Constrained minimisation — where it appears
Named by 8 essays across 4 fields — each of them below, with the objects they name alongside it.
The zero that is not a missing entry
A constrained minimisation produces a matrix with a zero block, and the zero is a theorem rather than a sparsity pattern. No pivot order makes it positive definite, no precision changes that, and Cholesky does not fail somewhere on it — it fails at the first constraint row, on a number the problem already contained.
Two ways to remove a constraint
A constrained system can be reduced by eliminating the multipliers or by eliminating the constrained directions. Both give the same answer in exact arithmetic and inherit different condition numbers — one of them squares the constraint's, and the other does not contain it at all.
When symmetry is not enough
The matrix [[0, 1], [1, 0]] is symmetric, nonsingular and perfectly conditioned, and there is no diagonal entry to pivot on. Every factorisation restricted to symmetric interchanges and one-by-one pivots fails on it, at any depth of searching, because every entry it could search is zero. The repair is to take two variables at once.
The basis nobody chose on purpose
A method that eliminates a constraint has to pick a basis for its null space, and every basis is correct. Their condition numbers are eight orders apart, the reduced problem inherits the square, and the choice is usually made by a one-line rule nobody thought of as a numerical decision.
A minimum the Hessian cannot see
A Hessian with four negative eigenvalues can sit at a constrained minimum, and a Cholesky of it stops at the third row. One symmetric indefinite factorisation of the saddle-point matrix settles the question anyway — ten positive pivots and four negative — without a basis for the null space ever being formed. The count is exact in the algebra and blind in floating point, in a band that grows like κ(A)²; the route through the null space is blind in one that grows like κ(A).
A shift that certifies a saddle
On a constrained problem whose Hessian has four negative eigenvalues, a saddle-point matrix is quasi-definite only once H + δI is positive definite — past δ = 5.08 here. Its pivot signs then count the curvature of ZᵀHZ + δI rather than of ZᵀHZ, so a saddle with a negative curvature of −1 is certified a minimum from δ = 1.05 on, and every saddle shallower than δ goes the same way. Iterative refinement against the unregularised matrix keeps the second-order test the count gave up: it contracts on the minimum at δ/(μ + δ), 0.980 a step at δ = 5, and on the saddle it grows at exactly 1.25.
The formula that was already optimal
Ask for the interpolation that minimises the energy of its own columns and the answer is the classical AMG formula — to zero at every row of the one-dimensional Laplacian, and to four digits in two dimensions. On the operator rotated to 45° the two part company, and the gap between them is a diagnostic that needs no reference solution.
The shift that stops at the first right count
A nonconvex solver that finds the wrong inertia adds δI to H and tries again, and the δ it settles on is used as though it measured the curvature it corrects. It does not. On a well-conditioned constraint it is the schedule's number — 1.8·10⁴ times the need at a curvature of 5.6·10⁻⁹, between one and 7.3 times above 10⁻² — and on an ill-conditioned one the loop stops wherever the count first reads right: 63 of 152 saddles at κ(A) = 10⁸, the deepest with curvature 56. Refining the shift by bisection removes the first error and adds to the second.
Named alongside it
The objects these essays reach for when they reach for this one.
Saddle-point systemsCondition numberIndefinite matrixReduced hessianInertiaLDLᵀ factorisationBunch–KaufmanCertificateSchur complementCholeskyNull-spaceNull-space method