{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:3YDYYIST5IJEUBMS5NPDYFKXTI","short_pith_number":"pith:3YDYYIST","canonical_record":{"source":{"id":"1501.03857","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-01-16T00:24:11Z","cross_cats_sorted":["physics.flu-dyn"],"title_canon_sha256":"cae04606ea10719f696fac72e43ed0c36c058f4ef8452b2a90da266217509e63","abstract_canon_sha256":"e0d91c8dc3c7f2c0bb83dc3fab6d10038f781964818b91fdbb266a940ef94771"},"schema_version":"1.0"},"canonical_sha256":"de078c2253ea124a0592eb5e3c15579a13909569a666b523a5ecb88f64533980","source":{"kind":"arxiv","id":"1501.03857","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.03857","created_at":"2026-05-18T02:25:40Z"},{"alias_kind":"arxiv_version","alias_value":"1501.03857v1","created_at":"2026-05-18T02:25:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.03857","created_at":"2026-05-18T02:25:40Z"},{"alias_kind":"pith_short_12","alias_value":"3YDYYIST5IJE","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_16","alias_value":"3YDYYIST5IJEUBMS","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_8","alias_value":"3YDYYIST","created_at":"2026-05-18T12:29:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:3YDYYIST5IJEUBMS5NPDYFKXTI","target":"record","payload":{"canonical_record":{"source":{"id":"1501.03857","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-01-16T00:24:11Z","cross_cats_sorted":["physics.flu-dyn"],"title_canon_sha256":"cae04606ea10719f696fac72e43ed0c36c058f4ef8452b2a90da266217509e63","abstract_canon_sha256":"e0d91c8dc3c7f2c0bb83dc3fab6d10038f781964818b91fdbb266a940ef94771"},"schema_version":"1.0"},"canonical_sha256":"de078c2253ea124a0592eb5e3c15579a13909569a666b523a5ecb88f64533980","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:25:40.005480Z","signature_b64":"PAOWMs2EaazYA9hkzuczweoLQW/Cm9KQS2YBN/OFBuAS2TBoVovRSorlfsp4Oi0E1YWVOsWAvHG5+AAX/TwZBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de078c2253ea124a0592eb5e3c15579a13909569a666b523a5ecb88f64533980","last_reissued_at":"2026-05-18T02:25:40.005048Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:25:40.005048Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1501.03857","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":"2026-05-18T02:25:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LQvMZIt48OlmLeDHImmpfEUNYkeiQMeHSuHWCJtMAmuyu5KGvMVtGanogbM0e+bXXhWLg/5TRHLX5yoRvKAkBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T02:22:56.070775Z"},"content_sha256":"828b8259c01167db3f5eded6062558d831a1a74b4094468eb5ebcc469bb45286","schema_version":"1.0","event_id":"sha256:828b8259c01167db3f5eded6062558d831a1a74b4094468eb5ebcc469bb45286"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:3YDYYIST5IJEUBMS5NPDYFKXTI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lattice Boltzmann modeling of boiling heat transfer: The boiling curve and the effects of wettability","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.flu-dyn"],"primary_cat":"physics.comp-ph","authors_text":"K. H. Luo, M. M. Francois, Q. J. Kang, Q. Li, Y. L. He","submitted_at":"2015-01-16T00:24:11Z","abstract_excerpt":"A hybrid thermal lattice Boltzmann (LB) model is presented to simulate thermal multiphase flows with phase change based on an improved pseudopotential LB approach [Q. Li, K. H. Luo, and X. J. Li, Phys. Rev. E 87, 053301 (2013)]. The present model does not suffer from the spurious term caused by the forcing-term effect, which was encountered in some previous thermal LB models for liquid-vapor phase change. Using the model, the liquid-vapor boiling process is simulated. The boiling curve together with the three boiling stages (nucleate boiling, transition boiling, and film boiling) is