Eigenfunction
Named by 2 essays across one field — each of them below, with the objects they name alongside it.
Also named here as heat equation, irreversibility — the same set of essays touches all of them, so they are one junction rather than several.
The corners go first
Fourier was not decomposing waves for the pleasure of it. He was solving the flow of heat, and the whole apparatus exists because each harmonic fades at a rate set by the square of its frequency — which is why a sharp profile smooths instantly and why the flow cannot be run backwards.
A plucked string keeps its corners
Heat smooths a sharp profile at once, because each harmonic decays at a rate set by the square of its frequency. Change one time derivative into two and nothing decays at all: each harmonic swings for ever, the corner of a pluck splits in two and runs along the string, and after one period the shape comes back exactly. The same sines, the same coefficients — and a flow that loses nothing.
Named alongside it
The objects these essays reach for when they reach for this one.
Fourier analysisHeat equationIrreversibilitySpectrumDiffusionExponential decayHarmonicsPeriodicitySuperpositionWave equation