{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:IAEW7I5U7R776J46EYONAVLAEO","short_pith_number":"pith:IAEW7I5U","schema_version":"1.0","canonical_sha256":"40096fa3b4fc7fff279e261cd0556023a738c6d69829fb1e7c024a3777dedc8a","source":{"kind":"arxiv","id":"1708.03467","version":4},"attestation_state":"computed","paper":{"title":"First-passage dynamics of linear stochastic interface models: numerical simulations and entropic repulsion effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.flu-dyn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Markus Gross","submitted_at":"2017-08-11T08:15:07Z","abstract_excerpt":"A fluctuating interfacial profile in one dimension is studied via Langevin simulations of the Edwards-Wilkinson equation with non-conserved noise and the Mullins-Herring equation with conserved noise. The profile is subject to either periodic or Dirichlet (no-flux) boundary conditions. We determine the noise-driven time-evolution of the profile between an initially flat configuration and the instant at which the profile reaches a given height $M$ for the first time. The shape of the averaged profile agrees well with the prediction of weak-noise theory (WNT), which describes the most-likely tra"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1708.03467","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-08-11T08:15:07Z","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"title_canon_sha256":"2ce0ce4bc516cda60126ec35aba92de920f0f89f8f280b76ca2493605e178cac","abstract_canon_sha256":"cd85096768b04802a931014da47b9a004cf2bb8e65fb5f6ef4de1e816bb1025e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:20:16.875110Z","signature_b64":"YqjsRpQCMeD2gwD+GKWnm5xJ8mkI42hmPyj78G4XUfPRzEVVhAYJKOCd7FJhMDOBIhdjEXBomyIjX9E5Yp2rAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"40096fa3b4fc7fff279e261cd0556023a738c6d69829fb1e7c024a3777dedc8a","last_reissued_at":"2026-05-18T00:20:16.874565Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:20:16.874565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"First-passage dynamics of linear stochastic interface models: numerical simulations and entropic repulsion effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.flu-dyn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Markus Gross","submitted_at":"2017-08-11T08:15:07Z","abstract_excerpt":"A fluctuating interfacial profile in one dimension is studied via Langevin simulations of the Edwards-Wilkinson equation with non-conserved noise and the Mullins-Herring equation with conserved noise. The profile is subject to either periodic or Dirichlet (no-flux) boundary conditions. We determine the noise-driven time-evolution of the profile between an initially flat configuration and the instant at which the profile reaches a given height $M$ for the first time. The shape of the averaged profile agrees well with the prediction of weak-noise theory (WNT), which describes the most-likely tra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.03467","kind":"arxiv","version":4},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1708.03467","created_at":"2026-05-18T00:20:16.874658+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.03467v4","created_at":"2026-05-18T00:20:16.874658+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.03467","created_at":"2026-05-18T00:20:16.874658+00:00"},{"alias_kind":"pith_short_12","alias_value":"IAEW7I5U7R77","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_16","alias_value":"IAEW7I5U7R776J46","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_8","alias_value":"IAEW7I5U","created_at":"2026-05-18T12:31:21.493067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO","json":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO.json","graph_json":"https://pith.science/api/pith-number/IAEW7I5U7R776J46EYONAVLAEO/graph.json","events_json":"https://pith.science/api/pith-number/IAEW7I5U7R776J46EYONAVLAEO/events.json","paper":"https://pith.science/paper/IAEW7I5U"},"agent_actions":{"view_html":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO","download_json":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO.json","view_paper":"https://pith.science/paper/IAEW7I5U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.03467&json=true","fetch_graph":"https://pith.science/api/pith-number/IAEW7I5U7R776J46EYONAVLAEO/graph.json","fetch_events":"https://pith.science/api/pith-number/IAEW7I5U7R776J46EYONAVLAEO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO/action/storage_attestation","attest_author":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO/action/author_attestation","sign_citation":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO/action/citation_signature","submit_replication":"https://pith.science/pith/IAEW7I5U7R776J46EYONAVLAEO/action/replication_record"}},"created_at":"2026-05-18T00:20:16.874658+00:00","updated_at":"2026-05-18T00:20:16.874658+00:00"}