2018
DOI: 10.1137/17m1117926
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On Mittag-Leffler Moments for the Boltzmann Equation for Hard Potentials Without Cutoff

Abstract: We establish the L 1 weighted propagation properties for solutions of the Boltzmann equation with hard potentials and non-integrable angular components in the collision kernel. Our method identifies null forms by angular averaging and deploys moment estimates of solutions to the Boltzmann equation whose summability is achieved by introducing the new concept of Mittag-Leffler moments -extensions of L 1 exponentially weighted norms. Such L 1 weighted norms of solutions to the Boltzmann equation are, both, genera… Show more

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Cited by 23 publications
(41 citation statements)
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References 31 publications
(63 reference statements)
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“…(v) The non-cutoff Boltzmann equation for hard potentials γ > 0 was studied in [11] where generation of stretched exponential moments of order s = γ was proved, and [13] where propagation of stretched exponential moments was proved depending on the singularity rate of the angular kernel. We extend the work of [13] to include the case γ = 0.…”
Section: The Main Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…(v) The non-cutoff Boltzmann equation for hard potentials γ > 0 was studied in [11] where generation of stretched exponential moments of order s = γ was proved, and [13] where propagation of stretched exponential moments was proved depending on the singularity rate of the angular kernel. We extend the work of [13] to include the case γ = 0.…”
Section: The Main Resultsmentioning
confidence: 99%
“…Finiteness of such sums can be studied by proving term-by-term geometric decay, or by showing that partial sums are uniformly bounded. Our proof is inspired by the works [1,13], where the partial sum approach is developed. Moreover, motivated by [13], we exploit the notion of Mittag-Leffler moments, which serve as a generalization of stretched exponential moments and which are very flexible for the calculations at hand.…”
Section: Introductionmentioning
confidence: 99%
“…Proof. We briefly point out that the main steps in the proofs are adaption of the proof given in [21]. Let us consider polynomial moment m δq [F](t) =: m δq , 0 < δ ≤ 2, q ≥ 0, and derive an ODI for it starting from (6.5) with k = δq.…”
Section: Generation and Propagation Of Exponential Momentsmentioning
confidence: 99%
“…We refer to [30] for a review of the classical results, as well as to e.g. [3,5,17,25,27] and references therein. The rough picture is that, for hard potentials (including hard spheres), the space homogeneous Boltzmann equation generates higher-order moments instantaneously as soon as the initial energy is finite.…”
Section: Introductionmentioning
confidence: 99%