2002
DOI: 10.1103/physreve.66.066111
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Dynamics of ballistic annihilation

Abstract: The problem of ballistically controlled annihilation is revisited for general initial velocity distributions and arbitrary dimension. An analytical derivation of the hierarchy equations obeyed by the reduced distributions is given, and a scaling analysis of the corresponding spatially homogeneous system is performed. This approach points to the relevance of the non-linear Boltzmann equation for dimensions larger than one and provides expressions for the exponents describing the decay of the particle density n(… Show more

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Cited by 35 publications
(113 citation statements)
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“…We demonstrate that for arbitrarily short but finite times the limit of the empirical density is not consistent with the mean-field theory. This shows that further assumptions are needed in the informal justification of the gainless Boltzmann equation in [PTD02]. In the proof we insert an additional layer between the single-body densities and the Nbody evolution: The probability distribution of trees which encode the collision history of the individual particles.…”
Section: V) (4)mentioning
confidence: 99%
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“…We demonstrate that for arbitrarily short but finite times the limit of the empirical density is not consistent with the mean-field theory. This shows that further assumptions are needed in the informal justification of the gainless Boltzmann equation in [PTD02]. In the proof we insert an additional layer between the single-body densities and the Nbody evolution: The probability distribution of trees which encode the collision history of the individual particles.…”
Section: V) (4)mentioning
confidence: 99%
“…Kinetic annihilation dynamics can be used to model growth and coarsening of surfaces, see [KS88], and has been studied extensively in the physics literature, see [EF85,Pia95,DFPR95,PTD02,CDPTW03].…”
Section: V) (4)mentioning
confidence: 99%
“…Such points, that can be coined "isobestic", have already been observed in a different context (see e.g. section IV-E in reference [41]), where their occurrence could not be rationalized.…”
Section: Discussionmentioning
confidence: 99%
“…Once Γ(θ) is known from DSMC measurements, one can construct a simple graphical method for solving (41) and classifying its possible solutions for different values of θ and α. Here we discuss only the ν models with σ = 1.…”
Section: Substitution Of F (C) = δ(C)+h(c) In the Collision Kernel Ofmentioning
confidence: 99%
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