Tuesday, 29 March 2011

pr.probability - diameter of a graph with random edge weights

The diameter is defined as d(G)=supx,yinGinfgammasumeingammawe,

where the infimum is over all paths gamma connecting x to y, and the sum is over the edges e which gamma crosses. The graph structure is very crucial to this problem. If the graph is very connected (as in your example), then the diameter is essentially the maximum value of the variables wi. A large fluctuation of a single wi will cause the diameter to be very large.



On the other hand, if you're dealing with something more like a lattice (e.g., a large, finite subset of mathbbZ2), then the diameter is a combination of many independent random variables. Large fluctuations of any single variable will be muted and not affect the diameter much, and limit theorems will apply. A variant of Kingman's subadditive ergodic theorem will show that d(G)simd(G).



Questions like this are very much in the realm of first-passage percolation. Check out this survey by Howard, as well as this one by Blair-Stahn on the arXiv.

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