{ "id": "2102.07135", "version": "v1", "published": "2021-02-14T12:12:15.000Z", "updated": "2021-02-14T12:12:15.000Z", "title": "Nested Closed Paths in Two-Dimensional Percolation", "authors": [ "Yu-Feng Song", "Xiao-Jun Tan", "Xin-Hang Zhang", "Jesper Lykke Jacobsen", "Bernard Nienhuis", "Youjin Deng" ], "comment": "5 pages, 5 figures plus supplemental material, 1 page 2 figures", "categories": [ "cond-mat.stat-mech" ], "abstract": "For two-dimensional percolation on a domain with the topology of a disc, we introduce a nested-path operator (NP) and thus a continuous family of one-point functions $W_k \\equiv \\langle \\mathcal{R} \\cdot k^\\ell \\rangle $, where $\\ell$ is the number of independent nested closed paths surrounding the center, $k$ is a path fugacity, and $\\mathcal{R}$ projects on configurations having a cluster connecting the center to the boundary. At criticality, we observe a power-law scaling $W_k \\sim L^{X_{\\rm NP}}$, with $L$ the linear system size, and we determine the exponent $X_{\\rm NP}$ as a function of $k$. On the basis of our numerical results, we conjecture an analytical formula, $X_{\\rm NP} (k) = \\frac{3}{4}\\phi^2 -\\frac{5}{48}\\phi^2/ (\\phi^2-\\frac{2}{3})$ where $k = 2 \\cos(\\pi \\phi)$, which reproduces the exact results for $k=0,1$ and agrees with the high-precision estimate of $X_{\\rm NP}$ for other $k$ values. In addition, we observe that $W_2(L)=1$ for site percolation on the triangular lattice with any size $L$, and we prove this identity for all self-matching lattices.", "revisions": [ { "version": "v1", "updated": "2021-02-14T12:12:15.000Z" } ], "analyses": { "subjects": [ "82B43", "60K35" ], "keywords": [ "two-dimensional percolation", "nested closed paths surrounding", "nested-path operator", "one-point functions", "path fugacity" ], "note": { "typesetting": "TeX", "pages": 5, "language": "en", "license": "arXiv", "status": "editable" } } }