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$χ^2$-cut-off phenomenon for Galerkin projections of Fokker-Planck equations with monomial potentials

Benny Avelin, Gerardo Barrera

Abstract

In this manuscript, we establish the existence/non-existence of the cut-off phenomenon for the Langevin-Kolmogorov random dynamics with monomial convex potentials, possible singular, and driven by a Brownian motion with small strength. We consider a truncated $χ^2$-distance, that is, a distance based on Galerkin projections of the eigensystem, and show that not only a refined knowledge of the eigenvalues is needed but also a refined asymptotics of the growth for the eigenfunctions of the Fokker-Planck equations associated to the Langevin-Kolmogorov dynamics. In addition, asymptotics of the mixing times are established.

$χ^2$-cut-off phenomenon for Galerkin projections of Fokker-Planck equations with monomial potentials

Abstract

In this manuscript, we establish the existence/non-existence of the cut-off phenomenon for the Langevin-Kolmogorov random dynamics with monomial convex potentials, possible singular, and driven by a Brownian motion with small strength. We consider a truncated -distance, that is, a distance based on Galerkin projections of the eigensystem, and show that not only a refined knowledge of the eigenvalues is needed but also a refined asymptotics of the growth for the eigenfunctions of the Fokker-Planck equations associated to the Langevin-Kolmogorov dynamics. In addition, asymptotics of the mixing times are established.

Paper Structure

This paper contains 17 sections, 21 theorems, 223 equations, 1 figure.

Key Result

Theorem 1.2

Assume that $\gamma \in (1/3,1)$, $\delta(\varepsilon) = \varepsilon^{\frac{1-\gamma}{1+\gamma}}$, and $n\in \mathbb{N}$. For any $x_0\neq 0$ window cut-off holds true in the sense of eq:def:wcut, where $d_{n,\varepsilon}$ is defined in eq:Ga, $t_\varepsilon$ is defined as the unique solution to in other words, and the time window is given by $w_\varepsilon:= \varepsilon^{\frac{1-\gamma}{1+\gamm

Figures (1)

  • Figure 1: The vector field for the angle ODE \ref{['eq:ODE:theta']} when $\gamma=1/2$ and $g=2$. The blue shaded region depicts the area between $[\theta_l=0,\theta_u]$, and the dotted curve are the asymptotes for the limits $\pi/2$ and $-\pi/2$. The $\omega$-limit is expected to be the set $\{-\pi/2,0,\pi/2\}$.

Theorems & Definitions (43)

  • Remark 1.1: Cut-off phenomenon: window and profile
  • Theorem 1.2: Window cut-off phenomenon for Galerkin projection, $\gamma\in (1/3,1)$
  • Remark 1.3: Explicit asymptotic bounds for the cut-off time for $\gamma\in (1/3,1)$
  • Theorem 1.4: Profile cut-off phenomenon for Galerkin projection, $\gamma\in (0,1/3\rbrack$
  • Remark 1.5: Explicit asymptotic bounds for the cut-off time for $\gamma\in (0,1/3\rbrack$
  • Theorem 1.6: No cut-off phenomenon for Galerkin projection, $\gamma>1$
  • Remark 1.7: Ornstein--Uhlenbeck process
  • Lemma 2.1: Scaling of the spectrum
  • Lemma 2.2: WKB expansion
  • Theorem 2.3: Growth of the eigenfunctions, $\varepsilon=1$ and $\gamma>0$
  • ...and 33 more