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Models. Measurements.
Reproducibility.

Explore, inspect, collaborate.

MAI Physics / Experiment atlas / Edition 30 October 2026 (UTC)

Questions that
changed physics.

Follow the experiment. Inspect the mathematics. Turn a historical question into a visual investigation.

An evolving history of physics, organised by decade. Current entries run from the 1704 publication of Opticks to 2024 nuclear spectroscopy; 2025–2026 source coverage remains pending.

1800s · TWO ROUTES. ONE PATTERN.Light → apertures → superposition → intensity
Computed teaching illustration of interference. This is a model, not an image from Young’s experiment. Wavefront playback is schematic; the intensity sketch stays fixed.

Paused. Schematic wavefront motion; not experimental data.

61curated milestones
7working educational labs
A · N · Vanalytical · numerical · visual pathways

The frontier, decade by decade / Opening collection

Retell the question.
Not just the answer.

Read a short story, interrogate its claim, then explore a model or original source. These opening episodes are educational retellings, not new MAI discoveries. The wider timeline is a working bibliography, not a complete history of every decade.

1800s / Two routes to one screen

When adding light
makes darkness.

Imagine expecting two openings to make a screen simply brighter. A wave model offers a different prediction: contributions reinforce at some positions and cancel at others. The intellectual shift is not the striped picture alone, but a rule that predicts how the stripes move.

Use the wavefront illustration above, then change the separation in the Young teaching model. It is a modern idealisation, not a reconstruction from Young’s measurements.

Try the interference model →

Checked primary text: Young, Experiments and Calculations Relative to Physical Optics (1804), facsimile. Read to the Royal Society on 24 November 1803; its card-edge interference experiment is not this modern two-slit schematic. Scan inspected 30 October 2026. Index date caveat →

Dialectic: does a picture prove a theory?

Fictional teaching dialogue; not historical quotations.

Observer: The bright and dark bands look persuasive. Is that enough?

Sceptic: Could a different model draw the same picture?

Investigator: Change one parameter. Ask both models to predict the next pattern before you see it.

Your challenge: Which measurement would separate the explanations rather than merely illustrate one?

1910s / The rare event

Let the outlier
change the model.

Most particles passing through a thin foil seem unsurprising. The difficult question is what a large deflection says about the distribution of charge. A scattering model makes the angle dependence inspectable; a dramatic image alone does not tell you whether the assumptions hold.

The index distinguishes the 1909 scattering observation from Rutherford’s 1911 interpretation. The laboratory uses ideal single Coulomb scattering, omitting screening, multiple scattering and nuclear size.

Inspect the scattering model →

Checked primary text: Rutherford’s 1911 paper (institution-hosted transcription), which cites Geiger and Marsden’s 1909 observations. Checked 30 October 2026. Index record →

Dialectic: when is an outlier evidence?

Fictional teaching dialogue; not historical quotations.

Observer: A rare deflection contradicts my expectation.

Sceptic: Or it exposes your apparatus, contamination or selection rule.

Investigator: Compare the rate, angular distribution and controls—not just one memorable event.

Your challenge: What control would you ask for before changing the model of the atom?

1980s / What correlations can decide

Turn a philosophy
into a bound.

Instead of asking only what reality “really is,” ask what combinations of correlations an explicitly defined class of explanations permits. A Bell-type inequality makes assumptions answerable to experiment. The model here samples a quantum prediction; it cannot independently prove that prediction.

Change visibility and compare the analytical CHSH value with the local bound of 2. Synthetic outcomes are drawn from an assumed distribution, not from a detector.

Explore correlations →

Checked primary abstract: Aspect, Dalibard & Roger (1982), reporting time-varying analyser measurements consistent with quantum predictions and violating a Bell inequality. Checked 30 October 2026. Index record →

Dialectic: what did the test rule out?

Fictional teaching dialogue; not historical quotations.

Observer: The inequality is violated. Have we explained everything?

Sceptic: Only if we forget the assumptions and experimental loopholes.

Investigator: State the class of models being tested. Separate an experimental violation from a simulation designed to produce one.

Your challenge: Why is the synthetic sampler on this page not a Bell experiment?

1990s / A changing identity

What if “missing”
means transformed?

A shortfall in one detected particle flavour can invite more than one explanation. Oscillation models turn the question into a dependence on distance and energy. The useful story is not “the missing particles were found,” but how an alternative explanation makes testable predictions.

The two-flavour vacuum laboratory compares numerical evolution with an analytical appearance probability. It leaves out matter effects, three-flavour mixing and detector response.

Run the oscillation model →

Checked primary abstract: Super-Kamiokande: Evidence for Oscillation of Atmospheric Neutrinos (1998). The observed directional dependence was consistent with flavour oscillation, not explained by the studied experimental and flux uncertainties. Checked 30 October 2026. Index record →

Dialectic: absence or transformation?

Fictional teaching dialogue; not historical quotations.

Observer: Fewer events arrived than expected.

Sceptic: Is the source wrong, the detector inefficient, or the propagation model incomplete?

Investigator: Look for a structured pattern, not only an overall deficit.

Your challenge: Which dependence would help distinguish those possibilities?

2010s / From a signal to a claim

A discovery is
a chain of evidence.

On 4 July 2012, ATLAS and CMS announced a new particle consistent with the Higgs boson. Identifying its properties took further study. That distinction—initial observation versus later characterisation—is part of the story, not a footnote.

GW150914 was detected on 14 September 2015 and announced on 11 February 2016. Detection date and publication or announcement date answer different questions. Preserve both when retelling a frontier.

Checked primary-institution anchors: CERN: discovering the Higgs; ATLAS: Higgs physics; LIGO discovery paper; LIGO: GW150914. Checked 30 October 2026. No measured-event animation is supplied here.

Dialectic: when may we call it a discovery?

Fictional teaching dialogue; not historical quotations.

Observer: The signal matches a prediction.

Sceptic: How were backgrounds, calibration and alternative explanations tested?

Investigator: Read the claim at its actual strength. Then follow the independent checks and later measurements.

Your challenge: What would be lost if the headline collapsed detection, announcement and confirmation into one date?

Editorial roadmap / Coverage, not a promise

Keep the gaps
in the open.

The index ranges from 1704 to 2024. Some decades have several entries; others, including the 1940s, have none in this selection. The selector shows only decades with records. A missing entry does not mean no physics happened.

Future episodes can connect a frontier question, an original source, an animated explanation and a debate over assumptions. They remain proposed until their evidence and teaching assets are ready. There is no complete paid course behind this page.

Inspect the available index →

Free to explore / Proposed collaborations

Bring a question worth teaching.

Interested in an educator workshop, a commissioned physics story or an institutional learning resource? Tell MAI Physics about your audience, topic and intended use. Scope, deliverables, permissions and any fees would be agreed separately.

Discuss a learning project →

This opens your email app; nothing is sent automatically. Memberships are a proposed direction, not available for purchase. No accounts, payment collection, credits or progress tracking are enabled.

01 / Historical index

From a measurement
to a new view.

Search by scientist, experiment, equation or topic. Open a row for its finding, original publication and three model pathways. “Interactive model” identifies a working simplified lab; other entries are specifications for future reconstruction. This selection is not exhaustive.

61 experiments

1704Prisms and the composition of white lightIsaac Newton · Light & electromagnetismModel specification

Question & finding

Does a prism create colours or separate components already present in white light?

Prism and recombination experiments support a spectrum of components with different refrangibility.

1704 publication; prism experiments began in the 1660s

Teaching equation

n₁(λ) sin θ₁ = n₂(λ) sin θ₂

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive wavelength-dependent refraction with Snell’s law.

Numerical pathway

Trace rays across two prism surfaces using a specified dispersion model.

Visual pathway

Move a prism and compare dispersed and recombined spectra.

Limits

The equation is a modern teaching model; a book published in 1704 reports substantially earlier experiments.

