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Scaling limit of a one-dimensional polymer in a repulsive i.i.d. environment

Nicolas Bouchot

Abstract

The purpose of this paper is to study a one-dimensional polymer penalized by its range and placed in a random environment $ω$. The law of the simple symmetric random walk up to time $n$ is modified by the exponential of the sum of $βω_z - h$ sitting on its range, with~$h$ and $β$ positive parameters. It is known that, at first order, the polymer folds itself to a segment of optimal size $c_h n^{1/3}$ with $c_h = π^{2/3} h^{-1/3}$. Here we study how disorder influences finer quantities. If the random variables $ω_z$ are i.i.d.\ with a finite second moment, we prove that the left-most point of the range is located near $-u_* n^{1/3}$, where $u_* \in [0,c_h]$ is a constant that only depends on the disorder. This contrast with the homogeneous model (i.e. when $β=0$), where the left-most point has a random location between $-c_h n^{1/3}$ and $0$. With an additional moment assumption, we are able to show that the left-most point of the range is at distance $\mathcal U n^{2/9}$ from $-u_* n^{1/3}$ and the right-most point at distance $\mathcal V n^{2/9}$ from $(c_h-u_*) n^{1/3}$. Here again, $\mathcal{U}$ and $\mathcal{V}$ are constants that depend only on $ω$.

Scaling limit of a one-dimensional polymer in a repulsive i.i.d. environment

Abstract

The purpose of this paper is to study a one-dimensional polymer penalized by its range and placed in a random environment . The law of the simple symmetric random walk up to time is modified by the exponential of the sum of sitting on its range, with~ and positive parameters. It is known that, at first order, the polymer folds itself to a segment of optimal size with . Here we study how disorder influences finer quantities. If the random variables are i.i.d.\ with a finite second moment, we prove that the left-most point of the range is located near , where is a constant that only depends on the disorder. This contrast with the homogeneous model (i.e. when ), where the left-most point has a random location between and . With an additional moment assumption, we are able to show that the left-most point of the range is at distance from and the right-most point at distance from . Here again, and are constants that depend only on .
Paper Structure (31 sections, 34 theorems, 251 equations, 2 figures)

This paper contains 31 sections, 34 theorems, 251 equations, 2 figures.

Key Result

Theorem 1.1

For all $h > 0$, define $c_h \vcentcolon= (\pi^2 h^{-1})^{1/3}$. Then, for any $h,\beta>0$, $\mathbb{P}$-almost surely we have the following convergence

Figures (2)

  • Figure 1: A typical trajectory under the polymer measure for a given $u_*$ and large $n$
  • Figure 2: Reflection of the trajectory $b \to (0,b]$ with respect to the horizontal line at $b$

Theorems & Definitions (64)

  • Theorem 1.1: berger2020one
  • Theorem 1.2: bouchot1
  • Theorem 1.3
  • Proposition 1.4
  • proof
  • Definition 1.1
  • Proposition 1.5
  • Theorem 1.6
  • Conjecture 1.7
  • proof : Proof of Theorem \ref{['th-1/6']}-\ref{['eq:th-1/6-part']}
  • ...and 54 more