{ "id": "2309.03155", "version": "v1", "published": "2023-09-06T16:52:04.000Z", "updated": "2023-09-06T16:52:04.000Z", "title": "Harmonic chain far from equilibrium: single-file diffusion, long-range order, and hyperuniformity", "authors": [ "Harukuni Ikeda" ], "comment": "17 pages, 7figures", "categories": [ "cond-mat.stat-mech", "cond-mat.soft" ], "abstract": "In one-dimensional many-particle systems, diffusion is strongly suppressed because particles cannot bypass each other. For this reason, the mean-square displacement (MSD) increases in proportion to the square of time, ${\\rm MSD}(t)\\sim t^{1/2}$ in equilibrium. This phenomenon is called single-file diffusion. Single-file diffusion is observed even in the harmonic lattice, which prevents the existence of long-range order in one dimension. We here study single-file diffusion of the harmonic chain far from equilibrium. We consider the following four types of driving forces that do not satisfy the detailed balance: (i) temporally correlated noise with the power-low Fourier-spectrum $D(\\omega)\\sim \\omega^{-2\\alpha}$, (ii) center-of-mass conserving noise, (iii) periodic driving force, and (iv) periodic deformations of particles. For the driving force (i) with $\\alpha>-1/4$, we observe ${\\rm MSD}(t)\\sim t^{1/2+2\\alpha}$ for large $t$. On the other hand, for the driving forces (i) with $\\alpha<-1/4$ and (ii)-(iv), ${\\rm MSD}$ remains finite. As a consequence, the harmonic chain exhibits the long-range order even in one dimension, which is prohibited by the Mermin-Wagner theorem in equilibrium. We also discuss that the model shows hyperuniformity when driven by the driving forces (i) with $\\alpha<0$ and (ii)-(iv).", "revisions": [ { "version": "v1", "updated": "2023-09-06T16:52:04.000Z" } ], "analyses": { "keywords": [ "harmonic chain far", "long-range order", "driving force", "equilibrium", "hyperuniformity" ], "note": { "typesetting": "TeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable" } } }