Quantum Physics II
Quantum mechanics rebuilt in Dirac notation — spin, dynamics and angular momentum.
What this course covers
- The Schrödinger Equation
- Wave Function Must Be Complex
- First-Order Time Evolution
- Linearity and Superposition
- Probability Density and the Born Rule
- Conservation of Normalization
- Probability Current and Continuity Equation
- Energy Eigenstates and the Time-Independent Schrödinger Equation
- The Spectrum and Degeneracy
- Orthonormality of Energy Eigenstates
- Physical Equivalence of Wave Functions Differing by a Phase
- Bound states in one dimension
- Time-independent Schrödinger equation scaling
- No degeneracy theorem for bound states
- Energy eigenstates can be chosen real
- Bound-state solutions are real up to a global phase
- Even potentials and parity of eigenstates
- Bound-state parity is strictly even or odd
- Wave functions as vectors
- Position operator X̂ in matrix form
- Expectation value of position
- Eigenstates of the position operator
- Momentum operator P̂ in position representation
- Canonical commutation relation [X̂, P̂] = iℏ
- Momentum operator as a matrix
- Eigenstates of the momentum operator
- Stern-Gerlach experiment and spin-½ quantization
- Two-dimensional complex vector space as spin state space
- Eigenstates and eigenvalues of the Ŝ_z operator
- Basis states and linear superposition
- Column-vector representation of spin states
- Orthonormality of basis states
- Bra vectors and the inner product
- Eigenvalues from matrix polynomial equations
- Trace and eigenvalue sum relationship
- Pauli matrix commutation algebra
- Anti-commutator and Pauli matrix anti-commutation
- General Pauli matrix product formula
- Vector of operators and dot product notation (A·σ)
- (A·σ)(B·σ) product formula
- Spin operator along arbitrary direction (Ŝₙ)
- Cross product of operator triplets and S×S
- Vector spaces: definition and axioms
- Linear maps (operators) definition
- Operators on a vector space
- Examples of linear operators
- Space of operators as a vector space
- Operator multiplication (composition)
- Non-commutativity of operators
- The commutator of two operators
- T-invariant subspaces
- Eigenvalue equation (abstract form)
- Spectrum of an operator
- Non-invertibility and eigenvalues
- Linear independence of eigenvectors with distinct eigenvalues
- Characteristic polynomial and eigenvalue existence
- Degenerate eigenvalues
- Inner product definition and motivation
- Properties of the dot product as inner product axioms
- Linear Functionals on Vector Spaces
- Representing Linear Functionals via Inner Products
- Proof of the Representation Theorem
- Definition of the Adjoint (Hermitian Conjugate) Operator
- Linearity of the Adjoint Operator
- Hermitian operators and real expectation values
- Eigenvalues of Hermitian operators are real
- Orthogonality of eigenvectors for distinct eigenvalues
- Degeneracy of eigenvalues
- Unitary operators and norm preservation
- Invertibility of unitary operators
- S†S = I for unitary operators
- Unitary operators preserve inner products
- Unitary transformations map orthonormal bases to orthonormal bases
- Quantum uncertainty of an operator
- Variance formula for uncertainty
- Computing uncertainty: worked spin example
- Statement of the general uncertainty principle
- Hermiticity of the commutator times 1/i
- Position-momentum uncertainty principle
- Proof via the Cauchy-Schwarz inequality
- Energy-time uncertainty and state overlap
- Uncertainty principle lower bound on ground state energy
- Expectation values of X and P in symmetric bound states
- Variance identity linking ΔP and ⟨P²⟩
- Expectation value inequality ⟨A²⟩ ≥ ⟨A⟩²
- Minimizing the bounding function to extract the energy bound
- Diagonalization of linear operators
- Unitary diagonalizability and orthonormal eigenbases
- Quantum harmonic oscillator definition
- Canonical commutation relation [X, P] = iħ
- Hilbert space of square-integrable functions
- Factorization of the Hamiltonian
- Ground state energy lower bound from factorization
- Creation and annihilation operators A† and A
- Number operator N = A†A
- Ladder operator commutators with H
- Algebraic construction of the energy spectrum
- Unitary time evolution operator
- Time-independent Hamiltonian: solving for U
- Functions of operators on eigenstates
- Time-dependent commuting Hamiltonian: solving for U
- Time-ordered exponential for general H(T)
- Heisenberg picture of quantum mechanics
- Heisenberg Picture Operators
- Time-Dependent Creation and Annihilation Operators
- Motivation for Coherent States
- Unitary Translation Operator
- Action of Translation Operator on X̂ and P̂
- Definition of Coherent States
- Expectation Values in Coherent States
- Classical Time Evolution of Coherent States
- Minimum Uncertainty and Shape Preservation
- Coherent States in the Energy Basis
- Coherent states review
- Complex alpha plane representation
- Photon number uncertainty in coherent states
- Phase-number uncertainty relation
- Position and momentum uncertainties of coherent states
