{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:FX4OU2QMSH7NLXDGQEBBA5YLEK","short_pith_number":"pith:FX4OU2QM","schema_version":"1.0","canonical_sha256":"2df8ea6a0c91fed5dc66810210770b229207b92a8c54489dcbb64d15b1f354a6","source":{"kind":"arxiv","id":"1603.01667","version":1},"attestation_state":"computed","paper":{"title":"Fully Coupled Simulation of the Plasma Liquid Interface and Interfacial Coefficient Effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Alexander Lindsay, David Graves, Steven Shannon","submitted_at":"2016-03-05T01:23:30Z","abstract_excerpt":"There is a growing interest in the study of coupled plasma-liquid systems because of their applications to biomedicine, biological and chemical disinfection, agriculture, and other areas. Without an understanding of the near-surface gas dynamics, modellers are left to make assumptions about the interfacial conditions. For instance it is commonly assumed that the surface loss or sticking coefficient of gas-phase electrons at the interface is equal to 1. In this work we explore the consequences of this assumption and introduce a couple of ways to think about the electron interfacial condition. I"},"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":"1603.01667","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-03-05T01:23:30Z","cross_cats_sorted":[],"title_canon_sha256":"e6f30e2d4185b5f4346d591fc379772c2f63e61e2d2c0b75af4ab1ee32c06141","abstract_canon_sha256":"81332a1aac33e97e0f0bcee626281ca56113ad650f4f47958a7792caab7e0867"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:04.403052Z","signature_b64":"TgFFNC0Dxuaccy+NgZQC2VAJUaRenkKf7Z9tU55NUAVezOO87sRXLQu0iPm6fl0IyQrly1Ft680lgaZWNcPyBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2df8ea6a0c91fed5dc66810210770b229207b92a8c54489dcbb64d15b1f354a6","last_reissued_at":"2026-05-18T01:12:04.402655Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:04.402655Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fully Coupled Simulation of the Plasma Liquid Interface and Interfacial Coefficient Effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Alexander Lindsay, David Graves, Steven Shannon","submitted_at":"2016-03-05T01:23:30Z","abstract_excerpt":"There is a growing interest in the study of coupled plasma-liquid systems because of their applications to biomedicine, biological and chemical disinfection, agriculture, and other areas. Without an understanding of the near-surface gas dynamics, modellers are left to make assumptions about the interfacial conditions. For instance it is commonly assumed that the surface loss or sticking coefficient of gas-phase electrons at the interface is equal to 1. In this work we explore the consequences of this assumption and introduce a couple of ways to think about the electron interfacial condition. I"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.01667","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1603.01667","created_at":"2026-05-18T01:12:04.402712+00:00"},{"alias_kind":"arxiv_version","alias_value":"1603.01667v1","created_at":"2026-05-18T01:12:04.402712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.01667","created_at":"2026-05-18T01:12:04.402712+00:00"},{"alias_kind":"pith_short_12","alias_value":"FX4OU2QMSH7N","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_16","alias_value":"FX4OU2QMSH7NLXDG","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_8","alias_value":"FX4OU2QM","created_at":"2026-05-18T12:30:15.759754+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/FX4OU2QMSH7NLXDGQEBBA5YLEK","json":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK.json","graph_json":"https://pith.science/api/pith-number/FX4OU2QMSH7NLXDGQEBBA5YLEK/graph.json","events_json":"https://pith.science/api/pith-number/FX4OU2QMSH7NLXDGQEBBA5YLEK/events.json","paper":"https://pith.science/paper/FX4OU2QM"},"agent_actions":{"view_html":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK","download_json":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK.json","view_paper":"https://pith.science/paper/FX4OU2QM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1603.01667&json=true","fetch_graph":"https://pith.science/api/pith-number/FX4OU2QMSH7NLXDGQEBBA5YLEK/graph.json","fetch_events":"https://pith.science/api/pith-number/FX4OU2QMSH7NLXDGQEBBA5YLEK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK/action/storage_attestation","attest_author":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK/action/author_attestation","sign_citation":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK/action/citation_signature","submit_replication":"https://pith.science/pith/FX4OU2QMSH7NLXDGQEBBA5YLEK/action/replication_record"}},"created_at":"2026-05-18T01:12:04.402712+00:00","updated_at":"2026-05-18T01:12:04.402712+00:00"}