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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.

MethodProblem TypeInputOutputControl ParameterStrengthsFailure ModesCanonical ExamplesRelated Volumes
Nondegenerate perturbationIsolated energy levelSolved Hamiltonian plus weak correctionEnergy and state correctionsPerturbation divided by level gapsDirect, systematic, good for spectroscopySmall denominators, degeneracy, divergent asymptoticsWeak anharmonicityCore formalism, AMO
Degenerate perturbationDegenerate multipletPerturbation matrix in degenerate subspaceSplittings and good zeroth-order statesGap to states outside subspaceHandles symmetry-protected degeneracyWrong basis, neglected near-degenerate statesStark and Zeeman-type splittingsSymmetry, spin, AMO
First-order transitionsWeak time-dependent driveInteraction-picture matrix elementTransition amplitude and probabilityDrive strength times durationShows resonance and phase matchingLong-time breakdown, strong drivingHarmonic perturbationsDynamics, AMO
Fermi’s golden ruleTransition into continuumMatrix element and density of statesRateWeak coupling and continuum limitConverts amplitudes into ratesDiscrete final states, strong coupling, short timesDecays and absorptionQFT bridge, open systems
Variational principleGround-state estimateTrial state familyUpper bound on ground energyTrial-space qualityWorks without small couplingRigid trial family, bad observablesGaussian trial statesComputational QM
Rayleigh-RitzFinite-basis eigenproblemBasis and matrix elementsRitz eigenvalues and vectorsBasis size and conditioningSystematic numerical routeTruncation artifacts, ill-conditioned overlapOscillator-basis diagonalizationNumerical methods
WKBSlowly varying one-dimensional potentialLocal momentumSemiclassical wavefunctionWavelength changes slowlyGives phases and asymptoticsTurning points, abrupt jumpsSmooth wellsCanonical systems
WKB tunnelingSmooth barrierUnder-barrier actionTransmission exponentBarrier action large compared with hbarRobust exponential estimatesPrefactor errors, near-top barriersField emission, alpha decayQuantum matter, QFT bridge
First Born approximationWeak short-range scatteringFourier transform of potentialScattering amplitudeWeak potential or high energySimple link between angle and potential structureStrong scattering, resonances, Coulomb tailsGaussian and Yukawa potentialsQFT bridge
Partial wavesCentral-potential scatteringRadial equations by angular momentumPhase shifts and amplitudeConvergent angular-momentum sumEnforces rotational symmetry and unitarityNoncentral potentials, long-range subtletiesLow-energy scatteringSymmetry, rigorous QM
Optical theoremScattering consistency checkForward amplitudeTotal cross section constraintUnitarityDetects probability-conservation failuresConvention mistakes, missing channelsPartial-wave proofQFT unitarity

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.

  • 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.