{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:MXO7NHYQSDQUIQRH6XD4OJ6OAH","short_pith_number":"pith:MXO7NHYQ","canonical_record":{"source":{"id":"2212.08776","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2022-12-17T01:40:01Z","cross_cats_sorted":["physics.ao-ph"],"title_canon_sha256":"75989ba6e21ca6631c99b38192283a7efb76fcbd24769eb66a0ceac168e3e4b4","abstract_canon_sha256":"b7ee73c61334a92b58ed828af988a07087e75f94a6ca33bbefdddfddf60cc811"},"schema_version":"1.0"},"canonical_sha256":"65ddf69f1090e1444227f5c7c727ce01cd70fdc7e55ba059cf51ab9d25361afa","source":{"kind":"arxiv","id":"2212.08776","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.08776","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"arxiv_version","alias_value":"2212.08776v1","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.08776","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"pith_short_12","alias_value":"MXO7NHYQSDQU","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"pith_short_16","alias_value":"MXO7NHYQSDQUIQRH","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"pith_short_8","alias_value":"MXO7NHYQ","created_at":"2026-07-05T05:26:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:MXO7NHYQSDQUIQRH6XD4OJ6OAH","target":"record","payload":{"canonical_record":{"source":{"id":"2212.08776","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2022-12-17T01:40:01Z","cross_cats_sorted":["physics.ao-ph"],"title_canon_sha256":"75989ba6e21ca6631c99b38192283a7efb76fcbd24769eb66a0ceac168e3e4b4","abstract_canon_sha256":"b7ee73c61334a92b58ed828af988a07087e75f94a6ca33bbefdddfddf60cc811"},"schema_version":"1.0"},"canonical_sha256":"65ddf69f1090e1444227f5c7c727ce01cd70fdc7e55ba059cf51ab9d25361afa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:26:14.247759Z","signature_b64":"y0YlCzVp5AGoAJ10zuyAvWivhF6O7aYkgBJE/0Z1Q7YKbjlq2auUrgdFKWRZKOIlcfUW3EwqNCPTuQLiQ3taDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"65ddf69f1090e1444227f5c7c727ce01cd70fdc7e55ba059cf51ab9d25361afa","last_reissued_at":"2026-07-05T05:26:14.247405Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:26:14.247405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2212.08776","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":"2026-07-05T05:26:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kOfYop6of00YceCP4ge/aJnYBnO3Q8bj7S/L7EBpvIRlxLbMuoy2hzROS7VXoy0AMw9hSXRv6JMedaZSDe/OAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:00:13.650123Z"},"content_sha256":"ea364821d9ba6a3f232bea0b967541ef1dabd9ef87ea9c01d4712f53ea6e73b9","schema_version":"1.0","event_id":"sha256:ea364821d9ba6a3f232bea0b967541ef1dabd9ef87ea9c01d4712f53ea6e73b9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:MXO7NHYQSDQUIQRH6XD4OJ6OAH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A new hybrid mass-flux/ high-order turbulence closure for ocean vertical mixing","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.ao-ph"],"primary_cat":"physics.flu-dyn","authors_text":"Amrapalli Garanaik, Brodie Pearson, Filipe Pereira, Katherine Smith, Luke Van Roekel, Qing Li, Rachel Robey","submitted_at":"2022-12-17T01:40:01Z","abstract_excerpt":"While various parameterizations of vertical turbulent fluxes at different levels of complexity have been proposed, each has its own limitations. For example, simple first-order closure schemes such as the K-Profile Parameterization (KPP) lack energetic constraints; two-equation models like $k-\\epsilon$ directly solve an equation for the turbulent kinetic energy but do not account for non-local fluxes, and high-order closures that include the non-local transport terms are computationally expensive. To address these, here we extend the Assumed-Distribution Higher-Order Closure (ADC) framework or"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.08776","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2212.08776/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T05:26:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0HFkoHN6/zDeC1+GXRjPgi1BBXAYsAkQgvyE0LQfuRRAIpmRO/s0w7M95oUc7FMJzGZJJRrNrwYxrxacT4zoCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:00:13.650746Z"},"content_sha256":"8eab932d122686fde4db256556bd826671b9e79750e3d4022e4f3e54c84ba9b1","schema_version":"1.0","event_id":"sha256:8eab932d122686fde4db256556bd826671b9e79750e3d4022e4f3e54c84ba9b1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MXO7NHYQSDQUIQRH6XD4OJ6OAH/bundle.json","state_url":"https://pith.science/