n
Time (sec)
n1 n2
0.0 2.0x10-10 4.0x10-10 6.0x10-100.0
2.0x1011
4.0x1011
6.0x1011
8.0x1011
Inte
nsity
Time (sec)
1.E+04
1.E+06
1.E+08
1.E+10
1.E+12
1.E+10 1.E+11 1.E+12 1.E+13
Out
put I
Lasing threshold
Populations n(t) Pumping vs. lasing intensity
Pump intensity
Out
put
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Lasing in a Random Clump of ZnO Particles
382380
E.I.
(a.u
.)
Wavelength (nm)
size ~ 1.7 m
Contains ~ 20,000 particles
Wavelength (nm)
E.I.
(a.
u.)
3.2 µmMeasured
2-D FDTDmodel
Source: H. Cao et al., Physical Review Letters, 2000.
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Biophotonics
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FDTD / PSTD Biophotonics Thrust Areas
• Optical detection of early-stage epithelialcancers (colon, lung, esophagus, cervix)
• Ultramicroscopy of individual living cellsto investigate physiological processes
• Optical propagation through millimeter-scale-thick living tissues
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What is the Difference Between TheseTwo Groups of Human Cells (observed
using conventional microscopy)?
Healthy cells Cells near death
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Backscattering Spectroscopy
Our FDTD modeling has shown that
observing the spectrum of retro-reflected
light from living tissues yields much greater
information regarding the health of these
tissues than existing diagnostic techniques.
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Backscattering Detection of Nanoscale Features
incidentlight
incidentlight
incidentlightLc = 100 nm Lc = 50 nm
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Emerging Clinical Application
My Northwestern University colleagues and
collaborators, Profs. Vadim Backman and
Xu Li, are applying this idea to develop
extraordinarily sensitive and accurate tests
for pre-cancerous conditions in human
epithelial tissues such as the colon.
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Source: Gastroenterology, 126, 1071-1081 (2004).
Bulk Backscattering Spectral Changes Are Observed Far EarlierThan Any Currently Known Histologic or Molecular Markers of
Precancerous Conditions in Colon Tissues
control AOM-treated (week 2)
Bac
ksca
tterin
g an
gle
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Using FDTD simulations to guide experiments,
we are pushing this concept even further to
acquire the backscattered spectra of individual
pixels of a microscope image.
This will allow monitoring of the physiological
processes involved in the progression of
precancerous conditions in living human cells.
Our Current Work: Backscattering SpectroscopicMicroscopy On a Pixel-by-Pixel Basis
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First, We Demonstrated Agreement of Measured andFDTD-Calculated Backscattering Microscope Images
Co-pol Cross-pol All-pol
Mea
sure
dF
DT
D
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Next, We Applied FDTD to Calculate the Spectra of Individual Pixels ofBackscattered Microscope Images of Various Layered Media Having
Lateral Inhomogeneities Near the Diffraction Limit
FDTD-calculated image
Modeled structure
Backscattered spectrum at
Backscattered spectrum at
Backscattered spectrum at
Backscattered spectrum at
nm
nm
nm
nm
+
+
+
+
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Backscattering microscopeintensity image of normal HT-29 cells
Same, but the HT-29 cells aretreated with sulindac sulfide
Finally, We Designed a Microscope System to Acquire Pixel-by-Pixel Backscattering Spectra of Individual Biological Cells
Single-pixel backscattering spectra
Normal cells have very differentpixel backscattering spectrathan the sulindac sulfide treatedcells (which are dying).
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PSTD Modeling of Clusters of Cells
We are applying PSTD modeling to better
understand the interaction of light with large
clusters of living cells.
We are particularly interested in direct
backscattering, which conveys much
information regarding tissue health.
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Validation of Fourier-Basis PSTD forScattering by a Single Sphere
Source: Tseng et al.,Radio Science, in press.
- - - PSTDMie
scattering angle (degrees)0˚ 50˚ 100˚ 150˚
–7
–8
–9
–10
–11
–12
–13
log
(diff
eren
tial c
ross
-sec
tion)
8 µm
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Validation of Fourier-Basis PSTD for Scattering by a20-µm-Diameter Cluster of 19 Dielectric Spheres
19 spheres,each d = 6 µm
and n = 1.2
20 µm
Total scattering cross-section
– • – PSTDMulti-sphere expansion
frequency (THz)0 100 200 300
TS
CS
(µm
2 )
0
400
800
1200
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PSTD-Calculated Total Scattering Cross-Section of a25-µm-Diameter Cluster of 192 Dielectric Spheres
192 spheres,each d = 3 m
and n = 1.2
Total scatteringcross-section
25 µm
TS
CS
(µm
2 )
frequency (THz)0 200 400 600
0
500
1000
1500
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Identification of the Component Sphere Sizein the 192-Sphere Cluster Via Cross Correlation
2 4 6 8 10
sphere diameter (µm)Peak correlationat d = 3.25 m
0
0.8
1
0.6
0.4
0.2
cros
s-co
rrel
atio
n co
effic
ient
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Future Prospects
• Nanophotonics, including as many quantum
effects as we can muster. Ultimately, achieve
a combination of quantum and classical
electrodynamics.
• Biophotonics, especially as applied to the
early-stage detection of dread diseases such
as cancer.
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My Personal Journey
I’ve been privileged to participate in the
advancement of FDTD theory, techniques, and
applications over the past 35 years.
It is very gratifying to see the current general
widespread usage of FDTD for engineering and
science applications that could not have been
envisioned back in the1970’s and 1980’s.
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Thanks for inviting me!