Abstract:We study a non-directed polymer model in random environments. The polymer is modeled by a simple symmetric random walk $S$ on $\mathbb{Z}^d$ with $d\geq2$, and the random environment is modeled by i.i.d. random variables whose tail probability decays polynomially. The interaction between the polymer and the random environment is captured by a Gibbs transform: at time $N$, the law of $S$ is tilted by the factor $\exp(\sum_{x\in\mathcal{R}_N}(\beta\omega_x-h))$, where $\mathcal{R}_N$ is the range of $S$ up to time $N$, $\beta\geq0$ is the inverse temperature, and $h\in\mathbb{R}$ is an external field. By appropriately tuning $\beta=\beta_N$ and $h=h_N$, we establish the phase diagram, analyze the fluctuations of $S$ under the Gibbs transform, and derive the scaling limits of the (logarithmic) partition function. This paper is a follow-up work of arxiv.org/abs/2101.05949. The main novelty and challenge arise from tuning the external field $h$, which brings in various range penalties, unlike in arxiv.org/abs/2101.05949, where $h$ is fixed and serves only as a centering term for the random environment.
From: Ran Wei [view email]
[v1]
Mon, 22 Sep 2025 02:49:37 UTC (32 KB)
[v2]
Thu, 2 Jul 2026 02:06:42 UTC (34 KB)
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