{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:LP57FFY664KX6XXLJWC7AM4HJT","short_pith_number":"pith:LP57FFY6","canonical_record":{"source":{"id":"0908.1898","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-08-13T13:42:08Z","cross_cats_sorted":[],"title_canon_sha256":"6ca0ddb58153b83e983e10b94801099e9f3f982e2b366c7b8ae0511dcd134fb5","abstract_canon_sha256":"00645069f67dd9c44c6a80ba6a516773a28ffc96a644cccdb5f4eee3f072a257"},"schema_version":"1.0"},"canonical_sha256":"5bfbf2971ef7157f5eeb4d85f033874cf70af1456ef1d144063fe6ef679a2849","source":{"kind":"arxiv","id":"0908.1898","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1898","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1898v2","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1898","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"pith_short_12","alias_value":"LP57FFY664KX","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_16","alias_value":"LP57FFY664KX6XXL","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_8","alias_value":"LP57FFY6","created_at":"2026-05-18T12:26:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:LP57FFY664KX6XXLJWC7AM4HJT","target":"record","payload":{"canonical_record":{"source":{"id":"0908.1898","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-08-13T13:42:08Z","cross_cats_sorted":[],"title_canon_sha256":"6ca0ddb58153b83e983e10b94801099e9f3f982e2b366c7b8ae0511dcd134fb5","abstract_canon_sha256":"00645069f67dd9c44c6a80ba6a516773a28ffc96a644cccdb5f4eee3f072a257"},"schema_version":"1.0"},"canonical_sha256":"5bfbf2971ef7157f5eeb4d85f033874cf70af1456ef1d144063fe6ef679a2849","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:12:34.598957Z","signature_b64":"MMV5x5vtI3FnGNgAGoDVtzLzEpIV1XrMkj+YxuXQl57HaUHA2bH3lLnph/XWOd+IiBhVC41SutzpAe0r0dEtAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5bfbf2971ef7157f5eeb4d85f033874cf70af1456ef1d144063fe6ef679a2849","last_reissued_at":"2026-05-18T02:12:34.598333Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:12:34.598333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0908.1898","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:12:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wN9t0DFo/jRhwnl1r5Gk2Mn7tobu1T2RxP1MHT6sMCZwqfoxqOdDq+umbAmj8/VolWMToDRD4gBuCblQSDH2DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T10:33:02.537833Z"},"content_sha256":"7c962db9ad04f7b44b0bf29eee54a814f44ec36363f1c51e61b2a57e8b04e351","schema_version":"1.0","event_id":"sha256:7c962db9ad04f7b44b0bf29eee54a814f44ec36363f1c51e61b2a57e8b04e351"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:LP57FFY664KX6XXLJWC7AM4HJT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamic approach to the dewetting instability in ultrathin films","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"H. Krishna, N.Shirato, R. Kalyanaraman","submitted_at":"2009-08-13T13:42:08Z","abstract_excerpt":"The fluid dynamics of the classical dewetting instability in ultrathin films is a non-linear process. However, the physical manifestation of the instability in terms of characteristic length and time scales can be described by a linearized form of the initial conditions of the films's dynamics. Alternately, the thermodynamic approach based on equating the rate of free energy decrease to the viscous dissipation [de Gennes, C. R. Acad. Paris.v298, 1984] can give similar information. Here we have evaluated dewetting in the presence of thermocapillary forces arising from a film-thickness (h) depen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1898","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:12:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9Ty2fMHlhC2nyCkQr1y5urn1zC+BzFfZeUj5Q9FZtNtndtbiYg81NajiVngddq4SRTZbUbNtlwrSCXF+hfG5Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T10:33:02.538168Z"},"content_sha256":"8a5a9288983e83c52ad5029946a511d3ca5aa91b1f2c1e1f5ae402e2dc91e87e","schema_version":"1.0","event_id":"sha256:8a5a9288983e83c52ad5029946a511d3ca5aa91b1f2c1e1f5ae402e2dc91e87e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LP57FFY664KX6XXLJWC7AM4HJT/bundle.json","state_url":"https://pith.science/pith/LP57FFY664KX6XXLJWC7AM4HJT