Numerical Linear Algebra
where the algebra stops being the arithmetic
Concept

Conductance — where it appears

The weight of edges leaving a set of vertices, divided by the total degree on the smaller side. It is the quantity a spectral partition is trying to minimise, and unlike an eigenvalue it is a property of the answer rather than of the matrix.

Named by 5 essays across one field — each of them below, with the objects they name alongside it.

10⁻³10⁻²10⁻¹110¹12345678910conductance, and the two bounds on itpathcyclegridbarbelltwo blockshypercubepreferentialstarcompletethe bar is the inequalitythe dot is the graph

Two Laplacians of one graph

D − A and D^{-1/2}(D − A)D^{-1/2} are built from the same object, are not similar to each other, and answer different questions. On a graph whose degrees are equal they coincide. On one whose degrees span an order of magnitude their second eigenvalues are sixteen times apart.

graph · graph laplacian 0481216202410⁻²10⁻¹1vertices on the smaller sideconductance of the prefix cut0.00752, the best prefixthe rounding stepλ₂0.14cuts considered23best conductance0.0075at k =12worst prefix1the dashed curve is the eigenvectorthe solid one is what it costs

The vector that has to be rounded

A spectral partition is an eigenvector, and an eigenvector is a real vector. The answer wanted is a subset. Something has to turn one into the other, and the something is a heuristic applied after the linear algebra has finished.

graph · spectral partition 10⁻³10⁻²10⁻¹110¹12345678910conductance, and the two bounds on itpathcyclegridbarbelltwo blockshypercubepreferentialstarcompletethe bar is the inequalitythe dot is the graph

A bound with a square root in it

Cheeger's inequality brackets a graph's best cut between λ₂/2 and √(2λ₂). The lower bound is attained exactly. The upper one is loose by a factor of fourteen — on the one graph in the census with a real bottleneck, which is the shape it is always quoted about.

graph · spectral partition 14710131619110¹indexeigenvalue of Lan eigenvalue with no vectorλ₂0.35λ₃0.35gap1.7·10⁻¹⁵partitions found3best conductance0.045worst0.045two eigenvalues, one valueand the answer is not a function of the graph

A partition decided in the last digit

On a graph with a symmetry there is no Fiedler vector — there is a plane, and every vector in it is an exact eigenvector. Twenty-four runs with the edge weights nudged by 10⁻¹² return ten different partitions of a cycle and, on a hypercube, two different qualities of answer.

graph · spectral partition 0173451688510211910⁻⁶10⁻⁵10⁻⁴10⁻³10⁻²10⁻¹1steps of the walkdistance from stationarya rate read as a timeλ₂ of the walk0.9steps measured122steps predicted131ratio0.93the dashed line is the eigenvaluethe curve is the walk

The rate is the second eigenvalue

A walk forgets where it started at a rate the graph's second eigenvalue names exactly. Across three orders of magnitude in the step count the prediction is five per cent high — and the published rate for PageRank is right for a reason nobody states, which is that a link graph is in pieces.

graph · random walk

Named alongside it

The objects these essays reach for when they reach for this one.

Algebraic connectivityFiedler vectorNormalised laplacianSpectral partitionCheeger inequalityGraph automorphismRelaxationSweep cutBipartiteBound tightnessCombinatorial optimumDegree sequence

All concepts