- Squeeze states via Hamiltonian change
- Bogoliubov transformation
- Squeezed uncertainties
- Photon states as quantum field theory
- Energy of the electromagnetic field
- Single-mode electromagnetic field configuration
- Electromagnetic energy as a harmonic oscillator
- Massless harmonic oscillator and unit analysis
- Quantization of the EM field via operator promotion
- Photon number states and energy quantization
- Electric field as a quantum operator
- Expectation value of electric field in photon number states
- General two-state Hamiltonian review
- Ammonia molecule as a two-state system
- Double-well potential and tunneling intuition
- Constructing the ammonia Hamiltonian
- Energy eigenvalues and the 2Δ energy gap
- Energy eigenstates as symmetric and antisymmetric superpositions
- Spin-direction picture for eigenstates
- Time evolution of the N-up state (Larmor precession)
- NMR spin Hamiltonian setup
- Non-commuting time-dependent Hamiltonians
- Rotating reference frame strategy
- Unitary transformation and rotated wave function
- Hamiltonian from a unitary operator
- Transformed Hamiltonian formula
- Similarity transformation of spin operators
- Time-independent rotating-frame Hamiltonian
- Tensor product vector space
- Zero vector in the tensor product space
- Inner product on the tensor product space
- Normalizing a two-particle state
- Entangled vs. separable states
- Determinant criterion for entanglement
- Singlet state properties
- Probability of joint spin measurements on entangled state
- Two-spin state overlap formula
- Physical realisation of entangled spin states
- Einstein–Podolsky–Rosen (EPR) argument
- Local realism: measurement corresponds to reality
- Local realism: locality (no distant influence)
- Hidden variables as implementation of local realism
- Vectors under rotations definition
- Scalars and vectors from dot and cross products
- Angular momentum commutation relations
- L_i commutes with L²
- General angular momentum algebra with J
- Vector identity for vectors under rotations
- L² in terms of R and P (operator identity)
- L² as an angular differential operator
- Hamiltonian for central potentials
- Spherical Harmonics as Angular Wavefunctions
- Differential Operator Forms of L², L_z, and L±
- Completeness and Orthogonality of Spherical Harmonics
- Constructing Spherical Harmonics via Ladder Operators
- Hamiltonian in Spherical Coordinates
- Separation of Variables for the 3D Schrödinger Equation
- The Radial Equation and the Substitution u = rF
- Central potential and radial wave function
- Effective potential and centrifugal barrier
- Energy spectrum diagram for central potentials
- Spherical Bessel functions for the free particle
- Infinite spherical well setup
- Bound states in 3D vs 1D potentials
- L=0 infinite spherical well solution
- Energy quantization and natural energy scale
- Zeros of spherical Bessel functions and general quantization
- Hellmann-Feynman Theorem
- First-Order Energy Correction via Perturbation
- Addition of Angular Momentum — Motivation
- Angular Momentum Algebra on a Vector Space
- Tensor Product of Angular Momentum Spaces
- Total Angular Momentum as a Sum
- Proof that Total Angular Momentum Satisfies the Algebra
- Spin-orbit coupling and fine structure
- Hyperfine structure from proton spin
- Magnetic dipole moments and g-factors
- Magnetic dipole field of the proton
- Hyperfine Hamiltonian construction
- Symmetry argument for angular integrals
- Ground-state hyperfine energy shift
- Addition of two spin-1/2 particles
- Addition of Angular Momentum
- Hydrogen Atom Energy Spectrum
- Runge-Lenz Vector Definition
- Conservation of the Runge-Lenz Vector
- R̂² in Terms of H and L²
- Orthogonality of R̂ and L̂
- Vector Operators Under Rotations
Syllabus
Lectures
- 1. Wave Mechanics
- 2. Wave Mechanics (continued)
- 3. Wave Mechanics (continued) and Stern-Gerlach Experiment
- 4. Spin One-half, Bras, Kets, and Operators
- 5. Linear Algebra: Vector Spaces and Operators
- 6. Linear Algebra: Vector Spaces and Operators (continued)
- 7. Linear Algebra: Vector Spaces and Operators (continued)
- 8. Linear Algebra: Vector Spaces and Operators (continued)
- 9. Dirac's Bra and Ket Notation
- 10. Uncertainty Principle and Compatible Observables
- 11. Uncertainty Principle and Compatible Observables (continued)
- 12. Quantum Dynamics
- 13. Quantum Dynamics (continued) | Heisenberg Picture
- 14. Quantum Dynamics (continued)
- 15. Quantum Dynamics (continued)
- 16. Quantum Dynamics (continued) and Two State Systems
- 17. Two State Systems (continued)
- 18. Two State Systems (continued), Multiparticle States and Tensor Products
- 19. Multiparticle States and Tensor Products (continued)
- 20. Multiparticle States and Tensor Products (continued) and Angular Momentum
- 21. Angular Momentum (continued)
- 22. Angular Momentum (continued)
- 23. Angular Momentum (continued)
- 24. Addition of Angular Momentum
- 25. Addition of Angular Momentum (continued)
- 26. Addition of Angular Momentum (continued)