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Primary Papers Index

This index identifies original and near-original papers that anchor historical claims in quantum mechanics. It is not a replacement for Classic Papers, which is the broader bibliography guide. This page is a routing table: when a historical page says “this was first argued, measured, or formulated here,” this index helps locate the source and the appropriate modern reading.

Primary papers should be used with care. They establish what was claimed in a historical setting; they do not automatically provide the cleanest modern notation or the final interpretation.

For each source, ask:

  • What claim does this paper actually support?
  • Which modern concept is a later reconstruction?
  • Which page owns the present-day formalism?
  • Which historical caution prevents a misleading slogan?

Use primary papers for dates, original arguments, apparatus reports, and historical interpretation. Use modern pages for standard calculations.

SourceAnchorsRead withHistorical caution
Planck, 1901, blackbody radiationRadiation law and energy elements in thermal equilibriumPlanck’s Radiation LawDo not turn this alone into the modern photon concept.
Einstein, 1905, light quantaFrequency-dependent energy transfer and photoelectric reasoningEinstein’s Light Quantum HypothesisThe paper is stronger than Planck’s oscillator quantization but still predates mature quantum electrodynamics.
Millikan, 1916, photoelectric measurementsPrecision tests of stopping potential versus frequencyMillikan’s Photoelectric MeasurementsThe data supported Einstein’s relation even while Millikan resisted the light-quantum interpretation.
Rutherford, 1911, nuclear atomLarge-angle alpha scattering and concentrated positive chargeRutherford ScatteringThe nuclear atom is not yet a quantum atom.
Bohr, 1913, atomic constitutionOld quantum theory explanation of hydrogen spectral regularitiesBohr ModelBohr orbits are not modern stationary states.
Franck and Hertz, 1914, inelastic collisionsDiscrete atomic excitation energiesFranck–Hertz ExperimentThe experiment supports discrete internal energies, not the full postulate package by itself.

Matter Waves, Matrices, and Wave Mechanics

Section titled “Matter Waves, Matrices, and Wave Mechanics”
SourceAnchorsRead withHistorical caution
de Broglie, 1924-1925, matter wavesWavelength-momentum relation for material particlesde Broglie Matter WavesMatter-wave reasoning was tied to old quantum theory before the full state-vector framework.
Heisenberg, 1925, reinterpretation paperTransition quantities and noncommuting structureHeisenberg’s Matrix MechanicsThe paper is not written as a modern linear-algebra textbook.
Born and Jordan, 1925, matrix formulationMatrix mechanics and canonical commutation structureBorn and Jordan’s Matrix FormulationModern operator notation is a reconstruction of a rapidly developing formalism.
Dirac, 1925-1926, transformation theoryAlgebraic transformation viewpoint and quantum bracketsDirac’s Transformation TheoryBra-ket notation was consolidated later; do not impose the later notation too early.
Schrödinger, 1926, eigenvalue papersWave mechanics and bound-state eigenvalue methodsSchrödinger’s Wave MechanicsWave mechanics is not a classical material wave theory.
Born, 1926, collision paperProbability interpretation of wave amplitudesBorn Rule HistoryThe general Born rule is the later canonical formulation, not the wording of the first scattering paper.
Davisson and Germer, 1927, electron diffractionReflection diffraction evidence for electron wavesDavisson–Germer ExperimentDiffraction supports matter-wave behavior; it does not make electrons classical waves.
G. P. Thomson and Reid, 1927, electron diffractionTransmission diffraction evidence for electron wavesG. P. Thomson ExperimentThe geometry differs from Davisson–Germer and should not be collapsed into one generic story.
SourceAnchorsRead withHistorical caution
Gerlach and Stern, 1922, atomic beam splittingDirectional quantization evidenceStern–Gerlach ExperimentThe original experiment predates the clean modern electron-spin account.
Pauli, 1925, exclusion principleNonclassical exclusion rule for atomic structurePauli Exclusion PrincipleExclusion was identified before the later spin-statistics theorem framework.
Bose, 1924, photon countingCounting argument leading to Bose statisticsBose’s Counting ArgumentThe argument was historically entangled with radiation theory and Einstein’s extension to material gases.
Fermi and Dirac, 1926, statisticsFermionic occupation and antisymmetric-state reasoningFermi–Dirac StatisticsDo not read full many-body Fock-space notation into the first papers without translation.
Heisenberg, 1927, uncertaintyMeasurement limits and noncommuting quantitiesUncertainty Historical OriginModern uncertainty relations are sharper operator statements than the first microscope-style arguments.
von Neumann, 1932, measurement formalismProjection, Hilbert-space formalism, and measurement idealizationMeasurement in the FormalismThe formal measurement model does not settle every interpretation of measurement.
SourceAnchorsRead withHistorical caution
Einstein, Podolsky, and Rosen, 1935Completeness, locality assumptions, and correlated systemsEPR ArgumentEPR is not simply “entanglement is weird”; it is an argument from specific assumptions.
Schrödinger, 1935, separated systems and catEntanglement language and macroscopic-superposition concernsSchrödinger’s CatThe cat argument is a measurement problem probe, not a laboratory recipe.
Bell, 1964Inequalities for local hidden-variable theoriesBell Theorem Historical Turning Point and Bell TheoremBell’s theorem targets precise assumptions; state them before drawing conclusions.
Clauser, Horne, Shimony, and Holt, 1969Experimentally usable Bell inequalityCHSH InequalityThe inequality and the experiment are different layers of the argument.
Freedman and Clauser, 1972Early optical Bell-test experimentBell Inequality ExperimentsEarly tests had loopholes that later experiments addressed.
Aspect, Grangier, Roger, and related 1982 papersLandmark polarization-correlation Bell testsAspect ExperimentsAspect-era tests are historically central but not the same as later loophole-free tests.
Hensen, Giustina, Shalm, and related 2015 testsLoophole-free Bell-test eraLoophole-Free Bell Tests“Loophole-free” means major experimental loopholes are closed under stated assumptions.

