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Computational Photonics-Salah Obayya

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发表于 2016-12-1 15:28 | 只看该作者 回帖奖励 |正序浏览 |阅读模式

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1 Introduction
9 }& `6 x. a2 B0 m( ~1 p$ a1.1 Photonics: the countless possibilities of light propagation
+ x3 g% S  V6 U" N1 s" ?. y, z1.2 Modelling photonics& k: W2 d0 ~+ b$ N" ^. ]9 D
2 Full-vectorial Beam Propagation Method( g( E2 F( t" B: S" W3 n
2.1 Introduction
5 d% i5 _6 l- R# C* N8 V' e2.2 Overview of the beam propagation methods' ^2 y* Y' S  ~% C# q; k
2.3 Maxwell’s Equations
& i' F- H& F' {& w2.4 Magnetic field formulation of the wave equation# j% u8 n- i) v) ]# W/ I" h
2.5 Electric field formulation of the wave equation: H- f6 S, H) f  s7 g; B5 a
2.6 Perfectly-Matched Layer! L+ u/ U9 b- z6 n3 U5 I3 X
2.7 Finite Element Analysis
! u% J! e' I, q) k0 V2 O2.8 Derivation of BPM Equations3 ?! W% i( Q" ]% E# M/ [  U
2.9 Imaginary-Distance BPM: Mode Solver
9 l: X  A( r0 j3 t9 W3 Assessment of Full-Vectorial Beam Propagation Method; |$ [8 ?+ g, `! T
3.1 Introduction- g" S; }. x, I
3.2 Analysis of Rectangular waveguide
6 Y* P; Y1 i* d3.3 Photonic Crystal Fibre
) K$ H7 I! L  T; o3.4 Liquid Crystal Based Photonic Crystal Fibre
5 P  M0 \' Y1 l$ ^, I3.5 Electro-optical Modulators( Y- I  d) I. g/ Z: U
3.6 Switches0 ~1 y4 |6 o; a  J$ c* _! R3 E6 A
4 Bidirectional Beam Propagation Method
* O0 Z" i" c. X& w  R4.1 Introduction& j5 u7 ?# n$ ?# P) u
4.2 Optical Waveguide Discontinuity Problem
) C9 n/ z$ n8 x# ?: c7 {4 t0 v! F4.3 Finite element analysis of discontinuity problems
) a- D$ K! L6 Y( w% T; ^4.4 Derivation of Finite Element Matrices
4 S0 h9 j  U, M$ h4.5 Application of Taylor’s Series Expansion
7 k5 p- U# Q0 d2 s( s8 @' L1 t4.6 Computation of Reflected, Transmitted and Radiation Waves' s4 t' H8 f  |4 k+ X' z
4.7 Optical fiber-facet problem
8 D' K3 d4 H3 U1 l5 M4 B  {+ M4.8 Finite element analysis of optical fiber facets
1 r. A9 }, t; ]! r) H4.9 Iterative analysis of multiple-discontinuities+ b3 K) M- \" Z
4.10 Numerical assessment
2 S# x/ v  E) y! L( N5 Complex-Envelope Alternating-Direction-Implicit Finite Difference Time Domain Method with Assessment
/ C& Q! q, Q( _' v- k5.1 Introduction
! p  \' i, P7 N* @% o, q5 c, ]& D5.2 Maxwell's equations1 f/ z' s4 y; V" ~. o
5.3 Brief history of Finite Difference Time Domain (FDTD) Method7 C" A- A: a0 U% [
5.4 Finite Difference Time Domain (FDTD) Method
, r* q: p; V, ~8 m2 @1 g5.5 -Direction-Implicit FDTD (ADI-FDTD): Beyond the Courant Limit
3 Q; b+ k" P) `2 y5 x5.6 Complex-Envelope ADI-FDTD (CE-ADI-
; Q1 _, a- V( U/ w/ L/ e: X2 X5.7 Perfectly Matched Layer (PML) Boundary Conditions
. `) N( }3 S' R5.8 Uniaxal Perfectly Matched Layer (UPML) Absorbing Boundary Condition) g. {' I$ S1 E4 t7 t6 I) S
5.9 PML Parameters
3 {2 \( z) d  e" g: e# T5.10 PML Boundary Conditions for CE-ADI-FDTD
' W# E- [' E8 _0 D6 d5 P- |0 k. J; g5.11 PhC Resonant Cavities. i+ H8 |" ?; X5 o% ^7 z) h
5.12 5x5 Rectangular Lattice PhC Cavity
