The Structure of Quantum Mechanics

States, Observables and Symmetry in 18 chapters — from “The wave function is not the state” to “Charged particles in electromagnetic fields”.

Chapters

  1. The wave function is not the state
    • One state in three representations
    • Amplitudes add before they square
    • The Born rule in general form
    • Global phase and relative phase
    • Superposition against mixture
    • The Schrodinger equation as a component statement
    • What is now settled about the wave function
    • Summary
    • Problems
  2. Hilbert space and Dirac notation
    • Inner products and the space of states
    • Kets, bras and the antilinear correspondence
    • Orthonormal basis, components and Parseval
    • Completeness and the resolution of the identity
    • Change of basis as change of description
    • What infinite dimension costs
    • Summary
    • Problems
  3. Observables, spectra and the spectral theorem
    • Linear operators, matrices and adjoints
    • Self-adjoint against Hermitian
    • The spectral theorem and what it is for
    • A degenerate eigenspace and its projector
    • Continuum normalisation and improper vectors
    • Observables defined by the spectral theorem
    • Summary
    • Problems
  4. The postulates, measurement and collapse
    • Three magnets and states as unit rays
    • Five postulates and the Born rule with projectors
    • State reduction and the experiment that forces it
    • Non-selective measurement, where kets run out
    • The measurement problem, stated exactly
    • Interpretive options and their prices
    • Summary
    • Problems
  5. Compatible observables and uncertainty as a theorem
    • Three labels for hydrogen
    • Compatible observables and simultaneous diagonalisation
    • The complete set of commuting observables
    • The uncertainty relation with its anticommutator term
    • Uncertainty is not disturbance
    • The energy-time relation without a time operator
    • What is now settled about compatibility and uncertainty
    • Summary
    • Problems
  6. Position, momentum and the origin of the canonical commutator
    • Which operator is momentum?
    • The translation operator and its generator
    • Momentum defined as the generator of translations
    • Canonical quantisation and its ambiguity
    • The bracket correspondence and its limits
    • Translation invariance and conservation
    • Summary
    • Problems
  7. Time evolution as a unitary group, and the three pictures
    • The evolution operator and its group property
    • The propagator
    • The time-ordered exponential
    • The Heisenberg picture
    • The interaction picture
    • Why no experiment distinguishes the pictures
    • Summary
    • Problems
  8. The oscillator as an algebra
    • The ladder algebra as a definition
    • The spectrum from the algebra alone
    • Matrix elements without integrals
    • The wave functions, as an afterthought
    • What has actually been solved
    • Summary
    • Problems
  9. Coherent states, Ehrenfest's theorem and the classical limit
    • Ehrenfest's theorem and its correction
    • The coherent state and the displacement operator
    • Poissonian number statistics
    • Rigid motion, non-orthogonality and overcompleteness
    • When a system has a trajectory
    • Summary
    • Problems
  10. The path integral
    • The propagator's phase as an action
    • Time slicing the propagator
    • The sum over paths
    • The free and quadratic path integrals
    • The classical limit as stationary phase
    • The phase a vector potential adds
    • Summary
    • Problems
  11. Slow change, sudden change and the Berry phase
    • Instantaneous eigenstates and the adiabatic theorem
    • The validity condition and where it fails
    • The sudden approximation and tritium decay
    • Dynamical and geometric phase
    • Spin one-half in a slowly rotating field
    • Where the geometric phase turns up
    • Summary
    • Problems
  12. Symmetries, generators and conservation laws
    • What a symmetry is
    • Generator, symmetry and conservation
    • Symmetry forces degeneracy
    • Parity
    • Lattice translation and Bloch's theorem
    • Time reversal and antiunitarity
    • Summary
    • Problems
  13. Angular momentum from the rotation group
    • What was thrown away
    • The generators of rotation and their algebra
    • The orbital case and the integer condition
    • Spherical harmonics as representation matrix elements
    • Finite rotations and the Wigner d matrices
    • Summary
    • Problems
  14. Spin one-half, SU(2) and two-level dynamics
    • SU(2) as the double cover of SO(3)
    • The Pauli algebra from the group
    • The Bloch sphere
    • The rotating frame and Rabi oscillation
    • Observing the 2π sign
    • Summary
    • Problems
  15. Adding angular momenta, tensor operators and Wigner-Eckart
    • The tensor product of two systems
    • The coupled basis and the decomposition rule
    • Building the Clebsch-Gordan coefficients
    • Irreducible tensor operators
    • The Wigner-Eckart theorem
    • What Part III bought
    • Summary
    • Problems
  16. Central potentials as a rotation problem
    • Separation as rotational decomposition
    • The radial equation, with the ordering settled
    • The node theorem and radial ordering
    • Spherical wells and the isotropic oscillator's extra degeneracy
    • What is now settled about central potentials
    • Summary
    • Problems
  17. Hydrogen, and the symmetry that explains it
    • The radial decomposition and hydrogen's nine states
    • The classical Runge-Lenz vector
    • The quantum Runge-Lenz vector and the SO(4) algebra
    • The spectrum with no differential equation
    • Which perturbation breaks which symmetry
    • Where the non-relativistic Coulomb problem stops
    • Summary
    • Problems
  18. Charged particles in electromagnetic fields
    • Minimal coupling of a charge to a field
    • Gauge covariance of the theory and kinetic momenta
    • Landau levels from the algebra
    • The Aharonov-Bohm effect
    • What the vector potential turns out to be
    • The end of the argument
    • Summary
    • Problems