An introduction to quantum physics : a first course for physicists, chemists, materials scientists, and engineers /: a first course for physicists, chemists, materials scientists, and engineers. (2017)

• Record Type: Book
• Further Information: Note: Stefanos Trachanas, Manolis Antonoyiannakis, Leonidas Tsetseris.
• Authors: Trachanas, Stephanos; Antonoyiannakis, Manolis; Tsetseris, Leonidas
• Contents: Foreword xix Preface xxiii Editors’ Note xxvii Part I Fundamental Principles 1 1 The Principle ofWave–Particle Duality: An Overview 3 1.1 Introduction 3 1.2 The Principle ofWave–Particle Duality of Light 4 1.2.1 The Photoelectric Effect 4 1.2.2 The Compton Effect 7 1.2.3 A Note on Units 10 1.3 The Principle ofWave–Particle Duality of Matter 11 1.3.1 From Frequency Quantization in ClassicalWaves to Energy Quantization in MatterWaves: The Most Important General Consequence of Wave–Particle Duality of Matter 12 1.3.2 The Problem of Atomic Stability under Collisions 13 1.3.3 The Problem of Energy Scales:Why Are Atomic Energies on the Order of eV, While Nuclear Energies Are on the Order of MeV? 15 1.3.4 The Stability of Atoms and Molecules Against External Electromagnetic Radiation 17 1.3.5 The Problem of Length Scales:Why Are Atomic Sizes on the Order of Angstroms, While Nuclear Sizes Are on the Order of Fermis? 19 1.3.6 The Stability of Atoms Against Their Own Radiation: Probabilistic Interpretation of MatterWaves 21 1.3.7 How Do Atoms Radiate after All? Quantum Jumps from Higher to Lower Energy States and Atomic Spectra 22 1.3.8 Quantized Energies and Atomic Spectra:The Case of Hydrogen 25 1.3.9 Correct and Incorrect Pictures for the Motion of Electrons in Atoms: Revisiting the Case of Hydrogen 25 1.3.10 The Fine Structure Constant and Numerical Calculations in Bohr’s Theory 29 1.3.11 Numerical Calculations with MatterWaves: Practical Formulas and Physical Applications 31 1.3.12 A Direct Confirmation of the Existence of MatterWaves:The Davisson–Germer Experiment 33 1.3.13 The Double-Slit Experiment: Collapse of theWavefunction Upon Measurement 34 1.4 Dimensional Analysis and Quantum Physics 41 1.4.1 The Fundamental Theorem and a Simple Application 41 1.4.2 Blackbody Radiation Using Dimensional Analysis 44 1.4.3 The Hydrogen Atom Using Dimensional Analysis 47 2 The Schrödinger Equation and Its Statistical Interpretation 53 2.1 Introduction 53 2.2 The Schrödinger Equation 53 2.2.1 The Schrödinger Equation for Free Particles 54 2.2.2 The Schrödinger Equation in an External Potential 57 2.2.3 Mathematical Intermission I: Linear Operators 58 2.3 Statistical Interpretation of Quantum Mechanics 60 2.3.1 The “Particle–Wave” Contradiction in Classical Mechanics 60 2.3.2 Statistical Interpretation 61 2.3.3 Why DidWe Choose P(x) = |'�(x)|2 as the Probability Density? 62 2.3.4 Mathematical Intermission II: Basic Statistical Concepts 63 2.3.4.1 Mean Value 63 2.3.4.2 Standard Deviation (or Uncertainty) 65 2.3.5 Position Measurements: Mean Value and Uncertainty 67 2.4 Further Development of the Statistical Interpretation: The Mean-Value Formula 71 2.4.1 The General Formula for the Mean Value 71 2.4.2 The General Formula for Uncertainty 73 2.5 Time Evolution ofWavefunctions and Superposition States 77 2.5.1 Setting the Stage 77 2.5.2 Solving the Schrödinger Equation. Separation of Variables 78 2.5.3 The Time-Independent Schrödinger Equation as an Eigenvalue Equation: Zero-Uncertainty States and Superposition States 81 2.5.4 Energy Quantization for Confined Motion: A Fundamental General Consequence of Schrödinger’s Equation 85 2.5.5 The Role of Measurement in Quantum Mechanics: Collapse of the Wavefunction Upon Measurement 86 2.5.6 Measurable Consequences of Time Evolution: Stationary and Nonstationary States 91 2.6 Self-Consistency of the Statistical Interpretation and the Mathematical Structure of Quantum Mechanics 95 2.6.1 Hermitian Operators 95 2.6.2 Conservation of Probability 98 2.6.3 Inner Product and Orthogonality 99 2.6.4 Matrix Representation of Quantum Mechanical Operators 101 2.7 Summary: Quantum Mechanics in a Nutshell 103 3 The Uncertainty Principle 107 3.1 Introduction 