{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:KLOVC7ETMYFYHOFWXGPB3VBHHV","short_pith_number":"pith:KLOVC7ET","schema_version":"1.0","canonical_sha256":"52dd517c93660b83b8b6b99e1dd4273d4841b63d5059d22facb16fc53e8f697e","source":{"kind":"arxiv","id":"2409.11060","version":3},"attestation_state":"computed","paper":{"title":"Measurement of photonuclear jet production in ultra-peripheral Pb+Pb collisions at $\\sqrt{s_{\\text{NN}}} = 5.02$ 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":"2024-09-17T10:39:44Z","abstract_excerpt":"In ultra-relativistic heavy ion collisions at the LHC, each nucleus acts a sources of high-energy real photons that can scatter off the opposing nucleus in ultra-peripheral photonuclear ($\\gamma+A$) collisions. Hard scattering processes initiated by the photons in such collisions provide a novel method for probing nuclear parton distributions in a kinematic region not easily accessible to other measurements. ATLAS has measured production of dijet and multi-jet final states in ultra-peripheral Pb+Pb collisions at $\\sqrt{s_{\\text{NN}}} = 5.02$ TeV using a data set recorded in 2018 with an integr"},"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":"2409.11060","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2024-09-17T10:39:44Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"11044502fe25cbf8663ad47d2b4458c32d604232463a6256c06cb2d5801051ce","abstract_canon_sha256":"4d32e08a5958448415971f2ebec6fa4ee602f8c0d49f71f834ac9ecc80e8538d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:40:12.888214Z","signature_b64":"D4DSNJpvXsDGc6fez4SvAB/ueLOauRqHKhTBqBpdZl8LU4PCQU0Nnrdw8Bi09NTDmAzUvbak36DsaL4ltH+mBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"52dd517c93660b83b8b6b99e1dd4273d4841b63d5059d22facb16fc53e8f697e","last_reissued_at":"2026-07-05T10:40:12.887754Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:40:12.887754Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of photonuclear jet production in ultra-peripheral Pb+Pb collisions at $\\sqrt{s_{\\text{NN}}} = 5.02$ 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":"2024-09-17T10:39:44Z","abstract_excerpt":"In ultra-relativistic heavy ion collisions at the LHC, each nucleus acts a sources of high-energy real photons that can scatter off the opposing nucleus in ultra-peripheral photonuclear ($\\gamma+A$) collisions. Hard scattering processes initiated by the photons in such collisions provide a novel method for probing nuclear parton distributions in a kinematic region not easily accessible to other measurements. ATLAS has measured production of dijet and multi-jet final states in ultra-peripheral Pb+Pb collisions at $\\sqrt{s_{\\text{NN}}} = 5.02$ TeV using a data set recorded in 2018 with an integr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.11060","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2409.11060/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":"2409.11060","created_at":"2026-07-05T10:40:12.887811+00:00"},{"alias_kind":"arxiv_version","alias_value":"2409.11060v3","created_at":"2026-07-05T10:40:12.887811+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.11060","created_at":"2026-07-05T10:40:12.887811+00:00"},{"alias_kind":"pith_short_12","alias_value":"KLOVC7ETMYFY","created_at":"2026-07-05T10:40:12.887811+00:00"},{"alias_kind":"pith_short_16","alias_value":"KLOVC7ETMYFYHOFW","created_at":"2026-07-05T10:40:12.887811+00:00"},{"alias_kind":"pith_short_8","alias_value":"KLOVC7ET","created_at":"2026-07-05T10:40:12.887811+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"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":10,"is_internal_anchor":false},{"citing_arxiv_id":"2509.04135","citing_title":"Measurement of coherent exclusive $J/\\psi\\to\\mu^+\\mu^-$ production in ultraperipheral Pb+Pb collisions at $\\sqrt{s_{\\textrm{NN}}}=5.36$ TeV with the ATLAS detector","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24435","citing_title":"Measurement of jet photoproduction in ultra-peripheral Pb+Pb collisions without nuclear breakup at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV with the ATLAS detector","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20559","citing_title":"Observation of impact parameter dependent modifications of nuclear parton distributions in photonuclear Pb+Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV with the ATLAS detector","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV","json":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV.json","graph_json":"https://pith.science/api/pith-number/KLOVC7ETMYFYHOFWXGPB3VBHHV/graph.json","events_json":"https://pith.science/api/pith-number/KLOVC7ETMYFYHOFWXGPB3VBHHV/events.json","paper":"https://pith.science/paper/KLOVC7ET"},"agent_actions":{"view_html":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV","download_json":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV.json","view_paper":"https://pith.science/paper/KLOVC7ET","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2409.11060&json=true","fetch_graph":"https://pith.science/api/pith-number/KLOVC7ETMYFYHOFWXGPB3VBHHV/graph.json","fetch_events":"https://pith.science/api/pith-number/KLOVC7ETMYFYHOFWXGPB3VBHHV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV/action/storage_attestation","attest_author":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV/action/author_attestation","sign_citation":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV/action/citation_signature","submit_replication":"https://pith.science/pith/KLOVC7ETMYFYHOFWXGPB3VBHHV/action/replication_record"}},"created_at":"2026-07-05T10:40:12.887811+00:00","updated_at":"2026-07-05T10:40:12.887811+00:00"}