Original publication record

Isaac Newton (1704). Opticks: or, A Treatise of the Reflexions, Refractions, Inflexions and Colours of Light. London: Sam. Smith and Benj. Walford; Book I.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1728Stellar aberrationJames Bradley · Cosmology & astrophysicsModel specification

Question & finding

Why do stellar positions trace an annual pattern different from parallax?

Annual aberration is explained by Earth’s orbital motion and the finite speed of light.

1727/1728 report; observations from 1725

Teaching equation

α ≈ v⊕/c (radians, small-angle limit)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive the first-order aberration angle from relative velocity.

Numerical pathway

Compute the annual projected displacement for a chosen stellar direction.

Visual pathway

Animate an apparent stellar ellipse beside Earth’s orbit.

Limits

Aberration is distinct from distance-dependent parallax; the exact historical publication date needs bibliographic verification.

Original publication record

James Bradley (1728). A Letter from the Reverend Mr. James Bradley Savilian Professor of Astronomy at Oxford, and F.R.S. to Dr. Edmond Halley Astronom. Reg. &c. Giving an Account of a New Discovered Motion of the Fix’d Stars. Philosophical Transactions 35, 637–661; historical volume/publication dating differs.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1752Atmospheric electricity and the electrical kiteBenjamin Franklin · Light & electromagnetismModel specification

Question & finding

Are storm clouds associated with electrical charge?

The reported kite experiment connected atmospheric electricity with laboratory electrical phenomena.

1752 report

Teaching equation

Q = CV; E = −∇V

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate potential difference, capacitance and induced charge.

Numerical pathway

Solve an idealised electrostatic potential around conductors.

Visual pathway

Show equipotential contours and charge induction in a virtual environment.

Limits

Historical evidence and priority need contextual treatment; this is a virtual illustration, not instructions for a dangerous storm experiment.

Original publication record

Benjamin Franklin (1752). A Letter of Benjamin Franklin, Esq; to Mr. Peter Collinson, F. R. S. concerning an Electrical Kite. Philosophical Transactions 47, 565–567.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1785Coulomb’s torsion balanceCharles-Augustin de Coulomb · Light & electromagnetismModel specification

Question & finding

How does electrostatic force depend on separation?

Torsion-balance measurements supported an inverse-square force law.

1785

Teaching equation

F = kₑq₁q₂/r²; κθ = FL

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Combine torque balance with the inverse-square law.

Numerical pathway

Fit an exponent p in F = Ar^(−p) to synthetic measurements.

Visual pathway

Rotate a torsion balance and plot force against distance.

Limits

Finite-size conductors, charge leakage and geometry affect a real apparatus.

Original publication record

Charles-Augustin de Coulomb (1785). Premier mémoire sur l’électricité et le magnétisme. Histoire de l’Académie royale des sciences, avec les mémoires, année 1785, pp. 569–577.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1798Weighing the Earth with a torsion balanceHenry Cavendish; apparatus initiated by John Michell · Relativity & gravityInteractive model

Question & finding

Can the weak attraction between laboratory masses reveal Earth’s mean density?

Cavendish measured Earth’s mean density using a torsion balance; the result can be expressed using G in modern notation.

1798

Open simplified lab →

Teaching equation

F = GMm/r²; κθ = τg

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive equilibrium deflection and the torsional oscillation period.

Numerical pathway

Integrate a damped torsion oscillator under gravitational torque.

Visual pathway

Compare balance deflection, settling time and inferred density.

Limits

Cavendish reported Earth’s density, not a modern direct measurement labelled G; calibration and nearby masses matter.

Original publication record

Henry Cavendish (1798). Experiments to Determine the Density of the Earth ↗. Philosophical Transactions 88, 469–526.

Bibliography draft. Original source and link not live-verified.

Working simplified demonstration available; full reconstruction remains a specification.

1801Interference of lightThomas Young · Light & electromagnetismInteractive model

Question & finding

Can overlapping light produce alternating brightness and darkness?

Interference observations supported a wave account of light.

1801 presentation; 1802 and 1804 papers

Open simplified lab →

Teaching equation

I(θ) ∝ sinc²(πa sinθ/λ) cos²(πd sinθ/λ)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive fringe spacing Δy ≈ λL/d and the single-slit envelope.

Numerical pathway

Sum complex amplitudes across two finite slits.

Visual pathway

Change wavelength, slit separation and width; compare fringes with the analytic curve.

Limits

The familiar two-slit apparatus is a modern teaching reconstruction, not a claim of exact replication of Young’s arrangement.

Original publication record

Thomas Young (1804). Experiments and Calculations Relative to Physical Optics ↗. Philosophical Transactions 94, 1–16.

Bibliography draft. Original source and link not live-verified.

Working simplified demonstration available; full reconstruction remains a specification.

1820Electric current deflects a compassHans Christian Ørsted · Light & electromagnetismModel specification

Question & finding

Does an electric current influence a magnetic needle?

A current-carrying wire produced a magnetic effect around the conductor.

1820

Teaching equation

B(r) = μ₀I/(2πr)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Use the later long-wire field law to predict direction and scaling.

Numerical pathway

Sum Biot–Savart contributions from a finite wire.

Visual pathway

Move a compass around a wire and reverse the current.

Limits

The equation is a later idealisation; the return path and Earth’s field affect the needle.

Original publication record

Hans Christian Ørsted (1820). Experimenta circa effectum conflictus electrici in acum magneticam. Copenhagen: privately printed Latin announcement, July 1820; subsequently translated and reprinted.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1827Brownian motionRobert Brown · Thermal & statisticalModel specification

Question & finding

Why do small suspended particles keep moving?

Brown documented persistent microscopic motion in organic and inorganic particles; the molecular explanation came later.

1827 observations; 1828 publication

Teaching equation

⟨x²⟩ = 2Dt; D = kBT/(6πηa)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive mean-square displacement from the diffusion equation.

Numerical pathway

Generate seeded random walks and estimate D with uncertainty.

Visual pathway

Track particles and compare empirical mean-square displacement with 2Dt.

Limits

Einstein’s and Smoluchowski’s later theory is used for modelling; Brown did not establish that theory.

Original publication record

Robert Brown (1828). A Brief Account of Microscopical Observations Made in the Months of June, July and August, 1827. Philosophical Magazine, series 2, 4, 161–173; also separately printed.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1831Electromagnetic inductionMichael Faraday · Light & electromagnetismModel specification

Question & finding

Can a changing magnetic environment produce an electric current?

Faraday observed induction from changing currents and magnet–coil motion.

1831 experiments; 1832 publication

Teaching equation

ε = −N dΦB/dt

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Calculate induced voltage for prescribed magnetic flux.

Numerical pathway

Integrate an RL circuit driven by a moving-magnet flux model.

Visual pathway

Move a magnet through a coil and compare flux, voltage and current.

Limits

The compact equation uses later notation; magnet geometry and circuit inductance must be specified.

Original publication record

Michael Faraday (1832). Experimental Researches in Electricity ↗. Philosophical Transactions 122, 125–162.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1845Mechanical equivalent of heatJames Prescott Joule · Thermal & statisticalModel specification

Question & finding

Can mechanical work be quantitatively related to heating?

Joule’s measurements established a repeatable relation between work and heat.

1840s experiments; definitive 1850 paper

Teaching equation

W ≈ mcΔT; dU = δQ + δWon

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Use an energy balance with a stated work-sign convention.

Numerical pathway

Integrate heating with Newtonian heat loss and apparatus heat capacity.

Visual pathway

Drop virtual weights, stir fluid and track the energy budget.

Limits

Adiabatic heating is idealised; bearings, calorimeter heat capacity and thermal losses require correction.

Original publication record

James Prescott Joule (1850). On the Mechanical Equivalent of Heat ↗. Philosophical Transactions 140, 61–82.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1849Terrestrial measurement of the speed of lightHippolyte Fizeau · Light & electromagnetismModel specification

Question & finding

Can light travel time be measured over a terrestrial path?

