Large deviations for empirical path measures in cycles of integer partitions

dc.creatorAdams, Stefan
dc.date2007-02-02
dc.date2007-02-05
dc.date.accessioned2026-07-07T07:44:31Z
dc.date.available2026-07-07T07:44:31Z
dc.descriptionConsider a large system of $N$ Brownian motions in $\mathbb{R}^d$ on some fixed time interval $[0,β]$ with symmetrised initial-terminal condition. That is, for any $i$, the terminal location of the $i$-th motion is affixed to the initial point of the $σ(i)$-th motion, where $σ$ is a uniformly distributed random permutation of $1,...,N$. In this paper, we describe the large-N behaviour of the empirical path measure (the mean of the Dirac measures in the $N$ paths) when $ Λ\uparrow\mathbb{R}^d $ and $ N/|Λ|\toρ$. The rate function is given as a variational formula involving a certain entropy functional and a Fenchel-Legendre transform. Depending on the dimension and the density $ ρ$, there is phase transition behaviour for the empirical path measure. For certain parameters (high density, large time horizon) and dimensions $ d\ge 3 $ the empirical path measure is not supported on all paths $ [0,\infty)\to\mathbb{R}^d $ which contain a bridge path of any finite multiple of the time horizon $ [0,β] $. For dimensions $ d=1,2 $, and for small densities and small time horizon $ [0,β] $ in dimensions $ d\ge 3$, the empirical path measure is supported on those paths. In the first regime a finite fraction of the motions lives in cycles of infinite length. We outline that this transition leads to an empirical path measure interpretation of {\it Bose-Einstein condensation}, known for systems of Bosons.
dc.identifierhttps://arxiv.org/abs/math/0702053
dc.identifierhttp://arxiv.org/abs/math/0702053
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/123226
dc.subjectProbability
dc.subjectMathematical Physics
dc.subject60F10; 60J65; 82B10; 82B26
dc.titleLarge deviations for empirical path measures in cycles of integer partitions
dc.typetext

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