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Fast Analysis of All-Dielectric Structures Using Rigorous Coupled-Wave Analysis SEMI-ANALYTICAL FORMULATION OF MAXWELLS EQUATIONS Wave Equation for i th Layer THE UNIVERSITY OF TEXAS AT EL PASO Pioneering 21 st Century Electromagnetics and Photonics Solution K Matrices ,1,1,1 ,1,1,2 , , , i i i iPQR k k k K Plane Wave Amplitudes ,1,1,1 ,1,1,1 ,1,1,2 ,1,1,2 , , , , , , i i i i i i iPQR iPQR U S U S U S u s Rigorous coupled-wave analysis (RCWA) is an extremely efficient algorithm for modeling scattering through all-dielectric structures. It is most efficient for devices with low to moderate dielectric contrast. THE CONVOLUTION MATRICES r ε 2 2 2 i i x x i i i y y d dz s s Ω 0 s s 2 1 1 , , , 1 1 , , , 1 1 , , , 1 1 , , , i i i x ri y ri x ri x i y ri y ri y ri x x ri y ri x ri x i y ri y ri y ri x Ω PQ K μ K ε K Q K μ K ε K K ε K μ K P K ε K μ K x z y z x y z z e z z e z λ λ s s W W 0 c ψ u V V 0 c u 1 V QWλ 2 2 eigen-vector matrix eigen-value matrix i i i W Ω λ THE SEMI-ANALYTICAL SOLUTION THE SCATTERING MATRIX 11 12 1 1 2 2 21 22 i i i i S S c c c c S S 1 1 1 11 1 2 2 1 2 2 1 1 1 1 1 12 1 2 2 1 2 2 2 2 1 1 1 21 2 1 1 2 1 1 1 1 1 1 1 22 2 1 1 2 1 1 2 2 i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i S A XB A XB XB A XA B S A XB A XB X A BAB S A XB A XB X A BAB S A XB A XB XB A XA B 1 1 1 1 ij i j i j ij i j i j A W W V V B W W V V 0 i i kL i e λ X THE SCATTERING MATRIX ALGORITHM Redheffer Star Product: a b S S S 1 11 11 12 11 22 11 21 1 12 12 11 22 12 1 21 21 22 11 21 1 22 22 21 22 11 22 12 S a a I ba ba S a I ba b S b I ab a S b b I ab ab 1 1 1 11 1 1 1 12 21 12 22 11 i i i i i i i i i i i i i i i i i i i i i i i i i i i i i S A XBA XB XBA XA B S A XBA XB X A BA B S S S S 1 1 0 0 1 1 0 0 i i i i i i A W W V V B W W V V The formulation for the general asymmetric case is Our improved formulation offers the following benefits: 1. Symmetric scattering matrices 2. Faster the calculate. 3. More memory efficient. 4. Interchangeable scattering matrices. , , p pq q x p q a S pq Assemble convolution matrix from FFT of unit cell.

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Page 1: y r i y r i y r i x S A X B A X B X A B A B «» US s 1 S A X B A X B X B …emlab.utep.edu/pdfs/Poster_RCWA.pdf · 2017-07-17 · Fast Analysis of All-Dielectric Structures Using

Fast Analysis of All-Dielectric Structures Using

Rigorous Coupled-Wave Analysis

SEMI-ANALYTICAL FORMULATION OF MAXWELL’S EQUATIONS

Wave Equation for ith Layer

THE UNIVERSITY OF TEXAS AT EL PASO

Pioneering 21st Century Electromagnetics and Photonics

Solution K Matrices

,1,1,1

,1,1,2

, , ,

i

i

i

i P Q R

k

k

k

K

Plane Wave Amplitudes

,1,1,1 ,1,1,1

,1,1,2 ,1,1,2

, , , , , ,

i i

i i

i i

i P Q R i P Q R

U S

U S

U S

u s

Rigorous coupled-wave analysis (RCWA) is an extremely efficient algorithm for modeling scattering through all-dielectric structures. It is most efficient for devices with low to moderate dielectric contrast.

THE CONVOLUTION MATRICES

r

ε

22

2

i i

x x

ii i

y y

d

dz

s sΩ 0

s s

2

1 1

, , ,

1 1

, , ,

1 1

, , ,

1 1

, , ,

i i i

x r i y r i x r i x

i

y r i y r i y r i x

x r i y r i x r i x

i

y r i y r i y r i x

Ω PQ

K μ K ε K μ KQ

K μ K ε K μ K

K ε K μ K ε KP

K ε K μ K ε K

x

zy

zx

y

z

z ez

z e

z

λ

λ

s

s W W 0 cψ

u V V 0 c

u

1V QWλ

2

2

eigen-vector matrix

eigen-value matrix

i

i

i

λ

THE SEMI-ANALYTICAL SOLUTION

THE SCATTERING MATRIX

11 121 1

2 221 22

i i

i i

S Sc c

c cS S

11 1

11 1 2 2 1 2 2 1 1

11 1

12 1 2 2 1 2 2 2 2

11 1

21 2 1 1 2 1 1 1 1

11 1

22 2 1 1 2 1 1 2 2

i

i i i i i i i i i i i i

i

i i i i i i i i i i i

i

i i i i i i i i i i i

i

i i i i i i i i i i i i

S A X B A X B X B A X A B

S A X B A X B X A B A B

S A X B A X B X A B A B

S A X B A X B X B A X A B

1 1

1 1

ij i j i j

ij i j i j

A W W V V

B W W V V

0i ik L

i e

λ

X

THE SCATTERING MATRIX ALGORITHM

Redheffer Star Product:

a bS S S

1

11 11 12 11 22 11 21

1

12 12 11 22 12

1

21 21 22 11 21

1

22 22 21 22 11 22 12

S a a I b a b a

S a I b a b

S b I a b a

S b b I a b a b

11 1

11

11 1

12

21 12

22 11

i

i i i i i i i i i i i i

i

i i i i i i i i i i i

i i

i i

S A X B A X B X B A X A B

S A X B A X B X A B A B

S S

S S

1 1

0 0

1 1

0 0

i i i

i i i

A W W V V

B W W V V

The formulation for the general asymmetric case is

Our improved formulation offers the following benefits:

1. Symmetric scattering matrices 2. Faster the calculate. 3. More memory efficient. 4. Interchangeable scattering matrices.

, ,p p q q x

p q

a S p q

Assemble convolution matrix from FFT of unit cell.