Detailed Licensing
- Page ID
- 389270
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Overview
Title: CH-331 Text
Webpages: 114
Applicable Restrictions: Noncommercial
All licenses found:
- CC BY-NC-SA 4.0: 93.9% (107 pages)
- Undeclared: 6.1% (7 pages)
By Page
- CH-331 Text —
CC BY-NC-SA 4.0
- Front Matter — Undeclared
- 1: The Dawn of the Quantum Theory —
CC BY-NC-SA 4.0
- 1.1: Blackbody Radiation Cannot Be Explained Classically — CC BY-NC-SA 4.0
- 1.2: Quantum Hypothesis used for Blackbody Radiation Law — CC BY-NC-SA 4.0
- 1.3: Photoelectric Effect Explained with Quantum Hypothesis — CC BY-NC-SA 4.0
- 1.4: The Hydrogen Atomic Spectrum — CC BY-NC-SA 4.0
- 1.5: The Rydberg Formula and the Hydrogen Atomic Spectrum — CC BY-NC-SA 4.0
- 1.6: Matter Has Wavelike Properties — CC BY-NC-SA 4.0
- 1.7: de Broglie Waves can be Experimentally Observed — CC BY-NC-SA 4.0
- 1.8: The Bohr Theory of the Hydrogen Atom — CC BY-NC-SA 4.0
- 1.9: The Heisenberg Uncertainty Principle — CC BY-NC-SA 4.0
- 1.E: The Dawn of the Quantum Theory (Exercises) — CC BY-NC-SA 4.0
- 2: The Classical Wave Equation —
CC BY-NC-SA 4.0
- 2.1: The One-Dimensional Wave Equation — CC BY-NC-SA 4.0
- 2.2: The Method of Separation of Variables — CC BY-NC-SA 4.0
- 2.3: Oscillatory Solutions to Differential Equations — CC BY-NC-SA 4.0
- 2.4: The General Solution is a Superposition of Normal Modes — CC BY-NC-SA 4.0
- 2.5: A Vibrating Membrane — CC BY-NC-SA 4.0
- 2.E: The Classical Wave Equation (Exercises) — CC BY-NC-SA 4.0
- 3: The Schrödinger Equation & a Particle in a Box —
CC BY-NC-SA 4.0
- 3.1: The Schrödinger Equation — CC BY-NC-SA 4.0
- 3.2: Linear Operators in Quantum Mechanics — CC BY-NC-SA 4.0
- 3.3: The Schrödinger Equation is an Eigenvalue Problem — CC BY-NC-SA 4.0
- 3.4: The Quantum Mechanical Free Particle — CC BY-NC-SA 4.0
- 3.5: Wavefunctions Have a Probabilistic Interpretation — CC BY-NC-SA 4.0
- 3.6: The Energy of a Particle in a Box is Quantized — CC BY-NC-SA 4.0
- 3.7: Wavefunctions Must Be Normalized — CC BY-NC-SA 4.0
- 3.8: The Average Momentum of a Particle in a Box is Zero — CC BY-NC-SA 4.0
- 3.9B: Particle in a Finite Box and Tunneling (optional) — CC BY-NC-SA 4.0
- 3.9: The Uncertainty Principle Redux - Estimating Uncertainties from Wavefunctions — CC BY-NC-SA 4.0
- 3.10: A Particle in a Two-Dimensional Box — CC BY-NC-SA 4.0
- 3.11: A Particle in a Three-Dimensional Box — CC BY-NC-SA 4.0
- 3.E: The Schrödinger Equation and a Particle in a Box (Exercises) — CC BY-NC-SA 4.0
- 4: Postulates and Principles of Quantum Mechanics —
CC BY-NC-SA 4.0
- 4.1: The Wavefunction Specifies the State of a System — CC BY-NC-SA 4.0
- 4.2: Quantum Operators Represent Classical Variables — CC BY-NC-SA 4.0
- 4.3: Observable Quantities Must Be Eigenvalues of Quantum Mechanical Operators — CC BY-NC-SA 4.0
- 4.4: The Time-Dependent Schrödinger Equation — CC BY-NC-SA 4.0
- 4.5: The Eigenfunctions of Operators are Orthogonal — CC BY-NC-SA 4.0
- 4.6: Heisenburg Uncertainy Principle III - Commuting Operators — CC BY-NC-SA 4.0
- 4.E: Postulates and Principles of Quantum Mechanics (Exercises) — CC BY-NC-SA 4.0
- 5: The Harmonic Oscillator and the Rigid Rotor —
CC BY-NC-SA 4.0
- 5.1: A Harmonic Oscillator Obeys Hooke's Law — CC BY-NC-SA 4.0
- 5.2: The Equation for a Harmonic-Oscillator Model of a Diatomic Molecule Contains the Reduced Mass of the Molecule — CC BY-NC-SA 4.0
- 5.3: The Harmonic Oscillator is an Approximation — CC BY-NC-SA 4.0
- 5.4: The Harmonic Oscillator Energy Levels — CC BY-NC-SA 4.0
- 5.5: The Harmonic Oscillator and Infrared Spectra — CC BY-NC-SA 4.0
- 5.6: The Harmonic-Oscillator Wavefunctions Involve Hermite Polynomials — CC BY-NC-SA 4.0
- 5.7: Hermite Polynomials are either Even or Odd Functions — CC BY-NC-SA 4.0
- 5.8: The Energy Levels of a Rigid Rotor — CC BY-NC-SA 4.0
- 5.9: The Rigid Rotator is a Model for a Rotating Diatomic Molecule — CC BY-NC-SA 4.0
- 5.E: The Harmonic Oscillator and the Rigid Rotor (Exercises) — CC BY-NC-SA 4.0
