Skip to content

Researcher Quick Reference

This is a dense lookup sheet for readers who already know quantum mechanics and need to check notation, assumptions, canonical pages, formulas, or source quality quickly. It is useful when reading a paper, preparing a lecture, comparing conventions across subfields, or deciding which canonical page should carry a result.

For a guided repair route, use the Researcher Refresher Roadmap. For student-facing problem workflow, use the Student Quick Reference.

TaskFast routeDo not skip
Check notationCommon Convention Translations and Common Symbols IndexUnits, Fourier signs, inner-product slot, tensor order.
Check a formulaCore Formulas IndexAssumptions and canonical-home link.
Identify a HamiltonianMost-Used HamiltoniansHilbert space, domain, gauge, and approximation.
Audit a calculationCommon Checks and Sanity TestsNormalization, positivity, dimensions, limits.
Find a sourceBibliography and Reading GuidesMatch source type to claim type.
Connect to fields or many-body languageQFT Bridge Index and Second QuantizationFixed-particle assumptions and particle-number sectors.
Judge claim statusEvidence LabelsStandard result, approximation, interpretation, active research, or speculation.

These are safe as lookup anchors only when their hypotheses are present.

StructureFormulaHypotheses to check
Pure-state probabilityP(Pa)=⟨ψ∣Pa∣ψ⟩P(P_a)=\langle\psi\vert P_a\vert\psi\rangleNormalized state; projector belongs to the measurement.
Density-operator expectation⟨A⟩=Tr⁡(ρA)\langle A\rangle=\operatorname{Tr}(\rho A)ρ\rho positive trace one; trace exists.
Reduced stateρA=Tr⁡BρAB\rho_A=\operatorname{Tr}_B\rho_{AB}Tensor-product ordering and traced subsystem are declared.
Spectral decompositionA=∑aaPaA=\sum_a aP_aDiscrete finite or controlled spectral case; otherwise use spectral measures.
Time-independent evolutionU(t)=e−iHt/ℏU(t)=e^{-iHt/\hbar}HH self-adjoint and time independent.
Heisenberg equationdAH/dt=(i/ℏ)[H,AH]+∂AH/∂tdA_H/dt=(i/\hbar)[H,A_H]+\partial A_H/\partial tDomains and explicit time dependence are controlled.
Canonical commutator[x^,p^]=iℏ[\hat x,\hat p]=i\hbarRepresentation and domains matter; not an ordinary matrix identity in finite dimension.
Perturbative splitH=H0+λVH=H_0+\lambda VSolved H0H_0, dimensionless small parameter, degeneracy checked.
Variational boundE0≤⟨ψ∣H∣ψ⟩/⟨ψ∣ψ⟩E_0\le\langle\psi\vert H\vert\psi\rangle/\langle\psi\vert\psi\rangleTrial state lies in the Hamiltonian form domain.
Scattering cross sectiondσ/dΩ=∣f(θ,ϕ)∣2d\sigma/d\Omega=\lvert f(\theta,\phi)\rvert^2Normalization, asymptotic convention, and flux convention match.
Many-particle HamiltonianHN=∑αh(α)+∑α<βv(αβ)H_N=\sum_\alpha h^{(\alpha)}+\sum_{\alpha<\beta}v^{(\alpha\beta)}Particle statistics, symmetry sector, and interaction convention are declared.

Canonical starts: Density Operators, Spectral Decomposition, Time-Evolution Operator, Canonical Commutation Relations, Choosing an Approximation Method, Scattering Amplitude, and Many-Particle Hamiltonians.

Before importing a result from a paper or another subfield, identify:

  1. Hilbert space, sector, and representation.
  2. State language: pure states, density operators, path integrals, Green functions, or occupation numbers.
  3. Hamiltonian, Lagrangian, generator, or effective model.
  4. Units, constants, Fourier convention, and phase convention.
  5. Boundary conditions, gauge choice, and self-adjoint domain when relevant.
  6. Symmetries, conserved quantities, and selection rules.
  7. Observable, measurement, correlation function, or response function being computed.
  8. Approximation method, expansion parameter, cutoff, or limiting process.
  9. Numerical discretization, convergence checks, or benchmark comparison.
  10. Claim type: theorem, derivation, approximation, experimental result, numerical evidence, interpretation, open problem, or speculative idea.

If a paper is excellent but uses different conventions, cite it honestly and translate explicitly. If a result depends on a convention or approximation, the page should say so near the formula, not only in a reference list.

FlagWhy it mattersFirst route
Unbounded operatorFormal symmetry is not self-adjointness. Domains can change spectra.Spectral Theorem: Practical Version
Continuous spectrumEigenkets are generalized objects; normalization is distributional.Discrete and Continuous Spectra
Trace or entropy in infinite dimensionTrace-class and convergence assumptions are not automatic.Trace-Class and Hilbert-Schmidt Operators
DegeneracyNondegenerate perturbation and naive eigenvector tracking can fail.Degenerate Perturbation Theory
Gauge fieldCanonical and kinetic momentum differ; phases may be gauge dependent.Minimal Coupling
Identical particlesSymmetric or antisymmetric sectors are part of the state space.Symmetrization Postulate
Thermodynamic or continuum limitOrder of limits can change the result.Many-Particle Hamiltonians
Open-system dynamicsA map on density operators needs positivity or complete positivity assumptions.Density Operators

When one of these flags appears, a compact reference entry is not enough. Follow the canonical page and cite a source whose level matches the issue.

