Quantum Mechanics
Quantum Mechanics in 28 chapters — from “Blackbody radiation and the photoelectric effect” to “The Dirac equation and quantum electrodynamics”.
Chapters
- Blackbody radiation and the photoelectric effect
- Classical physics at the turn of the century
- The ultraviolet catastrophe
- Planck’s resolution
- The photoelectric effect
- Einstein 1905: light quanta
- What was established, and what remained
- Summary and forward view
- Problems
- Atomic spectra and the Bohr model
- Atomic spectra before Bohr
- The Rutherford atom, 1911
- Bohr’s postulates, 1913
- Derivation of the Bohr spectrum
- The Franck-Hertz experiment, 1914
- What Bohr got right, and what he got wrong
- The correspondence principle
- Summary and forward view
- Problems
- Wave-particle duality and matter waves
- Light is a wave
- Light is a particle, too
- De Broglie’s hypothesis, 1924
- Davisson and Germer, 1927
- The double-slit experiment with electrons
- Schrödinger’s wave mechanics
- Born’s probability interpretation
- Summary and forward view
- Problems
- Spin and the Stern-Gerlach experiment
- What angular momentum was in 1921
- The Stern-Gerlach experiment, 1922
- The anomalous Zeeman effect and doubled spectral lines
- Pauli’s exclusion principle, 1925
- Uhlenbeck and Goudsmit, 1925
- The classical picture fails: Ehrenfest and Lorentz
- Dirac 1928: spin from the relativistic wave equation
- Summary and bridge to Part II
- Problems
- Two-state systems and the Stern-Gerlach experiment
- The Stern-Gerlach experiment as a datum
- States as vectors
- Observables as operators
- Measurement and probability
- The Pauli matrices
- The Bloch sphere
- Change of basis and the meaning of superposition
- Summary and forward view
- Problems
- Observables and measurement
- From two states to many
- Self-adjoint operators and the spectral theorem
- Commuting observables and simultaneous eigenstates
- Expectation values, variance, and uncertainty
- Continuous spectra and infinite-dimensional Hilbert spaces
- The Fourier transform as a basis change
- Projective measurements and POVMs
- Summary and forward view
- Problems
- Composite systems and entanglement
- Two systems, one Hilbert space
- Product states versus entangled states
- Partial trace and reduced density matrices
- Schmidt decomposition
- Measures of entanglement
- Bell states, Bell measurements, and the Bell basis
- The no-cloning theorem
- Summary and forward view
- Problems
- Time evolution and the Schrödinger equation
- From kinematics to dynamics
- The time-dependent Schrödinger equation
- The time-evolution operator and unitarity
- Energy eigenstates and the general solution
- The Heisenberg picture
- Three worked examples
- Symmetries and conservation laws
- Summary and forward view
- Problems
- Density matrices and decoherence
- Why we need density matrices
- The density matrix formalism
- Pure and mixed states
- The Bloch ball revisited
- Dynamics: the von Neumann equation
- Open quantum systems and the Lindblad equation
- Decoherence
- Summary and forward view
- Problems
- The harmonic oscillator
- Why this chapter matters
- The classical oscillator, briefly
- The quantum oscillator: ladder operator solution
- The ground state and wavefunctions
- Heisenberg picture and classical correspondence
- Coherent states
- The oscillator everywhere: vibrations, phonons, photons
- Summary and forward view
- Problems
- Angular momentum
- Why this chapter
- The algebra of angular momentum
- Eigenvalues from the algebra alone
- Matrix elements and the first few representations
- Orbital angular momentum and spherical harmonics
- Rotations and angular momentum as a generator
- Addition of two angular momenta
- Summary and forward view
- Problems
- Central potentials
- Why central potentials
- The Schrödinger equation in spherical coordinates
- The effective potential and asymptotic behaviour
- General features: nodes, degeneracy, and quantum numbers
- The 3D infinite spherical well
- The 3D isotropic harmonic oscillator
- Preview: the Coulomb problem
- Summary and forward view
- Problems
- Spin-orbit coupling and the addition of angular momenta
- Why spin-orbit coupling matters
- Origin of spin-orbit coupling
- Addition of orbital and spin angular momenta
- Fine structure of the hydrogen atom
- The anomalous Zeeman effect and the Landé g-factor
- The nuclear shell model and the magic numbers
- Summary and forward view
- Problems
- The hydrogen atom
- Why hydrogen
- The Coulomb radial equation
- The hydrogen wavefunctions
- Probability densities and expectation values
