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量子力学(英文版) 读者对象:本书适用于物理学专业人员
郑海荣主编的这本《量子力学(英文版)》内容 包括初等量子力学的基本理论、基本构架及解决问题 的基本方法;量子理论在典型题中的应用;简单近似 方法;全同粒子体系的量子理论;量子理论的最新进 展及实际应用举例;动画及模拟练习;问题讨论与练 习。本书可作为高等学校的教材。
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Content 目录
Preface 前言 Part I The Wave Funclion and Schrodinger Equalion 第一部分 波函数及薛定谔方程 Chapter 1 The wave function and Schrodinger equation 波函数和薛定谔方程 1 1.1 The wave-particle duality and matter wave 波粒工象性与物质波 1 1.2 Wave function and its statistica1 interpretation 波函数及其统计解释 5 1.3 The principle of superpos山on 态叠加原理 8 1.4 The Schradinger equation 薛定谔方程 9 Biography 人物档案 11 Essay 短文:Schrodinger cat and EPR paradox 薛定谔猫和EPR佯谬 14 Associated application 相关应用:TEM and SEM 透射及扫描电子显微镜 16 Animation and simulation 演示与模拟 18 Discussion questions 讨论问题 21 Exercises 习题 22 Chapter 2 Time-independent Schrodinger eqnation and its application in one dimension 定态薛定谔方程及其在一维问题中的应用 23 2.1 Time-independent Schradinger equation and the stationary state 定态薛定谔方程和定态 23 2.2 The bound state and discrete spectra 束缚态与分立谱 27 2.3 Reflection and transmission tunneling effect 反射与透射,隧穿效应 44 Biography 人物档案 54 Associated application 相关应用:STM 扫描隧道显微镜 55 Anima tion and sim ula tion 演示与模拟 56 Discussion questions 讨论问题 60 Exercises 习题 60 Part II Physical Observables and Representations 第二部分 可观测物理量及表象理论 Chapter 3 Physical observables and representations 可观测量及其表示理论 64 3.1 Observables and operators 力学量与算符 64 3.2 Eigenvalues and eigenvectors of Hermitian operators 厄米算符的本征值与本征矢量 71 3.3 Representations and their transformations 表象理论与表象变换 80 3.4 The uncertainty principle 不确定原理 89 3.5 Dirac notation and the occupation number representation 狄拉克符号与占有数表象 94 Biography 人物档案 102 Essay 短文:Heisenberg and matrix mechanics 海森伯与矩阵力学 102 Anima tion and sim ula tion 演示与模拟 103 Discussion questions 讨论问题 108 Exercises 习题 108 Part III Applicalions of Ihe Schrodinger Equalion in 3D 第三部分 薛定谔方程在三维空间中的应用 Chapter 4 A particle in a central field 中心力场中的粒子 110 4.1 A particle in a central field 中心力场中的粒子 110 4.2 The radial equation for an electron in the Coulomb potential 库仑场中运动电子的径向方程 118 4.3 The hydrogen atom 氢原子 124 Biography 人物档案 129 Essay 短文:Niels Bohr and his theory for the hydrogen atom 波尔和他的氢原子理论 130 Associated appli四,non 相关应用:Cluantum computer 量子计算机 131 Discussion questions 讨论问题 133 Exercises 习题 134 Part IV Approximalion Melhods 第四部分 近似方法 Chapter 5 Perturhation theory 微扰理论 135 5.1 Time-independent perturbation theory 定态微扰理论 136 5.2 Time-dependent perturbation theory 含时微扰理论 148 5.3 The adiabatic theorem 绝热理论 171 Biography 人物档案 174 Essay 短文:Berry phase Berry 相位 175 Associated application 相关应用:Laser 激光 177 Animation and simulation 演示与模拟 178 Discussion questions 讨论问题 180 Exercises 习题 182 Part V Spin and Idenlical Parlicle Syslem 第五部分 自旋和全同多粒子体系 Chapter 6 Spin and Identical Particle System 自旋和全同粒子体系 185 6.1 The Stern-Gerlach experiment and its interpretation 斯特恩-格拉赫实验及其解释 185 6.2 The description of spin 自旋的描述 189 6.3 The Schrodinger equation of charged particles in an external electromagnetic field 带电粒子在外电磁场中的薛定诗方程 194 6.4 Total angular momentum 总角动量 199 6.5 Fine structure of alkali atoms 碱金属原子的精细结构 205 6.6 The Zeeman effect 塞曼效应 208 6.7 Characteristics of identical particIes 全同粒子的特征 212 6.8 The wave function for a system of identical particles 全同粒子体系的波函数 214 6.9 Wave functions for two-electron system 两电子体系的波函数 218 6.10 The helium atom 氮原子 224 Biography 人物档案 228 Essay 短文:Quantum entanglement and Bell theorem 量子纠缠与Bell定理 232 Associated application 相关应用:Bose-Einstein condensation 玻色爱因斯坦凝聚 234 Anima tion and simulation 演示与模拟 237 Discussion questions 讨论问题 239 Exercises 习题 240 References 参考文献 242 Appendices 附录 244 Index 索引 263
Part I The Wave Function and Schrodinger Equation