A rotating toothed wheel and distant mirror yielded a terrestrial estimate of light speed.

1849

Teaching equation

c = 4LNf₁ (first extinction; N teeth and N equal gaps)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate round-trip travel time to a half tooth–gap period.

Numerical pathway

Compute transmitted intensity for a rotating finite-aperture wheel.

Visual pathway

Animate outgoing and returning rays as the wheel frequency changes.

Limits

Define the first-extinction convention explicitly; atmospheric path and wheel geometry affect observations.

Original publication record

Hippolyte Fizeau (1849). Sur une expérience relative à la vitesse de propagation de la lumière. Comptes rendus de l’Académie des sciences 29, 90–92.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1851Foucault pendulumLéon Foucault · Relativity & gravityModel specification

Question & finding

Can Earth’s rotation be demonstrated locally?

The pendulum’s oscillation plane precessed relative to the ground.

1851

Teaching equation

Ωp = Ω⊕ sin φ; T₀ ≈ 2π√(ℓ/g)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive latitude-dependent precession in the small-amplitude approximation.

Numerical pathway

Integrate the coupled horizontal equations including Coriolis acceleration.

Visual pathway

Compare pendulum traces at the equator, midlatitudes and poles.

Limits

The simple model neglects ellipticity, damping, suspension anisotropy and finite-amplitude corrections.

Original publication record

Léon Foucault (1851). Démonstration physique du mouvement de rotation de la Terre au moyen du pendule. Comptes rendus de l’Académie des sciences 32, 135–138.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1859Chemical identification by spectroscopyGustav Kirchhoff and Robert Bunsen · Atomic & quantumModel specification

Question & finding

Can characteristic spectral lines identify chemical elements?

Flame spectra provided a sensitive method of chemical analysis.

1859 discovery; 1860 joint paper

Teaching equation

ΔE = hc/λ; I(λ) = Σj Aj L(λ−λj)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Translate transition energies into wavelengths using a later quantum model.

Numerical pathway

Convolve a line catalogue with instrumental broadening and fit mixtures.

Visual pathway

Compare emission lines from individual elements and mixtures.

Limits

Quantum transition theory postdates the experiment; synthetic line strengths are not measured spectra.

Original publication record

Gustav Kirchhoff and Robert Bunsen (1860). Chemische Analyse durch Spectralbeobachtungen. Annalen der Physik und Chemie 110, 161–189.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1879Hall effectEdwin Hall · Condensed matterModel specification

Question & finding

Does a magnetic field cause a transverse voltage in a current-carrying conductor?

Hall observed a transverse electrical response to a magnetic field.

1879

Teaching equation

VH = IB/(nqt)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Balance magnetic and electric forces in a one-carrier model.

Numerical pathway

Explore Hall-voltage fits with measurement noise and geometry corrections.

Visual pathway

Reverse field or charge sign and inspect transverse voltage.

Limits

The single-carrier formula is inadequate for many real solids; thickness and sign conventions must be explicit.

Original publication record

Edwin H. Hall (1879). On a New Action of the Magnet on Electric Currents. American Journal of Mathematics 2, 287–292.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1887Michelson–Morley interferometerAlbert A. Michelson and Edward W. Morley · Relativity & gravityModel specification

Question & finding

Does rotating an interferometer reveal the expected ether-wind fringe shift?

The observed shift was much smaller than the classical stationary-ether prediction.

1887

Teaching equation

ΔNclassical ≈ 2Lv²/(λc²) for a 90° rotation

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Contrast the classical ether prediction with equal invariant light speed.

Numerical pathway

Propagate phase through two interferometer arms and rotate the apparatus.

Visual pathway

Compare predicted fringes under two explicitly labelled models.

Limits

A null result constrains the tested model and sensitivity; it is not a standalone derivation of special relativity.

Original publication record

Albert A. Michelson and Edward W. Morley (1887). On the Relative Motion of the Earth and the Luminiferous Ether ↗. American Journal of Science, series 3, 34, 333–345.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1888Generation and detection of electromagnetic wavesHeinrich Hertz · Light & electromagnetismModel specification

Question & finding

Do electromagnetic disturbances propagate and behave as waves?

Hertz generated and detected radio-frequency waves and investigated reflection and interference.

1887–1888 experiments

Teaching equation

c = 1/√(μ₀ε₀); ∂²E/∂t² = c²∇²E

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive a wave equation from Maxwell’s equations in vacuum.

Numerical pathway

Use a one-dimensional finite-difference time-domain solver with a stated Courant limit.

Visual pathway

Launch a pulse and display reflection and standing-wave nodes.

Limits

A one-dimensional field model omits the three-dimensional spark transmitter and detector.

Original publication record

Heinrich Hertz (1888). Ueber elektrodynamische Wellen im Luftraume und deren Reflexion. Annalen der Physik und Chemie 34, 609–623.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1895Discovery of X-raysWilhelm Conrad Röntgen · Light & electromagnetismModel specification

Question & finding

What penetrating radiation emerges from a discharge tube?

Röntgen reported a new penetrating radiation and demonstrated differential transmission through materials.

1895 discovery and initial report

Teaching equation

I(x) = I₀e^(−μx)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive exponential attenuation from independent absorption probability.

Numerical pathway

Ray-integrate a labelled attenuation phantom.

Visual pathway

Adjust virtual material thickness and inspect a synthetic radiograph.

Limits

Attenuation coefficients are energy-dependent; this is a virtual model with no diagnostic interpretation.

Original publication record

Wilhelm Conrad Röntgen (1895). Ueber eine neue Art von Strahlen (Vorläufige Mittheilung). Sitzungsberichte der Physikalisch-Medizinischen Gesellschaft zu Würzburg, 132–141.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1896Spontaneous radiation from uranium saltsHenri Becquerel · Nuclear & particleInteractive model

Question & finding

Can uranium compounds expose a photographic plate without illumination?

Becquerel observed penetrating emissions independent of recent exposure to sunlight.

1896

Open simplified lab →

Teaching equation

N(t) = N₀e^(−λt); A = λN

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate a later radioactive-decay law to activity and half-life.

Numerical pathway

Simulate Poisson detection counts over fixed exposure windows.

Visual pathway

Compare latent exposure, count statistics and a model decay curve.

Limits

The decay equation is later theory and does not represent a fitted Becquerel dataset.

Original publication record

Henri Becquerel (1896). Sur les radiations invisibles émises par les corps phosphorescents. Comptes rendus de l’Académie des sciences 122, 501–503; one report in the 1896 discovery series.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Working simplified demonstration available; full reconstruction remains a specification.

1896Zeeman effectPieter Zeeman · Atomic & quantumModel specification

Question & finding

Does a magnetic field alter emitted spectral lines?

Zeeman observed magnetic modification of spectral lines.

1896 observation; 1897 publication

Teaching equation

ΔE = μB g mJ B

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compute line shifts in the weak-field Zeeman regime.

Numerical pathway

Generate broadened multiplets from specified transitions and selection rules.

Visual pathway

Increase magnetic field and resolve line splitting and polarisation.

Limits

The modern quantum expression postdates the discovery; anomalous Zeeman structure requires spin and angular momentum coupling.

Original publication record

Pieter Zeeman (1897). On the Influence of Magnetism on the Nature of the Light Emitted by a Substance. Philosophical Magazine, series 5, 43, 226–239.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1897Cathode rays and the electronJ. J. Thomson · Nuclear & particleModel specification

Question & finding

Are cathode rays universal negatively charged particles?

Electric and magnetic deflections supported a common particle with a large charge-to-mass ratio.

1897

Teaching equation

v = E/B; |q|/m = v/(Br)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Combine a crossed-field velocity selector with magnetic curvature.

Numerical pathway

Integrate the Lorentz force for test particles.

Visual pathway

Adjust fields and track a beam’s deflection.

Limits

The teaching apparatus combines idealised measurements; nonrelativistic motion and uniform fields are assumed.

