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Global well-posedness and relaxation for solutions of the Fokker-Planck-Alignment equations

R. Shvydkoy

Abstract

In this paper we prove global existence of weak solutions, their regularization, and global relaxation to Maxwellian for a broad class of Fokker-Planck-Alignment models which appear in collective dynamics. The main feature of these results, as opposed to previously known ones, is the lack of regularity or no-vacuum requirements on the initial data. With a particular application to the classical kinetic Cucker-Smale model, we demonstrate that any bounded data with finite energy, $(1+ |v|^2) f_0 \in L^1$, $f_0 \in L^\infty$, and finite higher moment $|v|^q f\in L^2$, $q \gg 2$, gives rise to a global instantly smooth solution, satisfying entropy equality and relaxing exponentially fast. The results are achieved through the use of a new thickness-based renormalization, which circumvents the problem of degenerate diffusion in non-perturbative regime.

Global well-posedness and relaxation for solutions of the Fokker-Planck-Alignment equations

Abstract

In this paper we prove global existence of weak solutions, their regularization, and global relaxation to Maxwellian for a broad class of Fokker-Planck-Alignment models which appear in collective dynamics. The main feature of these results, as opposed to previously known ones, is the lack of regularity or no-vacuum requirements on the initial data. With a particular application to the classical kinetic Cucker-Smale model, we demonstrate that any bounded data with finite energy, , , and finite higher moment , , gives rise to a global instantly smooth solution, satisfying entropy equality and relaxing exponentially fast. The results are achieved through the use of a new thickness-based renormalization, which circumvents the problem of degenerate diffusion in non-perturbative regime.
Paper Structure (18 sections, 29 theorems, 327 equations, 1 table)

This paper contains 18 sections, 29 theorems, 327 equations, 1 table.

Key Result

Theorem 1.1

If the kernel is fat tail, $\int_0^\infty \phi(r) \, \hbox{d}r = \infty$, then solutions to e:CS align exponentially fast to the conserved mean velocity $\bar{v} = \frac{1}{ \sum_{j=1}^N m_j} \sum_{j=1}^N m_j v_j$, while the flock remains bounded where $C,\delta,\bar{D}$ depend only on the initial condition and parameters of the kernel.

Theorems & Definitions (53)

  • Theorem 1.1: CS2007aCS2007bHT2008HL2009
  • Theorem 1.2
  • Definition 2.1
  • Remark 2.2
  • Theorem 2.3: S-EA
  • Remark 2.4
  • Definition 2.5
  • Lemma 2.6
  • proof
  • Remark 2.7
  • ...and 43 more