- 6: The Hydrogen Atom —
CC BY-NC-SA 4.0
- 6.1: The Schrödinger Equation for the Hydrogen Atom Can Be Solved Exactly — CC BY-NC-SA 4.0
- 6.2: The Wavefunctions of a Rigid Rotator are Called Spherical Harmonics — CC BY-NC-SA 4.0
- 6.3: The Three Components of Angular Momentum Cannot be Measured Simultaneously with Arbitrary Precision — CC BY-NC-SA 4.0
- 6.4: Hydrogen Atomic Orbitals Depend upon Three Quantum Numbers — CC BY-NC-SA 4.0
- 6.5: s Orbitals are Spherically Symmetric — CC BY-NC-SA 4.0
- 6.6: Orbital Angular Momentum and the p-orbitals — CC BY-NC-SA 4.0
- 6.7: The Helium Atom Cannot Be Solved Exactly — CC BY-NC-SA 4.0
- 6.E: The Hydrogen Atom (Exercises) — CC BY-NC-SA 4.0
- 7: Approximation Methods —
CC BY-NC-SA 4.0
- 7.0: Slater's Rules for Shielding — CC BY-NC-SA 4.0
- 7.1: The Variational Method — CC BY-NC-SA 4.0
- 7.2: Linear Variational Method and the Secular Determinant — CC BY-NC-SA 4.0
- 7.3: Trial Functions Can Be Linear Combinations of Functions with Variational Parameters — CC BY-NC-SA 4.0
- 7.4: Perturbation Theory Expresses the Solutions in Terms of Solved Problems — CC BY-NC-SA 4.0
- 7.E: Approximation Methods (Exercises) — CC BY-NC-SA 4.0
- 8: Multielectron Atoms —
CC BY-NC-SA 4.0
- 8.1: Atomic and Molecular Calculations are Expressed in Atomic Units — CC BY-NC-SA 4.0
- 8.2: Perturbation Theory and the Variational Method for Helium — CC BY-NC-SA 4.0
- 8.3: Hartree-Fock Equations are Solved by the Self-Consistent Field Method — CC BY-NC-SA 4.0
- 8.4: An Electron Has An Intrinsic Spin Angular Momentum — CC BY-NC-SA 4.0
- 8.5: Wavefunctions must be Antisymmetric to Interchange of any Two Electrons — CC BY-NC-SA 4.0
- 8.6: Antisymmetric Wave Functions can be Represented by Slater Determinants — CC BY-NC-SA 4.0
- 8.7: Hartree-Fock Calculations Give Good Agreement with Experimental Data — CC BY-NC-SA 4.0
- 8.8: Term Symbols Gives Detailed Descriptions of an Electron Configuration — CC BY-NC-SA 4.0
- 8.8B: Multi-electron Considerations - A Closer Look at Helium — CC BY-NC-SA 4.0
- 8.9: The Allowed Values of J - the Total Angular Momentum Quantum Number — CC BY-NC-SA 4.0
- 8.10: Hund's Rules Determine the Term Symbols of the Ground Electronic States — CC BY-NC-SA 4.0
- 8.11: Using Atomic Term Symbols to Describe Atomic Spectra — CC BY-NC-SA 4.0
- 8.E: Multielectron Atoms (Exercises) — CC BY-NC-SA 4.0
- 9: The Chemical Bond: Diatomic Molecules —
CC BY-NC-SA 4.0
- 9.1: The Born-Oppenheimer Approximation Simplifies the Molecular Schrödinger Equation — CC BY-NC-SA 4.0
- 9.2: The H₂⁺ Prototypical Species — CC BY-NC-SA 4.0
- 9.2B: Solving the H₂⁺ System Exactly (Optional) — CC BY-NC-SA 4.0
- 9.3: The Overlap Integral — CC BY-NC-SA 4.0
- 9.3B: Evaluating the Overlap Integral (Optional) — CC BY-NC-SA 4.0
- 9.4: Chemical Bond Stability — CC BY-NC-SA 4.0
- 9.5: Bonding and Antibonding Orbitals — CC BY-NC-SA 4.0
- 9.6: A Simple Molecular-Orbital Treatment of H₂ Places Both Electrons in a Bonding Orbital — CC BY-NC-SA 4.0
- 9.7: Molecular Orbitals Can Be Ordered According to Their Energies — CC BY-NC-SA 4.0
- 9.8: Molecular-Orbital Theory Does not Predict a Stable Diatomic Helium Molecule — CC BY-NC-SA 4.0
- 9.9: Electrons Populate Molecular Orbitals According to the Pauli Exclusion Principle — CC BY-NC-SA 4.0
- 9.10: Molecular Orbital Theory Predicts that Molecular Oxygen is Paramagnetic — CC BY-NC-SA 4.0
- 9.E: The Chemical Bond: Diatomic Molecules (Exercises) — CC BY-NC-SA 4.0
- MathChapters —
CC BY-NC-SA 4.0
- A: Complex Numbers — CC BY-NC-SA 4.0
- B: Probability and Statistics — CC BY-NC-SA 4.0
- C: Vectors — CC BY-NC-SA 4.0
- D: Spherical Coordinates — CC BY-NC-SA 4.0
- E: Determinants — CC BY-NC-SA 4.0
- F: Matrices — CC BY-NC-SA 4.0
- G: Numerical Methods — CC BY-NC-SA 4.0
- H: Partial Differentiation — CC BY-NC-SA 4.0
- I: Series and Limits — CC BY-NC-SA 4.0
- J: The Binomial Distribution and Stirling's Appromixation — CC BY-NC-SA 4.0
- Back Matter — Undeclared