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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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
- 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