The event
V. E. Barnes et al., "Observation of a Hyperon with Strangeness Minus Three", Physical Review Letters 12, 204 to 206 (1964).
Physical seam / one event, held out
Nine baryons left one place empty. Trace the 1964 bubble-chamber event that filled it, then use the equal-spacing mass rule to predict the Omega-minus and test why it had to decay weakly.
A charged particle leaves a production vertex, travels far enough to draw a line, then ends at a second vertex. Choose that segment. The sums below are made from the particle assignments each time, not stored verdicts.
It must begin at the production vertex and end at the decay kink.
No candidate selected.
Authored topology diagram based on the reaction assignment in Barnes et al. It is not a geometric reconstruction and does not preserve the photograph's angles, curvature, scale, or camera view. The dashed neutral paths are inferred from the event assignment because neutral particles leave no direct bubble trail.
The nine known charge states supplied three rounded isospin-multiplet mass levels. Fit only those levels. Omega-minus is locked outside the fit, where a prediction can still fail.
Historical inputs from the discovery paper
The view switch changes only the held-out comparison. It never changes the fit inputs.
Calculating the historical fit.
Choose which Omega-minus mass to place below the lightest ground-state two-body channel with the same charge, baryon number, and strangeness.
calculating
Calculating the threshold.
Every result here is recomputed from the source values below. Published values remain labelled as published. The arithmetic beside them is live.
calculating
calculating
calculating
calculating
calculating
Paper prediction: about 1680 MeV/c²
First event: 1686 ± 12 MeV/c²
PDG 2026 fit: 1672.45 ± 0.29 MeV/c²
Source update. The candidate spec carried Xi-zero as 1314.82 ± 0.21 MeV. The cited 2026 PDG listing now prints 1314.86 ± 0.20 MeV. This page uses the listing, which changes the threshold to calculating MeV/c² and the current gap to calculating MeV/c².
Not from pixels alone. Charge sign follows curvature only after the magnetic-field direction and camera geometry are known. Momentum needs calibrated curvature in three dimensions. Particle identity also uses range, ionisation, decay assignments, and constrained kinematics.
One event, cautiously stated. Barnes et al. reported an event they believed to be the postulated particle and said the charge, inferred strangeness, and reconstructed mass justified the identification. They deferred a detailed mass discussion until more events and systematic errors were better understood.
Not a spin measurement. The decuplet supplied the spin-parity assignment. The photographed event itself did not measure spin-parity; later angular analyses tested spin.
Not the quark model's mature prediction. The 1964 event tested the Eightfold Way classification and unitary symmetry. Quark proposals appeared in the same year.
V. E. Barnes et al., "Observation of a Hyperon with Strangeness Minus Three", Physical Review Letters 12, 204 to 206 (1964).
Murray Gell-Mann, "Symmetries of Baryons and Mesons", Physical Review 125, 1067 to 1084 (1962).
Susumu Okubo, "Note on Unitary Symmetry in Strong Interactions", Progress of Theoretical Physics 27, 949 to 966 (1962).
F. Takahashi et al. (Particle Data Group), 2026 particle listings. This is an online data release cited as forthcoming in International Journal of Modern Physics A 41, 2630011.
Brookhaven National Laboratory, "Omega Minus", uploaded 29 December 2008, CC BY-NC-ND 2.0. It is linked rather than loaded, so this page makes no third-party request and does not modify the image.
The no-dependency verifier in research/omega-minus/verify-omega-minus.mjs independently transcribes the source anchors, recomputes every physical result displayed here, checks vertex quantum numbers, and fails on drift.