{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:UJ7RLWVZJZ76A5KHLS6ERQZCVD","short_pith_number":"pith:UJ7RLWVZ","canonical_record":{"source":{"id":"1812.06002","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-12-14T16:12:50Z","cross_cats_sorted":["cond-mat.stat-mech","nlin.AO","nlin.PS","physics.flu-dyn"],"title_canon_sha256":"f0544213555d52afd9f9a4f059fbb8f96f48b872f79f4c1c053aeff7f98e4586","abstract_canon_sha256":"2c90c060635997bd36907d5bf6d7a36a999565cede85cb1d0ae90c9c84b80239"},"schema_version":"1.0"},"canonical_sha256":"a27f15dab94e7fe075475cbc48c322a8c856c6d2e47147a53a149ea270502cfa","source":{"kind":"arxiv","id":"1812.06002","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.06002","created_at":"2026-05-17T23:39:40Z"},{"alias_kind":"arxiv_version","alias_value":"1812.06002v4","created_at":"2026-05-17T23:39:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.06002","created_at":"2026-05-17T23:39:40Z"},{"alias_kind":"pith_short_12","alias_value":"UJ7RLWVZJZ76","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"UJ7RLWVZJZ76A5KH","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"UJ7RLWVZ","created_at":"2026-05-18T12:32:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:UJ7RLWVZJZ76A5KHLS6ERQZCVD","target":"record","payload":{"canonical_record":{"source":{"id":"1812.06002","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-12-14T16:12:50Z","cross_cats_sorted":["cond-mat.stat-mech","nlin.AO","nlin.PS","physics.flu-dyn"],"title_canon_sha256":"f0544213555d52afd9f9a4f059fbb8f96f48b872f79f4c1c053aeff7f98e4586","abstract_canon_sha256":"2c90c060635997bd36907d5bf6d7a36a999565cede85cb1d0ae90c9c84b80239"},"schema_version":"1.0"},"canonical_sha256":"a27f15dab94e7fe075475cbc48c322a8c856c6d2e47147a53a149ea270502cfa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:40.049063Z","signature_b64":"UvkTx8FnjSmtPodsmpmJFCAZy3UbEuTaizUfrztY/R59obf5BZaHVKWNAuDF+PUf3dVV1qF1ziqvz2XJW/tfAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a27f15dab94e7fe075475cbc48c322a8c856c6d2e47147a53a149ea270502cfa","last_reissued_at":"2026-05-17T23:39:40.048365Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:40.048365Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.06002","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:39:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7+t4T2cK6Li3oQpSZ0utTLbnlmMXPIzioWLSpSxNlMhEzsZA6x6hVFqySrQuuoHMt6P5aljHdVMv8AdcLDDsCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T20:12:43.097696Z"},"content_sha256":"1841bbbd40e7d9ac8d348e704059b2b2167484d5d5275211848848354b491e40","schema_version":"1.0","event_id":"sha256:1841bbbd40e7d9ac8d348e704059b2b2167484d5d5275211848848354b491e40"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:UJ7RLWVZJZ76A5KHLS6ERQZCVD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Coexisting Ordered States, Local Equilibrium-like Domains, and Broken Ergodicity in a Non-turbulent Rayleigh-B\\'enard Convection at Steady-state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","nlin.AO","nlin.PS","physics.flu-dyn"],"primary_cat":"cond-mat.soft","authors_text":"Atanu Chatterjee, Germano Iannacchione, Nicholas Mears, Yash Yadati","submitted_at":"2018-12-14T16:12:50Z","abstract_excerpt":"A challenge in fundamental physics and especially in thermodynamics is to understand emergent order in far-from-equilibrium systems. While at equilibrium, temperature plays the role of a key thermodynamic variable whose uniformity in space and time defines the equilibrium state the system is in, this is not the case in a far-from-equilibrium driven system. When energy flows through a finite system at steady-state, temperature takes on a time-independent but spatially varying character. In this study, the convection patterns of a Rayleigh-B{\\'e}nard fluid cell at steady-state is used as a proto"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.06002","kind":"arxiv","version":4},"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":"2026-05-17T23:39:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KRyoM+llBnemm9an3JZy1wIdjOWkCqG0MtxKMjBe93tQwcpvStl/BDYW7Psi0E9LTz11R9opjXF+s9osrQNgCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T20:12:43.098097Z"},"content_sha256":"534fea1a0dca96f90a09217a016630576a9eb75179b4786ea1b3ee61c5a00fd4","schema_version":"1.0","event_id":"sha256:534fea1a0dca96f90a09217a016630576a9eb75179b4786ea1b3ee61c5a00fd4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UJ7RLWVZJZ76A5KHLS6ERQZCVD/bundle.json","state_url":"https://pith.science