107 3.2 The Position–Momentum Uncertainty Principle 108 3.2.1 Mathematical Explanation of the Principle 108 3.2.2 Physical Explanation of the Principle 109 3.2.3 Quantum Resistance to Confinement. A Fundamental Consequence of the Position–Momentum Uncertainty Principle 112 3.3 The Time–Energy Uncertainty Principle 114 3.4 The Uncertainty Principle in the Classical Limit 118 3.5 General Investigation of the Uncertainty Principle 119 3.5.1 Compatible and Incompatible Physical Quantities and the Generalized Uncertainty Relation 119 3.5.2 Angular Momentum: A Different Kind of Vector 122 Part II Simple Quantum Systems 127 4 Square Potentials. I: Discrete Spectrum—Bound States 129 4.1 Introduction 129 4.2 Particle in a One-Dimensional Box:The Infinite PotentialWell 132 4.2.1 Solution of the Schrödinger Equation 132 4.2.2 Discussion of the Results 134 4.2.2.1 Dimensional Analysis of the Formula En = (ℏ2'�2?M2mL2)n2. DoWe Need an Exact Solution to Predict the Energy Dependence on ℏ, m, and L? 135 4.2.2.2 Dependence of the Ground-State Energy on ℏ, m, and L :The Classical Limit 136 4.2.2.3 The Limit of Large Quantum Numbers and Quantum Discontinuities 137 4.2.2.4 The Classical Limit of the Position Probability Density 138 4.2.2.5 Eigenfunction Features: Mirror Symmetry and the Node Theorem 139 4.2.2.6 Numerical Calculations in Practical Units 139 4.3 The Square PotentialWell 140 4.3.1 Solution of the Schrödinger Equation 140 4.3.2 Discussion of the Results 143 4.3.2.1 Penetration into Classically Forbidden Regions 143 4.3.2.2 Penetration in the Classical Limit 144 4.3.2.3 The Physics and “Numerics” of the Parameter '� 145 5 Square Potentials. II: Continuous Spectrum—Scattering States 149 5.1 Introduction 149 5.2 The Square Potential Step: Reflection and Transmission 150 5.2.1 Solution of the Schrödinger Equation and Calculation of the Reflection Coefficient 150 5.2.2 Discussion of the Results 153 5.2.2.1 The Phenomenon of Classically Forbidden Reflection 153 5.2.2.2 Transmission Coefficient in the “Classical Limit” of High Energies 154 5.2.2.3 The Reflection Coefficient Depends neither on Planck’s Constant nor on the Mass of the Particle: Analysis of a Paradox 154 5.2.2.4 An Argument from Dimensional Analysis 155 5.3 Rectangular Potential Barrier: Tunneling Effect 156 5.3.1 Solution of the Schrödinger Equation 156 5.3.2 Discussion of the Results 158 5.3.2.1 Crossing a Classically Forbidden Region: The Tunneling Effect 158 5.3.2.2 Exponential Sensitivity of the Tunneling Effect to the Energy of the Particle 159 5.3.2.3 A Simple Approximate Expression for the Transmission Coefficient 160 5.3.2.4 Exponential Sensitivity of the Tunneling Effect to the Mass of the Particle 162 5.3.2.5 A Practical Formula for T 163 6 The Harmonic Oscillator 167 6.1 Introduction 167 6.2 Solution of the Schrödinger Equation 169 6.3 Discussion of the Results 177 6.3.1 Shape ofWavefunctions. Mirror Symmetry and the Node Theorem 178 6.3.2 Shape of Eigenfunctions for Large n:The Classical Limit 179 6.3.3 The Extreme Anticlassical Limit of the Ground State 180 6.3.4 Penetration into Classically Forbidden Regions:What Fraction of Its “Lifetime” Does the Particle “Spend” in the Classically Forbidden Region? 181 6.3.5 A Quantum Oscillator Never Rests: Zero-Point Energy 182 6.3.6 Equidistant Eigenvalues and Emission of Radiation from a Quantum Harmonic Oscillator 184 6.4 A Plausible Question: CanWe Use the PolynomialMethod to Solve Potentials Other than the Harmonic Oscillator? 187 7 The Polynomial Method: Systematic Theory and Applications 191 7.1 Introduction: The Power-Series Method 191 7.2 Sufficient Conditions for the Existence of Polynomial Solutions: Bidimensional Equations 194 7.3 The PolynomialMethod in Action: Exact Solution of the Kr
• Edition: 1st
• Publisher Details: Weinheim : Wiley-VCH
• Publication Date: 2017
• Extent: 1 online resource
• Subjects: 530.12; Quantum theory
• Languages: English
• ISBNs: 9783527676682; 9783527676651; 9783527676675
• Related ISBNs: 9783527412471
• Notes: Note: Description based on CIP data; resource not viewed.
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