Table of Contents
Fetching ...

Supercritical McKean-Vlasov SDE driven by cylindrical $α$-stable process

Zimo Hao, Chongyang Ren, Mingyan Wu

Abstract

In this paper, we study the following supercritical McKean-Vlasov SDE, driven by a symmetric non-degenerate cylindrical $α$-stable process in $\mathbb{R}^d$ with $α\in (0,1)$: $$ \mathord{\rm d} X_t = (K * μ_{t})(X_t)\mathord{\rm d}t + \mathord{\rm d} L_t^{(α)}, \quad X_0 = x \in \mathbb{R}^d, $$ where $K: \mathbb{R}^d \to \mathbb{R}^d$ is a $β$-order Hölder continuous function, and $μ_t$ represents the time marginal distribution of the solution $X$. We establish both strong and weak well-posedness under the conditions $β\in (1 - α/2, 1)$ and $β\in (1 - α, 1)$, respectively. Additionally, we demonstrate strong propagation of chaos for the associated interacting particle system, as well as the convergence of the corresponding Euler approximations. In particular, we prove a commutation property between the particle approximation and the Euler approximation.

Supercritical McKean-Vlasov SDE driven by cylindrical $α$-stable process

Abstract

In this paper, we study the following supercritical McKean-Vlasov SDE, driven by a symmetric non-degenerate cylindrical -stable process in with : where is a -order Hölder continuous function, and represents the time marginal distribution of the solution . We establish both strong and weak well-posedness under the conditions and , respectively. Additionally, we demonstrate strong propagation of chaos for the associated interacting particle system, as well as the convergence of the corresponding Euler approximations. In particular, we prove a commutation property between the particle approximation and the Euler approximation.

Paper Structure

This paper contains 26 sections, 23 theorems, 235 equations, 1 figure.

Key Result

Theorem 3

Assume that $\alpha \in (0,1)$, $T>0$, and (H$^\beta_b$) holds for some $\beta\in(1-\alpha,1)$. Then for any $\mu_0\in{\mathcal{P}}({\mathbb R}^d)$, there is a unique weak solution to DDSDE DDSDE, and a unique martingale solution ${\mathbb P}\in{\mathscr M}^{b}_{\mu_0}$ in the sense of martsol. More

Figures (1)

  • Figure 1: Propagation of chaos and Euler's approximations

Theorems & Definitions (45)

  • Definition 1: Weak solution
  • Definition 2: Strong solution
  • Theorem 3: Well-posedness
  • Theorem 4: Weak approximations I
  • Theorem 5: Weak approximations II
  • proof : Proof of \ref{['thm:appro1']} and \ref{['thm:appro1-1']}
  • Theorem 6: Strong approximations
  • proof
  • Definition 7: Besov space
  • Lemma 8: Bernstein's inequality
  • ...and 35 more