did-you-know? rent-now

Amazon no longer offers textbook rentals. We do!

did-you-know? rent-now

Amazon no longer offers textbook rentals. We do!

We're the #1 textbook rental company. Let us show you why.

9780486441535

The Fundamental Principles of Quantum Mechanics With Elementary Applications

by
  • ISBN13:

    9780486441535

  • ISBN10:

    0486441539

  • Edition: Revised
  • Format: Hardcover
  • Copyright: 2005-01-27
  • Publisher: Dover Publications
  • Purchase Benefits
  • Free Shipping Icon Free Shipping On Orders Over $35!
    Your order must be $35 or more to qualify for free economy shipping. Bulk sales, PO's, Marketplace items, eBooks and apparel do not qualify for this offer.
  • eCampus.com Logo Get Rewarded for Ordering Your Textbooks! Enroll Now
List Price: $85.00

Summary

Written by a professor of physics at Harvard University, this volume is an inductive presentation of quantum mechanics designed for graduate students or specialists in other branches of physics. Although some acquaintance with advanced mathematics and the data of the physical sciences is preferable, this treatment is simple, clear, and easily followed. Applications of the theory are interwoven with development of the basic mathematical structure.

Table of Contents

PREFACE vii
NOTATION xvii
REFERENCE ABBREVIATIONS xvii
* An asterisk before the number of a section or subsection indicates that the section or subsection so marked may be omitted or skimmed to advantage on first reading.
CHAPTER I INTRODUCTION TO DUALISTIC THEORY OF MATTER; DEVELOPMENT OF SCHRÖDINGER'S WAVE EQUATION 1(34)
1. Historical Introduction
1(3)
2. The Dualistic Theory of Radiation
4(3)
3. An Analogy between Geometrical Optics and Classical Mechanics
7(3)
4. Wave Packets and Group Velocity
10(4)
5. The Schrödinger Wave Equation for a Single Particle
14(5)
5a. The Time-free Equation
14(1)
5b. The Second (General) Schrödinger Equation
15(4)
*6. The Application of the Restricted Relativity Principle
19(2)
7. The Wave Equation for a System of Many Particles
21(8)
7a. Formulation of Equation
21(2)
7b. Relation of Schrödinger Equation to the Classical Hamiltonian Function
23(1)
*7c. The Schrödinger Equation and the Hamilton-Jacobi Equation
24(2)
*7d. The Wave Equation for a System of Charged Particles in a Classical External Electromagnetic Field
26(3)
8. The Physical Interpretation of the Wave Function and the Normalization Condition
29(6)
8a. Probability and Quadratic Integrability
29(2)
8b. Normalization and Mass Current Density
31(2)
8c. A System Consisting of Two Independent Parts
33(2)
CHAPTER II WAVE PACKETS AND THE RELATION BETWEEN CLASSICAL MECHANICS AND WAVE MECHANICS 35(43)
9. Wave Packets and Group Velocity in a One-dimensional Homogeneous Medium
35(6)
9a. The Fourier Integral Theorem
35(2)
9b. Derivation of Group-velocity Formula
37(4)
10. Wave Packets in Three Dimensions
41(2)
11. Wave Surfaces and the Hamilton-Jacobi Equation of the Classical Dynamics
43(3)
12. Wave Packets and the Motion of Particles in a Force Field; Fermat's Principle
46(3)
13. Direct Rigorous Proof of Newton's Second Law of Motion for Wave Packets
49(2)
14. The Statistical Interpretation of the Wave Theory of Matter
51(7)
14a. Review of Assumptions
51(2)
14b. Necessity of Introducing Assemblages
53(3)
14c. Multiplicity of Energy and Momentum Values for a Definite State
56(2)
15. The Wave Function and Measurements of Linear Momentum
58(14)
15a. Operational Definition of Momentum for Free Particles
58(2)
15b. Computation of Momentum Probabilities from a Wave Function.
60(3)
*15c. Momentum of Center of Gravity
63(3)
*15d. The Measurement of the Momenta of Particles Moving in a Force Field
66(2)
*15e. Individual Momenta of Particles in a System
68(1)
15f. Summary: The Determination of the Wave Function of an Assemblage
69(3)
16. The Heisenberg Uncertainty Principle
72(6)
CHAPTER III ONE-DIMENSIONAL ENERGY-LEVEL PROBLEMS 78(35)
17. Boundary and Continuity Conditions; Eigenvalues and Eigenfunctions
