{"paper":{"title":"Continuous condensation in nanogrooves","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Alexandr Malijevsk\\'y","submitted_at":"2018-05-09T08:23:41Z","abstract_excerpt":"We consider condensation in a capillary groove of width $L$ and depth $D$, formed by walls that are completely wet (contact angle $\\theta=0$), which is in a contact with a gas reservoir of the chemical potential $\\mu$. On a mesoscopic level, the condensation process can be described in terms of the midpoint height $\\ell$ of a meniscus formed at the liquid-gas interface. For macroscopically deep grooves ($D\\to\\infty$), and in the presence of long-range (dispersion) forces, the condensation corresponds to a second order phase transition, such that $\\ell\\sim (\\mu_{cc}-\\mu)^{-1/4}$ as $\\mu\\to\\mu_{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.03408","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}