{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:VGLSINXN4P6P2UCKJELGIPBQBG","short_pith_number":"pith:VGLSINXN","schema_version":"1.0","canonical_sha256":"a9972436ede3fcfd504a4916643c30099f8af13c6872173e29ecfff4cc0da47b","source":{"kind":"arxiv","id":"2505.13892","version":1},"attestation_state":"computed","paper":{"title":"Investigating quarkonium collectivity in heavy-ion collisions","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-ex","authors_text":"Victor Valencia Torres","submitted_at":"2025-05-20T03:55:18Z","abstract_excerpt":"The quark-gluon plasma (QGP) produced in ultrarelativistic heavy-ion collisions has exhibited properties of a mostly perfect fluid. These properties can be observed through the hydrodynamic expansion of the QGP. Experimentally, this was established by measuring azimuthal anisotropies in the final state, known as elliptic flow ($v_2$) or higher order harmonics such as triangular flow ($v_3$). These Fourier harmonic coefficients have been extensively measured in past experiments using inclusive charged particles or identified particles in the soft sector. Interestingly, measuring such coefficien"},"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":"2505.13892","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-ex","submitted_at":"2025-05-20T03:55:18Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"98adae5dd6496c1cccf53cc3e8a62ed0403069dafc89deec6545259c3b135a48","abstract_canon_sha256":"27f580258dbec5c08dc3e328c2d7bf42179ca7092a907c6030298afb1286efde"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:05:52.435014Z","signature_b64":"xuA6KV0m1r9a/WkgzDh5FeBUSEug37V9HUhRPWb3Qv4+jlEpXMUxOIqpkX4Rkl9DzEMGYNpdSU6hsqDK/OtmCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a9972436ede3fcfd504a4916643c30099f8af13c6872173e29ecfff4cc0da47b","last_reissued_at":"2026-07-05T11:05:52.434555Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:05:52.434555Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Investigating quarkonium collectivity in heavy-ion collisions","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-ex","authors_text":"Victor Valencia Torres","submitted_at":"2025-05-20T03:55:18Z","abstract_excerpt":"The quark-gluon plasma (QGP) produced in ultrarelativistic heavy-ion collisions has exhibited properties of a mostly perfect fluid. These properties can be observed through the hydrodynamic expansion of the QGP. Experimentally, this was established by measuring azimuthal anisotropies in the final state, known as elliptic flow ($v_2$) or higher order harmonics such as triangular flow ($v_3$). These Fourier harmonic coefficients have been extensively measured in past experiments using inclusive charged particles or identified particles in the soft sector. Interestingly, measuring such coefficien"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.13892","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.13892/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":"2505.13892","created_at":"2026-07-05T11:05:52.434631+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.13892v1","created_at":"2026-07-05T11:05:52.434631+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.13892","created_at":"2026-07-05T11:05:52.434631+00:00"},{"alias_kind":"pith_short_12","alias_value":"VGLSINXN4P6P","created_at":"2026-07-05T11:05:52.434631+00:00"},{"alias_kind":"pith_short_16","alias_value":"VGLSINXN4P6P2UCK","created_at":"2026-07-05T11:05:52.434631+00:00"},{"alias_kind":"pith_short_8","alias_value":"VGLSINXN","created_at":"2026-07-05T11:05:52.434631+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.07169","citing_title":"Bayesian Inference of Heavy-Quark Dissipation and Jet Transport Parameters from D-Meson observables in heavy-ion collisions at the LHC energies","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG","json":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG.json","graph_json":"https://pith.science/api/pith-number/VGLSINXN4P6P2UCKJELGIPBQBG/graph.json","events_json":"https://pith.science/api/pith-number/VGLSINXN4P6P2UCKJELGIPBQBG/events.json","paper":"https://pith.science/paper/VGLSINXN"},"agent_actions":{"view_html":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG","download_json":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG.json","view_paper":"https://pith.science/paper/VGLSINXN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.13892&json=true","fetch_graph":"https://pith.science/api/pith-number/VGLSINXN4P6P2UCKJELGIPBQBG/graph.json","fetch_events":"https://pith.science/api/pith-number/VGLSINXN4P6P2UCKJELGIPBQBG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG/action/storage_attestation","attest_author":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG/action/author_attestation","sign_citation":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG/action/citation_signature","submit_replication":"https://pith.science/pith/VGLSINXN4P6P2UCKJELGIPBQBG/action/replication_record"}},"created_at":"2026-07-05T11:05:52.434631+00:00","updated_at":"2026-07-05T11:05:52.434631+00:00"}