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标题: Computational Photonics-Salah Obayya [打印本页]

作者: zhoumi    时间: 2016-12-1 15:28
标题: Computational Photonics-Salah Obayya
1 Introduction
% g. A% n, ^6 y' a7 G3 c0 c+ O2 r1.1 Photonics: the countless possibilities of light propagation0 a& q: h  R  p7 M0 S
1.2 Modelling photonics3 {4 o( K7 x6 a7 @) g
2 Full-vectorial Beam Propagation Method
8 j6 T. B* j0 `1 j0 q2.1 Introduction
( q. j4 n1 M8 R' E' A7 Q2.2 Overview of the beam propagation methods
, {, x. y5 C5 [, O2.3 Maxwell’s Equations+ d; @5 w, C' J3 v( }! f
2.4 Magnetic field formulation of the wave equation
: U/ R8 Y+ @2 F, A. ^, K8 K2.5 Electric field formulation of the wave equation
2 j& L6 [$ J, v4 T$ h( E: @. `. E- F2.6 Perfectly-Matched Layer* [  y* U- p1 i
2.7 Finite Element Analysis# ?+ P" o/ ]; c/ q
2.8 Derivation of BPM Equations
& v4 r. S1 i. C' j3 m, R2.9 Imaginary-Distance BPM: Mode Solver
9 e' b$ X* h; B1 E, `# W+ K- c3 Assessment of Full-Vectorial Beam Propagation Method
& [! x7 }$ T. k! X3.1 Introduction
2 R, r; Z9 K6 S& `) a3.2 Analysis of Rectangular waveguide
( Q  S! ^! I- X3 E' Z$ I3.3 Photonic Crystal Fibre( M, n# B& v7 V6 ^- ?/ F
3.4 Liquid Crystal Based Photonic Crystal Fibre
0 {' c! ^3 ?) ^6 X6 _$ C3.5 Electro-optical Modulators
" U# U" l- h+ }+ r2 O5 y7 @3.6 Switches/ o- A0 s2 Z2 l, [' _
4 Bidirectional Beam Propagation Method1 p; H& v3 q' a. E9 R
4.1 Introduction
4 W) p. [" j5 E* ~* }. k% Y3 F1 I  g4.2 Optical Waveguide Discontinuity Problem
1 W& f- W7 N# @5 ?' U( f4.3 Finite element analysis of discontinuity problems) R8 e- M: b2 c) o$ p
4.4 Derivation of Finite Element Matrices
( U4 I" w. j8 a1 N' f4.5 Application of Taylor’s Series Expansion; s$ P7 ?, K' z& [
4.6 Computation of Reflected, Transmitted and Radiation Waves
$ U& b5 l1 Q- b' y9 E7 [8 b6 P4.7 Optical fiber-facet problem
( Y( U3 c4 L5 [$ E% \4.8 Finite element analysis of optical fiber facets
* X1 J+ E3 b# P+ \4.9 Iterative analysis of multiple-discontinuities% s) ^' J8 ^1 d9 ^( j9 x% j- d9 F% |
4.10 Numerical assessment3 O6 B* X* J" s+ J) L2 k
5 Complex-Envelope Alternating-Direction-Implicit Finite Difference Time Domain Method with Assessment
0 }& K+ _" j9 J0 ?) C5.1 Introduction
. W- i  [0 c, G/ d% Q5.2 Maxwell's equations
) r% M1 O# Q0 Y- K5.3 Brief history of Finite Difference Time Domain (FDTD) Method& l# E9 _# \$ z6 b+ D
5.4 Finite Difference Time Domain (FDTD) Method
6 D  @8 H' ]6 P* ~! A. D/ O5.5 -Direction-Implicit FDTD (ADI-FDTD): Beyond the Courant Limit, b& `; }1 K) @# J! i2 C# J, X! f
5.6 Complex-Envelope ADI-FDTD (CE-ADI-! U1 K5 X/ {# ^5 ?3 F; _. X5 w3 q# c
5.7 Perfectly Matched Layer (PML) Boundary Conditions+ K4 X: O% b2 _% p" B: A* c2 j3 H
5.8 Uniaxal Perfectly Matched Layer (UPML) Absorbing Boundary Condition
: z3 i6 x$ g( V* d( u* {  T" e5.9 PML Parameters& k2 P' u8 i2 V: V8 w8 p( @
5.10 PML Boundary Conditions for CE-ADI-FDTD
6 z# X2 _$ |: r8 t; y$ E5.11 PhC Resonant Cavities
9 y; i; I7 ~' h( j8 A" V5.12 5x5 Rectangular Lattice PhC Cavity7 W1 u3 N5 _% r/ ?9 d, F
5.13 Triangular Lattice PhC Cavity
