{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:MX2JQDCU65RD7B7XHAS7UQDHKP","short_pith_number":"pith:MX2JQDCU","schema_version":"1.0","canonical_sha256":"65f4980c54f7623f87f73825fa406753dae7cfb0b9eed4d3f6c4cff05b2c25ae","source":{"kind":"arxiv","id":"cond-mat/0205427","version":1},"attestation_state":"computed","paper":{"title":"Dynamical surface structures in multi-particle-correlated surface growths","license":"","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Hyunggyu Park (Inha Univ.), T. S. Kim (Kyung Hee Univ.), Yup Kim","submitted_at":"2002-05-21T04:35:38Z","abstract_excerpt":"We investigate the scaling properties of the interface fluctuation width for the $Q$-mer and $Q$-particle-correlated deposition-evaporation models. These models are constrained with a global conservation law that the particle number at each height is conserved modulo $Q$. In equilibrium, the stationary roughness is anomalous but universal with roughness exponent $\\alpha=1/3$, while the early time evolution shows nonuniversal behavior with growth exponent $\\beta$ varying with models and $Q$. Nonequilibrium surfaces display diverse growing/stationary behavior. The $Q$-mer model shows a faceted s"},"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":"cond-mat/0205427","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-05-21T04:35:38Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"2bcd18314c67db6b983b0350af688b7158255f951147f31031873bb8bd635371","abstract_canon_sha256":"c43de5cd6927c2e77257613750087696dcd9311456f982175fd8c13ff9e80e6a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:59.525583Z","signature_b64":"RplDJTOyPaaFgtsA7Qm/DqpJO5J3X7a9VbPKVSx3C5PfDhPQItN8KTlTA9hGDyAex6f5oCaygSUqzeXl2ENaDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"65f4980c54f7623f87f73825fa406753dae7cfb0b9eed4d3f6c4cff05b2c25ae","last_reissued_at":"2026-05-18T01:06:59.524868Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:59.524868Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical surface structures in multi-particle-correlated surface growths","license":"","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Hyunggyu Park (Inha Univ.), T. S. Kim (Kyung Hee Univ.), Yup Kim","submitted_at":"2002-05-21T04:35:38Z","abstract_excerpt":"We investigate the scaling properties of the interface fluctuation width for the $Q$-mer and $Q$-particle-correlated deposition-evaporation models. These models are constrained with a global conservation law that the particle number at each height is conserved modulo $Q$. In equilibrium, the stationary roughness is anomalous but universal with roughness exponent $\\alpha=1/3$, while the early time evolution shows nonuniversal behavior with growth exponent $\\beta$ varying with models and $Q$. Nonequilibrium surfaces display diverse growing/stationary behavior. The $Q$-mer model shows a faceted s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0205427","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":"cond-mat/0205427","created_at":"2026-05-18T01:06:59.524975+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0205427v1","created_at":"2026-05-18T01:06:59.524975+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0205427","created_at":"2026-05-18T01:06:59.524975+00:00"},{"alias_kind":"pith_short_12","alias_value":"MX2JQDCU65RD","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"MX2JQDCU65RD7B7X","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"MX2JQDCU","created_at":"2026-05-18T12:25:51.375804+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/MX2JQDCU65RD7B7XHAS7UQDHKP","json":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP.json","graph_json":"https://pith.science/api/pith-number/MX2JQDCU65RD7B7XHAS7UQDHKP/graph.json","events_json":"https://pith.science/api/pith-number/MX2JQDCU65RD7B7XHAS7UQDHKP/events.json","paper":"https://pith.science/paper/MX2JQDCU"},"agent_actions":{"view_html":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP","download_json":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP.json","view_paper":"https://pith.science/paper/MX2JQDCU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0205427&json=true","fetch_graph":"https://pith.science/api/pith-number/MX2JQDCU65RD7B7XHAS7UQDHKP/graph.json","fetch_events":"https://pith.science/api/pith-number/MX2JQDCU65RD7B7XHAS7UQDHKP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP/action/storage_attestation","attest_author":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP/action/author_attestation","sign_citation":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP/action/citation_signature","submit_replication":"https://pith.science/pith/MX2JQDCU65RD7B7XHAS7UQDHKP/action/replication_record"}},"created_at":"2026-05-18T01:06:59.524975+00:00","updated_at":"2026-05-18T01:06:59.524975+00:00"}