{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:TTS2D2R7WR3DR5G5ERAVMXKAB6","short_pith_number":"pith:TTS2D2R7","schema_version":"1.0","canonical_sha256":"9ce5a1ea3fb47638f4dd2441565d400fbac40ee720d703695a04072370fc1e56","source":{"kind":"arxiv","id":"1307.5586","version":2},"attestation_state":"computed","paper":{"title":"Kinetic Monte Carlo Simulation of Electrodeposition using the Embedded-Atom Method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","physics.comp-ph"],"primary_cat":"physics.chem-ph","authors_text":"Mark D. Pritzker, Nasser Mohieddin Abukhdeir, Tanyakarn Treeratanaphitak","submitted_at":"2013-07-22T02:57:24Z","abstract_excerpt":"A kinetic Monte Carlo (KMC) method is presented to simulate the electrodeposition of a metal on a single crystal surface of the same metal under galvanostatic conditions. This method utilizes the multi-body embedded-atom method (EAM) potential to characterize the interactions of metal atoms and adatoms. The KMC method accounts for deposition and surface diffusion processes including hopping, atom exchange and step-edge atom exchange. Steady-state deposition configurations obtained using the KMC method are validated by comparison with the structures obtained through the use of molecular dynamic"},"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":"1307.5586","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2013-07-22T02:57:24Z","cross_cats_sorted":["cond-mat.mtrl-sci","physics.comp-ph"],"title_canon_sha256":"fe1c756444b0fc0894a4f963d6dfb0ee7d9edc0f7f27be6e4b4db47e5f433515","abstract_canon_sha256":"9e3fdd04337c9304d6e73a19b4e15423e1a5fa6fcc74d3c37f08cd115613c469"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:03:09.866772Z","signature_b64":"NF3o0dMCLVA74XA5FOzEZscZVeiRvc6zjAX/Hfgn5tivyRRuEYSl0xubG4iJHI6Y1Tyrn/JKcxe5PbcZH+pvBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ce5a1ea3fb47638f4dd2441565d400fbac40ee720d703695a04072370fc1e56","last_reissued_at":"2026-05-18T03:03:09.866102Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:03:09.866102Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Kinetic Monte Carlo Simulation of Electrodeposition using the Embedded-Atom Method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","physics.comp-ph"],"primary_cat":"physics.chem-ph","authors_text":"Mark D. Pritzker, Nasser Mohieddin Abukhdeir, Tanyakarn Treeratanaphitak","submitted_at":"2013-07-22T02:57:24Z","abstract_excerpt":"A kinetic Monte Carlo (KMC) method is presented to simulate the electrodeposition of a metal on a single crystal surface of the same metal under galvanostatic conditions. This method utilizes the multi-body embedded-atom method (EAM) potential to characterize the interactions of metal atoms and adatoms. The KMC method accounts for deposition and surface diffusion processes including hopping, atom exchange and step-edge atom exchange. Steady-state deposition configurations obtained using the KMC method are validated by comparison with the structures obtained through the use of molecular dynamic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.5586","kind":"arxiv","version":2},"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":"1307.5586","created_at":"2026-05-18T03:03:09.866199+00:00"},{"alias_kind":"arxiv_version","alias_value":"1307.5586v2","created_at":"2026-05-18T03:03:09.866199+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.5586","created_at":"2026-05-18T03:03:09.866199+00:00"},{"alias_kind":"pith_short_12","alias_value":"TTS2D2R7WR3D","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_16","alias_value":"TTS2D2R7WR3DR5G5","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_8","alias_value":"TTS2D2R7","created_at":"2026-05-18T12:28:02.375192+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/TTS2D2R7WR3DR5G5ERAVMXKAB6","json":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6.json","graph_json":"https://pith.science/api/pith-number/TTS2D2R7WR3DR5G5ERAVMXKAB6/graph.json","events_json":"https://pith.science/api/pith-number/TTS2D2R7WR3DR5G5ERAVMXKAB6/events.json","paper":"https://pith.science/paper/TTS2D2R7"},"agent_actions":{"view_html":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6","download_json":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6.json","view_paper":"https://pith.science/paper/TTS2D2R7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1307.5586&json=true","fetch_graph":"https://pith.science/api/pith-number/TTS2D2R7WR3DR5G5ERAVMXKAB6/graph.json","fetch_events":"https://pith.science/api/pith-number/TTS2D2R7WR3DR5G5ERAVMXKAB6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6/action/storage_attestation","attest_author":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6/action/author_attestation","sign_citation":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6/action/citation_signature","submit_replication":"https://pith.science/pith/TTS2D2R7WR3DR5G5ERAVMXKAB6/action/replication_record"}},"created_at":"2026-05-18T03:03:09.866199+00:00","updated_at":"2026-05-18T03:03:09.866199+00:00"}