{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:YAVOKWNN2ZXFGLBDZCC2537VYG","short_pith_number":"pith:YAVOKWNN","canonical_record":{"source":{"id":"1603.06835","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-03-22T15:43:43Z","cross_cats_sorted":["physics.flu-dyn"],"title_canon_sha256":"a08bf31f544fcd615addda7b7118b437b365e32970a0dc5f9c8fae2d7d5cd3d2","abstract_canon_sha256":"3072128c7f1a5bc5b5058010fb0c93d008fe885a5f66e9a58730502041c9319c"},"schema_version":"1.0"},"canonical_sha256":"c02ae559add66e532c23c885aeeff5c1a69b27dd42bc9c5e4e0de9e673b09b5e","source":{"kind":"arxiv","id":"1603.06835","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.06835","created_at":"2026-05-18T01:18:13Z"},{"alias_kind":"arxiv_version","alias_value":"1603.06835v1","created_at":"2026-05-18T01:18:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.06835","created_at":"2026-05-18T01:18:13Z"},{"alias_kind":"pith_short_12","alias_value":"YAVOKWNN2ZXF","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YAVOKWNN2ZXFGLBD","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YAVOKWNN","created_at":"2026-05-18T12:30:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:YAVOKWNN2ZXFGLBDZCC2537VYG","target":"record","payload":{"canonical_record":{"source":{"id":"1603.06835","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-03-22T15:43:43Z","cross_cats_sorted":["physics.flu-dyn"],"title_canon_sha256":"a08bf31f544fcd615addda7b7118b437b365e32970a0dc5f9c8fae2d7d5cd3d2","abstract_canon_sha256":"3072128c7f1a5bc5b5058010fb0c93d008fe885a5f66e9a58730502041c9319c"},"schema_version":"1.0"},"canonical_sha256":"c02ae559add66e532c23c885aeeff5c1a69b27dd42bc9c5e4e0de9e673b09b5e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:13.646718Z","signature_b64":"93gfRMxaRaX+Pbdeov+3g6ttiGxSVdUAS8/DEagp1SK/v67D8/Rhv2IkrUdVE00+RuBxhivBZAAoFrruxBYcBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c02ae559add66e532c23c885aeeff5c1a69b27dd42bc9c5e4e0de9e673b09b5e","last_reissued_at":"2026-05-18T01:18:13.645865Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:13.645865Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1603.06835","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":"2026-05-18T01:18:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z1aGTntz/7qt2M5h6fCE0Ra1VCQNm8DJnKMukFgZoFrue6bTER+p5nNQ9lr6upJsE7Rr4zAieAo7HqowIMxdDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T23:32:19.428487Z"},"content_sha256":"6887fd9d0d5b42d475f314cbf04ed3b6afa2b4b2e4036de1f1f5a979a1794aae","schema_version":"1.0","event_id":"sha256:6887fd9d0d5b42d475f314cbf04ed3b6afa2b4b2e4036de1f1f5a979a1794aae"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:YAVOKWNN2ZXFGLBDZCC2537VYG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Oscillatory Double-Diffusive Convection in a Horizontal Cavity with Soret and Dufour Effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.flu-dyn"],"primary_cat":"physics.comp-ph","authors_text":"Jin Wang, Mo Yang, Yuwen Zhang","submitted_at":"2016-03-22T15:43:43Z","abstract_excerpt":"Oscillatory double-diffusive convection in horizontal cavity with Soret and Dufour effects is investigated numerically based on SIMPLE algorithm with QUICK scheme in non-uniform staggered grid system. The results show that double-diffusive convection develops from steady-state convection-dominated, periodic oscillatory, quasi-periodic oscillatory to chaotic flow, and finally return to periodic oscillation as buoyancy ratio increases. Moreover, fundamental frequency and fluctuation amplitude increase with buoyancy ratio. As Rayleigh number increases, transition trendy of oscillatory convection "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.06835","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":"2026-05-18T01:18:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Bug/h9qK+96eZ2qN7AKHIjRjS9yQAUAuhoOY3pwTP4HUUIPvflffe4iKXSPxhtUJOs3ztPccQvRFITklLJECAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T23:32:19.429227Z"},"content_sha256":"098460d45acf84679b133953c0131fe3790ed3661c096d7a84e03f2492ee58ec","schema_version":"1.0","event_id":"sha256:098460d45acf84679b133953c0131fe3790ed3661c096d7a84e03f2492ee58ec"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YAVOKWNN2ZXFGLBDZCC2537VYG/bundle.json","state_url":"https://pith.science/pith/YAVOKWNN2ZXFGLBDZCC2537VYG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YAVOKWNN2ZXFGLBDZCC2537VYG/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":"2026-06-11T23:32:19Z","links":{"resolver":"https://pith.science/pith/YAVOKWNN2ZXFGLBDZCC2537VYG","bundle":"https://pith.science/pith/YAVOKWNN2ZXFGLBDZCC2537VYG/bundle.json","state":"https://pith.science/pith/YAVOKWNN2ZXFGLBDZCC2537VYG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YAVOKWNN2ZXFGLBDZCC2537VYG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:YAVOKWNN2ZXFGLBDZCC2537VYG","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":"3072128c7f1a5bc5b5058010fb0c93d008fe885a5f66e9a58730502041c9319c","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-03-22T15:43:43Z","title_canon_sha256":"a08bf31f544fcd615addda7b7118b437b365e32970a0dc5f9c8fae2d7d5cd3d2"},"schema_version":"1.0","source":{"id":"1603.06835","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.06835","created_at":"2026-05-18T01:18:13Z"},{"alias_kind":"arxiv_version","alias_value":"1603.06835v1","created_at":"2026-05-18T01:18:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.06835","created_at":"2026-05-18T01:18:13Z"},{"alias_kind":"pith_short_12","alias_value":"YAVOKWNN2ZXF","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YAVOKWNN2ZXFGLBD","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YAVOKWNN","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:098460d45acf84679b133953c0131fe3790ed3661c096d7a84e03f2492ee58ec","target":"graph","created_at":"2026-05-18T01:18:13Z","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":"Oscillatory double-diffusive convection in horizontal cavity with Soret and Dufour effects is investigated numerically based on SIMPLE algorithm with QUICK scheme in non-uniform staggered grid system. The results show that double-diffusive convection develops from steady-state convection-dominated, periodic oscillatory, quasi-periodic oscillatory to chaotic flow, and finally return to periodic oscillation as buoyancy ratio increases. Moreover, fundamental frequency and fluctuation amplitude increase with buoyancy ratio. As Rayleigh number increases, transition trendy of oscillatory convection ","authors_text":"Jin Wang, Mo Yang, Yuwen Zhang","cross_cats":["physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-03-22T15:43:43Z","title":"Oscillatory Double-Diffusive Convection in a Horizontal Cavity with Soret and Dufour Effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.06835","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":"sha256:6887fd9d0d5b42d475f314cbf04ed3b6afa2b4b2e4036de1f1f5a979a1794aae","target":"record","created_at":"2026-05-18T01:18:13Z","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":"3072128c7f1a5bc5b5058010fb0c93d008fe885a5f66e9a58730502041c9319c","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-03-22T15:43:43Z","title_canon_sha256":"a08bf31f544fcd615addda7b7118b437b365e32970a0dc5f9c8fae2d7d5cd3d2"},"schema_version":"1.0","source":{"id":"1603.06835","kind":"arxiv","version":1}},"canonical_sha256":"c02ae559add66e532c23c885aeeff5c1a69b27dd42bc9c5e4e0de9e673b09b5e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c02ae559add66e532c23c885aeeff5c1a69b27dd42bc9c5e4e0de9e673b09b5e","first_computed_at":"2026-05-18T01:18:13.645865Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:18:13.645865Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"93gfRMxaRaX+Pbdeov+3g6ttiGxSVdUAS8/DEagp1SK/v67D8/Rhv2IkrUdVE00+RuBxhivBZAAoFrruxBYcBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:18:13.646718Z","signed_message":"canonical_sha256_bytes"},"source_id":"1603.06835","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6887fd9d0d5b42d475f314cbf04ed3b6afa2b4b2e4036de1f1f5a979a1794aae","sha256:098460d45acf84679b133953c0131fe3790ed3661c096d7a84e03f2492ee58ec"],"state_sha256":"c5911f7ca70a152e2fac03bd1f7b812ed5e177aeed8a91a026f525056648aefa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WP+32nmE4IJbgz73S1ngkNnrlkEy4oU7KiGoe3+BZCAEeihY4CpLGv33qzaLWidoiaO6HV1CZja2VoB1qYHYDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T23:32:19.433961Z","bundle_sha256":"8b3664dc862edfe5a94474c133a65f5b5c6a6e8dce0ac4fbb10783f4f1bc6396"}}