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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 |倒序浏览 |阅读模式

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1 Introduction7 ^0 ~6 c# a" `# _' j6 A
1.1 Photonics: the countless possibilities of light propagation
& E5 g9 e3 J; i' K4 u1.2 Modelling photonics8 A6 h  _9 H0 a+ {. u* a; E* ]
2 Full-vectorial Beam Propagation Method, @' }& a8 G, f- Q- L3 }' d
2.1 Introduction
+ d  g. Y2 e% {9 Q9 s' T2.2 Overview of the beam propagation methods
. p8 A; B$ @( t9 m. l2.3 Maxwell’s Equations/ J  ^3 F, A7 v+ B0 L9 S
2.4 Magnetic field formulation of the wave equation  {! w9 w5 o! p* q+ b" X* O* B7 F
2.5 Electric field formulation of the wave equation
7 w' V7 {. r& e$ R  I# l5 ^2.6 Perfectly-Matched Layer
2 A8 A) p0 [: ]9 a" v) Q+ V2.7 Finite Element Analysis1 n* V  o9 x/ {' W1 _
2.8 Derivation of BPM Equations
) u; Q8 }3 ^" G; J2.9 Imaginary-Distance BPM: Mode Solver
% S/ V! T2 F  v7 g3 ^$ ]2 t8 l3 Assessment of Full-Vectorial Beam Propagation Method
8 ^/ T9 _7 Q! M& K3.1 Introduction
4 Q+ {% o% w, Q$ _( A( t3.2 Analysis of Rectangular waveguide5 r' Q, T7 d& V" }% Y1 I
3.3 Photonic Crystal Fibre' h) b- j6 y; Z: e3 D
3.4 Liquid Crystal Based Photonic Crystal Fibre
7 |1 x* T$ p8 q  `3.5 Electro-optical Modulators
) S4 w. ]; u7 N# w3.6 Switches
5 K& E; W0 v: I7 P- r6 B4 Bidirectional Beam Propagation Method
- h9 k* Z( a2 o2 e( H; e+ l# ^4.1 Introduction" A- p7 Z5 d& `5 z. R
4.2 Optical Waveguide Discontinuity Problem- G$ p) |9 A' u0 L2 D
4.3 Finite element analysis of discontinuity problems
6 F. N/ t& j: i4 d" f( X' N4.4 Derivation of Finite Element Matrices1 G0 n( v% g6 S* ?, n" f5 L- s$ ?
4.5 Application of Taylor’s Series Expansion
4 ?. a. d/ L; ]* p& c" s4.6 Computation of Reflected, Transmitted and Radiation Waves& S" Y6 L8 x3 @; h2 S: W" H
4.7 Optical fiber-facet problem
: s8 I8 W" \5 a/ ]8 d) s: f4.8 Finite element analysis of optical fiber facets
/ d! r# w( J: x. Z4.9 Iterative analysis of multiple-discontinuities
8 x% ?, r/ L( ^+ D7 W# z; M4.10 Numerical assessment+ _; z9 W7 T% H8 C6 K/ L
5 Complex-Envelope Alternating-Direction-Implicit Finite Difference Time Domain Method with Assessment* e% z( d4 f3 W' L; i: o
5.1 Introduction- D; p9 O) A8 Z
5.2 Maxwell's equations
. A$ i- Y, V  ]- V8 F5.3 Brief history of Finite Difference Time Domain (FDTD) Method
9 v% k# E$ ?. L3 f: z7 |# {5.4 Finite Difference Time Domain (FDTD) Method" V" U9 d  u$ N
5.5 -Direction-Implicit FDTD (ADI-FDTD): Beyond the Courant Limit
* g* y4 j" J% Q- K% L5.6 Complex-Envelope ADI-FDTD (CE-ADI-" [2 b/ i7 F9 h& X5 J
5.7 Perfectly Matched Layer (PML) Boundary Conditions
) D. P' _' M) ?5.8 Uniaxal Perfectly Matched Layer (UPML) Absorbing Boundary Condition
3 |, U( q2 U3 [# o7 R+ d( d5.9 PML Parameters6 B7 K* h6 E. _# I1 G, W, M; ~
5.10 PML Boundary Conditions for CE-ADI-FDTD
* q5 d: p% H+ o( ^5.11 PhC Resonant Cavities. h) C* ]2 H- ]( L7 B7 I" t
