Rank — where it appears
Named by 10 essays across 5 fields — each of them below, with the objects they name alongside it.
A matrix that depends on its own eigenvalue
A damped structure does not produce Ax = λx. It produces (λ²M + λC + K)x = 0, where the matrix whose null vector is wanted is a function of the number being solved for — so there is nothing to factorise, an n × n problem has 2n answers, and the eigenvectors cannot be a basis.
A model that is a rational function
A state matrix has a hundred thousand rows and the thing anyone wants from it is a function of one complex variable. The number that says how much of that size was ever the complexity is a rank — and the rank a derivation writes down cannot be computed, while one built from samples alone can.
The number that decides nothing
The determinant is the first scalar anybody attaches to a matrix and the last one worth consulting. A tenth of the identity has a determinant of 10⁻⁶⁰ and a condition number of exactly one. The Hilbert matrix's determinant stops being right at n = 13 and stops being a number at n = 29, and nothing in between reports either.
Counting what is inside a circle
A trace of a matrix nobody wants to form, integrated around a contour, gives an integer — how many eigenvalues are inside. It converges exponentially, it is estimated with random probes, and the probe block is a ceiling that the answer does not mention.
A ceiling with a knob on it
A contour method returns at most as many eigenvalues as its probe block has columns, and the object that comes back does not distinguish that from having found everything. One line of the derivation multiplies the ceiling by a number the caller chooses, and it costs no extra solves at all.
A rank that depends on the thread count
One 60 × 14 matrix, one threshold, seven partitionings of the inner products that build its Gram matrix — and numerical ranks of 12, 12, 12, 10, 10, 11 and 11. Not a digit of an answer: the number of columns a model built from this matrix would have.
The conditioning that rises with the ceiling
Higher moments multiply a contour method's ceiling by K and grade its block Hankel over ρ to the 2K, so the two knobs are the same knob. One division per quadrature point separates them, and the measurement of what it is worth grows from twenty to twenty thousand.
The split nobody is in a position to choose
Hutch++ spends two thirds of its budget on a sketch and a third on probes, and the third is published as a constant. Swept across six rates of spectral decay at a fixed budget of 48 products, the best share is 0.45 on the fastest and 0.00 on the slowest — sketch nothing at all — and the published third costs between 1.09 and 4.11 times the best error. The decay that decides it is readable from the sketch's own singular values, for products the estimator was going to spend anyway.
One mass removed, and one eigenvalue gone
A coordinate with no inertia reads like a coordinate that has been deleted, and a chain of eight masses with one of them removed would then be a chain of seven, with fourteen eigenvalues. It has fifteen. The massless coordinate is still there, still carrying a damper, and it contributes a first-order equation rather than none.
Where a contour's budget should go
A contour method's ceiling is the number of probes times the number of moments, and the moments are free in solves while the probes are not. Four ways of reaching one ceiling come out four orders apart, the ordering is not monotone, and what separates the best two is not the usual draw but the unlucky one.
Named alongside it
The objects these essays reach for when they reach for this one.
Exact ground truthNumerical rankCondition numberContour integralNonlinear eigenvalue problemQuadratureContour eigensolverMomentRandom probeSingular valuesComplex arithmeticDeterminant