2008
DOI: 10.1103/physreve.78.061102
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Universal tree structures in directed polymers and models of evolving populations

Abstract: By measuring or calculating coalescence times for several models of coalescence or evolution, with and without selection, we show that the ratios of these coalescence times become universal in the large size limit and we identify a few universality classes.

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Cited by 23 publications
(34 citation statements)
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“…A particular -coalescent, usually called the Bolthausen-Sznitman coalescent, is thought to be an important object for describing the conjectured universal ultrametric structure of numerous mean-field spin glass models including the Sherrington-Kirkpatrick model (see [12,13,38]). The same coalescent has also been recently linked in [15] to scaling limits of directed polymers.…”
Section: Motivation and Main Resultsmentioning
confidence: 87%
See 1 more Smart Citation
“…A particular -coalescent, usually called the Bolthausen-Sznitman coalescent, is thought to be an important object for describing the conjectured universal ultrametric structure of numerous mean-field spin glass models including the Sherrington-Kirkpatrick model (see [12,13,38]). The same coalescent has also been recently linked in [15] to scaling limits of directed polymers.…”
Section: Motivation and Main Resultsmentioning
confidence: 87%
“…Recall the martingales (15). On the event As in (25), Doob's maximal inequality yields that for large enough n…”
Section: Lemma 52 For Any T > 0 We Have That Z (T) − → ∞ Almost Surementioning
confidence: 99%
“…These rates satisfy a self-consistency relation l b;k ¼ l bþ1;k þ l bþ1;kþ1 (see Pitman 1999;Sagitov 1999;Schweinsberg 2000;Brunet et al 2008). For the Moran model, we have for all b $ 2;…”
Section: B Coalescence Ratesmentioning
confidence: 99%
“…1. BBM is a prototypical model of evolution, but has also been extensively used as a simple model for reaction-diffusion systems, disordered systems, nuclear reactions, cosmic ray showers, epidemic spreads amongst others [20][21][22][23][24][25][26][27][28][29][30][31][32][33][34]. In one dimension, the position of the existing particles at time t constitute a set of strongly correlated variables that are naturally ordered according to their positions on the line with x 1 (t) > x 2 (t) > x 3 (t) .…”
mentioning
confidence: 99%