{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:3C2JMIDGP3K4KGJFQWOBRUKBPB","short_pith_number":"pith:3C2JMIDG","schema_version":"1.0","canonical_sha256":"d8b49620667ed5c51925859c18d1417863c686c3756df9d26306d4cb2d64d2e4","source":{"kind":"arxiv","id":"2103.08374","version":2},"attestation_state":"computed","paper":{"title":"Diffusion-free scaling in rotating spherical Rayleigh-B\\'enard convection","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.geo-ph"],"primary_cat":"physics.flu-dyn","authors_text":"Detlef Lohse, Guiquan Wang, Luca Santelli, Richard J. A. M. Stevens, Roberto Verzicco","submitted_at":"2021-03-15T13:26:10Z","abstract_excerpt":"Direct numerical simulations are employed to reveal three distinctly different flow regions in rotating spherical Rayleigh-B\\'enard convection. In the low-latitude region $\\mathrm{I}$ vertical (parallel to the axis of rotation) convective columns are generated between the hot inner and the cold outer sphere. The mid-latitude region $\\mathrm{II}$ is dominated by vertically aligned convective columns formed between the Northern and Southern hemispheres of the outer sphere. The diffusion-free scaling, which indicates bulk-dominated convection, originates from this mid-latitude region. In the equa"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2103.08374","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-03-15T13:26:10Z","cross_cats_sorted":["physics.geo-ph"],"title_canon_sha256":"48ca6ba1c11c034a80a25b4cce1193f4bb8f5b3d3258d3d0b6d7f8cee8e17643","abstract_canon_sha256":"7831d8d123296f94850489d76a9e477e0b39e2a67ca24666a79299fde2c7cb20"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:24:56.570803Z","signature_b64":"UYfO7QTXUR5NwWlcwrHeQ8erM+dxcUwZUtG6FJWIUtcdSGYiqn1MVdDbHWfTyF9X9VN4icHm3QGN6Ee4zINVCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8b49620667ed5c51925859c18d1417863c686c3756df9d26306d4cb2d64d2e4","last_reissued_at":"2026-07-05T03:24:56.570381Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:24:56.570381Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Diffusion-free scaling in rotating spherical Rayleigh-B\\'enard convection","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.geo-ph"],"primary_cat":"physics.flu-dyn","authors_text":"Detlef Lohse, Guiquan Wang, Luca Santelli, Richard J. A. M. Stevens, Roberto Verzicco","submitted_at":"2021-03-15T13:26:10Z","abstract_excerpt":"Direct numerical simulations are employed to reveal three distinctly different flow regions in rotating spherical Rayleigh-B\\'enard convection. In the low-latitude region $\\mathrm{I}$ vertical (parallel to the axis of rotation) convective columns are generated between the hot inner and the cold outer sphere. The mid-latitude region $\\mathrm{II}$ is dominated by vertically aligned convective columns formed between the Northern and Southern hemispheres of the outer sphere. The diffusion-free scaling, which indicates bulk-dominated convection, originates from this mid-latitude region. In the equa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.08374","kind":"arxiv","version":2},"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/2103.08374/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2103.08374","created_at":"2026-07-05T03:24:56.570448+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.08374v2","created_at":"2026-07-05T03:24:56.570448+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.08374","created_at":"2026-07-05T03:24:56.570448+00:00"},{"alias_kind":"pith_short_12","alias_value":"3C2JMIDGP3K4","created_at":"2026-07-05T03:24:56.570448+00:00"},{"alias_kind":"pith_short_16","alias_value":"3C2JMIDGP3K4KGJF","created_at":"2026-07-05T03:24:56.570448+00:00"},{"alias_kind":"pith_short_8","alias_value":"3C2JMIDG","created_at":"2026-07-05T03:24:56.570448+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB","json":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB.json","graph_json":"https://pith.science/api/pith-number/3C2JMIDGP3K4KGJFQWOBRUKBPB/graph.json","events_json":"https://pith.science/api/pith-number/3C2JMIDGP3K4KGJFQWOBRUKBPB/events.json","paper":"https://pith.science/paper/3C2JMIDG"},"agent_actions":{"view_html":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB","download_json":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB.json","view_paper":"https://pith.science/paper/3C2JMIDG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.08374&json=true","fetch_graph":"https://pith.science/api/pith-number/3C2JMIDGP3K4KGJFQWOBRUKBPB/graph.json","fetch_events":"https://pith.science/api/pith-number/3C2JMIDGP3K4KGJFQWOBRUKBPB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB/action/storage_attestation","attest_author":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB/action/author_attestation","sign_citation":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB/action/citation_signature","submit_replication":"https://pith.science/pith/3C2JMIDGP3K4KGJFQWOBRUKBPB/action/replication_record"}},"created_at":"2026-07-05T03:24:56.570448+00:00","updated_at":"2026-07-05T03:24:56.570448+00:00"}