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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
  ~! b" o3 V- I( @1.1 Photonics: the countless possibilities of light propagation1 E, f. Q$ |" [; E
1.2 Modelling photonics
6 r; d! F7 ]4 L2 Full-vectorial Beam Propagation Method3 ~6 N, X* M; g
2.1 Introduction0 F/ Z6 [" v3 \, G
2.2 Overview of the beam propagation methods
2 Y6 `9 P4 m2 E; }) H! k2.3 Maxwell’s Equations
4 f7 {5 _9 `1 V9 R) h) e" n( A2.4 Magnetic field formulation of the wave equation
* b; K8 m! u: ]* K2.5 Electric field formulation of the wave equation: C( [  e) D: h& l4 l7 q
2.6 PeRFectly-Matched Layer2 f! w3 b8 g; M
2.7 Finite Element Analysis
# O; ~; _' q! w3 r. v% N3 @4 W2.8 Derivation of BPM Equations9 e' k8 z- }  G) _) x% `- G/ Q
2.9 Imaginary-Distance BPM: Mode Solver
# k  _) J& K# w3 Assessment of Full-Vectorial Beam Propagation Method5 a# ]$ W2 Q- ?# V) s! O2 P8 ~/ [2 C3 n
3.1 Introduction( N" V5 G5 J. S, ]$ ~
3.2 Analysis of Rectangular waveguide
8 Y, v% L3 m& O  [- y" q9 a7 e) b3.3 Photonic Crystal Fibre
" z  i* X2 N- {. M6 a8 z. O2 u! u3.4 Liquid Crystal Based Photonic Crystal Fibre+ ?- s" F3 P  W- D+ B; R
3.5 Electro-optical Modulators# d: m4 J0 Z0 I; E: a+ _4 R& i
3.6 Switches6 R0 a( I" C+ X7 t* K$ q
4 Bidirectional Beam Propagation Method
% i) `8 @6 t7 P! D" U3 j. v4.1 Introduction
6 o& l2 L& w7 E: t/ X& R1 g4.2 Optical Waveguide Discontinuity Problem# v. o  t+ l' }. l- J' p9 n
4.3 Finite element analysis of discontinuity problems
  `9 i0 }8 n5 R* O$ O" p4.4 Derivation of Finite Element Matrices2 c% p4 z4 A* f: a) e' p& I) t7 y6 ?
4.5 Application of Taylor’s Series Expansion' R, i) l3 }1 J% [6 X* M( B% I' r
4.6 Computation of Reflected, Transmitted and Radiation Waves
  M, o& E5 B  q4 U. d4.7 Optical fiber-facet problem
6 l; {! O+ N" N4.8 Finite element analysis of optical fiber facets
! J/ Z6 K7 A3 J. W. d4.9 Iterative analysis of multiple-discontinuities
+ H, P  P; b/ R+ l  Z* p7 F" g4.10 Numerical assessment
4 B6 B" h& P* r5 Y5 N" g! z5 Complex-Envelope Alternating-Direction-Implicit Finite Difference Time Domain Method with Assessment3 p; y$ v2 g7 v0 C3 L$ L
5.1 Introduction. J" ^9 V+ G; P5 ~" A$ n
5.2 Maxwell's equations
+ `3 m4 f+ _8 j& ?1 |5.3 Brief history of Finite Difference Time Domain (FDTD) Method
, s5 q0 i4 i8 V, _5.4 Finite Difference Time Domain (FDTD) Method" _$ A; @6 j; X- j. z; V
5.5 -Direction-Implicit FDTD (ADI-FDTD): Beyond the Courant Limit
$ q5 \* J6 M, D; A& v) S: o2 @5 h5.6 Complex-Envelope ADI-FDTD (CE-ADI-* e: F) ^( J0 A8 P: j9 N* s
5.7 Perfectly Matched Layer (PML) Boundary Conditions
1 N2 v/ ]2 Q( K5.8 Uniaxal Perfectly Matched Layer (UPML) Absorbing Boundary Condition
% L) e+ A7 k6 b$ C: x2 k9 P$ B: I5.9 PML Parameters
0 O& F, x+ i, B, A5.10 PML Boundary Conditions for CE-ADI-FDTD1 x( K1 |8 L5 O
5.11 PhC Resonant Cavities
" s* J4 v5 @6 A2 s% Z- f5.12 5x5 Rectangular Lattice PhC Cavity
