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