5.12 5x5 Rectangular Lattice PhC Cavity, K& I( k! S" H6 n9 M
5.13 Triangular Lattice PhC Cavity' N* [3 S2 ?2 R6 x, U
5.14 Wavelength Division Multiplexing
6 I% W. j1 y; r5.15 Conclusions
& G$ @6 Z& E5 l6. Finite Volume time Domain (FVTD) Method
# O7 l- o+ ]3 H- U- _6.1 Introduction( c3 @. H9 C! O, L& p9 J
6.2 Numerical analysis
% j+ X( v( H( P8 h' z6.3 UPWIND Scheme for the Calculation0 Z3 q. m6 ?* X- w
6.4 NON-DIFFUSIVE Scheme for the Flux Calculation# g# J8 e% P7 F' r5 v8 x  v
6.5 2D Formulation of the FVTD Method7 h& l+ ~, h& K9 ~
6.6 Boundary Conditions/ k" R: ?" H' a- [( b
6.7 Nonlinear Optics
. ?1 p6 s  d2 j5 p4 E6.8 Nonlinear Optical Interactions5 ~' n* z% p8 o/ K4 P
6.9 Extension of the FDTD Method to Nonlinear Problems
3 E# `! q; M. F: R6.10 Extension of the FVTD Method to Nonlinear Problems0 G; U9 g7 t" J7 Z- T$ s
6.11 Conclusions6 Z: V1 m/ |( B: u
7 Numerical Analysis of Linear and Nonlinear PhC Based Devices
, \. J) Y2 t+ Z9 h7.1 Introduction
) b2 }; J! A# s% d4 M9 d! Z7.2 FVTD Method Assessment: PhC Cavity9 u) G7 ^, N. Z7 F& m' R2 p
7.3 FVTD Method Assessment: PhC Waveguide$ Y% ^% Y) M1 w+ u5 u
7.4 FVTD Method Assessment: PBG T-Branch
, Q: X/ O3 z2 y# |7.5 PhC Multimode Resonant Cavity
! O0 d6 a! d9 q. ]' G7.6 FDTD Analysis of Nonlinear Devices/ ~7 |1 {  M- k* h3 o: O% K
7.7 FVTD Analysis of Nonlinear Photonic Crystal Wires
/ N% n. d" P, b! ~% E7.8 Conclusions
/ W0 F, h; A9 e, ?5 [8 Multiresolution Time Domain
; ^: j) q) J- N" U+ C  O. T8.1 Introduction# R  u0 z" `& [# B. I$ H  d0 v
8.2 MRTD basics; G: E. |0 o$ ~6 f
8.3 MRTD update scheme- A! m# e7 D  Q* y0 U* {) r* t0 \2 m
8.4 Scaling-MRTD
  K( m$ Y+ G8 F$ J$ M; k8 n* w8.5 Conclusions# D6 Q0 J) Y; e1 y, J1 G5 w. P
9 MRTD Analysis of PhC-Devices3 e) H# h" y6 D: n& J! {% d
9.1 Introduction4 V1 x# L8 @! s' i' b
9.2 UPML-MRTD: test and code validation
8 E0 d) S' C1 J- P1 g9.3 MRTD vs FDTD for the analysis of linear photonic crystals. g. k: f/ f6 P3 Y
9.4 Conclusions
1 M& d7 w# e+ k% q3 O5 l* p7 `* P* D, w10 MRTD Analysis of SHG PhC-Devices0 a7 X7 U0 m) t
10.1 Introduction! A! |+ G2 V: o+ O& _
10.2 Second harmonic generation in optics
8 c: x  [: s4 K2 q* `* W6 q8 ?$ T2 X10.3 Extended S-MRTD for SHG analysis' L; @* D  A9 G* i0 Z* V5 ^! b
10.4 SHG in PhC-waveguide1 k+ ?4 _; k' x3 m# y1 z
10.5 Selective SHG in compound PhC-based structures7 R& B7 |" [0 i/ J, H: j/ |$ T
10.6 New design for selective SHG: PhC-microcavities coupling: n, s$ j/ k7 s( y- m
10.7 Conclusions8 }  d0 @& f, A  @4 I# N
11 Dispersive Nonlinear MRTD for SHG Applications% z; g, O# A9 B/ I; t
11.1 Introduction; O* h# ?# J0 Q7 ?1 e
11.2 Dispersion analysis" B2 A) f. k9 V! ~: Q4 ~& W
11.3 SHG-MRTD scheme for dispersive materials
& Y. A! z& `7 \1 @! O& F11.4 Simulation results( B7 U* \& B; k6 L7 \0 s/ S
11.5 Conclusions
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谢谢O(∩_∩)O哈哈~谢谢O(∩_∩)O哈哈7 V$ a% S8 C6 i
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