Semiconductor Boltzmann-Dirac-Benney equation with BGK-type collision operator: existence of solutions vs. ill-posedness
Marcel Braukhoff

TL;DR
This paper studies a semiconductor Boltzmann equation with a complex collision operator, proving local existence of solutions for analytic initial data and demonstrating ill-posedness in Sobolev spaces near equilibrium.
Contribution
It establishes local existence of solutions in Gevrey spaces and shows ill-posedness in Sobolev spaces for the semiconductor Boltzmann-Dirac-Benney equation with a singular potential.
Findings
Existence of local analytic solutions for initial data in Gevrey spaces.
Ill-posedness of the equation in Sobolev spaces near Fermi-Dirac equilibrium.
Analysis techniques adapted from Mouhout and Villani for Gevrey norms.
Abstract
A semiconductor Boltzmann equation with a non-linear BGK-type collision operator is analyzed for a cloud of ultracold atoms in an optical lattice: \[ \partial_t f + \nabla_p\epsilon(p)\cdot\nabla_x f - \nabla_x n_f\cdot\nabla_p f = n_f(1- n_f)(\mathcal{F}_f-f), \quad x\in\mathbb{R}^d, p\in\mathbb{T}^d, t>0. \] This system contains an interaction potential being significantly more singular than the Coulomb potential, which is used in the Vlasov-Poisson system. This causes major structural difficulties in the analysis. Furthermore, is the dispersion relation and denotes the Fermi-Dirac equilibrium distribution, which depends non-linearly on in this context. In a dilute plasma - without collisions (r.h.s) - this system is closely related to the Vlasov-Dirac-Benney…
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