( Z# u# K9 q9 b1 {+ L  h: d5.13 Triangular Lattice PhC Cavity
9 n# o4 P0 j2 Q& O5.14 Wavelength Division Multiplexing; O8 B0 J$ k% M9 k# Q. w8 v
5.15 Conclusions
. \2 F$ T* C$ [! e1 j6. Finite Volume time Domain (FVTD) Method# e# A- z$ ^  P1 k
6.1 Introduction
, z  P% A( p5 e3 V8 G( Q6.2 Numerical analysis
2 u5 v5 h; W) n6.3 UPWIND Scheme for the Calculation
( u- F% s. n7 {2 c! D+ p' b9 O7 i4 j6.4 NON-DIFFUSIVE Scheme for the Flux Calculation4 `) N) M8 m  G" L4 q
6.5 2D Formulation of the FVTD Method
) f* m# E) L: M3 z4 Y6.6 Boundary Conditions7 b& H% ^; e' Y1 V% k& J
6.7 Nonlinear Optics
6 e! k1 }. @  t+ k5 `/ d6.8 Nonlinear Optical Interactions
  L" E7 W4 A. x5 p6.9 Extension of the FDTD Method to Nonlinear Problems
1 C3 `! b2 j6 Q& z( D6.10 Extension of the FVTD Method to Nonlinear Problems
9 u: }3 H! h0 c5 V+ f% i6.11 Conclusions" x) s0 M5 ?3 i2 u' B
7 Numerical Analysis of Linear and Nonlinear PhC Based Devices
- c# ?- J/ k, Q) z7.1 Introduction8 ?8 h) R, g9 h! o  v& l
7.2 FVTD Method Assessment: PhC Cavity; A, P& J( V1 d6 L; k- S
7.3 FVTD Method Assessment: PhC Waveguide! i: W; H) l  S" ~1 ~  Y
7.4 FVTD Method Assessment: PBG T-Branch
) N3 o! F1 P% \& L7.5 PhC Multimode Resonant Cavity
0 Y3 y% S+ b* L  X7.6 FDTD Analysis of Nonlinear Devices
3 U9 y2 ~" z$ b0 K# t7.7 FVTD Analysis of Nonlinear Photonic Crystal Wires
! t- M3 L; w' A. X6 W) l7.8 Conclusions# i3 y& ~- N' p2 y4 e$ ~
8 Multiresolution Time Domain
" l! T/ h: ~. [3 Z$ ~, v8.1 Introduction/ J4 Z! l6 P( F+ z% I
8.2 MRTD basics
1 d; u2 c  ]( z" V4 R$ w0 e8.3 MRTD update scheme
# D7 o9 I; Q8 O$ n8.4 Scaling-MRTD) H, Y! x' U. x6 [& t9 l3 k7 m0 }
8.5 Conclusions7 ]5 r% |9 @8 K! x3 l; g
9 MRTD Analysis of PhC-Devices
( w- s* x1 O4 m( j, M, f6 c9.1 Introduction1 J7 N0 O. ~3 g/ M
9.2 UPML-MRTD: test and code validation! i% a" X& {; r
9.3 MRTD vs FDTD for the analysis of linear photonic crystals
3 F- ~2 q' W# O9.4 Conclusions
9 W; W- d+ u; g, ]2 K8 q10 MRTD Analysis of SHG PhC-Devices
% i" [, g& s/ U, C7 F10.1 Introduction
# s' g( R( Y% Q$ e, M. D/ `10.2 Second harmonic generation in optics- Q6 {: M# y0 E( t
10.3 Extended S-MRTD for SHG analysis2 P) C2 r7 B& C: G+ |
10.4 SHG in PhC-waveguide/ M0 r' I7 D8 H# x; w
10.5 Selective SHG in compound PhC-based structures
9 k/ o# `7 C3 t1 M3 R10.6 New design for selective SHG: PhC-microcavities coupling
+ w" g" S7 k% s: F9 Q! @10.7 Conclusions# d% R4 X6 Q: ^
11 Dispersive Nonlinear MRTD for SHG Applications
1 K# m4 Q# _/ ?, Q11.1 Introduction% C( @( V( j3 m; X/ D4 C
11.2 Dispersion analysis
1 @, Y  C7 D+ V: b3 w/ N11.3 SHG-MRTD scheme for dispersive materials
" }, R) K6 ]' r11.4 Simulation results6 \$ f9 Z4 X* A2 V, @3 M6 I
11.5 Conclusions
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发表于 2016-12-2 11:13 | 只看该作者
谢谢O(∩_∩)O哈哈~谢谢O(∩_∩)O哈哈
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发表于 2016-12-2 10:42 | 只看该作者
楼主威武霸气!
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 楼主| 发表于 2016-12-1 15:29 | 只看该作者
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