numericall"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.03857","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":"2026-05-18T02:25:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bGukCwKWE3zSFHUk91LsAZCTXhec4ANfTWkbOvB7HosEzP3IraVAADsh0CMiFSJojgn1Por123iZQGSqIe6kAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T02:22:56.071129Z"},"content_sha256":"0fd2d8a0efa6ff6796cf0119a2f3f16b5659216fbf7ba6dba7af6cb472aa86a0","schema_version":"1.0","event_id":"sha256:0fd2d8a0efa6ff6796cf0119a2f3f16b5659216fbf7ba6dba7af6cb472aa86a0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3YDYYIST5IJEUBMS5NPDYFKXTI/bundle.json","state_url":"https://pith.science/pith/3YDYYIST5IJEUBMS5NPDYFKXTI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3YDYYIST5IJEUBMS5NPDYFKXTI/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":"2026-06-24T02:22:56Z","links":{"resolver":"https://pith.science/pith/3YDYYIST5IJEUBMS5NPDYFKXTI","bundle":"https://pith.science/pith/3YDYYIST5IJEUBMS5NPDYFKXTI/bundle.json","state":"https://pith.science/pith/3YDYYIST5IJEUBMS5NPDYFKXTI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3YDYYIST5IJEUBMS5NPDYFKXTI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:3YDYYIST5IJEUBMS5NPDYFKXTI","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":"e0d91c8dc3c7f2c0bb83dc3fab6d10038f781964818b91fdbb266a940ef94771","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-01-16T00:24:11Z","title_canon_sha256":"cae04606ea10719f696fac72e43ed0c36c058f4ef8452b2a90da266217509e63"},"schema_version":"1.0","source":{"id":"1501.03857","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.03857","created_at":"2026-05-18T02:25:40Z"},{"alias_kind":"arxiv_version","alias_value":"1501.03857v1","created_at":"2026-05-18T02:25:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.03857","created_at":"2026-05-18T02:25:40Z"},{"alias_kind":"pith_short_12","alias_value":"3YDYYIST5IJE","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_16","alias_value":"3YDYYIST5IJEUBMS","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_8","alias_value":"3YDYYIST","created_at":"2026-05-18T12:29:02Z"}],"graph_snapshots":[{"event_id":"sha256:0fd2d8a0efa6ff6796cf0119a2f3f16b5659216fbf7ba6dba7af6cb472aa86a0","target":"graph","created_at":"2026-05-18T02:25:40Z","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 hybrid thermal lattice Boltzmann (LB) model is presented to simulate thermal multiphase flows with phase change based on an improved pseudopotential LB approach [Q. Li, K. H. Luo, and X. J. Li, Phys. Rev. E 87, 053301 (2013)]. The present model does not suffer from the spurious term caused by the forcing-term effect, which was encountered in some previous thermal LB models for liquid-vapor phase change. Using the model, the liquid-vapor boiling process is simulated. The boiling curve together with the three boiling stages (nucleate boiling, transition boiling, and film boiling) is numericall","authors_text":"K. H. Luo, M. M. Francois, Q. J. Kang, Q. Li, Y. L. He","cross_cats":["physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-01-16T00:24:11Z","title":"Lattice Boltzmann modeling of boiling heat transfer: The boiling curve and the effects of wettability"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.03857","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":"sha256:828b8259c01167db3f5eded6062558d831a1a74b4094468eb5ebcc469bb45286","target":"record","created_at":"2026-05-18T02:25:40Z","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":"e0d91c8dc3c7f2c0bb83dc3fab6d10038f781964818b91fdbb266a940ef94771","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-01-16T00:24:11Z","title_canon_sha256":"cae04606ea10719f696fac72e43ed0c36c058f4ef8452b2a90da266217509e63"},"schema_version":"1.0","source":{"id":"1501.03857","kind":"arxiv","version":1}},"canonical_sha256":"de078c2253ea124a0592eb5e3c15579a13909569a666b523a5ecb88f64533980","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"de078c2253ea124a0592eb5e3c15579a13909569a666b523a5ecb88f64533980","first_computed_at":"2026-05-18T02:25:40.005048Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:25:40.005048Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PAOWMs2EaazYA9hkzuczweoLQW/Cm9KQS2YBN/OFBuAS2TBoVovRSorlfsp4Oi0E1YWVOsWAvHG5+AAX/TwZBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:25:40.005480Z","signed_message":"canonical_sha256_bytes"},"source_id":"1501.03857","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:828b8259c01167db3f5eded6062558d831a1a74b4094468eb5ebcc469bb45286","sha256:0fd2d8a0efa6ff6796cf0119a2f3f16b5659216fbf7ba6dba7af6cb472aa86a0"],"state_sha256":"685363a6dbbb85b9295bfc262fea9c963cecc698c547e94b3e830ad02fab56a9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cxZbyVAdX7sfA9uvQ3jwliKD12gCuTMmByPudDWU+j+2EEzW/pXvhROJ5Vphu5ha7t/uxhg6GDmeQNpyDOFVAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T02:22:56.073098Z","bundle_sha256":"aa64583891a021ee4a631b4309b8a17d0c30f95d55aeaf2f36f7c56e24b6d65f"}}