{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:ISAJGACJ736BAZ4VNKG524OVBH","short_pith_number":"pith:ISAJGACJ","schema_version":"1.0","canonical_sha256":"4480930049fefc1067956a8ddd71d509f7c80ad964d45927ea20ca7e28c3c2da","source":{"kind":"arxiv","id":"2307.10860","version":2},"attestation_state":"computed","paper":{"title":"Measurement of inclusive charged-particle jet production in pp and 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":"2023-07-20T13:29:57Z","abstract_excerpt":"Measurements of inclusive charged-particle jet production in pp and p-Pb collisions at center-of-mass energy per nucleon-nucleon collision $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and the corresponding nuclear modification factor $R_{\\rm pPb}^{\\rm ch\\,jet}$ are presented, using data collected with the ALICE detector at the LHC. Jets are reconstructed in the central rapidity region $|\\eta_{\\rm jet}| < 0.5$ from charged particles using the anti-$k_{\\rm T}$ algorithm with resolution parameters $R = 0.2$, 0.3, and 0.4. The $p_{\\rm T}$-differential inclusive production cross section of charged-particle jets,"},"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":"2307.10860","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2023-07-20T13:29:57Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"ef2d7f942313f49bd5b688e9536aadb057d7eb3a49195c725f91dcb818e2bbab","abstract_canon_sha256":"e70b5b5c18ee41233766484515e202bc4c50ae056f7f126493213de4e04c5d49"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:28:33.307455Z","signature_b64":"M41U0M2LKZ4AISCVJuT+0QOjwDwZJUJOkpzHA3TJCTSvNRlRt+4wk24qHylQhEm/DKMcuUP60PCCSefGjlQICA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4480930049fefc1067956a8ddd71d509f7c80ad964d45927ea20ca7e28c3c2da","last_reissued_at":"2026-07-05T08:28:33.306971Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:28:33.306971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of inclusive charged-particle jet production in pp and 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":"2023-07-20T13:29:57Z","abstract_excerpt":"Measurements of inclusive charged-particle jet production in pp and p-Pb collisions at center-of-mass energy per nucleon-nucleon collision $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and the corresponding nuclear modification factor $R_{\\rm pPb}^{\\rm ch\\,jet}$ are presented, using data collected with the ALICE detector at the LHC. Jets are reconstructed in the central rapidity region $|\\eta_{\\rm jet}| < 0.5$ from charged particles using the anti-$k_{\\rm T}$ algorithm with resolution parameters $R = 0.2$, 0.3, and 0.4. The $p_{\\rm T}$-differential inclusive production cross section of charged-particle jets,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.10860","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/2307.10860/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":"2307.10860","created_at":"2026-07-05T08:28:33.307025+00:00"},{"alias_kind":"arxiv_version","alias_value":"2307.10860v2","created_at":"2026-07-05T08:28:33.307025+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.10860","created_at":"2026-07-05T08:28:33.307025+00:00"},{"alias_kind":"pith_short_12","alias_value":"ISAJGACJ736B","created_at":"2026-07-05T08:28:33.307025+00:00"},{"alias_kind":"pith_short_16","alias_value":"ISAJGACJ736BAZ4V","created_at":"2026-07-05T08:28:33.307025+00:00"},{"alias_kind":"pith_short_8","alias_value":"ISAJGACJ","created_at":"2026-07-05T08:28:33.307025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.19430","citing_title":"Bayesian Constraints on Pre-Equilibrium Jet Quenching and Predictions for Oxygen Collisions","ref_index":28,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH","json":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH.json","graph_json":"https://pith.science/api/pith-number/ISAJGACJ736BAZ4VNKG524OVBH/graph.json","events_json":"https://pith.science/api/pith-number/ISAJGACJ736BAZ4VNKG524OVBH/events.json","paper":"https://pith.science/paper/ISAJGACJ"},"agent_actions":{"view_html":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH","download_json":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH.json","view_paper":"https://pith.science/paper/ISAJGACJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2307.10860&json=true","fetch_graph":"https://pith.science/api/pith-number/ISAJGACJ736BAZ4VNKG524OVBH/graph.json","fetch_events":"https://pith.science/api/pith-number/ISAJGACJ736BAZ4VNKG524OVBH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH/action/storage_attestation","attest_author":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH/action/author_attestation","sign_citation":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH/action/citation_signature","submit_replication":"https://pith.science/pith/ISAJGACJ736BAZ4VNKG524OVBH/action/replication_record"}},"created_at":"2026-07-05T08:28:33.307025+00:00","updated_at":"2026-07-05T08:28:33.307025+00:00"}