{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:SRE246UT2R6JP6QTD445YEGKLQ","short_pith_number":"pith:SRE246UT","schema_version":"1.0","canonical_sha256":"9449ae7a93d47c97fa131f39dc10ca5c1411292434219032201ce9678d3da45c","source":{"kind":"arxiv","id":"1304.3753","version":2},"attestation_state":"computed","paper":{"title":"Second order viscous corrections to the harmonic spectrum in heavy ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Derek Teaney, Li Yan","submitted_at":"2013-04-13T00:31:02Z","abstract_excerpt":"We calculate the second order viscous correction to the kinetic distribution, $\\delta f_{(2)}$, and use this result in a hydrodynamic simulation of heavy ion collisions to determine the complete second order correction to the harmonic spectrum, $v_n$. At leading order in a conformal fluid, the first viscous correction is determined by one scalar function, $\\chi_{0p}$. One moment of this scalar function is constrained by the shear viscosity. At second order in a conformal fluid, we find that $\\delta f(\\p)$ can be characterized by two scalar functions of momentum, $\\chi_{1p}$ and $\\chi_{2p}$. Th"},"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":"1304.3753","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-04-13T00:31:02Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"272ebc021ba7f017877e2bf058b648a2c10e539c288224be251aea31e0b4e2ee","abstract_canon_sha256":"d174a7b2557fcc4393ae55b6c426b58cbcab24209d2ced3d7d04e027f03b157d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:02:21.108833Z","signature_b64":"uF0atf66MfKV0SlJBlsguEbzF2YDGo7PapYtxOga7cKhmcGhqDwDUOY/BqbsNMxA7iDhrFuuKMgBGG3gVDYzDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9449ae7a93d47c97fa131f39dc10ca5c1411292434219032201ce9678d3da45c","last_reissued_at":"2026-05-18T03:02:21.108128Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:02:21.108128Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Second order viscous corrections to the harmonic spectrum in heavy ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Derek Teaney, Li Yan","submitted_at":"2013-04-13T00:31:02Z","abstract_excerpt":"We calculate the second order viscous correction to the kinetic distribution, $\\delta f_{(2)}$, and use this result in a hydrodynamic simulation of heavy ion collisions to determine the complete second order correction to the harmonic spectrum, $v_n$. At leading order in a conformal fluid, the first viscous correction is determined by one scalar function, $\\chi_{0p}$. One moment of this scalar function is constrained by the shear viscosity. At second order in a conformal fluid, we find that $\\delta f(\\p)$ can be characterized by two scalar functions of momentum, $\\chi_{1p}$ and $\\chi_{2p}$. Th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.3753","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":"1304.3753","created_at":"2026-05-18T03:02:21.108219+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.3753v2","created_at":"2026-05-18T03:02:21.108219+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.3753","created_at":"2026-05-18T03:02:21.108219+00:00"},{"alias_kind":"pith_short_12","alias_value":"SRE246UT2R6J","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_16","alias_value":"SRE246UT2R6JP6QT","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_8","alias_value":"SRE246UT","created_at":"2026-05-18T12:27:59.945178+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/SRE246UT2R6JP6QTD445YEGKLQ","json":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ.json","graph_json":"https://pith.science/api/pith-number/SRE246UT2R6JP6QTD445YEGKLQ/graph.json","events_json":"https://pith.science/api/pith-number/SRE246UT2R6JP6QTD445YEGKLQ/events.json","paper":"https://pith.science/paper/SRE246UT"},"agent_actions":{"view_html":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ","download_json":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ.json","view_paper":"https://pith.science/paper/SRE246UT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.3753&json=true","fetch_graph":"https://pith.science/api/pith-number/SRE246UT2R6JP6QTD445YEGKLQ/graph.json","fetch_events":"https://pith.science/api/pith-number/SRE246UT2R6JP6QTD445YEGKLQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ/action/storage_attestation","attest_author":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ/action/author_attestation","sign_citation":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ/action/citation_signature","submit_replication":"https://pith.science/pith/SRE246UT2R6JP6QTD445YEGKLQ/action/replication_record"}},"created_at":"2026-05-18T03:02:21.108219+00:00","updated_at":"2026-05-18T03:02:21.108219+00:00"}