{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:E7MSWKAH7VJKDO66NZJ626PBLY","short_pith_number":"pith:E7MSWKAH","schema_version":"1.0","canonical_sha256":"27d92b2807fd52a1bbde6e53ed79e15e3466b8e97fd7b0d74169f56e50fcbed5","source":{"kind":"arxiv","id":"1403.4372","version":1},"attestation_state":"computed","paper":{"title":"Self-consistent rate theory for submonolayer surface growth of multi-component systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Mario Einax, Philipp Maass, Wolfgang Dieterich","submitted_at":"2014-03-18T08:51:33Z","abstract_excerpt":"The self-consistent rate theory for surface growth in the submonolayer regime is generalized from mono- to multi-component systems, which are formed by codeposition of different types of atoms or molecules. As a new feature, the theory requires the introduction of pair density distributions to enable a symmetric treatment of reactions among different species. The approach is explicitly developed for binary systems and tested against kinetic Monte Carlo simulations. Using a reduced set of rate equations, only a few differential equations need to be solved to obtain good quantitative predictions"},"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":"1403.4372","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-03-18T08:51:33Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"afec9c062551311ca6b666cc31ffab61ee5da149e22515798a6b7c3755ad68f5","abstract_canon_sha256":"0b208b5186c684cf5d26ce15bdc49fbf292fffac31483ce1ccbe90a29f66a34c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:44:00.072274Z","signature_b64":"iALQHFjTOzd+D37zr+JTfEP9W1DC/6kQOoEMCzMZ6S8X68+7ZvMIrLQXE+958lP8FTIrfGvuMYWMbPfSpkl9BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"27d92b2807fd52a1bbde6e53ed79e15e3466b8e97fd7b0d74169f56e50fcbed5","last_reissued_at":"2026-05-18T01:44:00.071589Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:44:00.071589Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Self-consistent rate theory for submonolayer surface growth of multi-component systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Mario Einax, Philipp Maass, Wolfgang Dieterich","submitted_at":"2014-03-18T08:51:33Z","abstract_excerpt":"The self-consistent rate theory for surface growth in the submonolayer regime is generalized from mono- to multi-component systems, which are formed by codeposition of different types of atoms or molecules. As a new feature, the theory requires the introduction of pair density distributions to enable a symmetric treatment of reactions among different species. The approach is explicitly developed for binary systems and tested against kinetic Monte Carlo simulations. Using a reduced set of rate equations, only a few differential equations need to be solved to obtain good quantitative predictions"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4372","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":"1403.4372","created_at":"2026-05-18T01:44:00.071702+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.4372v1","created_at":"2026-05-18T01:44:00.071702+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4372","created_at":"2026-05-18T01:44:00.071702+00:00"},{"alias_kind":"pith_short_12","alias_value":"E7MSWKAH7VJK","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_16","alias_value":"E7MSWKAH7VJKDO66","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_8","alias_value":"E7MSWKAH","created_at":"2026-05-18T12:28:25.294606+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/E7MSWKAH7VJKDO66NZJ626PBLY","json":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY.json","graph_json":"https://pith.science/api/pith-number/E7MSWKAH7VJKDO66NZJ626PBLY/graph.json","events_json":"https://pith.science/api/pith-number/E7MSWKAH7VJKDO66NZJ626PBLY/events.json","paper":"https://pith.science/paper/E7MSWKAH"},"agent_actions":{"view_html":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY","download_json":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY.json","view_paper":"https://pith.science/paper/E7MSWKAH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.4372&json=true","fetch_graph":"https://pith.science/api/pith-number/E7MSWKAH7VJKDO66NZJ626PBLY/graph.json","fetch_events":"https://pith.science/api/pith-number/E7MSWKAH7VJKDO66NZJ626PBLY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY/action/storage_attestation","attest_author":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY/action/author_attestation","sign_citation":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY/action/citation_signature","submit_replication":"https://pith.science/pith/E7MSWKAH7VJKDO66NZJ626PBLY/action/replication_record"}},"created_at":"2026-05-18T01:44:00.071702+00:00","updated_at":"2026-05-18T01:44:00.071702+00:00"}