Original publication record

J. J. Thomson (1897). Cathode Rays ↗. Philosophical Magazine, series 5, 44, 293–316.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1898Discovery of polonium and radiumMarie Curie, Pierre Curie and Gustave Bémont · Nuclear & particleModel specification

Question & finding

Does pitchblende contain more active substances than uranium?

Activity-guided chemical separation led to announcements of polonium and radium.

1898

Teaching equation

Amixture = Σi λiNi

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate a mixture’s total activity to its components.

Numerical pathway

Model activity enrichment during idealised separations with uncertainty.

Visual pathway

Track sample mass, enrichment factor and detected counts.

Limits

This is an abstraction of chemical separation, not a protocol; radionuclide identity cannot be inferred from count rate alone.

Original publication record

Pierre Curie, Marie Curie and Gustave Bémont (1898). Sur une nouvelle substance fortement radio-active, contenue dans la pechblende. Comptes rendus de l’Académie des sciences 127, 1215–1217; the radium announcement. The polonium report appeared earlier in the same volume.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1899Precision blackbody spectraOtto Lummer and Ernst Pringsheim · Atomic & quantumInteractive model

Question & finding

Which spectral law fits thermal radiation over a broad wavelength range?

Precision cavity-radiation measurements helped expose limits of existing spectral laws and motivated Planck’s work.

1899 measurements; extended in 1900

Open simplified lab →

Teaching equation

Bλ(T) = (2hc²/λ⁵)/(exp(hc/(λkBT))−1)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compare Planck, Wien and Rayleigh–Jeans limiting forms.

Numerical pathway

Integrate Planck’s spectrum and check the T⁴ scaling.

Visual pathway

Change temperature and inspect peak shift plus spectral-law residuals.

Limits

Planck’s law was introduced in 1900; curves are theoretical unless a measured dataset is explicitly provided.

Original publication record

Otto Lummer and Ernst Pringsheim (1899). Die Vertheilung der Energie im Spectrum des schwarzen Körpers. Verhandlungen der Deutschen Physikalischen Gesellschaft 1, 23–41; subsequent measurements followed.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Working simplified demonstration available; full reconstruction remains a specification.

1909Gold-foil scattering and the atomic nucleusHans Geiger, Ernest Marsden, Ernest Rutherford · Atomic & quantumInteractive model

Question & finding

How is positive charge distributed inside an atom?

Rare large-angle alpha scattering supported a compact positively charged nucleus.

1909 experiment; 1911 nuclear interpretation

Open simplified lab →

Teaching equation

dσ/dΩ = (Z z e² / (16π ε₀ E))² csc⁴(θ/2)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive the scattering angle from a Coulomb hyperbola and impact parameter.

Numerical pathway

Integrate classical Coulomb trajectories; compare angle histograms with the Rutherford cross-section.

Visual pathway

Animate incident trajectories and an angle-resolved detector.

Limits

Single scattering, point charges and nonrelativistic motion; screening and nuclear forces invalidate the model at extremes.

Original publication record

Ernest Rutherford (1911). The scattering of α and β particles by matter and the structure of the atom ↗.

Bibliography draft. Original source and link not live-verified.

Working simplified demonstration available; full reconstruction remains a specification.

1911Disappearance of resistance in mercuryHeike Kamerlingh Onnes and collaborators · Condensed matterModel specification

Question & finding

Does electrical resistance vanish at sufficiently low temperature?

Mercury showed an abrupt resistance drop near 4.2 K.

1911 experiment and report

Teaching equation

R(T < T_c) ≈ 0; V = I R

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compare a normal-state resistance curve with a phase-transition idealisation.

Numerical pathway

Sweep temperature in an explicitly illustrative transition model; vary transition width and noise.

Visual pathway

Show resistance versus temperature with the critical region enlarged.

Limits

A phenomenological curve is not a microscopic theory; zero resistance alone does not model the Meissner effect. Original report: Leiden Communications 120b; direct paper URL requires verification.

Original publication record

Heike Kamerlingh Onnes (1911). The resistance of pure mercury at helium temperatures.

Original edition identified bibliographically; a verified digital copy is still needed.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1913Quantisation of electric chargeRobert A. Millikan · Atomic & quantumModel specification

Question & finding

Is electric charge transferred in discrete units?

Oil-drop measurements supported a common elementary charge.

1913 precision report

Teaching equation

qE = (4πr³/3)(ρ_oil − ρ_air)g

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Balance weight, buoyancy and electric force; infer radius using Stokes drag.

Numerical pathway

Fit synthetic rise/fall velocities, including a selectable slip correction, to a charge lattice.

Visual pathway

Track drops between plates and plot inferred q/e values.

Limits

Historical air viscosity and slip corrections matter; synthetic data cannot establish the historical precision.

Original publication record

Robert A. Millikan (1913). On the Elementary Electrical Charge and the Avogadro Constant ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1916Photoelectric energy–frequency relationRobert A. Millikan · Atomic & quantumModel specification

Question & finding

How does emitted-electron energy depend on light frequency?

Stopping potentials followed a linear frequency relation, supporting the photon energy law.

1916 experimental report

Teaching equation

eV_stop = hν − φ

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive slope h/e and threshold ν₀ = φ/h.

Numerical pathway

Regress synthetic stopping-potential measurements with uncertainty and a work-function offset.

Visual pathway

Move a frequency slider and compare photon energy, threshold and stopping potential.

Limits

Surface condition and contact potentials affect measured intercepts; the ideal line omits these systematics.

Original publication record

Robert A. Millikan (1916). A Direct Photoelectric Determination of Planck’s h ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1919Starlight deflection during a solar eclipseFrank Dyson, Arthur Eddington, Charles Davidson · Relativity & gravityModel specification

Question & finding

Does light passing near the Sun bend as predicted by general relativity?

Eclipse-star positions were interpreted as supporting the relativistic deflection.

1919 eclipse; report published 1920

Teaching equation

α = 4GM/(c²b)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive the weak-field deflection and its inverse impact-parameter scaling.

Numerical pathway

Fit a deflection scale with plate translation, rotation and measurement noise.

Visual pathway

Compare apparent and reference star fields around the eclipsed Sun.

Limits

Historical plate quality and calibration differed between observing sites; a schematic is not a reanalysis of those plates.

Original publication record

F. W. Dyson, A. S. Eddington, C. Davidson (1920). A determination of the deflection of light by the Sun’s gravitational field, from observations made at the total eclipse of May 29, 1919 ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1922Space quantisation in a magnetic fieldWalther Gerlach, Otto Stern · Atomic & quantumModel specification

Question & finding

Are atomic magnetic-moment projections continuous or discrete?

A silver beam separated into discrete components in an inhomogeneous magnetic field.

1922 experiment and publication

Teaching equation

F_z = μ_z ∂B_z/∂z

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compute a beam deflection for two allowed magnetic-moment projections.

Numerical pathway

Sample beam velocity and aperture distributions to generate detector spots.

Visual pathway

Compare classical continuous projections with two-state beam splitting.

Limits

Electron spin was understood later; do not attribute the modern spin interpretation to the original 1922 explanation.

Original publication record

Walther Gerlach, Otto Stern (1922). Der experimentelle Nachweis der Richtungsquantelung im Magnetfeld ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1923Compton wavelength shiftArthur H. Compton · Atomic & quantumModel specification

Question & finding

Does X-ray scattering reveal photon momentum?

Scattered X-rays exhibited an angle-dependent wavelength shift.

1923 experimental/theoretical report

Teaching equation

λ′ − λ = (h/m_ec)(1 − cos θ)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Apply energy and momentum conservation to a photon and initially stationary electron.

Numerical pathway

Sample scattering angles and convolve spectral peaks with detector resolution.

Visual pathway

Rotate a detector and show the shifted and unshifted spectral components.

Limits

The basic equation assumes a free stationary electron; bound-electron and material effects need additional treatment.