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LP57FFY664KX6XXLJWC7AM4HJT/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":"2026-06-02T10:33:02Z","links":{"resolver":"https://pith.science/pith/LP57FFY664KX6XXLJWC7AM4HJT","bundle":"https://pith.science/pith/LP57FFY664KX6XXLJWC7AM4HJT/bundle.json","state":"https://pith.science/pith/LP57FFY664KX6XXLJWC7AM4HJT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LP57FFY664KX6XXLJWC7AM4HJT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:LP57FFY664KX6XXLJWC7AM4HJT","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":"00645069f67dd9c44c6a80ba6a516773a28ffc96a644cccdb5f4eee3f072a257","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-08-13T13:42:08Z","title_canon_sha256":"6ca0ddb58153b83e983e10b94801099e9f3f982e2b366c7b8ae0511dcd134fb5"},"schema_version":"1.0","source":{"id":"0908.1898","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1898","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1898v2","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1898","created_at":"2026-05-18T02:12:34Z"},{"alias_kind":"pith_short_12","alias_value":"LP57FFY664KX","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_16","alias_value":"LP57FFY664KX6XXL","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_8","alias_value":"LP57FFY6","created_at":"2026-05-18T12:26:00Z"}],"graph_snapshots":[{"event_id":"sha256:8a5a9288983e83c52ad5029946a511d3ca5aa91b1f2c1e1f5ae402e2dc91e87e","target":"graph","created_at":"2026-05-18T02:12:34Z","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":"The fluid dynamics of the classical dewetting instability in ultrathin films is a non-linear process. However, the physical manifestation of the instability in terms of characteristic length and time scales can be described by a linearized form of the initial conditions of the films's dynamics. Alternately, the thermodynamic approach based on equating the rate of free energy decrease to the viscous dissipation [de Gennes, C. R. Acad. Paris.v298, 1984] can give similar information. Here we have evaluated dewetting in the presence of thermocapillary forces arising from a film-thickness (h) depen","authors_text":"H. Krishna, N.Shirato, R. Kalyanaraman","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-08-13T13:42:08Z","title":"Thermodynamic approach to the dewetting instability in ultrathin films"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1898","kind":"arxiv","version":2},"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":"sha256:7c962db9ad04f7b44b0bf29eee54a814f44ec36363f1c51e61b2a57e8b04e351","target":"record","created_at":"2026-05-18T02:12:34Z","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":"00645069f67dd9c44c6a80ba6a516773a28ffc96a644cccdb5f4eee3f072a257","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-08-13T13:42:08Z","title_canon_sha256":"6ca0ddb58153b83e983e10b94801099e9f3f982e2b366c7b8ae0511dcd134fb5"},"schema_version":"1.0","source":{"id":"0908.1898","kind":"arxiv","version":2}},"canonical_sha256":"5bfbf2971ef7157f5eeb4d85f033874cf70af1456ef1d144063fe6ef679a2849","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5bfbf2971ef7157f5eeb4d85f033874cf70af1456ef1d144063fe6ef679a2849","first_computed_at":"2026-05-18T02:12:34.598333Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:12:34.598333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MMV5x5vtI3FnGNgAGoDVtzLzEpIV1XrMkj+YxuXQl57HaUHA2bH3lLnph/XWOd+IiBhVC41SutzpAe0r0dEtAw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:12:34.598957Z","signed_message":"canonical_sha256_bytes"},"source_id":"0908.1898","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7c962db9ad04f7b44b0bf29eee54a814f44ec36363f1c51e61b2a57e8b04e351","sha256:8a5a9288983e83c52ad5029946a511d3ca5aa91b1f2c1e1f5ae402e2dc91e87e"],"state_sha256":"2e12c123a2b8f30bd33983f05a8c76e31c955c203f66afe0d86e5fb76fe1f845"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lbCIrjwyoRrT28uWBdc9P8d26FtcXiiNidHIFaSGOssFpjfO/5gJ8S8JyCoedcWiwOFje+ii2gHYZ4hpB7wCDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T10:33:02.540056Z","bundle_sha256":"5dd905c0dc973139bff6cb1e4fd7645c6b7c3d43a2f7f07b12817103bc6b9852"}}