{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:HBPEK3N3NMAQKCK55LITH7CDG5","short_pith_number":"pith:HBPEK3N3","canonical_record":{"source":{"id":"1409.5694","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-09-19T15:24:34Z","cross_cats_sorted":["physics.comp-ph","physics.flu-dyn"],"title_canon_sha256":"4b0cd28ed0cdae227c7a81c7feafbd486f5f248627e322be36d2d3e0811435b2","abstract_canon_sha256":"5b3c4dcf98e76d68130d99fb56698c6560dd04a830b47b2c649f6bf3b590546e"},"schema_version":"1.0"},"canonical_sha256":"385e456dbb6b0105095dead133fc433762077eb5bcbb975348e9981da89ba459","source":{"kind":"arxiv","id":"1409.5694","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5694","created_at":"2026-05-18T01:41:59Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5694v1","created_at":"2026-05-18T01:41:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5694","created_at":"2026-05-18T01:41:59Z"},{"alias_kind":"pith_short_12","alias_value":"HBPEK3N3NMAQ","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"HBPEK3N3NMAQKCK5","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"HBPEK3N3","created_at":"2026-05-18T12:28:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:HBPEK3N3NMAQKCK55LITH7CDG5","target":"record","payload":{"canonical_record":{"source":{"id":"1409.5694","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-09-19T15:24:34Z","cross_cats_sorted":["physics.comp-ph","physics.flu-dyn"],"title_canon_sha256":"4b0cd28ed0cdae227c7a81c7feafbd486f5f248627e322be36d2d3e0811435b2","abstract_canon_sha256":"5b3c4dcf98e76d68130d99fb56698c6560dd04a830b47b2c649f6bf3b590546e"},"schema_version":"1.0"},"canonical_sha256":"385e456dbb6b0105095dead133fc433762077eb5bcbb975348e9981da89ba459","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:59.526055Z","signature_b64":"ilvC5P3V/UgIPPMSh44A8kLVibqaYhVncdvFBYRdc4Qkzd3kZXVBV/Q07Wyk4GC9PD4QWod4rbb6SevPtNX1BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"385e456dbb6b0105095dead133fc433762077eb5bcbb975348e9981da89ba459","last_reissued_at":"2026-05-18T01:41:59.525417Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:59.525417Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.5694","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:41:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3Yil4EzwPwg5UALUP9kK5ov4rHY2+XyJ89mgiRMz4KvoY9CPnQTNZyAh0J3JnbiX9RfbSTf7OUICIFZZBOHnAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:31:53.218334Z"},"content_sha256":"d8cae12f7ae7eccc8147697d431251a6e0e4f754386fe6d89c5a5bb3e3e41369","schema_version":"1.0","event_id":"sha256:d8cae12f7ae7eccc8147697d431251a6e0e4f754386fe6d89c5a5bb3e3e41369"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:HBPEK3N3NMAQKCK55LITH7CDG5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Kinetic roughening of a soft dewetting line under quenched disorder - a numerical study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph","physics.flu-dyn"],"primary_cat":"cond-mat.soft","authors_text":"Botond Tyukodi, Yves Brechet, Zoltan Neda","submitted_at":"2014-09-19T15:24:34Z","abstract_excerpt":"A molecular-dynamics type simulation method, which is suitable for investigating the dewetting dynamics of thin and viscous liquid layers, is discussed. The efficiency of the method is exemplified by studying a two-parameter depinning-like model defined on inhomogeneous solid surfaces. The morphology and the statistical properties of the contact line is mapped in the relevant parameter space, and as a result critical behavior in the vicinity of the depinning transition is revealed. The model allows for the tearing of the layer, which leads to a new propagation regime resulting in non-trivial c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5694","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:41:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZZCi/58goDvF2mgKSKpN9ghxUyMjW0hn3ERbYdpySeJsae+wFYK+onlqjZFY5KIYRFIlWG1YSSKjluY8F8sLDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:31:53.218732Z"},"content_sha256":"91f90a80463a4b6a7f38a43f3ed736cf433d2beab662ed099faeb93e77743b8e","schema_version":"1.0","event_id":"sha256:91f90a80463a4b6a7f38a43f3ed736cf433d2beab662ed099faeb93e77743b8e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HBPEK3N3NMAQKCK55LITH7CDG5/bundle.json","state_url":"https://pith.science/pith/HBPEK3N3NMAQKCK55LITH7CDG5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HBPEK3N3NMAQKCK55LITH7CDG5/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-31T16:31:53Z","links":{"resolver":"https://pith.science/pith/HBPEK3N3NMAQKCK55LITH7CDG5","bundle":"https://pith.science/pith/HBPEK3N3NMAQKCK55LITH7CDG5/bundle.json","state":"https://pith.science/pith/HBPEK3N3NMAQKCK55LITH7CDG5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HBPEK3N3NMAQKCK55LITH7CDG5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:HBPEK3N3NMAQKCK55LITH7CDG5","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"5b3c4dcf98e76d68130d99fb56698c6560dd04a830b47b2c649f6bf3b590546e","cross_cats_sorted":["physics.comp-ph","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-09-19T15:24:34Z","title_canon_sha256":"4b0cd28ed0cdae227c7a81c7feafbd486f5f248627e322be36d2d3e0811435b2"},"schema_version":"1.0","source":{"id":"1409.5694","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5694","created_at":"2026-05-18T01:41:59Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5694v1","created_at":"2026-05-18T01:41:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5694","created_at":"2026-05-18T01:41:59Z"},{"alias_kind":"pith_short_12","alias_value":"HBPEK3N3NMAQ","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_16","alias_value":"HBPEK3N3NMAQKCK5","created_at":"2026-05-18T12:28:30Z"},{"alias_kind":"pith_short_8","alias_value":"HBPEK3N3","created_at":"2026-05-18T12:28:30Z"}],"graph_snapshots":[{"event_id":"sha256:91f90a80463a4b6a7f38a43f3ed736cf433d2beab662ed099faeb93e77743b8e","target":"graph","created_at":"2026-05-18T01:41:59Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"A molecular-dynamics type simulation method, which is suitable for investigating the dewetting dynamics of thin and viscous liquid layers, is discussed. The efficiency of the method is exemplified by studying a two-parameter depinning-like model defined on inhomogeneous solid surfaces. The morphology and the statistical properties of the contact line is mapped in the relevant parameter space, and as a result critical behavior in the vicinity of the depinning transition is revealed. The model allows for the tearing of the layer, which leads to a new propagation regime resulting in non-trivial c","authors_text":"Botond Tyukodi, Yves Brechet, Zoltan Neda","cross_cats":["physics.comp-ph","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-09-19T15:24:34Z","title":"Kinetic roughening of a soft dewetting line under quenched disorder - a numerical study"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5694","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:d8cae12f7ae7eccc8147697d431251a6e0e4f754386fe6d89c5a5bb3e3e41369","target":"record","created_at":"2026-05-18T01:41:59Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"5b3c4dcf98e76d68130d99fb56698c6560dd04a830b47b2c649f6bf3b590546e","cross_cats_sorted":["physics.comp-ph","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-09-19T15:24:34Z","title_canon_sha256":"4b0cd28ed0cdae227c7a81c7feafbd486f5f248627e322be36d2d3e0811435b2"},"schema_version":"1.0","source":{"id":"1409.5694","kind":"arxiv","version":1}},"canonical_sha256":"385e456dbb6b0105095dead133fc433762077eb5bcbb975348e9981da89ba459","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"385e456dbb6b0105095dead133fc433762077eb5bcbb975348e9981da89ba459","first_computed_at":"2026-05-18T01:41:59.525417Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:59.525417Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ilvC5P3V/UgIPPMSh44A8kLVibqaYhVncdvFBYRdc4Qkzd3kZXVBV/Q07Wyk4GC9PD4QWod4rbb6SevPtNX1BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:59.526055Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.5694","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d8cae12f7ae7eccc8147697d431251a6e0e4f754386fe6d89c5a5bb3e3e41369","sha256:91f90a80463a4b6a7f38a43f3ed736cf433d2beab662ed099faeb93e77743b8e"],"state_sha256":"8062ed191757812ff8b62fe31c19769efa69c1e90e50341cc1b9c06279466360"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tuWnj+VWQuTDCPBgL1hK3NGp9v04xS7XQreUTz+N/6yBZuwt9Nm89tQ+0dW5kjXCoU9JTuMIKZQf55Ze7SDPDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T16:31:53.221107Z","bundle_sha256":"3a4756ce638d53731e6b4dc0767276e031045a9d64bb20b42cf4d77221172449"}}