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How to simulate Lévy flights in a steep potential: An explicit splitting numerical scheme

Ilya Pavlyukevich, Olga Aryasova, Alexei Chechkin, Oleksii Kulyk

TL;DR

This work addresses numerical simulation of Lévy-driven SDEs with superlinear drift in steep confining potentials, where classical Euler methods can explode or misrepresent moments. It introduces a direct splitting scheme that decouples the deterministic drift flow from the stochastic jump part, ensuring boundedness and exact-like preservation of moments up to order just below the tail index (e.g., q < 9 for Cauchy noise). An error analysis on linear systems demonstrates superior stability and moment accuracy over Euler and reverse splitting, especially in stiff regimes, and the general formulation extends to multi-dimensional settings with convergence guarantees. The paper also presents ready-to-use examples with explicit drift flows, enabling practical implementation across a range of nonlinear, heavy-tailed systems, and provides rigorous conditions under which convergence holds. Overall, the direct splitting approach delivers stable, tail-preserving simulations of Lévy flights in steep potentials with broad applicability and improved reliability for moment and autocorrelation estimation.

Abstract

We propose an effective explicit numerical scheme for simulating solutions of stochastic differential equations with confining superlinear drift terms, driven by multiplicative heavy-tailed Lévy noise. The scheme is designed to prevent explosion and accurately capture all finite moments of the solutions. In the purely Gaussian case, it correctly reproduces moments of sub-Gaussian tails of the solutions. This method is particularly well-suited for approximating statistical moments and other probabilistic characteristics of Lévy flights in steep potential landscapes.

How to simulate Lévy flights in a steep potential: An explicit splitting numerical scheme

TL;DR

This work addresses numerical simulation of Lévy-driven SDEs with superlinear drift in steep confining potentials, where classical Euler methods can explode or misrepresent moments. It introduces a direct splitting scheme that decouples the deterministic drift flow from the stochastic jump part, ensuring boundedness and exact-like preservation of moments up to order just below the tail index (e.g., q < 9 for Cauchy noise). An error analysis on linear systems demonstrates superior stability and moment accuracy over Euler and reverse splitting, especially in stiff regimes, and the general formulation extends to multi-dimensional settings with convergence guarantees. The paper also presents ready-to-use examples with explicit drift flows, enabling practical implementation across a range of nonlinear, heavy-tailed systems, and provides rigorous conditions under which convergence holds. Overall, the direct splitting approach delivers stable, tail-preserving simulations of Lévy flights in steep potentials with broad applicability and improved reliability for moment and autocorrelation estimation.

Abstract

We propose an effective explicit numerical scheme for simulating solutions of stochastic differential equations with confining superlinear drift terms, driven by multiplicative heavy-tailed Lévy noise. The scheme is designed to prevent explosion and accurately capture all finite moments of the solutions. In the purely Gaussian case, it correctly reproduces moments of sub-Gaussian tails of the solutions. This method is particularly well-suited for approximating statistical moments and other probabilistic characteristics of Lévy flights in steep potential landscapes.

Paper Structure

This paper contains 9 sections, 135 equations, 10 figures.

Figures (10)

  • Figure 1: A sample path of a Cauchy process $Z$ on the time grid $\{kh\}_{k\in\mathbb{N}_0}$, $h=10^{-3}$.
  • Figure 2: The absolute moments of the limit distribution $\mathbf{E} |X_\infty|^q$, $q\in[0,9)$.
  • Figure 3: The blow up of the explicit Euler scheme after a large jump at time $k_*h=2.837$; $h=10^{-3}$, $x=0$.
  • Figure 4: Relative number of stable paths of $X^{\mathrm{E},h}_{kh}$, $kh\leq t$, for the explicit Euler scheme for $h=10^{-3}$, $h=10^{-4}$, $h=10^{-5}$, $N=10^6$, $x=0$, $t\in[0,20]$, and their approximations \ref{['e:stable']} on the time interval $t\in[0,30]$ (dashed).
  • Figure 5: "Available-case" empirical absolute moments of the Euler scheme, $h=10^{-5}$, $N=10^6$, $x=0$, calculated from $N_\mathrm{ac}\approx 5\cdot 10^5$ non-exploding trajectories on the interval $kh\in [0,5]$. The dashed lines represent the corresponding moments of the limit distribution $X_\infty$.
  • ...and 5 more figures

Theorems & Definitions (21)

  • Example 6.1: Parabolic potential
  • Example 6.2: Symmetric steep one-well potential, $d=1$
  • Example 6.3: Symmetric steep double-well potential, $d=1$
  • Example 6.4: Symmetric steep one-well potential with "quadratic" minumum, $d=1$
  • Example 6.5: Asymmetric quartic one-well potential with a cubic term, $d=1$
  • Example 6.6: Asymmetric steep potentials, $d=1$
  • Example 6.7: Nonlinear friction models
  • Example 6.8: Random motion in a rough potential, $d=1$
  • Example 6.9: Rotationally invariant $d$-dimensional potential
  • Example 6.10: Diagonal $d$-dimensional potential
  • ...and 11 more