Quantum Mechanics, Volume 2

Höfundur Claude Cohen-Tannoudji; Bernard Diu; Franck Laloë

Útgefandi Wiley Global Research (STMS)

Snið ePub

Print ISBN 9783527345540

Útgáfa 2

Útgáfuár 2019

15.390 kr.

Description

Efnisyfirlit

  • Cover
  • Foreword
  • Acknowledgments
  • Chapter VIII: An elementary approach to the quantum theory of scattering by a potential
  • A. Introduction
  • B. Stationary scattering states. Calculation of the cross section
  • C. Scattering by a central potential. Method of partial waves
  • COMPLEMENTS OF CHAPTER VIII, READER’S GUIDE
  • Complement AVIII The free particle: stationary states with well-defined angular momentum
  • 1. The radial equation
  • 2. Free spherical waves
  • 3. Relation between free spherical waves and plane waves
  • Complement BVIII Phenomenological description of collisions with absorption
  • 1. Principle involved
  • 2. Calculation of the cross sections
  • Complement CVIII Some simple applications of scattering theory
  • 1. The Born approximation for a Yukawa potential
  • 2. Low energy scattering by a hard sphere
  • 3. Exercises
  • Chapter IX: Electron spin
  • A. Introduction of electron spin
  • B. Special properties of an angular momentum 1/2
  • C. Non-relativistic description of a spin 1/2 particle
  • COMPLEMENTS OF CHAPTER IX, READER’S GUIDE
  • Complement AIX Rotation operators for a spin 1/2 particle
  • 1. Rotation operators in state space
  • 2. Rotation of spin states
  • 3. Rotation of two-component spinors
  • Complement BIX Exercises
  • Chapter X: Addition of angular momenta
  • A. Introduction
  • B. Addition of two spin 1/2’s. Elementary method
  • C. Addition of two arbitrary angular momenta. General method
  • COMPLEMENTS OF CHAPTER X, READER’S GUIDE
  • Complement AX Examples of addition of angular momenta
  • 1. Addition of j1 = 1 and j2 = 1
  • 2. Addition of an integral orbital angular momentum and a spin 1/2
  • Complement BX Clebsch-Gordan coefficients
  • 1. General properties of Clebsch-Gordan coefficients
  • 2. Phase conventions. Reality of Clebsch-Gordan coefficients
  • 3. Some useful relations
  • Complement CX Addition of spherical harmonics
  • 1. The functions ΦMJ(Ω1; Ω2)
  • 2. The functions Fml (Ω)
  • 3. Expansion of a product of spherical harmonics; the integral of a product of three spherical harmonics
  • Complement DX Vector operators: the Wigner-Eckart theorem
  • 1. Definition of vector operators; examples
  • 2. The Wigner-Eckart theorem for vector operators
  • 3. Application: calculation of the Landé gJ factor of an atomic level
  • Complement EX Electric multipole moments
  • 1. Definition of multipole moments
  • 2. Matrix elements of electric multipole moments
  • Complement FX Two angular momenta J1 and J2 coupled by an interaction aJ1 J2
  • 1. Classical review
  • 2. Quantum mechanical evolution of the average values 〈J1〉 and 〈J2〉
  • 3. The special case of two spin 1/2’s
  • 4. Study of a simple model for the collision of two spin 1/2 particles
  • Complement GX Exercises
  • Chapter XI: Stationary perturbation theory
  • A. Description of the method
  • B. Perturbation of a non-degenerate level
  • C. Perturbation of a degenerate state
  • COMPLEMENTS OF CHAPTER XI, READER’S GUIDE
  • Complement AXI A one-dimensional harmonic oscillator subjected to a perturbing potential in x, x2, x3
  • 1. Perturbation by a linear potential
  • 2. Perturbation by a quadratic potential
  • 3. Perturbation by a potential in x3
  • Complement BXI Interaction between the magnetic dipoles of two spin 1/2 particles
  • 1. The interaction Hamiltonian W
  • 2. Effects of the dipole-dipole interaction on the Zeeman sublevels of two fixed particles
  • 3. Effects of the interaction in a bound state
  • Complement CXI Van der Waals forces
  • 1. The electrostatic interaction Hamiltonian for two hydrogen atoms
  • 2. Van der Waals forces between two hydrogen atoms in the 1s ground state
  • 3. Van der Waals forces between a hydrogen atom in the 1s state and a hydrogen atom in the 2p state
  • 4. Interaction of a hydrogen atom in the ground state with a conducting wall
  • Complement DXI The volume effect: the influence of the spatial extension of the nucleus on the atomic levels
  • 1. First-order energy correction
  • 2. Application to some hydrogen-like systems
  • Complement EXI The variational method
  • 1. Principle of the method
  • 2. Application to a simple example
  • 3. Discussion
  • Complement FXI Energy bands of electrons in solids: a simple model
  • 1. A first approach to the problem: qualitative discussion
  • 2. A more precise study using a simple model
  • Complement GXI A simple example of the chemical bond: the H+2 ion
  • 1. Introduction
  • 2. The variational calculation of the energies
  • 3. Critique of the preceding model. Possible improvements 1201
  • 4. Other molecular orbitals of the H+2 ion
