Method Comparison Table
Use this table to choose a method after identifying the observable, the available exact starting point, and the small or large dimensionless parameter. Common Symbols provides a compact notation key for the entries below.
| Method | Problem Type | Input | Output | Control Parameter | Strengths | Failure Modes | Canonical Examples | Related Volumes |
|---|---|---|---|---|---|---|---|---|
| Nondegenerate perturbation | Isolated energy level | Solved Hamiltonian plus weak correction | Energy and state corrections | Perturbation divided by level gaps | Direct, systematic, good for spectroscopy | Small denominators, degeneracy, divergent asymptotics | Weak anharmonicity | Core formalism, AMO |
| Degenerate perturbation | Degenerate multiplet | Perturbation matrix in degenerate subspace | Splittings and good zeroth-order states | Gap to states outside subspace | Handles symmetry-protected degeneracy | Wrong basis, neglected near-degenerate states | Stark and Zeeman-type splittings | Symmetry, spin, AMO |
| First-order transitions | Weak time-dependent drive | Interaction-picture matrix element | Transition amplitude and probability | Drive strength times duration | Shows resonance and phase matching | Long-time breakdown, strong driving | Harmonic perturbations | Dynamics, AMO |
| Fermi’s golden rule | Transition into continuum | Matrix element and density of states | Rate | Weak coupling and continuum limit | Converts amplitudes into rates | Discrete final states, strong coupling, short times | Decays and absorption | QFT bridge, open systems |
| Variational principle | Ground-state estimate | Trial state family | Upper bound on ground energy | Trial-space quality | Works without small coupling | Rigid trial family, bad observables | Gaussian trial states | Computational QM |
| Rayleigh-Ritz | Finite-basis eigenproblem | Basis and matrix elements | Ritz eigenvalues and vectors | Basis size and conditioning | Systematic numerical route | Truncation artifacts, ill-conditioned overlap | Oscillator-basis diagonalization | Numerical methods |
| WKB | Slowly varying one-dimensional potential | Local momentum | Semiclassical wavefunction | Wavelength changes slowly | Gives phases and asymptotics | Turning points, abrupt jumps | Smooth wells | Canonical systems |
| WKB tunneling | Smooth barrier | Under-barrier action | Transmission exponent | Barrier action large compared with hbar | Robust exponential estimates | Prefactor errors, near-top barriers | Field emission, alpha decay | Quantum matter, QFT bridge |
| First Born approximation | Weak short-range scattering | Fourier transform of potential | Scattering amplitude | Weak potential or high energy | Simple link between angle and potential structure | Strong scattering, resonances, Coulomb tails | Gaussian and Yukawa potentials | QFT bridge |
| Partial waves | Central-potential scattering | Radial equations by angular momentum | Phase shifts and amplitude | Convergent angular-momentum sum | Enforces rotational symmetry and unitarity | Noncentral potentials, long-range subtleties | Low-energy scattering | Symmetry, rigorous QM |
| Optical theorem | Scattering consistency check | Forward amplitude | Total cross section constraint | Unitarity | Detects probability-conservation failures | Convention mistakes, missing channels | Partial-wave proof | QFT unitarity |
How to Read the Table
Section titled “How to Read the Table”First choose the row by observable, not by preference. Energy shifts, transition rates, wavefunctions, tunneling exponents, and cross sections are different outputs. A method that is excellent for one output may be the wrong language for another.
Second identify the control parameter. It may be a small coupling, a large action, a large basis, a weak drive, a large energy gap, or a symmetry restriction. If there is no plausible control parameter, state that explicitly and compare against numerical or exact limiting cases.
Third check the failure modes before calculating. Most serious approximation errors come from using the right formula in the wrong regime.
Before reporting the result, run the Error-Estimate Checklist.
References
Section titled “References”- C. M. Bender and S. A. Orszag, Advanced Mathematical Methods for Scientists and Engineers, Springer, 1999.
- R. Shankar, Principles of Quantum Mechanics, 2nd ed., Springer, 1994.
- J. J. Sakurai and J. Napolitano, Modern Quantum Mechanics, 3rd ed., Cambridge University Press, 2020.
- J. R. Taylor, Scattering Theory: The Quantum Theory of Nonrelativistic Collisions, Dover, 2006.