{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:P6S6U2FCBAPECZI2VG5O5I45SF","short_pith_number":"pith:P6S6U2FC","schema_version":"1.0","canonical_sha256":"7fa5ea68a2081e41651aa9baeea39d916da67110cd7e80e75c42c4a1f51da6c2","source":{"kind":"arxiv","id":"1609.09316","version":1},"attestation_state":"computed","paper":{"title":"Large scale spatio-temporal behaviour in surface growth","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nlin.PS","authors_text":"Jogundas Armaitis, Julius Ruseckas, Vaidas Juknevicius","submitted_at":"2016-09-29T12:27:12Z","abstract_excerpt":"This paper presents new findings concerning the dynamics of the slow height variations in surfaces produced by the two-dimensional isotropic Kuramoto-Sivashinsky equation with an additional nonlinear term. In addition to the disordered patterns of specific size evident at small scales, slow height variations of scale-free character become increasingly evident when the system size is increased. The surface spectrum at small wave numbers has a power-law shape with a lower cut-off due to the finite system size. The temporal properties of these long-range height variations are investigated by anal"},"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":"1609.09316","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2016-09-29T12:27:12Z","cross_cats_sorted":[],"title_canon_sha256":"b9e7fd2737a594571759adf9bf1a8b8112d9bad3800bc01986e175cc75e6ba95","abstract_canon_sha256":"a1bd65750c1ec97524361e4940dedde92c8fbbc86b667116c04dda978c4de14c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:03:38.201011Z","signature_b64":"dIO2NgLq7f3LkWJGPibxr3x8IyNXt1VAdkCEp3kWFfPb4qZ3rX4tMAPAS4E2V4a6IKoerEZatOzGZGznDmY6AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7fa5ea68a2081e41651aa9baeea39d916da67110cd7e80e75c42c4a1f51da6c2","last_reissued_at":"2026-05-18T01:03:38.200535Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:03:38.200535Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large scale spatio-temporal behaviour in surface growth","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nlin.PS","authors_text":"Jogundas Armaitis, Julius Ruseckas, Vaidas Juknevicius","submitted_at":"2016-09-29T12:27:12Z","abstract_excerpt":"This paper presents new findings concerning the dynamics of the slow height variations in surfaces produced by the two-dimensional isotropic Kuramoto-Sivashinsky equation with an additional nonlinear term. In addition to the disordered patterns of specific size evident at small scales, slow height variations of scale-free character become increasingly evident when the system size is increased. The surface spectrum at small wave numbers has a power-law shape with a lower cut-off due to the finite system size. The temporal properties of these long-range height variations are investigated by anal"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.09316","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":"1609.09316","created_at":"2026-05-18T01:03:38.200621+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.09316v1","created_at":"2026-05-18T01:03:38.200621+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.09316","created_at":"2026-05-18T01:03:38.200621+00:00"},{"alias_kind":"pith_short_12","alias_value":"P6S6U2FCBAPE","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"P6S6U2FCBAPECZI2","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"P6S6U2FC","created_at":"2026-05-18T12:30:39.010887+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/P6S6U2FCBAPECZI2VG5O5I45SF","json":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF.json","graph_json":"https://pith.science/api/pith-number/P6S6U2FCBAPECZI2VG5O5I45SF/graph.json","events_json":"https://pith.science/api/pith-number/P6S6U2FCBAPECZI2VG5O5I45SF/events.json","paper":"https://pith.science/paper/P6S6U2FC"},"agent_actions":{"view_html":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF","download_json":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF.json","view_paper":"https://pith.science/paper/P6S6U2FC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.09316&json=true","fetch_graph":"https://pith.science/api/pith-number/P6S6U2FCBAPECZI2VG5O5I45SF/graph.json","fetch_events":"https://pith.science/api/pith-number/P6S6U2FCBAPECZI2VG5O5I45SF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF/action/storage_attestation","attest_author":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF/action/author_attestation","sign_citation":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF/action/citation_signature","submit_replication":"https://pith.science/pith/P6S6U2FCBAPECZI2VG5O5I45SF/action/replication_record"}},"created_at":"2026-05-18T01:03:38.200621+00:00","updated_at":"2026-05-18T01:03:38.200621+00:00"}