pith/MXO7NHYQSDQUIQRH6XD4OJ6OAH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MXO7NHYQSDQUIQRH6XD4OJ6OAH/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":"2026-08-03T18:00:13Z","links":{"resolver":"https://pith.science/pith/MXO7NHYQSDQUIQRH6XD4OJ6OAH","bundle":"https://pith.science/pith/MXO7NHYQSDQUIQRH6XD4OJ6OAH/bundle.json","state":"https://pith.science/pith/MXO7NHYQSDQUIQRH6XD4OJ6OAH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MXO7NHYQSDQUIQRH6XD4OJ6OAH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:MXO7NHYQSDQUIQRH6XD4OJ6OAH","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":"b7ee73c61334a92b58ed828af988a07087e75f94a6ca33bbefdddfddf60cc811","cross_cats_sorted":["physics.ao-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2022-12-17T01:40:01Z","title_canon_sha256":"75989ba6e21ca6631c99b38192283a7efb76fcbd24769eb66a0ceac168e3e4b4"},"schema_version":"1.0","source":{"id":"2212.08776","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.08776","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"arxiv_version","alias_value":"2212.08776v1","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.08776","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"pith_short_12","alias_value":"MXO7NHYQSDQU","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"pith_short_16","alias_value":"MXO7NHYQSDQUIQRH","created_at":"2026-07-05T05:26:14Z"},{"alias_kind":"pith_short_8","alias_value":"MXO7NHYQ","created_at":"2026-07-05T05:26:14Z"}],"graph_snapshots":[{"event_id":"sha256:8eab932d122686fde4db256556bd826671b9e79750e3d4022e4f3e54c84ba9b1","target":"graph","created_at":"2026-07-05T05:26:14Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2212.08776/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"While various parameterizations of vertical turbulent fluxes at different levels of complexity have been proposed, each has its own limitations. For example, simple first-order closure schemes such as the K-Profile Parameterization (KPP) lack energetic constraints; two-equation models like $k-\\epsilon$ directly solve an equation for the turbulent kinetic energy but do not account for non-local fluxes, and high-order closures that include the non-local transport terms are computationally expensive. To address these, here we extend the Assumed-Distribution Higher-Order Closure (ADC) framework or","authors_text":"Amrapalli Garanaik, Brodie Pearson, Filipe Pereira, Katherine Smith, Luke Van Roekel, Qing Li, Rachel Robey","cross_cats":["physics.ao-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2022-12-17T01:40:01Z","title":"A new hybrid mass-flux/ high-order turbulence closure for ocean vertical mixing"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.08776","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:ea364821d9ba6a3f232bea0b967541ef1dabd9ef87ea9c01d4712f53ea6e73b9","target":"record","created_at":"2026-07-05T05:26:14Z","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":"b7ee73c61334a92b58ed828af988a07087e75f94a6ca33bbefdddfddf60cc811","cross_cats_sorted":["physics.ao-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2022-12-17T01:40:01Z","title_canon_sha256":"75989ba6e21ca6631c99b38192283a7efb76fcbd24769eb66a0ceac168e3e4b4"},"schema_version":"1.0","source":{"id":"2212.08776","kind":"arxiv","version":1}},"canonical_sha256":"65ddf69f1090e1444227f5c7c727ce01cd70fdc7e55ba059cf51ab9d25361afa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"65ddf69f1090e1444227f5c7c727ce01cd70fdc7e55ba059cf51ab9d25361afa","first_computed_at":"2026-07-05T05:26:14.247405Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:26:14.247405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"y0YlCzVp5AGoAJ10zuyAvWivhF6O7aYkgBJE/0Z1Q7YKbjlq2auUrgdFKWRZKOIlcfUW3EwqNCPTuQLiQ3taDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T05:26:14.247759Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.08776","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ea364821d9ba6a3f232bea0b967541ef1dabd9ef87ea9c01d4712f53ea6e73b9","sha256:8eab932d122686fde4db256556bd826671b9e79750e3d4022e4f3e54c84ba9b1"],"state_sha256":"3139c277670ddf3533edabea54a19a8797042444b9e0524eb4178b8f14eec8a4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"38dH9Pl5bIbzGoVpc8z1A73jgYRc5nx+a0svlq4qQnTHpJWYoAh+xw0/FUl49UOxxGHdmsB3HF+npczN7fN3Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T18:00:13.656268Z","bundle_sha256":"92966d3cc4aea8fac672c70e5f1abdbe6f555fcace8c6eefa0e648cbb93b3d87"}}