When a page uses one of these papers, cite it with a sentence that says why it is being cited:

This paper is cited for the original experimental report, not for modern notation.

or

This paper is cited for the historical introduction of the argument; the formal theorem is stated on the modern theorem page.

Do not cite a famous paper merely because it is famous. A citation should support a specific historical, experimental, or conceptual claim.

  • M. Planck, “Ueber das Gesetz der Energieverteilung im Normalspectrum,” Annalen der Physik 4, 553-563, 1901, DOI: 10.1002/andp.19013090310.
  • A. Einstein, “Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt,” Annalen der Physik 17, 132-148, 1905, DOI: 10.1002/andp.19053220607.
  • E. Rutherford, “The Scattering of α\alpha and β\beta Particles by Matter and the Structure of the Atom,” Philosophical Magazine 21, 669-688, 1911, DOI: 10.1080/14786440508637080.
  • N. Bohr, “On the Constitution of Atoms and Molecules,” Philosophical Magazine 26, 1-25, 1913, DOI: 10.1080/14786441308634955.
  • W. Heisenberg, “Über quantentheoretische Umdeutung kinematischer und mechanischer Beziehungen,” Zeitschrift für Physik 33, 879-893, 1925, DOI: 10.1007/BF01328377.
  • M. Born and P. Jordan, “Zur Quantenmechanik,” Zeitschrift für Physik 34, 858-888, 1925, DOI: 10.1007/BF01328531.
  • E. Schrödinger, “Quantisierung als Eigenwertproblem,” Annalen der Physik 79, 361-376, 1926, DOI: 10.1002/andp.19263840404.
  • M. Born, “Zur Quantenmechanik der Stoßvorgänge,” Zeitschrift für Physik 37, 863-867, 1926, DOI: 10.1007/BF01397477.
  • C. Davisson and L. H. Germer, “Reflection of Electrons by a Crystal of Nickel,” Physical Review 30, 705-740, 1927, DOI: 10.1103/PhysRev.30.705.
  • A. Einstein, B. Podolsky, and N. Rosen, “Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?,” Physical Review 47, 777-780, 1935, DOI: 10.1103/PhysRev.47.777.
  • J. S. Bell, “On the Einstein Podolsky Rosen Paradox,” Physics Physique Fizika 1, 195-200, 1964, DOI: 10.1103/PhysicsPhysiqueFizika.1.195.
  • J. F. Clauser, M. A. Horne, A. Shimony, and R. A. Holt, “Proposed Experiment to Test Local Hidden-Variable Theories,” Physical Review Letters 23, 880-884, 1969, DOI: 10.1103/PhysRevLett.23.880.
  • A. Aspect, J. Dalibard, and G. Roger, “Experimental Test of Bell’s Inequalities Using Time-Varying Analyzers,” Physical Review Letters 49, 1804-1807, 1982, DOI: 10.1103/PhysRevLett.49.1804.
  • M. Jammer, The Conceptual Development of Quantum Mechanics, 2nd ed., American Institute of Physics, 1989.
  • J. Mehra and H. Rechenberg, The Historical Development of Quantum Theory, Springer, 1982-2001.
  1. A page says “Planck discovered photons.” Which primary-source distinction should correct it?
Solution

Planck’s blackbody work introduced energy elements in the radiation problem, while Einstein’s 1905 paper made the stronger light-quantum argument. The mature photon concept developed later. The correction should cite Planck for the radiation law and Einstein for the light-quantum hypothesis, while avoiding the anachronistic photon claim.

  1. Why should Bell’s 1964 paper and CHSH 1969 be indexed separately?
Solution

Bell’s 1964 paper gives the foundational theorem for local hidden-variable constraints. CHSH gives an experimentally useful inequality for correlation tests. They serve different roles: theorem anchor and experiment-facing formulation.