Original publication record

Arthur H. Compton (1923). A Quantum Theory of the Scattering of X-rays by Light Elements ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1927Diffraction of electrons by a crystalClinton Davisson, Lester Germer · Atomic & quantumModel specification

Question & finding

Do matter particles display wave interference?

Electron scattering from nickel showed diffraction consistent with a de Broglie wavelength.

1927 experiment and publication

Teaching equation

λ = h/p; 2d sin θ = nλ

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Connect accelerating voltage to nonrelativistic wavelength and Bragg angles.

Numerical pathway

Sum phase contributions from a finite lattice and sweep voltage and detector angle.

Visual pathway

Display a lattice, scattered waves and an angular-intensity plot.

Limits

Crystal orientation, surface preparation and multiple scattering exceed the elementary Bragg model.

Original publication record

C. Davisson, L. H. Germer (1927). Diffraction of Electrons by a Crystal of Nickel ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1932Evidence for the neutronJames Chadwick · Nuclear & particleModel specification

Question & finding

What neutral radiation can eject energetic recoil protons?

Recoil kinematics supported a neutral particle with mass close to that of a proton.

1932 discovery letter

Teaching equation

E_recoil,max = 4m_n M E_n/(m_n + M)²

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compare elastic-collision energy transfer for different target masses.

Numerical pathway

Sample two-body scattering and propagate recoil-energy resolution.

Visual pathway

Compare neutron and photon recoil hypotheses using target sliders.

Limits

This is a kinematic model; production spectra, detector response and nuclear reaction channels are simplified.

Original publication record

James Chadwick (1932). Possible Existence of a Neutron ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1932The positive electronCarl D. Anderson · Nuclear & particleModel specification

Question & finding

Can cosmic-ray tracks reveal a positively charged electron?

Cloud-chamber tracks provided evidence for a positive particle with electron-like mass.

1932 observation; detailed report 1933

Teaching equation

p = |q|Br

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Infer momentum and charge sign from magnetic curvature with a known travel direction.

Numerical pathway

Integrate charged-particle motion with a schematic energy loss through an absorber.

Visual pathway

Trace opposite-curvature particle tracks on either side of a lead plate.

Limits

Curvature alone does not determine mass; direction and energy-loss evidence are essential.

Original publication record

Carl D. Anderson (1933). The Positive Electron ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1938Neutron-induced fission of uraniumOtto Hahn, Fritz Strassmann; interpretation by Lise Meitner and Otto Frisch · Nuclear & particleModel specification

Question & finding

What products appear when uranium is irradiated with neutrons?

Chemical identification of barium established evidence subsequently interpreted as nuclear fission.

1938 experiments; report published 1939

Teaching equation

Q = (m_initial − m_final)c²

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Calculate energy release from stated nuclear masses for an illustrative channel.

Numerical pathway

Sample a clearly labelled illustrative fragment-mass distribution.

Visual pathway

Show nuclear deformation, separated fragments and an energy balance.

Limits

The original work was chemical identification; a liquid-drop animation is a later model and does not reproduce reaction yields.

Original publication record

Otto Hahn, Fritz Strassmann (1939). Über den Nachweis und das Verhalten der bei der Bestrahlung des Urans mittels Neutronen entstehenden Erdalkalimetalle ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1956Detection of the electron antineutrinoClyde Cowan, Frederick Reines and collaborators · Nuclear & particleModel specification

Question & finding

Can the weakly interacting neutrino be detected directly?

Prompt/delayed coincidence signals supported reactor antineutrino detection.

1956 experimental report

Teaching equation

ν̄_e + p → e⁺ + n

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Explain the inverse-beta threshold and positron/neutron coincidence signature.

Numerical pathway

Simulate Poisson signal/background arrivals and delayed neutron captures.

Visual pathway

Plot an event timeline and compare coincident with accidental counts.

Limits

A toy rate is not the measured reactor flux; efficiencies, shielding and backgrounds must be supplied for a physical prediction.

Original publication record

C. L. Cowan Jr., F. Reines, F. B. Harrison, H. W. Kruse, A. D. McGuire (1956). Detection of the Free Neutrino: a Confirmation ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1957Parity violation in beta decayChien-Shiung Wu and collaborators · Nuclear & particleModel specification

Question & finding

Are weak interactions invariant under spatial reflection?

Beta emission from polarised cobalt-60 was asymmetric, demonstrating parity violation.

1956 experiment; report published 1957

Teaching equation

W(θ) ∝ 1 + A P β cos θ

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Show how the spin–momentum correlation changes under parity.

Numerical pathway

Sample angular distributions for adjustable polarisation P and asymmetry A.

Visual pathway

Compare mirror-related detector counts around a polarised source.

Limits

The displayed angular law is an educational reduction; nuclear spin, transition structure and detector acceptance matter.

Original publication record

C. S. Wu, E. Ambler, R. W. Hayward, D. D. Hoppes, R. P. Hudson (1957). Experimental Test of Parity Conservation in Beta Decay ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1960Gravitational redshift across a laboratory towerRobert Pound, Glen Rebka · Relativity & gravityModel specification

Question & finding

Does photon frequency change with gravitational potential?

A Mössbauer-resonance experiment measured the gravitational frequency shift over a terrestrial height.

1960 measurement report

Teaching equation

Δν/ν ≈ gh/c²

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate a weak-field gravitational shift to a compensating Doppler velocity.

Numerical pathway

Convolve a resonance line with a scanned source velocity and fit the shift.

Visual pathway

Show emission/absorption heights alongside the shifted resonance curves.

Limits

The weak-field approximation applies; thermal shifts and vibration require experimental controls.

Original publication record

R. V. Pound Jr., G. A. Rebka Jr. (1960). Apparent Weight of Photons ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1960Coherent light from a ruby laserTheodore H. Maiman · Light & electromagnetismModel specification

Question & finding

Can stimulated emission produce sustained coherent optical output?

Pulsed ruby emission demonstrated laser operation.

1960 demonstration and publication

Teaching equation

dN/dt = R_p − N/τ − gNS

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Explain inversion, gain and threshold in a simplified rate-equation model.

Numerical pathway

Integrate coupled population and photon-number rate equations.

Visual pathway

Plot pump energy, inversion and pulse buildup in a cavity schematic.

Limits

A reduced rate model omits ruby sublevels, spatial modes and detailed pumping kinetics.

Original publication record

T. H. Maiman (1960). Stimulated Optical Radiation in Ruby ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1965Cosmic microwave background excessArno Penzias, Robert Wilson · Cosmology & astrophysicsModel specification

Question & finding

What causes the persistent microwave antenna-temperature excess?

A nearly isotropic excess antenna temperature was reported and interpreted cosmologically in a companion paper.

1965 report

Teaching equation

B_ν(T) = (2hν³/c²)/(exp(hν/k_BT) − 1)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate Rayleigh–Jeans antenna temperature to specific intensity.

Numerical pathway

Fit a synthetic microwave excess with atmospheric and instrumental terms.

Visual pathway

Compare antenna noise components and a separately labelled ideal blackbody spectrum.

Limits

The 1965 experiment did not measure the full blackbody spectrum; later observations established that spectrum precisely.

Original publication record

A. A. Penzias, R. W. Wilson (1965). A Measurement of Excess Antenna Temperature at 4080 Mc/s ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1969Substructure inside the protonSLAC–MIT electron-scattering collaboration · Nuclear & particleModel specification

Question & finding

Is the proton pointlike at high momentum transfer?

Deep-inelastic electron scattering revealed proton structure associated with pointlike constituents.

1969 published scattering results

Teaching equation

Q² = 4EE′ sin²(θ/2); x_B = Q²/(2Mν)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compute Bjorken x and momentum transfer from electron kinematics.

Numerical pathway

Bin synthetic events in x and Q² to illustrate approximate scaling.

Visual pathway

Map detector angle and scattered energy to a structure-function plot.

Limits

Toy parton distributions are illustrative; QCD evolution, radiative corrections and acceptance are required for quantitative extraction.