78(3)
18. The One-Dimensional Anharmonic Oscillator
81(1)
19. The Qualitative Behavior of the Integral Curves: Existence of Class A Eigenfunctions
82(5)
19a. Behavior of Integral Curves in Regions of Positive and Negative Kinetic Energy
82(2)
19b. The Discrete Eigenfunctions
84(1)
19c. The Continuous Spectrum of Class B Eigenfunctions
85(1)
19d. The Paradox of the Nodes
86(1)
20. The Planck Ideal Linear Oscillator
87(3)
20a. The Sommerfeld Polynomial Method
87(2)
20b. Determination of the Eigenvalues
89(1)
20c. The Eigenfunctions and Their Properties
89(1)
21. An Approximation Method Which Correlates the Eigenvalues of Wave Mechanics with the Energy Levels of the Bohr Theory
90(23)
21a. The B.W.K. Approximations for ψ(x)
90(3)
21b. Application to Eigenvalue Problem
93(2)
*21c. Zwaan's Method and the Stokes Phenomenon
95(2)
*21d. Analysis of the Stokes Phenomenon
97(3)
*21e. Derivation of the Connection Formulas
100(3)
*21f. Derivation of the Sommerfeld Phase-integral Quantum Condition
103(4)
*21g. Higher Approximations
107(1)
*21h. Modification of Method for Radial Motion in Two-particle Problem
107(1)
21i. Asymptotic Agreement of Wave Theory and Classical Theory Regarding Position of Particle
108(1)
21j. The Transmission of Progressive Matter Waves through a Potential Hill
109(4)
CHAPTER IV THE MATHEMATICAL THEORY OF COMPLETE SYSTEMS OF ORTHOGONAL FUNCTIONS 113(27)
22. Scalar Products and Systems of Orthogonal Functions
113(8)
22a. Expansion in a Series of Functions
113(1)
22b. Comparison of Properties of Vectors and Functions
114(1)
22c. Scalar Products of Vectors
115(1)
22d. Scalar Products of Quadratically Integrable Functions of m Variables
116(3)
22e. Spaces of Infinitely Many Dimensions
119(1)
22f. Proof of Orthogonality of Eigenfunctions of the One-dimensional Anharmonic Oscillator Problem
120(1)
23. Self-adjoint Operators and Equations. The Sturm-Liouville Problem.
121(9)
23a. Self-adjoint Differential Operators in One Dimension
121(2)
23b. Orthogonality with Respect to a Density Function p
123(1)
23c. The Sturm-Liouville Problem
124(1)
23d. Singular-point Boundary Conditions
125(3)
*23e. Existence of Discrete Eigenvalues for Sturm-Liouville Problems with Singular End Points
128(2)
24. Reduction of Eigenvalue Problems Based on Self-adjoint Differential Equations to Variational Form
130(2)
25. Completeness of System of Discrete Eigenfunctions of a Sturm-Liouville Problem
132(8)
*25a. The Eigenvalues as Absolute Minima
132(3)
*25b. The Expansion of Arbitrary Functions in Terms of Eigenfunctions
135(5)
CHAPTER V THE DISCRETE ENERGY SPECTRUM OF THE TWO-PARTICLE CENTRAL-FIELD PROBLEM 140(22)
26. The Behavior of Solutions of an Ordinary Second-order Differential Equation near a Singular Point
140(3)
27. The Legendre Polynomials
143(3)
27a. General Properties of the Legendre Equation
143(1)
27b. Explicit Determination of Eigenvalues and Eigenfunctions
144(2)
28. The Energy Levels of the Two-particle Problem
146(11)
28a. The Wave Equation
146(1)
28b. Separation of the Variables
146(1)
28c. The Azimuthal Factor of the Wave Function
147(1)
28d. Determination of &Theta(theta) and Its Eigenvalues
148(1)
28e. Completeness of System of Eigenfunctions
149(1)
28f. Physical Interpretation of Quantum Numbers l and m
150(2)
28g. Behavior of Radial Wave Functions at Boundary Points
152(3)
28h. The Dumbbell Model of the Diatomic Molecule
155(2)
29. The Hydrogenic Atom
157(5)
29a. Application of the B.W.K. Method
157(1)
29b. Application of Polynomial Method
158(2)
29c. Generalized Laguerre Polynomials
160(1)
29d. The Most General Eigenfunction
161(1)
CHAPTER VI THE CONTINUOUS SPECTRUM AND THE BASIC PROPERTIES OF SOLUTIONS OF THE MANY-PARTICLE PROBLEM 162(57)
30. The Continuous Spectrum in One-dimensional Problems
162(16)
30a. The Nature and Use of the Eigenfunctions of the Continuous Spectrum
162(1)
30b. The Weyl Theory
163(2)
*30c. Formal Treatment of Continuous Spectrum as the Limit of a Discrete Spectrum
165(3)
