{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:T76H3ZQI4XPHSNGNJYGXFOFYHF","short_pith_number":"pith:T76H3ZQI","schema_version":"1.0","canonical_sha256":"9ffc7de608e5de7934cd4e0d72b8b8396ade214627f8ea8b7d8215a8723eb469","source":{"kind":"arxiv","id":"1506.08808","version":2},"attestation_state":"computed","paper":{"title":"Centrality dependence of inclusive J/$\\psi$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 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":"2015-06-29T19:59:28Z","abstract_excerpt":"We present a measurement of inclusive J/$\\psi$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\\rm T}$, in the backward ($-4.46 < y_{\\rm cms} < -2.96$) and forward ($2.03 < y_{\\rm cms} < 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 < y_{\\rm cms} < 0.43$) in the dielectron decay channel. The backward and forward rapidity i"},"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":"1506.08808","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2015-06-29T19:59:28Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"260613fd94cc1ee7c24f9f04550ad931e771f3db52edde53d63ef1b6f6f3c126","abstract_canon_sha256":"38df3bb2e01b552edf75bcd0cd15afd29198307b1de9a496a18442d6f69847e9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:57.366029Z","signature_b64":"gz5Hvr3ciLRgAtEMz/I/lolNs64iZxsIC73LZiw+wny6fRgLESC25A3S7EJi8pT6wnEnlJ7bP5rbo5eGBw64Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ffc7de608e5de7934cd4e0d72b8b8396ade214627f8ea8b7d8215a8723eb469","last_reissued_at":"2026-05-18T01:18:57.365654Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:57.365654Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Centrality dependence of inclusive J/$\\psi$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 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":"2015-06-29T19:59:28Z","abstract_excerpt":"We present a measurement of inclusive J/$\\psi$ production in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\\rm T}$, in the backward ($-4.46 < y_{\\rm cms} < -2.96$) and forward ($2.03 < y_{\\rm cms} < 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 < y_{\\rm cms} < 0.43$) in the dielectron decay channel. The backward and forward rapidity i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.08808","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":""},"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":"1506.08808","created_at":"2026-05-18T01:18:57.365721+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.08808v2","created_at":"2026-05-18T01:18:57.365721+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.08808","created_at":"2026-05-18T01:18:57.365721+00:00"},{"alias_kind":"pith_short_12","alias_value":"T76H3ZQI4XPH","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"T76H3ZQI4XPHSNGN","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"T76H3ZQI","created_at":"2026-05-18T12:29:42.218222+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.17454","citing_title":"Nuclear Cold QCD: Review and Future Strategy","ref_index":100,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF","json":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF.json","graph_json":"https://pith.science/api/pith-number/T76H3ZQI4XPHSNGNJYGXFOFYHF/graph.json","events_json":"https://pith.science/api/pith-number/T76H3ZQI4XPHSNGNJYGXFOFYHF/events.json","paper":"https://pith.science/paper/T76H3ZQI"},"agent_actions":{"view_html":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF","download_json":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF.json","view_paper":"https://pith.science/paper/T76H3ZQI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.08808&json=true","fetch_graph":"https://pith.science/api/pith-number/T76H3ZQI4XPHSNGNJYGXFOFYHF/graph.json","fetch_events":"https://pith.science/api/pith-number/T76H3ZQI4XPHSNGNJYGXFOFYHF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF/action/storage_attestation","attest_author":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF/action/author_attestation","sign_citation":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF/action/citation_signature","submit_replication":"https://pith.science/pith/T76H3ZQI4XPHSNGNJYGXFOFYHF/action/replication_record"}},"created_at":"2026-05-18T01:18:57.365721+00:00","updated_at":"2026-05-18T01:18:57.365721+00:00"}