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 (propaga- tion 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 < ε−α, such an error flows to zero with the average density ε, for short times, as εγk, for some positive α,γ ∈ (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 ε. The result requires a rearrangement of Lanford perturbative series into a cumulant type expansion, and an analysis of many–recollision events.
The Boltzmann–grad limit of a hard sphere system. Analysis of the correlation error / Pulvirenti, Mario; Simonella, Sergio. - In: INVENTIONES MATHEMATICAE. - ISSN 0020-9910. - 207:3(2017), pp. 1135-1237. [10.1007/s00222-016-0682-4]
The Boltzmann–grad limit of a hard sphere system. Analysis of the correlation error
PULVIRENTI, Mario
;SIMONELLA, SERGIO
2017
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, the correlation errors, measuring the deviations in time from the statistical independence of particles (propaga- tion 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 < ε−α, such an error flows to zero with the average density ε, for short times, as εγk, for some positive α,γ ∈ (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 ε. The result requires a rearrangement of Lanford perturbative series into a cumulant type expansion, and an analysis of many–recollision events.File | Dimensione | Formato | |
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