  • 5. The origin of the chemical bond; the virial theorem
  • Complement HXI Exercises
  • Chapter XII: An application of perturbation theory: the fine and hyperfine structure of hydrogen
  • A. Introduction
  • B. Additional terms in the Hamiltonian
  • C. The fine structure of the n = 2 level
  • D. The hyperfine structure of the n = 1 level
  • E. The Zeeman effect of the 1s ground state hyperfine structure
  • COMPLEMENTS OF CHAPTER XII, READER’S GUIDE
  • Complement AXII The magnetic hyperfine Hamiltonian
  • 1. Interaction of the electron with the scalar and vector potentials created by the proton
  • 2. The detailed form of the hyperfine Hamiltonian
  • 3. Conclusion: the hyperfine-structure Hamiltonian
  • Complement BXII Calculation of the average values of the fine-structure Hamiltonian in the 1s, 2s and 2p states
  • 1. Calculation of 〈1/R〉, 〈1/R2〉 and 〈1/R3〉
  • 2. The average values 〈Wmv〉
  • 3. The average values 〈WD〉
  • 4. Calculation of the coefficient ξ2p associated with WSO in the 2p level
  • Complement CXII The hyperfine structure and the Zeeman effect for muonium and positronium
  • 1. The hyperfine structure of the 1s ground state
  • 2. The Zeeman effect in the 1s ground state
  • Complement DXII The influence of the electronic spin on the Zeeman effect of the hydrogen resonance line
  • 1. Introduction
  • 2. The Zeeman diagrams of the 1s and 2s levels
  • 3. The Zeeman diagram of the 2p level
  • 4. The Zeeman effect of the resonance line
  • Complement EXII The Stark effect for the hydrogen atom
  • 1. The Stark effect on the n = 1 level
  • 2. The Stark effect on the n = 2 level
  • Chapter XIII: Approximation methods for time-dependent problems
  • A. Statement of the problem
  • B. Approximate solution of the Schrödinger equation
  • C. An important special case: a sinusoidal or constant perturbation
  • D. Random perturbation
  • E. Long-time behavior for a two-level atom
  • COMPLEMENTS OF CHAPTER XIII, READER’S GUIDE
  • Complement AXIII Interaction of an atom with an electromagnetic wave
  • 1. The interaction Hamiltonian. Selection rules
  • 2. Non-resonant excitation. Comparison with the elastically bound electron model
  • 3. Resonant excitation. Absorption and induced emission
  • Complement BXIII Linear and non-linear responses of a two-level system subject to a sinusoidal perturbation
  • 1. Description of the model
  • 2. The approximate solution of the Bloch equations of the system
  • 3. Discussion
  • 4. Exercises: applications of this complement
  • Complement CXIII Oscillations of a system between two discrete states under the effect of a sinusoidal resonant perturbation
  • 1. The method: secular approximation
  • 2. Solution of the system of equations
  • 3. Discussion
  • Complement DXIII Decay of a discrete state resonantly coupled to a continuum of final states
  • 1. Statement of the problem
  • 2. Description of the model
  • 3. Short-time approximation. Relation to first-order perturbation theory .
  • 4. Another approximate method for solving the Schrödinger equation
  • 5. Discussion
  • Complement EXIII Time-dependent random perturbation, relaxation
  • 1. Evolution of the density operator
  • 2. Relaxation of an ensemble of spin 1/2’s
  • 3. Conclusion
  • Complement FXIII Exercises
  • Chapter XIV Systems of identical particles
  • A. Statement of the problem
  • B. Permutation operators
  • C. The symmetrization postulate
  • D. Discussion
  • COMPLEMENTS OF CHAPTER XIV, READER’S GUIDE
  • Complement AXIV Many-electron atoms. Electronic configurations
  • 1. The central-field approximation
  • 2. Electron configurations of various elements
  • Complement BXIV Energy levels of the helium atom. Configurations, terms, multi-plets
  • 1. The central-field approximation. Configurations
  • 2. The effect of the inter-electron electrostatic repulsion: exchange energy, spectral terms
  • 3. Fine-structure levels; multiplets
  • Complement CXIV Physical properties of an electron gas. Application to solids
  • 1. Free electrons enclosed in a box
  • 2. Electrons in solids
  • Complement DXIV Exercises
  • Appendix I: Fourier series and Fourier transforms
  • 1. Fourier series
  • 2. Fourier transforms
  • Appendix II: The Dirac δ-”function”
  • 1. Introduction; principal properties
  • 2. The -”function” and the Fourier transform
  • 3. Integral and derivatives of the δ-”function”
  • 4. The δ-”function” in three-dimensional space
  • Appendix III: Lagrangian and Hamiltonian in classical mechanics
  • 1. Review of Newton’s laws
  • 2. The Lagrangian and Lagrange’s equations
  • 3. The classical Hamiltonian and the canonical equations
  • 4. Applications of the Hamiltonian formalism
  • 5. The principle of least action
  • BIBLIOGRAPHY OF VOLUMES I and II
  • Index [The notation (ex.) refers to an exercise]
  • End User License Agreement

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