Shift selection — where it appears
Named by 3 essays across 3 fields — each of them below, with the objects they name alongside it.
Where to put the poles of a rational function
Three times in one field the same question arrives from different directions — ADI shifts, rational approximation of a square root, the decay of a Gramian — and it has one answer. Cluster them geometrically towards wherever the function is difficult, and the alternative that looks reasonable costs orders.
An error committed before the arithmetic
Before a nonlinear eigenvalue problem is solved, somebody says where they think the eigenvalues are. That sentence sets the accuracy of everything that follows by five orders, costs nothing to say, and cannot be revised once the approximation built on it is in hand.
The push a pivot needs belongs to the matrix
An indefinite factorisation's most negative pivot looks like an estimate of the most negative eigenvalue, and on one planted family Bunch–Kaufman's, pushed a tenth further, was a usable shift for inverse iteration. On thirty random symmetric matrices neither rule's pivot is: unpushed it is nearest the smallest eigenvalue on 12 and 5 of them, pushed a tenth on 13 and 9, and only a push of two serves 29. The push each matrix needs runs from 0.59 to 2.27 for Bunch–Kaufman — whose pivot is more negative than every eigenvalue on eight matrices and under half the smallest on others — and from 0.85 to 2.01 for the bounded rule. What does work needs no push at all: multiply the shift by a quarter until the factorisation of A − σI has no negative pivot, which Sylvester's law says is exactly when σ is below the spectrum. It lands every time, in a median of two or three factorisations.
Named alongside it
The objects these essays reach for when they reach for this one.
Condition numberRational approximationZolotarev numberADI iterationApproximation before linearisationBranch pointBunch–KaufmanEquioscillationGramianInertiaInverse iterationLanczos algorithm