{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:VIOKSIZD3PWS5N32XRGYQL745P","short_pith_number":"pith:VIOKSIZD","schema_version":"1.0","canonical_sha256":"aa1ca92323dbed2eb77abc4d882ffcebe3dc08e814f7843249d4d7e23bbf8cc0","source":{"kind":"arxiv","id":"1402.0371","version":1},"attestation_state":"computed","paper":{"title":"Detrended Structure-Function in Fully Developed Turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"physics.flu-dyn","authors_text":"Y.X. Huang","submitted_at":"2014-02-03T12:48:15Z","abstract_excerpt":"The classical structure-function (SF) method in fully developed turbulence or for scaling processes in general is influenced by large-scale energetic structures, known as infrared effect. Therefore, the extracted scaling exponents $\\zeta(n)$ might be biased due to this effect. In this paper, a detrended structure-function (DSF) method is proposed to extract scaling exponents by constraining the influence of large-scale structures. This is accomplished by removing a $1$st-order polynomial fitting within a window size $\\ell$ before calculating the velocity increment. By doing so, the scales larg"},"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":"1402.0371","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-02-03T12:48:15Z","cross_cats_sorted":["physics.data-an"],"title_canon_sha256":"51ff6f4ad838a1eb1e2f1e4cf73c54cd6e4e16b6018b307f53c490e89f987a5d","abstract_canon_sha256":"82abdc64bf79f7173fa9c18810d0180956eb25fe9c6697020a72fa9381a13b24"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:44:53.422938Z","signature_b64":"jXDXHYoiZixu5iWfX4OypLfAVukv7teAZ43Ow8ZzIjtih+l0n/Vj6GSpJPqV0hsb/QqiizfMfauKQzsv7x/KBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa1ca92323dbed2eb77abc4d882ffcebe3dc08e814f7843249d4d7e23bbf8cc0","last_reissued_at":"2026-05-18T01:44:53.422323Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:44:53.422323Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Detrended Structure-Function in Fully Developed Turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"physics.flu-dyn","authors_text":"Y.X. Huang","submitted_at":"2014-02-03T12:48:15Z","abstract_excerpt":"The classical structure-function (SF) method in fully developed turbulence or for scaling processes in general is influenced by large-scale energetic structures, known as infrared effect. Therefore, the extracted scaling exponents $\\zeta(n)$ might be biased due to this effect. In this paper, a detrended structure-function (DSF) method is proposed to extract scaling exponents by constraining the influence of large-scale structures. This is accomplished by removing a $1$st-order polynomial fitting within a window size $\\ell$ before calculating the velocity increment. By doing so, the scales larg"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.0371","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":""},"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":"1402.0371","created_at":"2026-05-18T01:44:53.422406+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.0371v1","created_at":"2026-05-18T01:44:53.422406+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.0371","created_at":"2026-05-18T01:44:53.422406+00:00"},{"alias_kind":"pith_short_12","alias_value":"VIOKSIZD3PWS","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"VIOKSIZD3PWS5N32","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"VIOKSIZD","created_at":"2026-05-18T12:28:54.890064+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/VIOKSIZD3PWS5N32XRGYQL745P","json":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P.json","graph_json":"https://pith.science/api/pith-number/VIOKSIZD3PWS5N32XRGYQL745P/graph.json","events_json":"https://pith.science/api/pith-number/VIOKSIZD3PWS5N32XRGYQL745P/events.json","paper":"https://pith.science/paper/VIOKSIZD"},"agent_actions":{"view_html":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P","download_json":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P.json","view_paper":"https://pith.science/paper/VIOKSIZD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.0371&json=true","fetch_graph":"https://pith.science/api/pith-number/VIOKSIZD3PWS5N32XRGYQL745P/graph.json","fetch_events":"https://pith.science/api/pith-number/VIOKSIZD3PWS5N32XRGYQL745P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P/action/storage_attestation","attest_author":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P/action/author_attestation","sign_citation":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P/action/citation_signature","submit_replication":"https://pith.science/pith/VIOKSIZD3PWS5N32XRGYQL745P/action/replication_record"}},"created_at":"2026-05-18T01:44:53.422406+00:00","updated_at":"2026-05-18T01:44:53.422406+00:00"}