{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:ZTXC5BDKJY3KYA2RKP6OBAAL7O","short_pith_number":"pith:ZTXC5BDK","schema_version":"1.0","canonical_sha256":"ccee2e846a4e36ac035153fce0800bfba59182af04de72017bbaa3ec30929ef9","source":{"kind":"arxiv","id":"1203.5131","version":2},"attestation_state":"computed","paper":{"title":"Anisotropy and non-universality in scaling laws of the large scale energy spectrum in rotating turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"physics.flu-dyn","authors_text":"Amrik Sen, Annick Pouquet, Duane Rosenberg, Pablo D. Mininni","submitted_at":"2012-03-22T21:24:52Z","abstract_excerpt":"Rapidly rotating turbulent flow is characterized by the emergence of columnar structures that are representative of quasi-two dimensional behavior of the flow. It is known that when energy is injected into the fluid at an intermediate scale $L_f$, it cascades towards smaller as well as larger scales. In this paper we analyze the flow in the \\textit{inverse cascade} range at a small but fixed Rossby number, {$\\mathcal{R}o_f \\approx 0.05$}. Several {numerical simulations with} helical and non-helical forcing functions are considered in periodic boxes with unit aspect ratio. In order to resolve t"},"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":"1203.5131","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2012-03-22T21:24:52Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"7356a8b25d6a992094bf02b9eb7b1f35f24c9b68a59c76fd1110b3387029e33d","abstract_canon_sha256":"3323c7d1be7ef49a9937b375b87f68308e4abcaba243d0d97214f6081264a9c2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:04.205113Z","signature_b64":"5LCJrNe3ar9izj0jUX/7i44xdpQBj3odVG7cExcVoS9YX3YqkWFszK/eoJxG2+mW4gQmPUxPjjQvEHqFb9QnCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ccee2e846a4e36ac035153fce0800bfba59182af04de72017bbaa3ec30929ef9","last_reissued_at":"2026-05-18T01:58:04.204638Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:04.204638Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anisotropy and non-universality in scaling laws of the large scale energy spectrum in rotating turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"physics.flu-dyn","authors_text":"Amrik Sen, Annick Pouquet, Duane Rosenberg, Pablo D. Mininni","submitted_at":"2012-03-22T21:24:52Z","abstract_excerpt":"Rapidly rotating turbulent flow is characterized by the emergence of columnar structures that are representative of quasi-two dimensional behavior of the flow. It is known that when energy is injected into the fluid at an intermediate scale $L_f$, it cascades towards smaller as well as larger scales. In this paper we analyze the flow in the \\textit{inverse cascade} range at a small but fixed Rossby number, {$\\mathcal{R}o_f \\approx 0.05$}. Several {numerical simulations with} helical and non-helical forcing functions are considered in periodic boxes with unit aspect ratio. In order to resolve t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.5131","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":""},"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":"1203.5131","created_at":"2026-05-18T01:58:04.204712+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.5131v2","created_at":"2026-05-18T01:58:04.204712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.5131","created_at":"2026-05-18T01:58:04.204712+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZTXC5BDKJY3K","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZTXC5BDKJY3KYA2R","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZTXC5BDK","created_at":"2026-05-18T12:27:30.460161+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/ZTXC5BDKJY3KYA2RKP6OBAAL7O","json":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O.json","graph_json":"https://pith.science/api/pith-number/ZTXC5BDKJY3KYA2RKP6OBAAL7O/graph.json","events_json":"https://pith.science/api/pith-number/ZTXC5BDKJY3KYA2RKP6OBAAL7O/events.json","paper":"https://pith.science/paper/ZTXC5BDK"},"agent_actions":{"view_html":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O","download_json":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O.json","view_paper":"https://pith.science/paper/ZTXC5BDK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.5131&json=true","fetch_graph":"https://pith.science/api/pith-number/ZTXC5BDKJY3KYA2RKP6OBAAL7O/graph.json","fetch_events":"https://pith.science/api/pith-number/ZTXC5BDKJY3KYA2RKP6OBAAL7O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O/action/storage_attestation","attest_author":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O/action/author_attestation","sign_citation":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O/action/citation_signature","submit_replication":"https://pith.science/pith/ZTXC5BDKJY3KYA2RKP6OBAAL7O/action/replication_record"}},"created_at":"2026-05-18T01:58:04.204712+00:00","updated_at":"2026-05-18T01:58:04.204712+00:00"}