2018
DOI: 10.3934/krm.2018025
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Propagation of stretched exponential moments for the Kac equation and Boltzmann equation with Maxwell molecules

Abstract: We study the spatially homogeneous Boltzmann equation for Maxwell molecules, and its 1-dimensional model, the Kac equation. We prove propagation in time of stretched exponential moments of their weak solutions, both for the angular cutoff and the angular non-cutoff case. The order of the stretched exponential moments in question depends on the singularity rate of the angular kernel of the Boltzmann and the Kac equation. One of the main tools we use are Mittag-Leffler moments, which generalize the exponential o… Show more

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Cited by 14 publications
(7 citation statements)
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“…In particular, exponential moments of order γ are shown to generate in a finite time, while Gaussian moments propagate if initially are finite, which holds independently of γ. Moreover, all these result were generalized when the angular part is not integrable (in the angular non-cutoff regime) [41,30,16,37,2].…”
Section: Introductionmentioning
confidence: 88%
“…In particular, exponential moments of order γ are shown to generate in a finite time, while Gaussian moments propagate if initially are finite, which holds independently of γ. Moreover, all these result were generalized when the angular part is not integrable (in the angular non-cutoff regime) [41,30,16,37,2].…”
Section: Introductionmentioning
confidence: 88%
“…The generation results were improved to obtain exponential moments of order γ, while Gaussian moments were propagated for any initial data that would have that property, independent of γ. All these results were extended to the angular noncutoff regime (lack of angular integrability) in [21,15] still for hard potentials with γ ∈ (0, 2], and in [7,18] for pseudo-Maxwellian and Maxwellian case (γ = 0). In the later referenced work, these non-Gaussian tailed moments are called Mittag-Leffler moments as in fact the summability of partial sums is shown to converge to an L 1 -Mittag-Leffler function weighted norm for the unique probability density function solving the initial value problem associated to the Boltzmann equation, whose order and rate depend on the initial data as much as on the order of singularity in the angular section.…”
Section: Introductionmentioning
confidence: 92%
“…This yields Theorem 1.2 (a). It is worth mentioning that the derivation of exponential bounds for solutions to kinetic equations is a very active field of research nowadays, in particular for Boltzmann equations, see [1,11,10,17,18] and the references therein. Finally, we sketch in Section 5 the computations leading to the explicit solutions given in Proposition 1.1.…”
Section: 2)mentioning
confidence: 99%