{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:QUUOWWKYPXY7ZC4LFIFYMB4VZC","short_pith_number":"pith:QUUOWWKY","schema_version":"1.0","canonical_sha256":"8528eb59587df1fc8b8b2a0b860795c8a74f23f69e75746910f0db9ddcf9f2a8","source":{"kind":"arxiv","id":"1910.13978","version":2},"attestation_state":"computed","paper":{"title":"Transverse momentum and process dependent azimuthal anisotropies in $\\sqrt{s_{\\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"ATLAS Collaboration","submitted_at":"2019-10-30T16:48:46Z","abstract_excerpt":"The azimuthal anisotropy of charged particles produced in $\\sqrt{s_{\\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions is measured with the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $165$ $\\mathrm{nb}^{-1}$ that was collected in 2016. Azimuthal anisotropy coefficients, elliptic $v_2$ and triangular $v_3$, extracted using two-particle correlations with a non-flow template fit procedure, are presented as a function of particle transverse momentum ($p_\\mathrm{T}$) between $0.5$ and $50$ GeV. The $v_2$ results are also reported as a function of centrality in three differ"},"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":"1910.13978","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2019-10-30T16:48:46Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"4819f3ab1e0b6390c999edb6858ebc34f55680cc6c6577865e7143fbba790ab4","abstract_canon_sha256":"c0d23320489d890e8824407c2b5f4c58c4b30eec7fa9773da64d0683d5d0a243"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:49:00.829619Z","signature_b64":"KyPbZG/VYHHe+oGysmL/gwquR6Den9m9LX+smJ0Hgn4wOXC1ARMNKuzw9fjtYk/vdoDZx4pLizoH8PfAeQlMBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8528eb59587df1fc8b8b2a0b860795c8a74f23f69e75746910f0db9ddcf9f2a8","last_reissued_at":"2026-07-05T00:49:00.829199Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:49:00.829199Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transverse momentum and process dependent azimuthal anisotropies in $\\sqrt{s_{\\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"ATLAS Collaboration","submitted_at":"2019-10-30T16:48:46Z","abstract_excerpt":"The azimuthal anisotropy of charged particles produced in $\\sqrt{s_{\\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions is measured with the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $165$ $\\mathrm{nb}^{-1}$ that was collected in 2016. Azimuthal anisotropy coefficients, elliptic $v_2$ and triangular $v_3$, extracted using two-particle correlations with a non-flow template fit procedure, are presented as a function of particle transverse momentum ($p_\\mathrm{T}$) between $0.5$ and $50$ GeV. The $v_2$ results are also reported as a function of centrality in three differ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1910.13978","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/1910.13978/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":"1910.13978","created_at":"2026-07-05T00:49:00.829259+00:00"},{"alias_kind":"arxiv_version","alias_value":"1910.13978v2","created_at":"2026-07-05T00:49:00.829259+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1910.13978","created_at":"2026-07-05T00:49:00.829259+00:00"},{"alias_kind":"pith_short_12","alias_value":"QUUOWWKYPXY7","created_at":"2026-07-05T00:49:00.829259+00:00"},{"alias_kind":"pith_short_16","alias_value":"QUUOWWKYPXY7ZC4L","created_at":"2026-07-05T00:49:00.829259+00:00"},{"alias_kind":"pith_short_8","alias_value":"QUUOWWKY","created_at":"2026-07-05T00:49:00.829259+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.10258","citing_title":"Nonflow Subtraction Beyond Two-Particle Correlations","ref_index":19,"is_internal_anchor":false},{"citing_arxiv_id":"2504.02638","citing_title":"Characterization of nuclear breakup as a function of hard-scattering kinematics using dijets measured by ATLAS in $p$+Pb collisions","ref_index":42,"is_internal_anchor":false},{"citing_arxiv_id":"2509.19430","citing_title":"Bayesian Constraints on Pre-Equilibrium Jet Quenching and Predictions for Oxygen Collisions","ref_index":29,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC","json":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC.json","graph_json":"https://pith.science/api/pith-number/QUUOWWKYPXY7ZC4LFIFYMB4VZC/graph.json","events_json":"https://pith.science/api/pith-number/QUUOWWKYPXY7ZC4LFIFYMB4VZC/events.json","paper":"https://pith.science/paper/QUUOWWKY"},"agent_actions":{"view_html":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC","download_json":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC.json","view_paper":"https://pith.science/paper/QUUOWWKY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1910.13978&json=true","fetch_graph":"https://pith.science/api/pith-number/QUUOWWKYPXY7ZC4LFIFYMB4VZC/graph.json","fetch_events":"https://pith.science/api/pith-number/QUUOWWKYPXY7ZC4LFIFYMB4VZC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC/action/storage_attestation","attest_author":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC/action/author_attestation","sign_citation":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC/action/citation_signature","submit_replication":"https://pith.science/pith/QUUOWWKYPXY7ZC4LFIFYMB4VZC/action/replication_record"}},"created_at":"2026-07-05T00:49:00.829259+00:00","updated_at":"2026-07-05T00:49:00.829259+00:00"}