& ?' x! E- a! s9 r6 ~  T# [5.14 Wavelength Division Multiplexing7 \' g6 R5 _- G0 Q* V, F8 I. s
5.15 Conclusions" A5 V' _6 K5 ?) |4 s8 ^4 [, Z
6. Finite Volume time Domain (FVTD) Method
3 U# o- `( I, n" V: H4 l9 q6.1 Introduction
: ?+ J  u) f" d5 B$ p6.2 Numerical analysis
3 d" c1 x% q9 T" |0 G9 O# m) k6.3 UPWIND Scheme for the Calculation* f" S" P+ d0 ?
6.4 NON-DIFFUSIVE Scheme for the Flux Calculation, E- J7 f4 Q2 `2 X  f
6.5 2D Formulation of the FVTD Method& {6 w8 E% W/ u5 u8 d+ q
6.6 Boundary Conditions) C! d) X9 ]& R  D* b" F+ j
6.7 Nonlinear Optics: a5 S- p4 x: r- m/ v
6.8 Nonlinear Optical Interactions, j9 d8 O' b0 r, i3 M
6.9 Extension of the FDTD Method to Nonlinear Problems
) I. S7 o) q# `6.10 Extension of the FVTD Method to Nonlinear Problems& I  u( I8 x2 Z  e4 i3 a5 b$ Z
6.11 Conclusions
% r+ s" g1 {  c0 ?7 Numerical Analysis of Linear and Nonlinear PhC Based Devices5 i* l* p3 R3 Q. y- w* l
7.1 Introduction# a( m. Z" H/ c1 ?5 ]+ Z+ A* P
7.2 FVTD Method Assessment: PhC Cavity6 b& m% w$ z  ~* g5 F
7.3 FVTD Method Assessment: PhC Waveguide
. A3 U# Z6 c$ J* ~; l7.4 FVTD Method Assessment: PBG T-Branch
* y2 p5 D7 f7 Q7.5 PhC Multimode Resonant Cavity: n6 ^+ l8 J3 U0 G
7.6 FDTD Analysis of Nonlinear Devices( _) [  p" ~- W/ v7 I/ y
7.7 FVTD Analysis of Nonlinear Photonic Crystal Wires( ], p; c* i# ], D" A
7.8 Conclusions$ L0 l& C% B9 b% s% n( j: u
8 Multiresolution Time Domain6 h, h1 p( T* s* d8 k% E/ |$ G* J
8.1 Introduction
/ T: y1 z, {4 w. I4 g8.2 MRTD basics
3 o% y7 E. p% Y6 L" {8.3 MRTD update scheme. a; i) H" L9 T" }" _
8.4 Scaling-MRTD4 |* E- W8 y7 e2 h5 S' z
8.5 Conclusions
& F1 [& ~% x# L# P8 |9 MRTD Analysis of PhC-Devices2 p* [: k* Q; a, z
9.1 Introduction0 K5 P+ u( B  B% Q3 j' a
9.2 UPML-MRTD: test and code validation- E3 s5 @! ^2 M9 L
9.3 MRTD vs FDTD for the analysis of linear photonic crystals& E/ h' `) I6 B9 B- e9 E! b! V
9.4 Conclusions
" E1 O6 F. |6 L+ w0 ^) G10 MRTD Analysis of SHG PhC-Devices
! Y5 v; Q3 k& z) d3 g% z( \10.1 Introduction& M. r/ e( @  y( a4 Y6 d
10.2 Second harmonic generation in optics* Q$ [. n- s0 N1 I. c& q% m
10.3 Extended S-MRTD for SHG analysis2 ^* ^$ l2 U& S0 P, r7 J# B
10.4 SHG in PhC-waveguide4 v7 y0 L, O& }
10.5 Selective SHG in compound PhC-based structures9 s) Y; x- W. q) Z  U! t4 G1 o
10.6 New design for selective SHG: PhC-microcavities coupling
' g7 x- @- N7 W# U4 Q+ g10.7 Conclusions
7 Z0 ^" B  c/ L2 t11 Dispersive Nonlinear MRTD for SHG Applications
/ G% r+ r1 b- _- g- S- H& j11.1 Introduction
+ K1 h) N# U! c0 a$ H" ]11.2 Dispersion analysis
. C: _) x+ |$ v9 ]11.3 SHG-MRTD scheme for dispersive materials
* y6 F5 O0 y3 y2 I% g11.4 Simulation results
$ a( g' Y! g' g) A; M3 n11.5 Conclusions
作者: zhoumi    时间: 2016-12-1 15:29
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Computational_Photonics.pdf

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作者: hasky    时间: 2016-12-2 10:42
楼主威武霸气!( x7 T# F# |% r

作者: fish1352    时间: 2016-12-2 11:13
谢谢O(∩_∩)O哈哈~谢谢O(∩_∩)O哈哈# P* J6 \8 W% e6 z4 b( P. p$ A0 h





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