第一部分波函数及薛定谔方程 Chapter 1 The wave function and Schrodinger equation 波函数和薛定谔方程 The wave-particle duality and matter wave 波粒二象性与物质波 Particles and waves are two distinct entities in classical physics. As we have learned from both text books and daily experiences,a particle is a localized bundle of energy and momentum. At any tnstant, it can be described by state parameters,such as position q and momentum p (or velocity v if the mass is a constant). The parameters q and p evolve \n time according to some equations of motion,such as Newton’s law F = dp /dt. Given the tnitial values q (tz) and p (t ) at time tt, the position q (t) and momentum pit) at any time t can be deduced from the equations of motion. In contrast to the particle, a wave is considered as a periodic disturbance spread over space. It usually appears as some kind of periodic movement transferring energy from one point to another. A wave satisfies the superposition rules and presents jnterference and diffraction phenomena. 1.1.1 The wave-particle duality of light 光的波粒二象性 In the 17lh century, two competing theories of light were proposed during the debate about the nature of light: one was offered by Christian Huygens and the other by Isaac Newton. According to the theories,light was thought either to consist of waves (Huygens) or of corpuscles/particles (Newton). Huygens proposed that each point on a light wave front acted as a spherical point source for the progressing wave. Newton’s argument satisfactorily and more simply explained geometric optics and did not presume a medium for particle travel.At the beginning of 1 9lh century (801?1805),Thomas Young conducted the famous double-slit experiment showing that light from two slits interfere to produce a fringe pattern on a screen,a phenomenon that cannot be described by classical particles. In 1909?Geoffrey Ingram Taylor conducted an experiment that showed the interference phenomena by individual photons. The double-slit experiment has been repeated in many ways over the years and has become a standard demonstration of wave-like motion. But neither Newton nor Young were quite convincing about the nature of light. Light could not be described purely as a wave or as consisting of particles. In 1900, Max Planck postulated that the energy of oscillators in a black body is an integer multiple of hv,where h is the Planck constant and v is the frequency of the oscillator. The problem was that the wave nature of light was widely accepted at that time,the concept have been completely formulated in Maxwell’s theory and confirmed by interference and diffraction experiments. After Planck’s quanta hypothesis, Albert Einstein postulated the concept of the photon to explain the photoelectric effect in 1 905, which also was used later to explain Compton scattering. According to Einstein’s assumption, electromagnetic radiation of frequency v consists of discrete units (quanta) of energy hv. That is, electromagnetic energy itself is quantized,and a single quantum is called photon. Thus, mater can absorb energy from a monochromatic beam of light of frequency v only in units of hv because the light arrives in the form of discrete quanta, each with energy hv. Einstein had re-introduced the problem of wave- particle duality for light! The relation between the light wave (v,A ) and the light photon (e,_p)is presented by the equations where h is the Planck constant. Eqs (1.1.1) and (1.1.2) are called the Planck- Einstein relations,which reflect the wave-particle duality of light. 1.1.2 Matter wave and the wave -particle duality of matter 物质波及物质的波粒二象性 If the light could sometimes behave like particles, then should matter particles also show wave-like behavior? Upon examining Einstein’s idea of the parallelism between the light and matter,Louis de Broglie in 1 924 proposed that electrons,which generally are believed to be particles, should exhibit wave-like behavior. The wavelength and frequency of a quantum mechanical particle are associated with its momentum and energy by de Broglie’s hypothesis Where e and p are the energy and momentum of the particle,and v represents the frequency. The wavelength of the matter wave associated with the particle, A, is also called de Broglie wavelength. In the case of non-relativistic theory,the de Broglie wavelength for a free particle with mass m and energy e is The wave nature of an electron and de Broglie’s hypothesis have been experimentally confirmed by electron diffraction experiments by G. P. Thompson, and C. Davisson & L. Germer. In short, any matter must be considered as having both the particle-like and wave -like properties. You may want to argue that common sense tells us that billiard balls and ping-pong balls travel along definite trajectories and do not show any wave-like properties! The point is that the wave nature of matter is not apparent for macroscopic phenomena since Planck’s constant h is so small. For example, s ……
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