{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:IVLHAYNGI6MUWDSGSEB2AE2G6I","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":"b76f7f257a0aaba03aec31ef77f16ce17937d02b264f287441806928704baee8","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-02-07T17:25:39Z","title_canon_sha256":"c0223c67788175a86b352901340550229c990cce86ba3cf1a03c1b817de61e73"},"schema_version":"1.0","source":{"id":"2302.03621","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2302.03621","created_at":"2026-07-05T08:49:23Z"},{"alias_kind":"arxiv_version","alias_value":"2302.03621v2","created_at":"2026-07-05T08:49:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.03621","created_at":"2026-07-05T08:49:23Z"},{"alias_kind":"pith_short_12","alias_value":"IVLHAYNGI6MU","created_at":"2026-07-05T08:49:23Z"},{"alias_kind":"pith_short_16","alias_value":"IVLHAYNGI6MUWDSG","created_at":"2026-07-05T08:49:23Z"},{"alias_kind":"pith_short_8","alias_value":"IVLHAYNG","created_at":"2026-07-05T08:49:23Z"}],"graph_snapshots":[{"event_id":"sha256:fb513956b9da1501d2da9b15cf2c52403a7aa6ed0065325f774c0f3dfa8c446e","target":"graph","created_at":"2026-07-05T08:49:23Z","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/2302.03621/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Fully compressible turbulent convection beyond the Oberbeck-Boussinesq limit and anelastic regime is studied in three-dimensional numerical simulations. Superadiabaticity $\\epsilon$ and dissipation number $D$, which measures the strength of stratification of adiabatic equilibria, cause two limits of compressible convection -- nearly top-down-symmetric, strongly superadiabatic and highly top-down-asymmetric, strongly stratified convection. Highest turbulent Mach numbers $M_t$ follow for a symmetric blend of these two limits which we term the fully compressible case. Particularly, the strongly s","authors_text":"John Panickacheril John, J\\\"org Schumacher","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-02-07T17:25:39Z","title":"Strongly superadiabatic and stratified limits of compressible convection"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.03621","kind":"arxiv","version":2},"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":"sha256:67d23b611238265c47eac6ade464688ba55d4e325903a62ed56efa40e2ec317f","target":"record","created_at":"2026-07-05T08:49:23Z","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":"b76f7f257a0aaba03aec31ef77f16ce17937d02b264f287441806928704baee8","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-02-07T17:25:39Z","title_canon_sha256":"c0223c67788175a86b352901340550229c990cce86ba3cf1a03c1b817de61e73"},"schema_version":"1.0","source":{"id":"2302.03621","kind":"arxiv","version":2}},"canonical_sha256":"45567061a647994b0e469103a01346f21f5bbb4cfdb41fadd415d2069bd57146","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"45567061a647994b0e469103a01346f21f5bbb4cfdb41fadd415d2069bd57146","first_computed_at":"2026-07-05T08:49:23.763090Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:49:23.763090Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"b3ZqbX3M8WUZXsj9I+pTy1pwydoJmwR6kF9HziXxhuUnhba+O+2WdCGpPJITH7v7xOGbx13W0ujbr2H0D2ccDA==","signature_status":"signed_v1","signed_at":"2026-07-05T08:49:23.763499Z","signed_message":"canonical_sha256_bytes"},"source_id":"2302.03621","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:67d23b611238265c47eac6ade464688ba55d4e325903a62ed56efa40e2ec317f","sha256:fb513956b9da1501d2da9b15cf2c52403a7aa6ed0065325f774c0f3dfa8c446e"],"state_sha256":"374cdcbb9d7afbf38527d526134ffb5ce02a45440d4f7a386ff883ac31ff41de"}