Symmetry-adapted basis — where it appears
Named by 2 essays across 2 fields — each of them below, with the objects they name alongside it.
Where two levels must meet
At most wavevectors nothing of a crystal's symmetry survives, and its levels are as unconstrained as any operator's. At a handful of them a whole point group survives, and where that group has a two-dimensional representation, two levels are obliged to coincide — before anything about the material is known.
The shell that splits into kinds
The neighbours of an atom carry a space of functions as large as the shell, and the group does not treat that space as one thing. It splits into pieces of a few kinds, in whole numbers, and the count is the cheapest character in the subject: how many neighbours each operation leaves where they are.
Named alongside it
The objects these essays reach for when they reach for this one.
Irreducible representationBloch stateBurnside lemmaCharacterCharacter tableDegeneracyLittle groupMultiplicityOrbitPermutation representationWavevector