非线性纤维光学(第4版)
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品牌: 阿瓜瓦尔
基本信息·出版社：世界图书出版公司
·页码：529 页
·出版日期：2009年
·ISBN：7506292572/9787506292573
·条形码：9787506292573
·包装版本：4版
·装帧：平装
·开本：24
·正文语种：中文
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内容简介《非线性纤维光学》(第4版)是一本内容非常新颖的非线性纤维光学的研究生教材。自1989年初版以来,随着非线性纤维光学的迅速发展,作者对其内容不断地更新和扩充。
编辑推荐《非线性纤维光学》(第4版)虽保留了第1版的大部分内容，但更重要的是它全面介绍了非线性纤维光学领域的最新研究成果，这一特点使得该书不仅是一本优秀的教材，也是相关领域的科学家和工程师的一本重要的参考书。
目录
~Preface
1 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
References
2 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
References
Group-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
References
4 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
References
5 Optical Solitons
5.1 Modulation Instability
5.1.1 Linear Stability Analysis
5.1.2 Gain Spectrum
5.1.3 Experimental Results
5.1.4 Ultrashort Pulse Generation
5.1.5 Impact cn Lightwave Systems
5.2 Fiber Solitons
5.2.1 Inverse Scattering Method
5.2.2 Fundamental Soliton
5.2.3 Higher-Order Solitons
5.2.4 Experimental Confirmation
5.2.5 Soliton Stability
5.3 Other Types of Solitons
5.3.1 Dark Solitons
5.3.2 Dispersion-Managed Solitons
5.3.3 Bistable Solitons
5.4 Perturbation ef Solitons
5.4.1 Perturbation Methods
5.4.2 Fiber Losses
5.4.3 Soliton Amplification
5.4.4 Soliton Interaction
5.5 Higher-Order Effects
5.5.1 Moment Equations for Pulse Parameters
5.5.2 Third-Order Dispersion
5.5.3 Self-Steepening
5.5.4 Intrapulse Raman Scattering
5.5.5 Propagation of Femtosecond Pulses
Problems
References
6 Polarization Effects
6.1 Nonlinear Birefringence
6.1.1 Origin of Nonlinear Birefringence
6.1.2 Ccupled-Mode Equations
6.1.3 Elliptically Birefringent Fibers
6.2 Nonlinear Phase Shift
6.2.1 Nondispersive XPM
6.2.2 Optical Kerr Effect
6.2.3 Pulse Shaping
6.3 Evolution of Polarization State
6.3.1 Analytic Solution
6.3.2 Poincare-Sphere Representation
6.3.3 Polarization Instability
6.3.4 Polarization Chaos
6.4 Vector Modulation Instability
6.4.1 Low-Birefringence Fibers
6.4.2 High-Birefringence Fibers
6.4.3 Isotropic Fibers
6.4.4 Experimental Results
6.5 Birefringence and Solitons
6.5.1 Low-Birefringence Fibers
6.5.2 High-Birefringence Fibers
6.5.3 Soliton-Dragging Logic Gates
6.5.4 Vector Solitons
6.6 Random Birefringence
6.6.1 Polarization-Mode Dispersion
6.6.2 Vector Form of the NLS Equation
6.6.3 Effects of PMD on Solitons
Problems
References
7 Cross-Phase Modulation
7.1 XPM-Induced Nonlinear Coupling
7.1.1 Nonlinear Refractive Index
7.1.2 Coupled NLS Equations
7.2 XPM-Induced Modulation Instability
7.2.1 Linear Stability Analysis
7.2.2 Experimental Results
7.3 XPM-Paired Solitons
7.3.1 Bright-Dark Soliton Pair
7.3.2 Bright-Gray Soliton Pair
7.3.3 Periodic Solutions
7.3.4 Multiple Coupled NLS Equations
7.4 Spectral and Temporal Effects
7.4.1 Asymmetric Spectral Broadening
7.4.2 Asymmetric Temporal Changes
7.4.3 Higher-Order Nonlinear Effects
7.5 Applications of XPM
7.5.1 XPM-Induced Pulse Compression
7.5.2 XPM-Induced Optical Switching
7.5.3 XPM-Induced Nonreciprocity
7.6 Polarization Effects
7.6.1 Vector Theory of XPM
7.6.2 Polarization Evolution
7.6.3 Polarization-Dependent Spectral Broadening
7.6.4 Pulse Trapping and Compression
7.6.5 XPM-Induced Wave Breaking
7.7 XPM Effects in Birefringent Fibers
7.7.1 Fibers with Low Birefringence
7.7.2 Fibers with High Birefringence
Problems
References
8 Stimulated Raman Scattering
9 Stimulated Brillouin Scattering
10 Four-Wave Mixing
11 Highly Nonlinear Fibers
12 Novel Nonlinear Phenomena
A System of Units
B Numerical Code for the NLS Equation
C List of Acronyms
Index~
……[看更多目录]
序言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.
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