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The Boltzmann-Grad Limit of a Hard Sphere System: Analysis of the Correlation Error

Published 19 May 2014 in math-ph, cond-mat.stat-mech, math.AP, and math.MP | (1405.4676v2)

Abstract: We present a quantitative analysis of the Boltzmann-Grad (low-density) limit of a hard sphere system. We introduce and study a set of functions (correlation errors) measuring the deviations in time from the statistical independence of particles (propagation of chaos). In the context of the BBGKY hierarchy, a correlation error of order $k$ measures the event where $k$ particles are connected by a chain of interactions preventing the factorization. We show that, provided $k < \varepsilon{-\alpha}$, such an error flows to zero with the average density $\varepsilon$, for short times, as $\varepsilon{\gamma k}$, for some positive $\alpha,\gamma \in (0,1)$. This provides an information on the size of chaos, namely, $j$ different particles behave as dictated by the Boltzmann equation even when $j$ diverges as a negative power of $\varepsilon$. The result requires a rearrangement of Lanford perturbative series into a cumulant type expansion, and an analysis of many-recollision events.

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