dorsal/arxiv
View SchemaDivergent Fluctuations from an Infrared 2D-Mode Catastrophe
| Authors | Richard G. Hennig, Clotilde S. Cucinotta |
|---|---|
| Categories | |
| ArXiv ID | 2601.09009vv1 |
| URL | https://arxiv.org/abs/2601.09009 |
| License | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ |
Abstract
Molecular simulations of interfacial polar media routinely employ periodic boundary conditions parallel to the interface. We show that this geometry injects a uniform plane mode ($q_{\parallel}=0$) that converts the plane-averaged electrostatic potential into a cumulative sum of plane-dipole increments, a random walk in $z$. Consequently, the variance of the plane-averaged potential grows linearly with depth in semi-infinite slabs and follows a parabolic Brownian-bridge profile in finite cells with both ends fixed, with an amplitude inversely proportional to the cell's lateral area. Hence, at any finite area, the variance diverges with slab thickness, a 2D-mode catastrophe. In contrast, a pure 1D chain (no lateral replication) and a fully 3D, nonperiodic medium both exhibit bounded fluctuations that saturate with distance. The mechanism is generic to any solver of Poisson's equation with 2D periodicity, so the apparent growth and ultimate divergence in potential fluctuation are artifacts of boundary conditions rather than material response, and we provide a simple scaling criterion for choosing slab sizes that keeps these artifacts under quantitative control.
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"abstract": "Molecular simulations of interfacial polar media routinely employ periodic boundary conditions parallel to the interface. We show that this geometry injects a uniform plane mode ($q_{\\parallel}=0$) that converts the plane-averaged electrostatic potential into a cumulative sum of plane-dipole increments, a random walk in $z$. Consequently, the variance of the plane-averaged potential grows linearly with depth in semi-infinite slabs and follows a parabolic Brownian-bridge profile in finite cells with both ends fixed, with an amplitude inversely proportional to the cell\u0027s lateral area. Hence, at any finite area, the variance diverges with slab thickness, a 2D-mode catastrophe. In contrast, a pure 1D chain (no lateral replication) and a fully 3D, nonperiodic medium both exhibit bounded fluctuations that saturate with distance. The mechanism is generic to any solver of Poisson\u0027s equation with 2D periodicity, so the apparent growth and ultimate divergence in potential fluctuation are artifacts of boundary conditions rather than material response, and we provide a simple scaling criterion for choosing slab sizes that keeps these artifacts under quantitative control.",
"arxiv_id": "2601.09009",
"authors": [
"Richard G. Hennig",
"Clotilde S. Cucinotta"
],
"categories": [
"cond-mat.stat-mech",
"cond-mat.mtrl-sci",
"physics.comp-ph"
],
"license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"title": "Divergent Fluctuations from an Infrared 2D-Mode Catastrophe",
"url": "https://arxiv.org/abs/2601.09009",
"version": "v1"
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