Random walks on small world networks

We study the mixing time of random walks on small-world networks modelled as follows: starting with the 2-dimensional periodic grid, each pair of vertices {𝑢, 𝑣 } with distance 𝑑 > 1 is added as a “long-range" edge with probability proportional to 𝑑−𝑟, where 𝑟 ≥ 0 is a parameter of the model...

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Main Authors: Dyer, ME, Galanis, A, Goldberg, L, Jerrum, M, Vigoda, E
Format: Journal article
Language:English
Published: Association for Computing Machinery 2020
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author Dyer, ME
Galanis, A
Goldberg, L
Jerrum, M
Vigoda, E
author_facet Dyer, ME
Galanis, A
Goldberg, L
Jerrum, M
Vigoda, E
author_sort Dyer, ME
collection OXFORD
description We study the mixing time of random walks on small-world networks modelled as follows: starting with the 2-dimensional periodic grid, each pair of vertices {𝑢, 𝑣 } with distance 𝑑 > 1 is added as a “long-range" edge with probability proportional to 𝑑−𝑟, where 𝑟 ≥ 0 is a parameter of the model. Kleinberg studied a close variant of this network model and proved that the (decentralised) routing time is 𝑂( (log𝑛)2) when 𝑟 = 2 and 𝑛Ω(1) when 𝑟 ≠ 2. Here, we prove that the random walk also undergoes a phase transition at 𝑟 = 2, but in this case the phase transition is of a different form. We establish that the mixing time is Θ(log𝑛) for 𝑟 < 2, 𝑂( (log𝑛)4) for 𝑟 = 2 and 𝑛 Ω(1) for 𝑟 > 2.
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spelling oxford-uuid:20b89e0c-63a0-46eb-bc3d-9b97ab00b0de2022-03-26T11:29:15ZRandom walks on small world networksJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:20b89e0c-63a0-46eb-bc3d-9b97ab00b0deEnglishSymplectic ElementsAssociation for Computing Machinery2020Dyer, MEGalanis, AGoldberg, LJerrum, MVigoda, EWe study the mixing time of random walks on small-world networks modelled as follows: starting with the 2-dimensional periodic grid, each pair of vertices {𝑢, 𝑣 } with distance 𝑑 > 1 is added as a “long-range" edge with probability proportional to 𝑑−𝑟, where 𝑟 ≥ 0 is a parameter of the model. Kleinberg studied a close variant of this network model and proved that the (decentralised) routing time is 𝑂( (log𝑛)2) when 𝑟 = 2 and 𝑛Ω(1) when 𝑟 ≠ 2. Here, we prove that the random walk also undergoes a phase transition at 𝑟 = 2, but in this case the phase transition is of a different form. We establish that the mixing time is Θ(log𝑛) for 𝑟 < 2, 𝑂( (log𝑛)4) for 𝑟 = 2 and 𝑛 Ω(1) for 𝑟 > 2.
spellingShingle Dyer, ME
Galanis, A
Goldberg, L
Jerrum, M
Vigoda, E
Random walks on small world networks
title Random walks on small world networks
title_full Random walks on small world networks
title_fullStr Random walks on small world networks
title_full_unstemmed Random walks on small world networks
title_short Random walks on small world networks
title_sort random walks on small world networks
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AT galanisa randomwalksonsmallworldnetworks
AT goldbergl randomwalksonsmallworldnetworks
AT jerrumm randomwalksonsmallworldnetworks
AT vigodae randomwalksonsmallworldnetworks