*30d. The Spacing of Energy Levels in Problems β and α
168(1)
530e. The Eigendifferentials
169(2)
*30f. Passage from the Completeness Theorem for Problem β to That for Problem α
171(2)
30g. The Fourier Integral Formulas a Special Case
173(1)
30h. Normal Packet Functions in One Dimension
174(1)
30i. Normal Packet Functions for the Two-particle Problem
174(2)
*30j. Normalization of the Class B Radial Eigenfunctions for the Hydrogenic Atom
176(2)
31. Weak Quantization. Theory of Radioactive Emission of Alpha Particles
178(17)
31a. Weak Quantization in General
178(1)
31b. A Model for Alpha Particle Disintegration
179(2)
31c. Resonant Energy Intervals
181(5)
31d. Energy Distribution in Weakly Quantized States
186(1)
31e. The Disintegration Process
187(5)
*31f. Complex Eigenvalues
192(3)
32. The Existence and Properties of Solutions of the Many-particle Schrödinger Eigenvalue-eigenfunction Problem
195(24)
32a. Introduction
195(2)
32b. New Boundary Conditions for Physically Admissible Wave Functions
197(4)
*32c. Approximating Arbitrary Quadratically Integrable Functions by Means of Class D Functions
201(1)
32d. Hermitian Character of the Hamiltonian Operator
202(4)
32e. Reduction of the Eigenvalue-eigenfunction Problem for Discrete Spectra to Variational Form
206(1)
32f. A Lower Bound for the Energy Integral
207(1)
32g. Behavior of Solutions of the Differential Equation at Singular Domains
208(5)
32h. The Auger Effect
213(1)
32i. The Discrete Eigenfunctions of the Differential Equation as Minimizing Functions
214(1)
32j. The Continuous Spectrum and the Completeness of the System of Eigenfunctions
215(2)
32k. Degeneracy
217(2)
CHAPTER VII DYNAMICAL VARIABLES AND OPERATORS 219(59)
33. The Mean Values of the Cartesian Coordinates and Conjugate Linear Momenta
219(5)
33a. The Statistical Mean Values of the Coordinates
219(1)
33b. The Linear Momentum Operator
220(4)
34. The Angular-momentum Operators
224(10)
34a. Definition of Operators
224(1)
34b. Hermitian Character of Angular-momentum Operators
225(1)
34c. The Expansion Theorem
226(1)
34d. Angular Momentum of a System of Particles
227(2)
34e. Mean Values
229(1)
34f. The Vector Angular Momentum and Its Square; the Symmetric Top
230(4)
35. The Energy Operators
234(6)
35a. Calculation of Probabilities and Mean Values of Energy
234(3)
*35b. Transformation of Hamiltonian Operator
237(3)
36. Dynamical Variables in General
240(38)
36a. Remarks on the Value of the General Theory
240(2)
36b. Possibility of Defining Physical Quantities by Operators
242(3)
36c. The Transformation of Probability Amplitudes and Dynamical Variables
245(3)
36d. Type 1 Operators as Dynamical Variables
248(8)
36e. Calculation of Probabilities
256(3)
36f. Type 2 Operators as Dynamical Variables; the Method of von Neumann
259(6)
36g. The Method of Dirac and Jordan
265(3)
*36h. Multiplication Operators in Many Dimensions
268(2)
36i. Transformation of Probability Amplitudes from One Arbitrary Coordinate Scheme to Another
270(5)
36j. Dynamical Variables with Complex Eigenvalues
275(3)
CHAPTER VIII COMMUTATION RULES AND RELATED MATTERS 278(40)
37. Simultaneous Eigenfunctions and the Commutation of Dynamical Variables
278(10)
37a. Operator Algebra
278(1)
37b. Functions of a Single Operator
279(2)
37c. Commutative Operators
281(5)
37d. Functions of a Normal Set of Commuting Dynamical Variables.
286(2)
38. The Conservation Laws
288(5)
38a. Conservation of Energy
288(1)
38b. Variation of Energy When the Hamiltonian Depends on the Time
289(1)
38c. Conservation of an Arbitrary Dynamical Variable
290(1)
38d. Commutation Properties of the Hamiltonian and the Angular Momentum
291(2)
39. Conjugate Dynamical Variables and Quantum-mechanical Equations of Motion
293(10)
39a. Conjugate Dynamical Variables
293(7)
39b. Functions of Non-commuting Linear Operators
300(1)
39c. An Operator Form of Hamilton's Equations of Motion
301(2)
40. Symmetry Properties of the Wave Equation
303(15)
40a. Symmetry Properties in General
303(2)
40b. The Reflection Operators
