Lebesgue constant
Named by 2 essays across one field — each of them below, with the objects they name alongside it.
The ripples that make a series run away
Adding up the first N terms of a Fourier series is the same as averaging the function against one fixed wiggly curve. Its area is always one, but the area of its absolute value grows like the logarithm of N, without limit — and that single number is enough to force a continuous function, with no jump and no corner anywhere, whose Fourier series diverges at a point. Averaging the partial sums removes the negative ripples, and with them the whole problem.
The best nodes have no formula
Interpolating through n points magnifies any error in the data by at most the Lebesgue constant of the points. Chebyshev's points keep it near (2/π)·log n; stretching them to the ends of the interval brings it within two hundredths of the best possible; and the best possible points, characterised in 1978 by having every bump of the error curve the same height, have never been given a formula.
Named alongside it
The objects these essays reach for when they reach for this one.
Cesaro summationChebyshev nodesConditioningContinuityConvergenceCounterexampleDirichlet kernelEquioscillationFourier analysisGrowth rateInterpolationPolynomial approximation