Original publication record

E. D. Bloom and collaborators (1969). High-Energy Inelastic e-p Scattering at 6° and 10° ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1974The J/ψ resonanceSamuel Ting and the Brookhaven collaboration; parallel SLAC discovery · Nuclear & particleModel specification

Question & finding

Are there previously unknown narrow particle resonances?

A narrow resonance near 3.1 GeV was discovered, central to the identification of charmonium.

1974 discovery report

Teaching equation

m²c⁴ = (E₁ + E₂)² − c²|p₁ + p₂|²

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Construct the invariant mass of a detected lepton pair.

Numerical pathway

Generate a resonance plus smooth background and smear detector energies.

Visual pathway

Build an invariant-mass histogram event by event.

Limits

A synthetic peak is not discovery evidence; physical production, background modelling and significance need real data. The linked paper is the Brookhaven half of the simultaneous discovery.

Original publication record

J. J. Aubert and collaborators (1974). Experimental Observation of a Heavy Particle J ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1974A binary pulsar as a gravity laboratoryRussell Hulse, Joseph Taylor · Relativity & gravityModel specification

Question & finding

Can pulsar timing reveal orbital motion and test gravity?

Periodic timing changes revealed a pulsar in a binary system; later monitoring tested orbital decay.

1974 discovery; paper published 1975

Teaching equation

Δt_R ≈ a_p sin i · sin φ / c

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate light-travel-time delay to an ideal circular orbit.

Numerical pathway

Solve Kepler’s equation for an eccentric timing-delay model.

Visual pathway

Animate the orbit and aligned pulse-arrival residuals.

Limits

The discovery paper is not the later orbital-decay measurement; a circular formula is only an introduction to the eccentric timing model.

Original publication record

R. A. Hulse, J. H. Taylor (1975). Discovery of a Pulsar in a Binary System ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1980Integer quantum Hall effectKlaus von Klitzing, Gerhard Dorda, Michael Pepper · Condensed matterModel specification

Question & finding

Can Hall resistance become accurately quantised?

A two-dimensional electron system exhibited quantised Hall-resistance plateaus.

1980 experiment and publication

Teaching equation

R_xy = h/(νe²); ν ∈ positive integers

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Calculate quantised plateau values and filling factor ν = nh/(eB).

Numerical pathway

Plot a phenomenological broadened Landau-level model with disorder clearly labelled.

Visual pathway

Sweep magnetic field across plateaus and longitudinal-resistance minima.

Limits

An ideal clean Landau-level diagram alone does not explain finite plateau widths; disorder/localisation are essential.

Original publication record

K. von Klitzing, G. Dorda, M. Pepper (1980). New Method for High-Accuracy Determination of the Fine-Structure Constant Based on Quantized Hall Resistance ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1982Bell test with changing analyser settingsAlain Aspect, Jean Dalibard, Gérard Roger · Atomic & quantumInteractive model

Question & finding

Can local hidden-variable models reproduce entangled-photon correlations?

Measured correlations violated a Bell inequality under the experiment’s assumptions.

1982 experiment and publication

Open simplified lab →

Teaching equation

E(a,b) = −cos[2(a − b)]; |S_CHSH| ≤ 2

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compare a Bell bound with the ideal quantum maximum 2√2.

Numerical pathway

Sample photon-pair detection outcomes and estimate correlations with statistical uncertainty.

Visual pathway

Rotate polariser angles and display correlation curves and an explicitly pedagogical CHSH value.

Limits

CHSH is a teaching model, not a claim that the 1982 apparatus implemented this exact calculation; detection and other loopholes remained.

Original publication record

A. Aspect, J. Dalibard, G. Roger (1982). Experimental Test of Bell’s Inequalities Using Time-Varying Analyzers ↗.

Bibliography draft. Original source and link not live-verified.

Working simplified demonstration available; full reconstruction remains a specification.

1995Bose–Einstein condensation in a dilute gasEric Cornell, Carl Wieman, Michael Anderson and collaborators · Condensed matterModel specification

Question & finding

Can a dilute atomic gas macroscopically occupy its lowest quantum state?

A trapped rubidium gas showed a sharp low-momentum condensate component.

1995 experiment and publication

Teaching equation

N₀/N ≈ 1 − (T/T_c)³

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive the ideal harmonically trapped gas condensate fraction.

Numerical pathway

Generate thermal-plus-condensate density profiles or solve a simplified Gross–Pitaevskii equation.

Visual pathway

Show temperature-dependent density and time-of-flight profiles.

Limits

The ideal-gas expression omits interactions, finite-size corrections and imaging dynamics.

Original publication record

M. H. Anderson, J. R. Ensher, M. R. Matthews, C. E. Wieman, E. A. Cornell (1995). Observation of Bose-Einstein Condensation in a Dilute Atomic Vapor ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

1998Atmospheric neutrino oscillationsSuper-Kamiokande Collaboration · Nuclear & particleInteractive model

Question & finding

Do neutrino flavours change during propagation?

A zenith-angle-dependent atmospheric muon-neutrino deficit supported neutrino oscillations.

1998 experimental report

Open simplified lab →

Teaching equation

P(ν_μ→ν_μ) = 1 − sin²(2θ) sin²(1.267 Δm²L/E)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive the two-flavour vacuum survival probability; use Δm² in eV², L in km and E in GeV.

Numerical pathway

Average the probability over illustrative energy and path-length distributions.

Visual pathway

Pass neutrinos through Earth and plot survival versus L/E.

Limits

A two-flavour vacuum model omits three-flavour mixing, matter effects and detector/event reconstruction.

Original publication record

Y. Fukuda and collaborators (1998). Evidence for Oscillation of Atmospheric Neutrinos ↗.

Bibliography draft. Original source and link not live-verified.

Working simplified demonstration available; full reconstruction remains a specification.

1998Accelerating cosmic expansion from supernovaeHigh-z Supernova Search Team; parallel Supernova Cosmology Project · Cosmology & astrophysicsModel specification

Question & finding

Is cosmic expansion slowing or accelerating?

Type Ia supernova distances favoured an accelerating expansion within the fitted cosmological framework.

1998 observational report

Teaching equation

μ = 5 log₁₀(d_L/Mpc) + 25

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate luminosity distance to the expansion history in a stated FLRW cosmology.

Numerical pathway

Integrate d_L(z) for flat matter-plus-Λ models and compare synthetic distance moduli.

Visual pathway

Plot a supernova Hubble diagram with adjustable matter density.

Limits

A simplified fit is not a reproduction of the paper; calibration, dust, population effects and cosmological assumptions must be accounted for.

Original publication record

Adam G. Riess and collaborators (1998). Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2002SNO resolves solar-neutrino flavour changeQ. R. Ahmad et al. · SNO Collaboration · Nuclear & particleModel specification

Question & finding

Did the missing solar electron neutrinos disappear, or change flavour?

Neutral-current and charged-current measurements separated total active-neutrino flux from electron-neutrino flux, providing direct evidence of flavour transformation.

2002 · neutral-current result

Teaching equation

Phi_NC = Phi_e + Phi_mu + Phi_tau; Phi_CC = Phi_e

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Compare flavour-sensitive and flavour-independent reaction rates; use a two-flavour oscillation model only as an introduction.

Numerical pathway

Integrate a neutrino spectrum against reaction cross sections and detector response, then fit flux components.

Visual pathway

Flux bands intersect in the electron versus non-electron neutrino plane.

Limits

Solar propagation requires matter effects and, for precision, three-flavour mixing; a vacuum sinusoid alone does not reproduce SNO.

Original publication record

Q. R. Ahmad et al. (SNO Collaboration) (2002). Direct Evidence for Neutrino Flavor Transformation from Neutral-Current Interactions in the Sudbury Neutrino Observatory ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2004Electric field effect in atomically thin carbonK. S. Novoselov, A. K. Geim and colleagues · Condensed matterModel specification

Question & finding

Can an isolated atomic carbon sheet operate as a gate-controlled electronic material?