305(1)
40c. The Rotation Operator
306(2)
40d. The Permutation Operators
308(2)
40e. Degeneracy and the Integrals of the Schrödinger Equation
310(3)
40f. The Normal Degeneracy of the Energy Levels of Free Atomic Systems
313(5)
CHAPTER IX THE MEASUREMENT OF DYNAMICAL VARIABLES 318(30)
41. General Theory of Measurement
318(16)
41a. Fundamental Characteristics of Measurements
318(2)
41b. Pure States and Mixtures
320(2)
41c. Postulates Regarding Retrospective and Predictive Measurements
322(4)
41d. The Reduction of the Wave Packet
326(5)
41e. Classical Orbits and Wave Packets
331(3)
42. More About Measurements
334(14)
42a. Conjugate Variables and Measurements
334(1)
42b. Impossibility of Measurements Which Imply Distinction between Particles of Same Species
335(6)
42c. A Classification of Observations
341(1)
42d. Measurements as Correlations
342(1)
42e. The Observing Mechanism Not Entirely Classical
343(5)
CHAPTER X MATRIX THEORY 348(32)
43. Matrix Algebra
348(4)
44. Matrices and Operators
352(14)
44a. The Derivation of Matrices from Operators
352(3)
44b. Canonical Matrix Transformations
355(4)
44c. Matrix Form of the Eigenvalue-eigenfunction Problem
359(4)
*44d. Matrices with Continuous Elements
363(3)
45. The Matrix Theory of Heisenberg, Born, and Jordan
366(8)
45a. Fundamental Postulates
366(2)
45b. Correlation of the Heisenberg and Schrödinger Theories
368(2)
45c. Solution of Matrix Equations of Motion for an Ideal Linear Oscillator
370(2)
45d. Reduction of the Fundamental Problem of Matrix Mechanics to a Principal-axis Transformation
372(2)
46. The Bohr Correspondence Principle and Its Relationship to Matrix Theory
374(6)
46a. The Bohr Postulates
374(1)
46b. The Bohr Correspondence Principle and the Heisenberg Matrix Theory
375(5)
CHAPTER XI THEORY OF PERTURBATIONS WHICH Do NOT INVOLVE THE TIME 380(47)
47. The Perturbation Theory for Nondegenerate Problems
380(8)
47a. First-order Perturbations
380(4)
47b. Second-order Perturbations
384(2)
47c. An Example: The Diatomic Molecule
386(2)
48. The Perturbation Theory for Degenerate Problems
388(10)
48a. First-order Energy Perturbations
388(3)
48b. Second-order Energy Perturbations
391(3)
*48c. Van Vleck's Method for Second-order Perturbations
394(2)
48d. Simplification of Perturbation Calculations by Means of Integrals of the Perturbed Hamiltonian
396(2)
49. The Energy Levels of an Hydrogenic Atom in a Uniform Magnetic Field (Spin Neglected)
398(5)
49a. Derivation of Hamiltonian Operator
398(1)
49b. Legitimacy of the Perturbation Method
399(1)
49c. First-order Energy Correction; Relation to Magnetic Moment and Larmor Precession
400(2)
49d. The Second-order Energy Correction
402(1)
50. The Energy Levels of an Hydrogenic Atom in a Uniform Electric Field.
403(5)
51. The Variational Method
408(11)
51a. Reduction of the Variational Problem to Algebraic Form
408(2)
51b. The Ritz Method
410(5)
*51c. Higher Roots of the Secular Equation
415(1)
51d. General Observations Regarding the Use of the Variational Method
416(2)
51e. Modifications of the Method; Construction of Eigenfunctions from Non-orthogonal System
418(1)
52. The Problem of the Hydrogen Molecule
419(8)
52a. The Fixed-nuclei Problem
419(1)
52b. The Heitler and London Calculation
420(5)
52c. The Method of James and Coolidge
425(2)
CHAPTER XII QUANTUM STATISTICAL MECHANICS AND THE EINSTEIN TRANSITION PROBABILITIES 427(47)
53. Quantum Statistical Mechanics
427(21)
53a. The General Theory of Perturbations Which May Involve the Time
427(4)
53b. The Adiabatic Theorem
431(1)
53c. The Fundamental Problems of Quantum Statistical Mechanics
432(2)
53d. The Conventional Characterization of a Chaotic Assemblage
434(5)
53e. Transition Probabilities and Statistical Equilibrium for Chaotic Assemblages
439(7)
53f. The Gibbs Canonical Assemblage for Systems of the Most General Type
446(2)
54. The Absorption and Emission of Radiation: Perturbation of an Atomic System by a Classical Radiation Field
448(21)
54a. The Einstein Derivation of the Planck Radiation Formula