/pith/UJ7RLWVZJZ76A5KHLS6ERQZCVD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UJ7RLWVZJZ76A5KHLS6ERQZCVD/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":"2026-06-25T20:12:43Z","links":{"resolver":"https://pith.science/pith/UJ7RLWVZJZ76A5KHLS6ERQZCVD","bundle":"https://pith.science/pith/UJ7RLWVZJZ76A5KHLS6ERQZCVD/bundle.json","state":"https://pith.science/pith/UJ7RLWVZJZ76A5KHLS6ERQZCVD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UJ7RLWVZJZ76A5KHLS6ERQZCVD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:UJ7RLWVZJZ76A5KHLS6ERQZCVD","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":"2c90c060635997bd36907d5bf6d7a36a999565cede85cb1d0ae90c9c84b80239","cross_cats_sorted":["cond-mat.stat-mech","nlin.AO","nlin.PS","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-12-14T16:12:50Z","title_canon_sha256":"f0544213555d52afd9f9a4f059fbb8f96f48b872f79f4c1c053aeff7f98e4586"},"schema_version":"1.0","source":{"id":"1812.06002","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.06002","created_at":"2026-05-17T23:39:40Z"},{"alias_kind":"arxiv_version","alias_value":"1812.06002v4","created_at":"2026-05-17T23:39:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.06002","created_at":"2026-05-17T23:39:40Z"},{"alias_kind":"pith_short_12","alias_value":"UJ7RLWVZJZ76","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"UJ7RLWVZJZ76A5KH","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"UJ7RLWVZ","created_at":"2026-05-18T12:32:56Z"}],"graph_snapshots":[{"event_id":"sha256:534fea1a0dca96f90a09217a016630576a9eb75179b4786ea1b3ee61c5a00fd4","target":"graph","created_at":"2026-05-17T23:39:40Z","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 challenge in fundamental physics and especially in thermodynamics is to understand emergent order in far-from-equilibrium systems. While at equilibrium, temperature plays the role of a key thermodynamic variable whose uniformity in space and time defines the equilibrium state the system is in, this is not the case in a far-from-equilibrium driven system. When energy flows through a finite system at steady-state, temperature takes on a time-independent but spatially varying character. In this study, the convection patterns of a Rayleigh-B{\\'e}nard fluid cell at steady-state is used as a proto","authors_text":"Atanu Chatterjee, Germano Iannacchione, Nicholas Mears, Yash Yadati","cross_cats":["cond-mat.stat-mech","nlin.AO","nlin.PS","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-12-14T16:12:50Z","title":"Coexisting Ordered States, Local Equilibrium-like Domains, and Broken Ergodicity in a Non-turbulent Rayleigh-B\\'enard Convection at Steady-state"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.06002","kind":"arxiv","version":4},"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":"sha256:1841bbbd40e7d9ac8d348e704059b2b2167484d5d5275211848848354b491e40","target":"record","created_at":"2026-05-17T23:39:40Z","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":"2c90c060635997bd36907d5bf6d7a36a999565cede85cb1d0ae90c9c84b80239","cross_cats_sorted":["cond-mat.stat-mech","nlin.AO","nlin.PS","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-12-14T16:12:50Z","title_canon_sha256":"f0544213555d52afd9f9a4f059fbb8f96f48b872f79f4c1c053aeff7f98e4586"},"schema_version":"1.0","source":{"id":"1812.06002","kind":"arxiv","version":4}},"canonical_sha256":"a27f15dab94e7fe075475cbc48c322a8c856c6d2e47147a53a149ea270502cfa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a27f15dab94e7fe075475cbc48c322a8c856c6d2e47147a53a149ea270502cfa","first_computed_at":"2026-05-17T23:39:40.048365Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:39:40.048365Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UvkTx8FnjSmtPodsmpmJFCAZy3UbEuTaizUfrztY/R59obf5BZaHVKWNAuDF+PUf3dVV1qF1ziqvz2XJW/tfAg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:39:40.049063Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.06002","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1841bbbd40e7d9ac8d348e704059b2b2167484d5d5275211848848354b491e40","sha256:534fea1a0dca96f90a09217a016630576a9eb75179b4786ea1b3ee61c5a00fd4"],"state_sha256":"e8af7a6f6a0178a5d7f07be18203be23c41557182169accb2c77d60e34c68d29"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zZ9za2wnOG9c4Rphn6WKfBCMfWRNAxa6ccuSsGDU/dVdlZDgMtOBdSzTOkRzG7uRgXrkfmGRRg05C03AuzuhCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T20:12:43.100487Z","bundle_sha256":"4bbb9308871a35095af2efd3674551060fa275c6a69cf999670ef42bae4312f0"}}