- Hidden symmetry: the Runge-Lenz vector and SO(4)
- Fine structure and the Lamb shift
- Summary and forward view
- Problems
- Symmetries and conservation laws
- Why symmetries matter
- Continuous symmetries and conservation laws
- Discrete symmetries: parity and time reversal
- Hidden symmetries: Coulomb SO(4) and oscillator SU(3)
- Selection rules from the Wigner-Eckart theorem
- Gauge symmetry: a preview
- Summary and forward view
- Problems
- Time-independent perturbation theory
- Why perturbation theory
- Non-degenerate perturbation theory
- Degenerate perturbation theory
- The Stark effect on hydrogen
- Hydrogen fine structure via perturbation theory
- The Zeeman effect: weak, strong, and intermediate regimes
- Summary and forward view
- Problems
- Identical particles, many-body ground states, and intro to statistical mechanics
- Why identical particles
- The symmetrisation postulate
- The helium atom
- Slater determinants and multi-electron atoms
- The periodic table and Hund’s rules
- Bose-Einstein and Fermi-Dirac distributions
- Summary and forward view
- Problems
- Variational and WKB methods
- Why variational and WKB
- The variational principle
- Variational calculations in practice: helium and H2+
- The WKB approximation
- Bound states: the Bohr-Sommerfeld quantisation rule
- Tunnelling and the Gamow factor
- Summary of Chapter 18
- Problems
- Time-dependent perturbation theory and transition rates
- Why time-dependent perturbation theory
- The interaction picture and the Dyson series
- Harmonic perturbations and the resonance structure
- Fermi’s golden rule
- Electric-dipole transitions and selection rules
- Spontaneous emission and the Einstein coefficients
- Summary and forward view
- Problems
- Quantum information fundamentals
- Why quantum information
- Qubits and quantum gates
- Quantum circuits
- The no-cloning theorem
- Quantum teleportation
- Superdense coding
- BB84 quantum key distribution
- Summary and forward view
- Problems
- Quantum algorithms
- Why quantum algorithms matter
- Quantum parallelism and interference
- The Deutsch-Jozsa algorithm
- Grover’s search algorithm
- The quantum Fourier transform
- Shor’s factoring algorithm
- Complexity classes and quantum supremacy
- Summary and forward view
- Problems
- Quantum error correction and fault tolerance
- Why error correction matters for quantum computing
- Classical repetition codes
- The 3-qubit bit-flip code
- The 3-qubit phase-flip code
- Shor’s 9-qubit code
- The stabiliser formalism
- The threshold theorem and fault-tolerant computation
- The surface code
- Summary and forward view
- Problems
- Foundations and interpretations
- The measurement problem
- The Copenhagen interpretation
- The many-worlds interpretation
- De Broglie-Bohm pilot-wave theory
- Consistent histories
- Objective-collapse theories
- QBism and epistemic interpretations
- What is empirically at stake?
- Summary and forward view
- Problems
- Open quantum systems
- Why open systems
- Quantum channels: Kraus operators
- The Lindblad master equation
- Example: the damped harmonic oscillator
- Decoherence and pointer states
- Amplitude damping and phase damping: T1 and T2
- Non-Markovian dynamics: a brief look
- Summary and forward view
- Problems
- Path integrals
- Why path integrals
- The propagator from time slicing
- The free particle
- Quadratic Lagrangians and the harmonic oscillator
- The classical limit and stationary phase
- Imaginary time: Wick rotation and statistical mechanics
- Toward quantum field theory
- Summary and forward view
- Problems
- Quantisation of the electromagnetic field
- Why quantise the field
- Classical EM field in a cavity
- Quantisation: creation and annihilation operators
- The vacuum and its energy
- Spontaneous emission rigorously derived
- The Casimir effect
- Toward quantum electrodynamics
- Summary and forward view
- Problems
- Relativistic wave equations and the problem of antiparticles
- Why relativistic QM
- Special relativity refresher
- The Klein-Gordon equation
- Problems with the one-particle interpretation
- The Klein-Gordon field as a quantum field
- Antiparticles and charge conjugation
- Interactions
- Summary and forward view
- Problems
- The Dirac equation and quantum electrodynamics
- Why the Dirac equation
- Gamma matrices and the Clifford algebra
- Free Dirac plane waves
- Non-relativistic limit: the Pauli equation and g=2
- Hydrogen from the Dirac equation
- Dirac field quantisation and QED
- Where this book ends, and what comes next
- Summary of Chapter 28
- Problems