448(2)
54b. Elementary Approaches to the Quantum Theory of the Einstein Transition Probabilities
450(2)
54c. The Perturbing Hamiltonian for a Classical Radiation Field
452(2)
54d. The Born Transition Probability
454(4)
54e. The Einstein Transition Probabilities
458(4)
54f. Spectroscopic Stability
462(1)
*54g. Magnetic Dipole and Electric Quadrupole Radiation
462(7)
55. Some Elementary Selection Rules for Electric Dipole Radiation
469(5)
55a. The Harmonic Oscillator
469(1)
55b. Selection Rules for the Two-particle Problem
470(1)
55c. Fine Structure and Polarization of Spectrum Lines in Simple Zeeman Effect
471(3)
CHAPTER XIII INTRODUCTION TO THE PROBLEM OF ATOMIC STRUCTURE: ELECTRON SPIN. 474(49)
56. The Atomic Problem as a Two-particle Problem
474(7)
56a. The Empirical Basis for the Idealized Bohr Atom Model
474(4)
56b. Derivation of the Ritz Formula
478(3)
57. The Bohr Assignment of Electronic Quantum Numbers
481(10)
57a. The Quantum Numbers of the Valence Electrons in the Spectra of the Alkalies and Alkaline Earths
481(3)
57b. Perturbation Theory and the Significance of an Assignment of Quantum Numbers to Inner Electrons
484(7)
58. The Electron-spin Hypothesis
491(12)
58a. The Empirical Fine Structure of Spectrum Lines
491(4)
58b. The Combination of Angular Momenta
495(3)
58c. The Lande Magnetic Core Theory
498(2)
58d. Solution of the Fine-structure Problem by the Electron-spin Hypothesis
500(3)
59. The Fine Structure of the Spectra of Atomic Systems with a Single Valence Electron
503(4)
60. The Approximate Relativistic Theory of the Hydrogen Atom
507(3)
61. The Pauli Wave-mechanical Formulation of the Theory of Electron Spin
510(13)
61a. Nature of the Configuration Space and Wave Functions
510(2)
61b. Preliminary Discussion of Spin Operators and Spin Matrices
512(7)
61c. Application of the Pauli Theory to the Alkali Doublets
519(4)
CHAPTER XIV THE THEORY OF THE STRUCTURE OF MANY-ELECTRON ATOMS 523(34)
62. General Formulation of the Problem
523(5)
62a. The Configuration Space
523(1)
62b. The Hamiltonian Operator
524(2)
62c. The Perturbation Form of the General Atomic Problem
526(2)
63. Problem B: The Spin-orbit Energy Neglected
528(12)
63a. Integrals of the Motion
528(5)
63b. Antisymmetric Functions and the Empirical Pauli Exclusion Rule
533(3)
63c. Closed Shells
536(1)
63d. Terms Originating in a Given Configuration
537(3)
64. Selection Rules for Electric Dipole Radiation
540(7)
64a. The Laporte Rule
540(1)
64b. Selection Rules for the Central-field Problem
541(2)
64c. Selection Rules for Problems B and C
543(4)
65. The Helium Atom and Exchange Energy
547(8)
65a. Two-electron Atoms
547(6)
65b. The Exchange Phenomenon
553(2)
66. Diagonal Sums and the Problem B Energy Levels
555(2)
APPENDICES 557(42)
A. The Calculus of Variations and the Principle of Least Action
557(7)
B. Derivation of Equation (15.7)
564(4)
C. Theorems Regarding the Linear Oscillator Problem
568(4)
D. Mathematical Notes on the B.W.K. Method
572(7)
E. The Reduction of Certain Boundary-value Problems Based on Self-adjoint Differential Equations to Variational Form
579(4)
F. The Legendre Polynomials and Associated Legendre Functions
583(2)
G. The Generalized Laguerre Orthogonal Functions
585(3)
H. Two Theorems Relating to the Continuous Spectrum
588(4)
I. Concerning the Expansion of Hf in Spherical Harmonics
592(2)
J. The Jacobi Polynomials
594(2)
K. Schlapp's Method
596(3)
NAME INDEX 599(4)
SUBJECT INDEX 603

Supplemental Materials

What is included with this book?

The New copy of this book will include any supplemental materials advertised. Please check the title of the book to determine if it should include any access cards, study guides, lab manuals, CDs, etc.

The Used, Rental and eBook copies of this book are not guaranteed to include any supplemental materials. Typically, only the book itself is included. This is true even if the title states it includes any access cards, study guides, lab manuals, CDs, etc.

Rewards Program