High-spin — where it appears
Named by 3 essays across one field — each of them below, with the objects they name alongside it.
The pairing energy decides the moment
Whether the sixth d electron pairs up in the lower set or goes alone into the upper one is a competition between the splitting and the cost of pairing. Run the filling rules over the whole shell and exactly four configurations have a choice — and every one of them changes state at Δ = P exactly.
The double hump and what removes it
The hydration enthalpies of the first transition series do not lie on a line — they rise, dip at manganese, rise and dip again at zinc. Subtract the ligand field stabilisation computed from the same model that describes their spectra and what is left is a line, with the one fitted parameter landing inside the range a spectrum measures.
The same count, two oxidation states
Count a complex by the neutral method and by the ionic one and the total is the same integer every time — eighteen for ferrocene, sixteen for tetrachloroplatinate, twenty for hexaaquanickel. The oxidation state and the d count are not: hexaaquairon is d⁶ on one convention and d⁸ on the other, and the two predict spin-only moments of 4.90 and 2.83 against a measured 5.40.
Named alongside it
The objects these essays reach for when they reach for this one.
d orbitalsLigand fieldCoordination complexLow spinMagnetic momentModel limitSplittingAngular overlapApproximationBarycentreConventionEighteen-electron rule