The procedure is pure measurement plus arithmetic — no nuclear model of any kind:
Every input is a weighed mass. No strong force, no shell model, no liquid drop, no geometry, no fitted parameter enters. So the binding energy is an empirical fact about the nucleus — a measured mass deficit — not the output of any theory. There is no more reason to doubt it than to doubt a weight read off a scale.
The identification "mass deficit = energy" is not an arbitrary naming. It rests on E = mc², verified directly to ~10−7 (Rainville 2005), and the binding energy is independently measurable as an energy: the deuteron's 2.2246 MeV "missing mass" is also the measured γ-ray energy; larger nuclei give it as photodisintegration thresholds and reaction Q-values (product kinetic energies). Mass-route and energy-route agree. So the deficit is a cross-checked, doubly-anchored energy — "binding energy" is the right name, not a rebranding.
RealNucleus does something categorically different: it sets up a model (unit charges in domains, Coulomb only) and computes a binding energy — measuring nothing about the nucleus itself. It is a genuine predictive, explanatory theory: it attempts the why (a mechanism), where the mass deficit gives only the what (the value). Standard nuclear models (liquid drop, shell, χEFT) also compute binding — so "computing it" is not unique to RealNucleus; the distinction there is parameter economy (RealNucleus ~1 vs 5–30). But against the measurement, the distinction is stark and clean: one is weighed, the other is derived from a model.
| nuclei | RealNucleus (computed) | measured | reading |
|---|---|---|---|
| alpha-conjugate (He-4, C-12, O-16) | ~107%, parameter-free | exact | real, impressive |
| He-3, tritium, Li-6 (odd) | 21–248%, geometry-dependent | exact | undetermined |
Against the measured floor, RealNucleus wins cleanly on the alpha-conjugate line — one calibration, pure Coulomb, ~107% — and is structurally undetermined off it: for the odd nuclei the computed binding swings by a factor of ten with the assumed geometry, and the tritium/He-3 ratio comes out ~2.3 where the measured near-degeneracy is ~1.1. The sweet spot is the even alpha-conjugate closed shells — not the magic numbers (it gets non-magic C-12 right) and not mere N=Z balance (it misses balanced Li-6).
← Back to the Gallery · companion: computability and the only arbiter