Atomically thin carbon films exhibited an electric field effect with electron and hole conduction controlled by a gate.

2004 · paper

Teaching equation

n = C_g (V_g - V_D) / e; sigma ≈ e mu |n|

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate gate capacitance to carrier density and the Drude approximation away from charge neutrality.

Numerical pathway

Fit conductance against gate voltage with residual density and contact resistance included.

Visual pathway

Gate-voltage slider moves the Fermi level through a schematic Dirac cone and updates a conductance curve.

Limits

The simple conductivity expression fails near charge neutrality; a Dirac-cone picture is a model, not a direct image of this apparatus.

Original publication record

K. S. Novoselov et al. (2004). Electric Field Effect in Atomically Thin Carbon Films ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2012Daya Bay measures a nonzero neutrino mixing angleF. P. An et al. · Daya Bay Collaboration · Nuclear & particleModel specification

Question & finding

Do reactor electron antineutrinos disappear over kilometre-scale distances?

Near and far detectors observed electron-antineutrino disappearance and established nonzero theta_13.

2012 · paper

Teaching equation

P_ee ≈ 1 − sin²(2 theta_13) sin²(1.267 Delta_m² L/E)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Explore the leading oscillation term using Delta_m² in eV², L in metres and E in MeV.

Numerical pathway

Average the survival probability over reactor baselines, spectra and detector energy resolution.

Visual pathway

Near/far spectrum ratios and an adjustable L/E oscillation curve.

Limits

The displayed formula is a leading approximation; precision analysis includes the solar term, multiple reactors and systematic covariance.

Original publication record

F. P. An et al. (Daya Bay Collaboration) (2012). Observation of Electron-Antineutrino Disappearance at Daya Bay ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2012ATLAS and CMS discover a Higgs-like bosonATLAS and CMS Collaborations · CERN LHC · Nuclear & particleModel specification

Question & finding

Is there a new boson consistent with the Higgs mechanism?

Independent collision experiments observed a new boson near 125 GeV; subsequent measurements tested its Higgs properties.

2012 · discovery papers

Teaching equation

m²c⁴ = (sum E_i)² − c² |sum p_i|²

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive invariant mass from four-momentum conservation and explain signal significance.

Numerical pathway

Generate a labelled synthetic signal-plus-background mass distribution and perform a Poisson likelihood fit.

Visual pathway

Two-photon events build an invariant-mass histogram with signal and background overlays.

Limits

Synthetic events are teaching data, not CERN measurements. Discovery of a boson and confirmation of its detailed properties are separate steps.

Original publication record

G. Aad et al. (ATLAS Collaboration) (2012). Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ↗.

S. Chatrchyan et al. (CMS Collaboration) (2012). Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2015Loophole-free Bell inequality testB. Hensen and colleagues · Delft · Atomic & quantumModel specification

Question & finding

Can distant spin correlations violate a Bell inequality while closing the major detection and locality loopholes?

Entangled electron spins separated by 1.3 kilometres violated a Bell inequality in an event-ready experiment.

2015 · experiment and paper

Teaching equation

S = |E(a,b) + E(a,b′) + E(a′,b) − E(a′,b′)|; S_local ≤ 2

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Derive the CHSH bound under local hidden-variable assumptions and compare the quantum maximum 2 sqrt(2).

Numerical pathway

Sample binary outcomes with finite trial counts; inspect uncertainty and sensitivity to measurement angles.

Visual pathway

Adjust four analyser angles and compare local and quantum correlation bounds.

Limits

Bell violations do not enable faster-than-light communication; experimental inference retains stated assumptions about setting choices and statistics.

Original publication record

B. Hensen et al. (2015). Loophole-free Bell inequality violation using electron spins separated by 1.3 kilometres ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2015LIGO directly detects gravitational wavesB. P. Abbott et al. · LIGO Scientific and Virgo Collaborations · Relativity & gravityModel specification

Question & finding

Can laser interferometers measure spacetime strain from a distant compact-binary merger?

GW150914 was observed at two LIGO detectors and interpreted as the merger of two stellar-mass black holes.

2015 · detection; 2016 · paper

Teaching equation

h = Delta_L/L; df/dt = (96/5) pi^(8/3) (G M_c/c³)^(5/3) f^(11/3)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate strain to arm-length change and derive the leading inspiral chirp scaling.

Numerical pathway

Integrate the inspiral frequency evolution and compare a template with labelled synthetic detector noise.

Visual pathway

Two detector traces, a rising-frequency spectrogram and a schematic interferometer.

Limits

The leading chirp formula stops before merger; accurate merger and ringdown modelling requires relativity-based waveforms. Stretch is visually exaggerated.

Original publication record

B. P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration) (2016). Observation of Gravitational Waves from a Binary Black Hole Merger ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2017GW170817 opens binary-neutron-star multimessenger astronomyLIGO Scientific and Virgo Collaborations with electromagnetic observatories · Cosmology & astrophysicsModel specification

Question & finding

Can gravitational-wave and electromagnetic observations identify the same neutron-star merger?

A binary-neutron-star gravitational-wave signal was associated with a gamma-ray burst and a widely observed electromagnetic counterpart.

2017 · detection and paper

Teaching equation

Delta_t_arrival = Delta_t_emission + D(1/v_EM − 1/v_GW)

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Separate intrinsic emission delay from propagation delay when comparing signals.

Numerical pathway

Explore sky triangulation with detector arrival-time differences and measurement errors.

Visual pathway

Aligned gravitational-wave, gamma-ray and optical timelines with distinct physical emission mechanisms.

Limits

A timing offset is not directly a wave-speed difference without assumptions about the emission delay.

Original publication record

B. P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration) (2017). GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2019Event Horizon Telescope images M87*Event Horizon Telescope Collaboration · Cosmology & astrophysicsModel specification

Question & finding

Can Earth-scale radio interferometry resolve emission around a supermassive black hole?

Reconstructed millimetre-wave images revealed a bright ring and central brightness depression consistent with a black-hole shadow.

2017 · observations; 2019 · papers

Teaching equation

V(u,v) = integral I(l,m) exp[−2 pi i(ul+vm)] dl dm

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Explain the Fourier relationship between sky brightness and interferometric visibility under small-field approximations.

Numerical pathway

Sample a synthetic ring in the Fourier plane and compare reconstructions as baseline coverage changes.

Visual pathway

Toggle telescopes to see sparse Fourier coverage and the resulting image uncertainty.

Limits

The image is a reconstruction of radio emission, not a visible-light photograph or an image of an event horizon surface.

Original publication record

Event Horizon Telescope Collaboration (2019). First M87 Event Horizon Telescope Results. I. The Shadow of the Supermassive Black Hole ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2019Programmable quantum processor samples random circuitsF. Arute and colleagues · Google AI Quantum · Atomic & quantumModel specification

Question & finding

Can a quantum processor perform a specific sampling task beyond the classical methods available in the benchmark?

A superconducting processor demonstrated random-circuit sampling reported as quantum computational supremacy for the chosen benchmark.

2019 · paper

Teaching equation

p(x) = |<x|U|0...0>|²

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Use Born probabilities and circuit composition to explain random-circuit sampling.

Numerical pathway

Simulate small circuits exactly and add a simple noise channel; compare output distributions.

Visual pathway

A small editable quantum circuit updates bit-string probabilities and sampling histograms.

Limits

The result concerns a specialised benchmark, not general useful quantum speedup; classical algorithms and hardware comparisons subsequently improved.

Original publication record

F. Arute et al. (2019). Quantum supremacy using a programmable superconducting processor ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2021Fermilab measures the muon magnetic anomalyB. Abi et al. · Muon g−2 Collaboration · Nuclear & particleModel specification

Question & finding

How precisely does a muon's spin precess relative to its orbital motion in a magnetic field?

The first Fermilab result measured the positive-muon anomalous magnetic moment with 0.46 ppm precision and agreed with the earlier Brookhaven measurement.

