{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:LGXTZKKK3PTMLU6F7JXTM2BH4M","short_pith_number":"pith:LGXTZKKK","canonical_record":{"source":{"id":"2106.01158","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-02T13:50:26Z","cross_cats_sorted":[],"title_canon_sha256":"2e1d99a7fe7cb7c32005f663e7331277c5159ad3457f7bfc90e154d50e7f2bce","abstract_canon_sha256":"2402849b3a4c4adedbef34e9968c2bb67d6af2f7aab7d0ca2cecdbb695852a1e"},"schema_version":"1.0"},"canonical_sha256":"59af3ca94adbe6c5d3c5fa6f366827e31cd74d5633dccc083a2af220d7bc3013","source":{"kind":"arxiv","id":"2106.01158","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2106.01158","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"arxiv_version","alias_value":"2106.01158v4","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.01158","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"pith_short_12","alias_value":"LGXTZKKK3PTM","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"pith_short_16","alias_value":"LGXTZKKK3PTMLU6F","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"pith_short_8","alias_value":"LGXTZKKK","created_at":"2026-07-05T04:00:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:LGXTZKKK3PTMLU6F7JXTM2BH4M","target":"record","payload":{"canonical_record":{"source":{"id":"2106.01158","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-02T13:50:26Z","cross_cats_sorted":[],"title_canon_sha256":"2e1d99a7fe7cb7c32005f663e7331277c5159ad3457f7bfc90e154d50e7f2bce","abstract_canon_sha256":"2402849b3a4c4adedbef34e9968c2bb67d6af2f7aab7d0ca2cecdbb695852a1e"},"schema_version":"1.0"},"canonical_sha256":"59af3ca94adbe6c5d3c5fa6f366827e31cd74d5633dccc083a2af220d7bc3013","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:00:53.491540Z","signature_b64":"epmS1+tQV24xzimCCRy6nBH0foh7xFRlZS2dGyvJVg9i9kBdDgseTajRxmop8oZNlgSJD3GuxMjEvX0qcLxEDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"59af3ca94adbe6c5d3c5fa6f366827e31cd74d5633dccc083a2af220d7bc3013","last_reissued_at":"2026-07-05T04:00:53.491091Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:00:53.491091Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2106.01158","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":"2026-07-05T04:00:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Redg/vytc6QC6/UfaZs7rLe8n56q3V5QSHb69LEUcl58noVw8S+1pJPnjH+9r3ZEIjkl9QFGTZ5kJQNxDp3CBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-19T01:51:21.719934Z"},"content_sha256":"e74a9eede7fd15e9d578e13263594ac6ad795a91aebba63cd406910aaf6b187a","schema_version":"1.0","event_id":"sha256:e74a9eede7fd15e9d578e13263594ac6ad795a91aebba63cd406910aaf6b187a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:LGXTZKKK3PTMLU6F7JXTM2BH4M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Discontinuous Transitions Towards Vortex Condensates in Buoyancy-Driven Rotating Turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Andr\\'es J. Aguirre Guzm\\'an, Herman J.H. Clercx, Rudie P.J. Kunnen, Xander M. de Wit","submitted_at":"2021-06-02T13:50:26Z","abstract_excerpt":"Using direct numerical simulations of rotating Rayleigh-B\\'enard convection, we explore the transitions between turbulent states from a 3D flow state towards a quasi-2D condensate known as the large-scale vortex (LSV). We vary the Rayleigh number $Ra$ as control parameter and study the system response (strength of the LSV) in terms of order parameters assessing the energetic content in the flow and the upscale energy flux. By sensitively probing the boundaries of the region of existence of the LSV in parameter space, we find discontinuous transitions and we identify the presence of a hysteresi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.01158","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2106.01158/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":"2026-07-05T04:00:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XdbgxMwtjkuTYbQikuhoZoVNFm3k8gJDTov/DYzxVXPCP2jP8osZ3zlRDd+76m60FAfZn9Xh00clhCeoVehxAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-19T01:51:21.720333Z"},"content_sha256":"53761537545cbfceda11e8973990a154249f8aff5925cb55231ae70505542b33","schema_version":"1.0","event_id":"sha256:53761537545cbfceda11e8973990a154249f8aff5925cb55231ae70505542b33"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LGXTZKKK3PTMLU6F7JXTM2BH4M/bundle.json","state_url":"https://pith.science/pith/LGXTZKKK3PTMLU6F7JXTM2BH4M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LGXTZKKK3PTMLU6F7JXTM2BH4M/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":"2026-07-19T01:51:21Z","links":{"resolver":"https://pith.science/pith/LGXTZKKK3PTMLU6F7JXTM2BH4M","bundle":"https://pith.science/pith/LGXTZKKK3PTMLU6F7JXTM2BH4M/bundle.json","state":"https://pith.science/pith/LGXTZKKK3PTMLU6F7JXTM2BH4M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LGXTZKKK3PTMLU6F7JXTM2BH4M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:LGXTZKKK3PTMLU6F7JXTM2BH4M","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":"2402849b3a4c4adedbef34e9968c2bb67d6af2f7aab7d0ca2cecdbb695852a1e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-02T13:50:26Z","title_canon_sha256":"2e1d99a7fe7cb7c32005f663e7331277c5159ad3457f7bfc90e154d50e7f2bce"},"schema_version":"1.0","source":{"id":"2106.01158","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2106.01158","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"arxiv_version","alias_value":"2106.01158v4","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.01158","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"pith_short_12","alias_value":"LGXTZKKK3PTM","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"pith_short_16","alias_value":"LGXTZKKK3PTMLU6F","created_at":"2026-07-05T04:00:53Z"},{"alias_kind":"pith_short_8","alias_value":"LGXTZKKK","created_at":"2026-07-05T04:00:53Z"}],"graph_snapshots":[{"event_id":"sha256:53761537545cbfceda11e8973990a154249f8aff5925cb55231ae70505542b33","target":"graph","created_at":"2026-07-05T04:00:53Z","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/2106.01158/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Using direct numerical simulations of rotating Rayleigh-B\\'enard convection, we explore the transitions between turbulent states from a 3D flow state towards a quasi-2D condensate known as the large-scale vortex (LSV). We vary the Rayleigh number $Ra$ as control parameter and study the system response (strength of the LSV) in terms of order parameters assessing the energetic content in the flow and the upscale energy flux. By sensitively probing the boundaries of the region of existence of the LSV in parameter space, we find discontinuous transitions and we identify the presence of a hysteresi","authors_text":"Andr\\'es J. Aguirre Guzm\\'an, Herman J.H. Clercx, Rudie P.J. Kunnen, Xander M. de Wit","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-02T13:50:26Z","title":"Discontinuous Transitions Towards Vortex Condensates in Buoyancy-Driven Rotating Turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.01158","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:e74a9eede7fd15e9d578e13263594ac6ad795a91aebba63cd406910aaf6b187a","target":"record","created_at":"2026-07-05T04:00:53Z","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":"2402849b3a4c4adedbef34e9968c2bb67d6af2f7aab7d0ca2cecdbb695852a1e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-02T13:50:26Z","title_canon_sha256":"2e1d99a7fe7cb7c32005f663e7331277c5159ad3457f7bfc90e154d50e7f2bce"},"schema_version":"1.0","source":{"id":"2106.01158","kind":"arxiv","version":4}},"canonical_sha256":"59af3ca94adbe6c5d3c5fa6f366827e31cd74d5633dccc083a2af220d7bc3013","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"59af3ca94adbe6c5d3c5fa6f366827e31cd74d5633dccc083a2af220d7bc3013","first_computed_at":"2026-07-05T04:00:53.491091Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:00:53.491091Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"epmS1+tQV24xzimCCRy6nBH0foh7xFRlZS2dGyvJVg9i9kBdDgseTajRxmop8oZNlgSJD3GuxMjEvX0qcLxEDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:00:53.491540Z","signed_message":"canonical_sha256_bytes"},"source_id":"2106.01158","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e74a9eede7fd15e9d578e13263594ac6ad795a91aebba63cd406910aaf6b187a","sha256:53761537545cbfceda11e8973990a154249f8aff5925cb55231ae70505542b33"],"state_sha256":"b053d4ef84042d7369579f0a930d94e1b9858d7e69d7fd546e29c414d850c474"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+sPtl72R2DlW3aMjZ0lPvF9wNZKV3e/xTp9UBifZE+1TfdD0HzKZEplBgKFFq9X509oiSU7CmkKOlDqbBPTQAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-19T01:51:21.723300Z","bundle_sha256":"7ce06d90141542ad548b713e86e5d8a6c562e12245f6e7e797b02a11087489a7"}}