Use symmetry before calculation.

  • If [H,A]=0[H,A]=0, check whether AA gives a conserved quantity or block diagonalization.
  • If a perturbation is odd under parity, diagonal matrix elements in parity eigenstates may vanish.
  • If angular momentum is present, identify whether LL, SS, or JJ is the relevant generator.
  • If time reversal is present, check whether the symmetry is antiunitary.
  • If a theorem assumes unitary symmetries, do not silently apply it to antiunitary symmetries.

Canonical starts: Quantum Symmetries, Unitary Symmetries, Antiunitary Symmetries, and Symmetry Constraints on Hamiltonians.

Do not record an approximation as a formula without its control statement.

MethodControl question
Nondegenerate perturbation theoryAre off-diagonal couplings small compared with relevant energy gaps?
Degenerate perturbation theoryHas the perturbation been diagonalized in the degenerate or nearly degenerate subspace?
Variational methodIs the trial family in the correct domain and does the bound direction matter?
WKBIs the de Broglie wavelength slowly varying away from turning points?
Born approximationIs the scattering potential weak in the relevant dimensionless sense?
Effective HamiltonianWhat subspace was retained and what scale was integrated out?
Numerical diagonalizationAre basis size, grid spacing, boundary conditions, and benchmark cases checked?

Useful starts: Choosing an Approximation Method, Small Parameters and Error Estimates, First Born Approximation, and Phase Shifts.

The Reference should usually be the canonical index, not the canonical derivation. When adding or editing a research-facing entry:

  1. Link to the canonical derivation instead of repeating it.
  2. State the assumptions and convention in the entry itself.
  3. Cite a source appropriate to the claim.
  4. Mark frontier claims with evidence labels.
  5. Do not upgrade a conjectural or interpretive statement into settled formalism.
  6. Add a changelog entry only for reader-facing corrections, convention changes, major reorganizations, or formula-level fixes.

Use Citation Standards, Versioning and Review Policy, and Contribute for the maintenance rules.

Claim typeStrong source type
Standard derivationGraduate textbook or monograph.
Operator-domain theoremMathematical physics monograph or rigorous text.
Historical priorityOriginal paper plus reliable secondary history.
Active research resultRecent review and primary papers.
Experimental claimExperimental paper, collaboration paper, or review with data context.
Software behaviorOfficial documentation and method paper when behavior affects results.
Convention comparisonThe source whose convention is being translated plus the canonical convention page.

Start with Textbooks and Classic Papers, then add topic-specific sources as the Reference expands.

  • Recognizing a formula but not its convention.
  • Treating a finite-dimensional proof as valid for unbounded operators.
  • Importing a result from a different normalization or scattering convention.
  • Forgetting that a density matrix representation is basis dependent.
  • Treating a numerical plot as evidence without convergence or benchmark checks.
  • Letting a paper’s interpretive framing replace the operational content of the formalism.
  • Turning a compact reference entry into a duplicate derivation.
  • Citing a source for authority without checking that its assumptions match the page.
  • J. J. Sakurai and J. Napolitano, Modern Quantum Mechanics, 3rd ed., Cambridge University Press, 2020.
  • R. Shankar, Principles of Quantum Mechanics, 2nd ed., Springer, 1994.
  • C. Cohen-Tannoudji, B. Diu, and F. Laloë, Quantum Mechanics, Wiley, 1977.
  • M. Reed and B. Simon, Methods of Modern Mathematical Physics I: Functional Analysis, Academic Press, 1980.
  • B. C. Hall, Quantum Theory for Mathematicians, Springer, 2013.
  • A. Peres, Quantum Theory: Concepts and Methods, Kluwer, 1995.
  1. A paper states [x^,p^]=i[\hat x,\hat p]=i and U(t)=e−iHtU(t)=e^{-iHt}. What should a reference entry do before citing its formula?
Solution

Identify that the paper is using ℏ=1\hbar=1, translate the formulas to the default explicit-ℏ\hbar convention, and state the translation near the formula if the cited result is imported.

  1. A derivation uses a formally Hermitian differential operator but never states boundary conditions. What is the research-level warning?
Solution

The operator may not yet be self-adjoint. Boundary conditions and domains can change the spectrum and whether the Hamiltonian generates unitary evolution. The page should either state the domain assumptions or link to a source that does.

  1. A compact reference entry starts to reproduce a four-page perturbation derivation already present elsewhere. What should happen?
Solution

Keep the reference entry compact: state the result, assumptions, and warning, then link to the canonical derivation. Repeating the derivation risks stale duplicated content.