: _6 a+ o# f3 q; A6 q. k4 S9 H, Y5.13 Triangular Lattice PhC Cavity
, b% V0 @$ m" o' `3 y5.14 Wavelength Division Multiplexing
# r# H' g/ S0 \' h* O' y5.15 Conclusions
4 C- Z/ j  H: B6. Finite Volume time Domain (FVTD) Method
  \5 s" c2 F  k6 O  Q4 [% q6.1 Introduction
% f8 ], H7 f9 R6.2 Numerical analysis
" i' S8 d# d4 }" l* n6 k* B6.3 UPWIND Scheme for the Calculation3 L, R$ Q6 f* {3 F4 R
6.4 NON-DIFFUSIVE Scheme for the Flux Calculation+ R$ O1 a; {7 h; _, k; A
6.5 2D Formulation of the FVTD Method
& `* L6 R, S$ r5 L6 `0 d" Z( r+ ~6.6 Boundary Conditions1 z  i( i' H0 D4 t
6.7 Nonlinear Optics
8 G4 E( [2 E+ s9 Y: K' y6.8 Nonlinear Optical Interactions9 o1 J& G0 ?; T* X! X
6.9 Extension of the FDTD Method to Nonlinear Problems
( K' _$ ~$ \5 f1 V: w( @6 P6.10 Extension of the FVTD Method to Nonlinear Problems
/ @# s7 `" Z* s9 C* d; D: D6.11 Conclusions
1 @: [1 s% ^+ t4 p+ r! {7 Numerical Analysis of Linear and Nonlinear PhC Based Devices2 S5 C# L( {& l+ v5 ~
7.1 Introduction
: t# x: ]" O- C0 P4 w+ T' m  u7.2 FVTD Method Assessment: PhC Cavity
0 n- F0 U( g$ L$ c+ E$ X/ l7.3 FVTD Method Assessment: PhC Waveguide7 H0 E* V: L' A" |# [4 ^" j0 w
7.4 FVTD Method Assessment: PBG T-Branch& `' D5 Z5 O* J' E8 f
7.5 PhC Multimode Resonant Cavity
6 }% }4 `( n( y( A7 H* K7 G) @5 k7.6 FDTD Analysis of Nonlinear Devices& \, m" C9 N; d$ R$ n
7.7 FVTD Analysis of Nonlinear Photonic Crystal Wires3 _' C  I7 L' t5 ]& g1 W( _) j
7.8 Conclusions2 \9 W4 {) y* ]  M6 i7 a
8 Multiresolution Time Domain. c" S8 Q7 `9 p5 s$ {+ Y
8.1 Introduction% D4 K# r! C  o; z5 j
8.2 MRTD basics
% g* [0 B+ s2 ?5 \) W+ X4 ^8.3 MRTD update scheme
6 P3 F% {: ~! Y3 `' Y8.4 Scaling-MRTD" L; U% v- U" [5 t. u2 S, L
8.5 Conclusions0 ~+ v: U+ C% {9 o% P5 @) R( s
9 MRTD Analysis of PhC-Devices" X4 {/ d, H* m+ T7 D" m
9.1 Introduction
7 U3 x" |' p$ Z8 p7 e3 }8 S9.2 UPML-MRTD: test and code validation
8 H& N9 S& ^- s5 H& P' z0 M9.3 MRTD vs FDTD for the analysis of linear photonic crystals
: o! |- f1 a3 E" D( {. m! ]- b9.4 Conclusions+ _: p# J* U, |/ Z: @# p7 k
10 MRTD Analysis of SHG PhC-Devices; k6 J( J/ O8 _" O' \
10.1 Introduction
0 D% R* |4 @$ C! p$ x  {+ t10.2 Second hARMonic generation in optics$ F7 A/ t' q! I, m: C
10.3 Extended S-MRTD for SHG analysis
* U+ g& C4 j7 Z0 e10.4 SHG in PhC-waveguide
4 F9 k* A1 |1 t. l# g% c- Y8 [8 R10.5 Selective SHG in compound PhC-based structures. x5 V( r4 G3 K/ x9 r) N- X
10.6 New design for selective SHG: PhC-microcavities coupling
$ i/ ~7 u1 Z. L- M( A/ u) w! {10.7 Conclusions
0 k  P7 D& p  {# W11 Dispersive Nonlinear MRTD for SHG Applications
; ~7 d& h1 Y0 H% |7 Y' P: C6 }5 g7 M11.1 Introduction
2 V$ `6 y  ^- i1 |11.2 Dispersion analysis
& X) z  P+ k2 z11.3 SHG-MRTD scheme for dispersive materials1 W& d+ T8 V0 E& |5 {+ a0 h
11.4 Simulation results
1 N% W" ^, x" d( H2 _' l11.5 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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