文摘
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, the 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.