Double root — where it appears
Named by 4 essays across one field — each of them below, with the objects they name alongside it.
Also named here as hyperbolic quadratic — the same set of essays touches all of them, so they are one junction rather than several.
Every eigenvalue real, and a test that says so
A quadratic eigenvalue problem has no reason to have real eigenvalues. One class does, as a property rather than an outcome, and the proof is a Cholesky that completes. The boundary of the class has a closed form, and at the boundary the arithmetic loses half its digits with nothing ill conditioned anywhere.
A class a longer chain takes away
Symmetry survives a bigger problem. Hyperbolicity does not. The damping that certifies a chain of seven masses is refused by a chain of eight, the damping the class demands grows like the length without bound, and the certificate has to be earned again at every size — which costs one Cholesky, and the alternative is a proof quietly inherited from a smaller problem.
A guarantee paid for in digits
A hyperbolic quadratic has a real spectrum, but the route that computed it so far, a companion linearisation and a nonsymmetric Schur form, only happens to return one. The theory offers a route on which it cannot do otherwise: a symmetric linearisation that is a definite pencil, reduced by a Cholesky to a symmetric eigenproblem. Near the class's boundary that guarantee is the expensive route. On a damped chain at damping β*(1 + ε) the definite pencil's Crawford number — what its Cholesky divides by — vanishes like 0.228ε, every combination of the pencil shrinking with it, while the colliding pair the companion route has to resolve separates like 0.98√ε. At ε = 10⁻¹² the definite route keeps two or three digits and the companion route eight or nine. And on twenty rotated chains the companion route returns no complex pair at any margin from 10⁻⁴ to 10⁻¹², only on the boundary itself.
Real or complex by the sign of an error
A hyperbolic quadratic has only real eigenvalues, and an unstructured solver that knows nothing of the class returned a complex pair for one only at the boundary. The prediction was that the first complex pair would appear at a margin between 10⁻¹⁶ and 10⁻¹⁴ above the boundary, where the colliding pair's separation shrinks to the solver's own perturbation of it, and never at 10⁻¹³ or above. Both hold. Below 10⁻¹⁵ the solver returns a complex pair on almost exactly half of a hundred rotated chains — the same at the boundary itself — because its error in the pair's squared separation has the same size at every margin and either sign, and that one distribution, read at the boundary, predicts the whole curve. The structured route that guarantees a real answer loses every digit first.
Named alongside it
The objects these essays reach for when they reach for this one.
Hyperbolic quadraticQuadratic eigenvalue problemCholeskyCondition numberExact ground truthOverdampingDefective matrixInertiaLinearisationBackward errorCompanion formDefinite pencil