Topics in stochastic processes with special reference to first passage percolation theory
<p>First passage percolation theory in its most general form is the randomised version of the well-known shortest route problem. It thus has several important physical applications. Ordinary percolation theory is but a special case of this more general problem which we formulate as follows. &l...
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Format: | Thesis |
Sprog: | English |
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1964
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author | Welsh, JAD |
author2 | Hammersley, JM |
author_facet | Hammersley, JM Welsh, JAD |
author_sort | Welsh, JAD |
collection | OXFORD |
description | <p>First passage percolation theory in its most general form is the randomised version of the well-known shortest route problem. It thus has several important physical applications. Ordinary percolation theory is but a special case of this more general problem which we formulate as follows. </p>
<p>To each arc of an arbitrary, countably infinite, connected graph we independently assign a non-negative random variable called the time coordinate of that arc. This assignment of random variables induces a time state 'w' on g. The 'length' of any path of g is the sum of the time coordinates of its component arcs.</p>
<p>[This abstract continues in the thesis file.]</p> |
first_indexed | 2024-03-07T08:25:56Z |
format | Thesis |
id | oxford-uuid:4787cf63-9e81-4d9c-a49b-d7ccae6286f3 |
institution | University of Oxford |
language | English |
last_indexed | 2024-03-07T08:25:56Z |
publishDate | 1964 |
record_format | dspace |
spelling | oxford-uuid:4787cf63-9e81-4d9c-a49b-d7ccae6286f32024-02-15T14:29:56ZTopics in stochastic processes with special reference to first passage percolation theoryThesishttp://purl.org/coar/resource_type/c_db06uuid:4787cf63-9e81-4d9c-a49b-d7ccae6286f3EnglishHyrax Deposit1964Welsh, JADHammersley, JM<p>First passage percolation theory in its most general form is the randomised version of the well-known shortest route problem. It thus has several important physical applications. Ordinary percolation theory is but a special case of this more general problem which we formulate as follows. </p> <p>To each arc of an arbitrary, countably infinite, connected graph we independently assign a non-negative random variable called the time coordinate of that arc. This assignment of random variables induces a time state 'w' on g. The 'length' of any path of g is the sum of the time coordinates of its component arcs.</p> <p>[This abstract continues in the thesis file.]</p> |
spellingShingle | Welsh, JAD Topics in stochastic processes with special reference to first passage percolation theory |
title | Topics in stochastic processes with special reference to first passage percolation theory |
title_full | Topics in stochastic processes with special reference to first passage percolation theory |
title_fullStr | Topics in stochastic processes with special reference to first passage percolation theory |
title_full_unstemmed | Topics in stochastic processes with special reference to first passage percolation theory |
title_short | Topics in stochastic processes with special reference to first passage percolation theory |
title_sort | topics in stochastic processes with special reference to first passage percolation theory |
work_keys_str_mv | AT welshjad topicsinstochasticprocesseswithspecialreferencetofirstpassagepercolationtheory |