非線性纖維光學(xué)

前言

　　Since the publication of the first edition of this book in 1989， the field of nonlinear fiber optics has remained an active area of research and has thus continued to grow at a rapid pace. During the 1990s， a major factor behind such a sustained growth was the advent of fiber amplifiers and lasers， made by doping silica fibers with rare-earth materials such as erbium and ytterbium. Erbium-doped fiber amplifiers revolutionized the design of fiber-optic communication systems， including those making use of optical solitons， whose very existence stems from the presence of nonlinear effects in optical fibers. Optical amplifiers permit propagation of lightwave signals over thousands of kilometers as they can compensate for all losses encountered by the signal in the optical domain. At the same time， fiber amplifiers enable the use of massive wavelength-division multiplexing， a technique that led by 1999 to the development of lightwave systems with capacities exceeding 1 Tb/s. Nonlinear fiber optics plays an important role in the design of such high-capacity lightwave systems. In fact， an understanding of various nonlinear effects occurring inside optical fibers is almost a prerequisite for a lightwave-system designer.　　Starting around 2000， a new development occurred in the field of nonlinear fiber optics that changed the focus of research and has led to a number of advances and novel applications in recent years. Several kinds of new fibers， classified as highly nonlinear fibers， have been developed. They are referred to with names such as microstructured fibers， holey fibers， or photonic crystal fibers， and share the common property that a relatively narrow core is surrounded by a cladding containing a large number of air holes. The nonlinear effects are enhanced dramatically in such fibers to the extent that they can be observed even when the fiber is only a few centimeters long. Their dispersive properties are also quite different compared with those of conventional fibers devel-oped for telecommunication applications. Because of these changes， microstructured fibers exhibit a variety of novel nonlinear effects that are finding applications in fields as diverse as optical coherence tomography and high-precision frequency metrology.

內(nèi)容概要

這是一本內(nèi)容非常新穎的非線性纖維光學(xué)的研究生教材。自1989年初版以來,隨著非線性纖維光學(xué)的迅速發(fā)展,作者對其內(nèi)容不斷地更新和擴(kuò)充。這最新版雖保留了第1版的大部分內(nèi)容，但更重要的是它全面介紹了非線性纖維光學(xué)領(lǐng)域的最新研究成果，這一特點使得該書不僅是一本優(yōu)秀的教材，也是相關(guān)領(lǐng)域的科學(xué)家和工程師的一本重要的參考書。

書籍目錄

Preface1  Introducdon  1.1  Historical Perspective  1.2  FiberCharacteristics      1.2.1  Matedal and Fabrication　　1.2.2  Fiber Losses    1.2.3  Chromatic Dispersion    1.2.4  Polarization.Mode Dispersion　1.3  FiberNonlinearities    1.3.1  NonlinearRefraction　　1.3.2  Stimulated Inelastic Scattering　　1.3.3  Importance of Nonlinear Effects　1.4  0verview　Problems　References2 ndsc Propagation in Fibers  2.1  Maxwell’S Equations  2.2  FlberModes    2.2.1  Eigenvalue Equation    2.2.2  Single.ModeCondition    2.2.3  Charactedstics of the Fundamental Mode  2.3  Pulse.PropagationEquation    2.3.1  NonlinearPulsePropagation    2.3.2  Higher-OrderNonlinearEffects    2.4  NumericalMethods    2.4.1  Split-Step FourierMethod    2.4.2  nniCC.Difference Methods　Problems　ReferencesGroup-Velocity Dispersion　3.1  Different Propagation Regimes　3.2  Dispersion-Induced Pulse Broadening    3.2.1  Gaussian Pulses    3.2.2  Chirped Gaussian Pulses    3.2.3  Hyperbolic Secant Pulses    3.2.4  Super-Gaussian Pulses    3.2.5  Experimental Results　3.3  Third-Order Dispersion    3.3.1  Evolution of Chirped Gaussian Pulses     3.3.2  Broadening Factor    3.3.3  Arbitrary-Shape Pulses    3.3.4  Ultrashort-Pulse Measurements　3.4  DispersionManagement    3.4.1  GvD.InducedLimitations    3.4.2  DispersionCompensation    3.4.3  Compensation of Thifd—Order Dispersion.　Problems  　References4  Self.Phase Modulafion  4.1  SPM-Induced Spectral Changes    4.1.1  NonlinearPhase Shift      4.1.2  ChangesinPulseSpectra    4.1.3  Effect of Pulse Shape and Initial Chirp    4.1.4  EffCC[ofPartial Coherence  4.2  Effect of Group-Velocity Dispersion    4.2.1  PulseEvolution    4。2.2  BroadeningFactor    4.2.3  0ptic~wave Breaking    4.2.4  ExperimentalResults    4.2.5  Effect of Third，Order Dispersion    4.2.6  SPMEffectsinFiberAmplifiers　4.3  Semianalytic Techniques    4.3.1  MomentMethod    4.3.2  VariationalMethod    4.3.3  Specific Analytic Solutions　4.4  Higher-OrderNonlinearEffects     4.4.1  Self-Steepening    4.4.2  Effect of GVD on Optical Shocks    4.4.3  Intrapulse Raman Scat~fing　Problems 　References5　Optical Solitons6　Polarization Effects7　Cross-Phase Modulation8　Stimulated Raman Scattering9　Stimulated Brillouin Scattering10　Four-Wave Mixing11　Highly Nonlinear Fibers12　Novel Nonlinear PhenomenaA　System of UnitsB　Numerical Code for the NLS EquationC　List of AcronymsIndex

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