Parity (g and u) — where it appears
Named by 5 essays across 3 fields — each of them below, with the objects they name alongside it.
Exactly zero
Where symmetry forbids an interaction the overlap is not small. It is zero — and computing it and finding arithmetic noise is a different kind of statement from computing it and finding a small number.
Selection rules are one theorem
An integral over all space vanishes unless the integrand is totally symmetric. Every selection rule in spectroscopy is that sentence with a different integrand — and the rule of mutual exclusion falls out rather than being remembered.
Why a d–d band is weak
In a centrosymmetric complex the transition between the two halves of a split d shell is forbidden — exactly, by parity, with no small quantity anywhere. What makes it visible at all is that the molecule is never quite centrosymmetric, and the computation says which vibrations do the work.
Mutual exclusion does not prove a centre
A centrosymmetric molecule shows no band in both its infrared and its Raman spectrum. The rule is a theorem and its converse is read off as though it were part of it — but ferrocene in the gas phase has no centre of inversion and no coincidence either, and the reason is that a fivefold axis separates the coordinates from their products where a threefold or fourfold axis cannot.
The group of a molecule that will not hold still
A point group is a group of rotations of space, and it presupposes a structure for them to act on. Ethane has no one structure — its methyl groups turn billions of times a second — and the group that describes its spectrum has thirty-six elements where the point group has twelve, out of two thousand eight hundred and eighty conceivable.
Named alongside it
The objects these essays reach for when they reach for this one.
Selection rulesPoint groupSymmetry-forbidden transitionsVibrational modesCharacter tableIrreducible representationsLaporte's ruleThe rule of mutual exclusionTransition momentAbsorptionConjugacy classD d transition