{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:NLKR76G6JKOTGY5O3KIS27PRLB","short_pith_number":"pith:NLKR76G6","schema_version":"1.0","canonical_sha256":"6ad51ff8de4a9d3363aeda912d7df1585fd62a654c6ca444fc58d4d0f40efb7b","source":{"kind":"arxiv","id":"1709.03089","version":3},"attestation_state":"computed","paper":{"title":"Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\\mathrm{TeV}$ 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":"2017-09-10T12:20:17Z","abstract_excerpt":"The modification of the production of $J/\\psi$, $\\psi(\\mathrm{2S})$, and $\\mit{\\Upsilon}(n\\mathrm{S})$ ($n = 1, 2, 3$) in $p$+Pb collisions with respect to their production in $pp$ collisions has been studied. The $p$+Pb and $pp$ datasets used in this paper correspond to integrated luminosities of $28$ $\\mathrm{nb}^{-1}$ and $25$ $\\mathrm{pb}^{-1}$ respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. The quarkonium states are reconstructed in the dimuon decay channel. The yields of $J/\\psi$ and $\\psi(\\mathrm{2S"},"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":"1709.03089","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2017-09-10T12:20:17Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"b433f6d03b46cacbfca4aa3762cf594fd03f0648cb5bf2c757fa95454bece217","abstract_canon_sha256":"d7e4d1ff608e1044a2429e717e89dab2dd47a277af07553f20ec6cb959db16f4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:05.703761Z","signature_b64":"6VUqDFxZkI2s+ziyuaL1cO99cGEKJBnUUobDf+upwEG1eA92u2jFb3wMAnJS1J4/GIjgJY6MyvGf+akq9fyXCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ad51ff8de4a9d3363aeda912d7df1585fd62a654c6ca444fc58d4d0f40efb7b","last_reissued_at":"2026-05-18T00:22:05.703137Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:05.703137Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\\mathrm{TeV}$ 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":"2017-09-10T12:20:17Z","abstract_excerpt":"The modification of the production of $J/\\psi$, $\\psi(\\mathrm{2S})$, and $\\mit{\\Upsilon}(n\\mathrm{S})$ ($n = 1, 2, 3$) in $p$+Pb collisions with respect to their production in $pp$ collisions has been studied. The $p$+Pb and $pp$ datasets used in this paper correspond to integrated luminosities of $28$ $\\mathrm{nb}^{-1}$ and $25$ $\\mathrm{pb}^{-1}$ respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. The quarkonium states are reconstructed in the dimuon decay channel. The yields of $J/\\psi$ and $\\psi(\\mathrm{2S"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.03089","kind":"arxiv","version":3},"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":"1709.03089","created_at":"2026-05-18T00:22:05.703235+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.03089v3","created_at":"2026-05-18T00:22:05.703235+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.03089","created_at":"2026-05-18T00:22:05.703235+00:00"},{"alias_kind":"pith_short_12","alias_value":"NLKR76G6JKOT","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_16","alias_value":"NLKR76G6JKOTGY5O","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_8","alias_value":"NLKR76G6","created_at":"2026-05-18T12:31:31.346846+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.31357","citing_title":"Signals of New Resonances from Di-Lepton Non-Universality in the Bottomonium Mass Region at the Large Hadron Collider","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB","json":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB.json","graph_json":"https://pith.science/api/pith-number/NLKR76G6JKOTGY5O3KIS27PRLB/graph.json","events_json":"https://pith.science/api/pith-number/NLKR76G6JKOTGY5O3KIS27PRLB/events.json","paper":"https://pith.science/paper/NLKR76G6"},"agent_actions":{"view_html":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB","download_json":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB.json","view_paper":"https://pith.science/paper/NLKR76G6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.03089&json=true","fetch_graph":"https://pith.science/api/pith-number/NLKR76G6JKOTGY5O3KIS27PRLB/graph.json","fetch_events":"https://pith.science/api/pith-number/NLKR76G6JKOTGY5O3KIS27PRLB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB/action/storage_attestation","attest_author":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB/action/author_attestation","sign_citation":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB/action/citation_signature","submit_replication":"https://pith.science/pith/NLKR76G6JKOTGY5O3KIS27PRLB/action/replication_record"}},"created_at":"2026-05-18T00:22:05.703235+00:00","updated_at":"2026-05-18T00:22:05.703235+00:00"}