{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:UEU3ODVHJ7WESAP4Y62SACXPX3","short_pith_number":"pith:UEU3ODVH","schema_version":"1.0","canonical_sha256":"a129b70ea74fec4901fcc7b5200aefbef589580b76ae1679b050c5c3256f3c3c","source":{"kind":"arxiv","id":"0710.5932","version":2},"attestation_state":"computed","paper":{"title":"Simulating elliptic flow with viscous hydrodynamics","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"D. Teaney, K. Dusling","submitted_at":"2007-10-31T19:21:31Z","abstract_excerpt":"In this work we simulate a viscous hydrodynamical model of non-central Au-Au collisions in 2+1 dimensions, assuming longitudinal boost invariance. The model fluid equations were proposed by \\\"{O}ttinger and Grmela \\cite{OG}. Freezeout is signaled when the viscous corrections become large relative to the ideal terms. Then viscous corrections to the transverse momentum and differential elliptic flow spectra are calculated. When viscous corrections to the thermal distribution function are not included, the effects of viscosity on elliptic flow are modest. However, when these corrections are inclu"},"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":"0710.5932","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2007-10-31T19:21:31Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"30ab5cba2f0d5c57fadbce04d372e47044008c67574f53e4c41e5d9062b714db","abstract_canon_sha256":"3298a3d354edc1122ad1bee66e92c79fef9df78647d64854205d886dd424497c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:24:58.007630Z","signature_b64":"BeO1PR5kS01p3SnOOEw4ToGW15GF77necMiybUHUUQr7Nju4/ycUqDtDfVZOGJ1m6g6evssJY/6kYGdQHFGeCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a129b70ea74fec4901fcc7b5200aefbef589580b76ae1679b050c5c3256f3c3c","last_reissued_at":"2026-07-04T17:24:58.007194Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:24:58.007194Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulating elliptic flow with viscous hydrodynamics","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"D. Teaney, K. Dusling","submitted_at":"2007-10-31T19:21:31Z","abstract_excerpt":"In this work we simulate a viscous hydrodynamical model of non-central Au-Au collisions in 2+1 dimensions, assuming longitudinal boost invariance. The model fluid equations were proposed by \\\"{O}ttinger and Grmela \\cite{OG}. Freezeout is signaled when the viscous corrections become large relative to the ideal terms. Then viscous corrections to the transverse momentum and differential elliptic flow spectra are calculated. When viscous corrections to the thermal distribution function are not included, the effects of viscosity on elliptic flow are modest. However, when these corrections are inclu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0710.5932","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/0710.5932/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":"0710.5932","created_at":"2026-07-04T17:24:58.007261+00:00"},{"alias_kind":"arxiv_version","alias_value":"0710.5932v2","created_at":"2026-07-04T17:24:58.007261+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0710.5932","created_at":"2026-07-04T17:24:58.007261+00:00"},{"alias_kind":"pith_short_12","alias_value":"UEU3ODVHJ7WE","created_at":"2026-07-04T17:24:58.007261+00:00"},{"alias_kind":"pith_short_16","alias_value":"UEU3ODVHJ7WESAP4","created_at":"2026-07-04T17:24:58.007261+00:00"},{"alias_kind":"pith_short_8","alias_value":"UEU3ODVH","created_at":"2026-07-04T17:24:58.007261+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.13646","citing_title":"Observable Dependence of Viscous Corrections in QGP: Heavy Quarks and Dileptons in Chapman--Enskog Theory","ref_index":18,"is_internal_anchor":true},{"citing_arxiv_id":"2404.09767","citing_title":"Electrical conductivity of QGP with quasiparticle quarks and Gribov gluon","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2601.14967","citing_title":"Shear and bulk viscosities of the gluon plasma across the transition temperature from lattice QCD","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3","json":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3.json","graph_json":"https://pith.science/api/pith-number/UEU3ODVHJ7WESAP4Y62SACXPX3/graph.json","events_json":"https://pith.science/api/pith-number/UEU3ODVHJ7WESAP4Y62SACXPX3/events.json","paper":"https://pith.science/paper/UEU3ODVH"},"agent_actions":{"view_html":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3","download_json":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3.json","view_paper":"https://pith.science/paper/UEU3ODVH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0710.5932&json=true","fetch_graph":"https://pith.science/api/pith-number/UEU3ODVHJ7WESAP4Y62SACXPX3/graph.json","fetch_events":"https://pith.science/api/pith-number/UEU3ODVHJ7WESAP4Y62SACXPX3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3/action/storage_attestation","attest_author":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3/action/author_attestation","sign_citation":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3/action/citation_signature","submit_replication":"https://pith.science/pith/UEU3ODVHJ7WESAP4Y62SACXPX3/action/replication_record"}},"created_at":"2026-07-04T17:24:58.007261+00:00","updated_at":"2026-07-04T17:24:58.007261+00:00"}