{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:MGY4AGXE22F47ST5WB7DFV3M2I","short_pith_number":"pith:MGY4AGXE","schema_version":"1.0","canonical_sha256":"61b1c01ae4d68bcfca7db07e32d76cd2286de6c6b822d7966663b5e504363929","source":{"kind":"arxiv","id":"2206.04587","version":2},"attestation_state":"computed","paper":{"title":"Anisotropic flow and flow fluctuations of identified hadrons in Pb$-$Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"ALICE Collaboration","submitted_at":"2022-06-09T16:09:04Z","abstract_excerpt":"The first measurements of elliptic flow of $\\pi^\\pm$, ${\\rm K}^\\pm$, p+$\\overline{\\rm p}$, ${\\rm K_{S}^0}$, $\\Lambda$+$\\overline{\\Lambda}$, $\\phi$, $\\Xi^-$+$\\Xi^+$, and $\\Omega^-$+$\\Omega^+$ using multiparticle cumulants in Pb$-$Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV are presented. Results obtained with two- ($v_2\\{2\\}$) and four-particle cumulants ($v_2\\{4\\}$) are shown as a function of transverse momentum, $p_{\\rm T}$, for various collision centrality intervals. Combining the data for both $v_2\\{2\\}$ and $v_2\\{4\\}$ also allows us to report the first measurements of the mean elliptic"},"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":"2206.04587","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2022-06-09T16:09:04Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"a17109af274f9332f50bdaf1d0fd68ee4c1cc99eb597566e7ea82cbbefcb25d4","abstract_canon_sha256":"eb0d0cb03dd37d26d4c62d60a98b04b935059745160806da3e8d966071bcf1ad"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:21:03.587204Z","signature_b64":"OhJ803K65lzdPtIQZ1QO0dMRONl790s4IxpqkYUUCFHYFNGIKZSgCoX7qg2CLmd/qONWdPUnCuIksrvl2xGfAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61b1c01ae4d68bcfca7db07e32d76cd2286de6c6b822d7966663b5e504363929","last_reissued_at":"2026-07-05T06:21:03.586861Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:21:03.586861Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anisotropic flow and flow fluctuations of identified hadrons in Pb$-$Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"ALICE Collaboration","submitted_at":"2022-06-09T16:09:04Z","abstract_excerpt":"The first measurements of elliptic flow of $\\pi^\\pm$, ${\\rm K}^\\pm$, p+$\\overline{\\rm p}$, ${\\rm K_{S}^0}$, $\\Lambda$+$\\overline{\\Lambda}$, $\\phi$, $\\Xi^-$+$\\Xi^+$, and $\\Omega^-$+$\\Omega^+$ using multiparticle cumulants in Pb$-$Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV are presented. Results obtained with two- ($v_2\\{2\\}$) and four-particle cumulants ($v_2\\{4\\}$) are shown as a function of transverse momentum, $p_{\\rm T}$, for various collision centrality intervals. Combining the data for both $v_2\\{2\\}$ and $v_2\\{4\\}$ also allows us to report the first measurements of the mean elliptic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.04587","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/2206.04587/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":"2206.04587","created_at":"2026-07-05T06:21:03.586917+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.04587v2","created_at":"2026-07-05T06:21:03.586917+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.04587","created_at":"2026-07-05T06:21:03.586917+00:00"},{"alias_kind":"pith_short_12","alias_value":"MGY4AGXE22F4","created_at":"2026-07-05T06:21:03.586917+00:00"},{"alias_kind":"pith_short_16","alias_value":"MGY4AGXE22F47ST5","created_at":"2026-07-05T06:21:03.586917+00:00"},{"alias_kind":"pith_short_8","alias_value":"MGY4AGXE","created_at":"2026-07-05T06:21:03.586917+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.27254","citing_title":"Species-Resolved Scaling of Azimuthal Anisotropy: Constraining Attenuation, Collective Expansion, and Hadronic Dynamics in Hydrodynamic Simulations","ref_index":22,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I","json":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I.json","graph_json":"https://pith.science/api/pith-number/MGY4AGXE22F47ST5WB7DFV3M2I/graph.json","events_json":"https://pith.science/api/pith-number/MGY4AGXE22F47ST5WB7DFV3M2I/events.json","paper":"https://pith.science/paper/MGY4AGXE"},"agent_actions":{"view_html":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I","download_json":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I.json","view_paper":"https://pith.science/paper/MGY4AGXE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.04587&json=true","fetch_graph":"https://pith.science/api/pith-number/MGY4AGXE22F47ST5WB7DFV3M2I/graph.json","fetch_events":"https://pith.science/api/pith-number/MGY4AGXE22F47ST5WB7DFV3M2I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I/action/storage_attestation","attest_author":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I/action/author_attestation","sign_citation":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I/action/citation_signature","submit_replication":"https://pith.science/pith/MGY4AGXE22F47ST5WB7DFV3M2I/action/replication_record"}},"created_at":"2026-07-05T06:21:03.586917+00:00","updated_at":"2026-07-05T06:21:03.586917+00:00"}