2021 · first Fermilab result

Teaching equation

a_mu = (g−2)/2; omega_a ≈ a_mu qB/m_mu

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Connect the anomalous precession frequency to the magnetic anomaly in an ideal uniform field.

Numerical pathway

Fit a decaying oscillatory event-count model to labelled synthetic decay-electron counts.

Visual pathway

Muon spin and orbit rotate at different rates beside a decay-count trace.

Limits

The simplified relation omits electric-field and pitch corrections. New-physics significance depends on the theory calculation; this is not a current 2026 anomaly claim.

Original publication record

B. Abi et al. (Muon g−2 Collaboration) (2021). Measurement of the Positive Muon Anomalous Magnetic Moment to 0.46 ppm ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2022KATRIN reaches sub-electronvolt neutrino-mass sensitivityM. Aker et al. · KATRIN Collaboration · Nuclear & particleModel specification

Question & finding

What does the endpoint of tritium beta decay reveal about the effective electron-antineutrino mass?

A direct kinematic analysis placed a sub-electronvolt upper bound on the effective electron-antineutrino mass.

2022 · sub-electronvolt-limit paper

Teaching equation

dN/dE ∝ F(Z,E) p(E+m_e c²)(E_0−E) sqrt[(E_0−E)²−m_beta² c⁴]

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Examine the beta-spectrum endpoint and the effective mass m_beta² = sum |U_ei|² m_i².

Numerical pathway

Convolve endpoint spectra with an instrumental response and fit a background plus endpoint model.

Visual pathway

Magnify the last few electronvolts of the spectrum as an assumed neutrino mass changes.

Limits

An upper limit is not a nonzero mass detection. Molecular final states and instrumental response are essential to the real analysis; later results are not represented here.

Original publication record

M. Aker et al. (KATRIN Collaboration) (2022). Direct neutrino-mass measurement with sub-electronvolt sensitivity ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2022NIF obtains fusion target gain above unityH. Abu-Shawareb et al. · Indirect Drive ICF Collaboration · Thermal & statisticalModel specification

Question & finding

Can an inertial-confinement fusion shot produce more fusion energy than the laser energy delivered to the target?

The December 2022 experiment achieved target gain above one; the peer-reviewed result appeared in 2024.

2022 · experiment; 2024 · paper

Teaching equation

G_target = E_fusion / E_laser,target

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Track energy accounting across laser, target and whole-facility boundaries.

Numerical pathway

Explore a labelled toy energy-balance model; retain separate laser efficiency and target gain parameters.

Visual pathway

Energy-flow diagram shows fusion output, target input and electrical input as distinct quantities.

Limits

Target gain above one is not net electrical power generation. A toy energy model is not a radiation-hydrodynamics simulation of the NIF capsule.

Original publication record

H. Abu-Shawareb et al. (Indirect Drive ICF Collaboration) (2024). Achievement of Target Gain Larger than Unity in an Inertial Fusion Experiment ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2023ALPHA observes gravity acting on antihydrogenE. K. Anderson et al. · ALPHA Collaboration · Nuclear & particleModel specification

Question & finding

Does trapped antihydrogen respond to terrestrial gravity with downward acceleration?

Antihydrogen released from a magnetic trap showed gravitational behaviour consistent with downward attraction.

2023 · paper

Teaching equation

m z_ddot = −m_g g − dU_magnetic/dz

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Distinguish gravitational and magnetic forces in a trap-release model.

Numerical pathway

Integrate ensembles of one-dimensional trajectories with varied initial energies and magnetic gradients.

Visual pathway

A trap-release schematic compares upper and lower escape fractions under different gravitational assumptions.

Limits

The experiment is not a precision equivalence-principle test at ordinary-matter accuracy; trap fields and initial distributions materially affect the inference.

Original publication record

E. K. Anderson et al. (ALPHA Collaboration) (2023). Observation of the effect of gravity on the motion of antimatter ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2023Pulsar timing reveals evidence for a gravitational-wave backgroundG. Agazie et al. · NANOGrav Collaboration · Cosmology & astrophysicsModel specification

Question & finding

Do pulsar timing residuals contain the angular correlations expected from a nanohertz gravitational-wave background?

The 15-year dataset showed evidence for a gravitational-wave background through correlated pulsar timing signals.

2023 · 15-year dataset paper

Teaching equation

Gamma(theta) = 1/2 + (3/2)x ln(x) − x/4; x = (1−cos theta)/2

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Plot the Hellings–Downs correlation for distinct pulsar pairs; use the limit x ln(x) → 0 at x → 0.

Numerical pathway

Sample a pulsar network and simulated timing residuals with correlated background and independent noise.

Visual pathway

Pairs of pulsars populate an angular-correlation plot as observing time and noise change.

Limits

This is statistical evidence for a background, not the identification of one individual binary; the background's source population is an inference.

Original publication record

G. Agazie et al. (NANOGrav Collaboration) (2023). The NANOGrav 15 yr Data Set: Evidence for a Gravitational-wave Background ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

2024Laser excitation of the thorium-229 nucleusJ. Tiedau and colleagues · Nuclear & particleModel specification

Question & finding

Can laser light directly drive the unusually low-energy nuclear transition in thorium-229?

Direct laser excitation of the thorium-229 nuclear transition established a key experimental step toward nuclear optical clocks.

2024 · paper

Teaching equation

E_transition = h nu; R(Delta) ∝ 1/[1 + (2 Delta/Gamma)²]

Equations may be later models of the experiment; they are not quotations from the original paper.

Analytical pathway

Relate nuclear transition energy, resonant frequency and an idealised Lorentzian line shape.

Numerical pathway

Fit synthetic fluorescence counts to a broadened resonance with background and frequency uncertainty.

Visual pathway

Scan laser frequency across a resonance and compare electronic and nuclear energy-level schematics.

Limits

An excitation demonstration is not by itself a fully realised high-accuracy clock. The line-shape example is idealised and does not reproduce all solid-state shifts.

Original publication record

J. Tiedau et al. (2024). Laser Excitation of the Th-229 Nucleus ↗.

Bibliography draft. Original source and link not live-verified.

Analytical, numerical and visual pathways specified; interactive reconstruction not implemented.

02 / Numerical & analytical laboratory

Make a prediction.
Change one thing.

Every plot is generated locally from a stated model. Compare an analytical prediction with an independent numerical method where applicable. For blackbody radiation the independent comparison is its integral; Bell sampling demonstrates statistical variation.

Analytical referenceNumerical / sampled values
Assumptions & limits. All values are synthetic. Agreement with an analytical solution verifies this implementation under its assumptions; it does not validate a reconstruction against physical evidence.

03 / How to use the index

Keep the chain
of reasoning visible.

Each entry has a stable identifier. New records can be added without changing the navigation structure. A historical experiment, a later theoretical model and a modern numerical demonstration are different parts of the evidence chain.

A / ANALYTICAL

Derive a prediction.

State assumptions, units and initial conditions. Work out a closed-form result or a controlled approximation. Identify the conditions under which it stops being reliable.

N / NUMERICAL

Check the calculation.

Use an independent algorithm, refine its resolution and measure error. Preserve random seeds when sampling. Export model values with their parameter settings.

V / VISUAL

Connect it to evidence.

Label axes and distinguish synthetic predictions from measurements. A visually compelling match is only useful when the data, uncertainty and comparison method are inspectable.

MAI Physics research method →

04 / 2025–2026 frontier

A date is not
evidence of a result.

The requested horizon extends to 2026. This edition leaves 2025–2026 open because its coverage has not yet been reviewed against current original papers. That gap is explicit, rather than filled with guessed discoveries.

Next verification priorities: updated neutrino-mass limits, muon magnetic-moment measurements and theory comparisons, gravitational-wave catalogues, nuclear-clock spectroscopy and fusion target-gain records.

Before adding a result: retrieve the original paper, distinguish measurement date from publication date, check uncertainty and peer-review status, then record what the result actually supports.