Abstract

We show that in preferential attachment models with power-law exponent τ∈(2,3)τ\in(2,3) the distance between randomly chosen vertices in the giant component is asymptotically equal to (4+o(1)) log⁡log⁡N−log⁡(τ−2)(4+o(1))\, \frac{\log\log N}{-\log (τ-2)}, where NN denotes the number of nodes. This is twice the value obtained for several types of configuration models with the same power-law exponent. The extra factor reveals the different structure of typical shortest paths in preferential attachment graphs.

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