{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:FYQ6FCECLNTBK7EK4OJ7S3A4XE","short_pith_number":"pith:FYQ6FCEC","schema_version":"1.0","canonical_sha256":"2e21e288825b66157c8ae393f96c1cb91d60b28ef4fbd3173497684aa10860d2","source":{"kind":"arxiv","id":"2506.02223","version":1},"attestation_state":"computed","paper":{"title":"Investigating the inclusive $D^0$ photoproduction in ultraperipheral $PbPb$ collisions at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Luana Santana, Victor P. Goncalves, Wolfgang Sch\\\"afer","submitted_at":"2025-06-02T20:06:35Z","abstract_excerpt":"The inclusive $D^0$ photoproduction in $PbPb$ collisions at the center - of - mass energies of the Large Hadron Collider (LHC) is investigated considering the color dipole $S$ - matrix approach. The analytical expressions for the differential distributions are derived in the impact parameter and transverse momentum spaces and predictions for the rapidity and transverse momentum distributions are presented considering three distinct models for the unintegrated gluon distribution of the nuclear target. In particular, we compare the predictions derived assuming a linear dynamics, with and without"},"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":"2506.02223","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-06-02T20:06:35Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"19660f5deb94d3ec5c7dd613c1f9e8607a224386f602dd5920347e7fcf74cf7f","abstract_canon_sha256":"b6987b88da3e8ca3a942ac4ba60fedcb67760738873d44dbe5677bf1630f13f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:14:34.754248Z","signature_b64":"+bAXIybqxZZj8xSaCmKGoqPzJKrL45sQm1LpES9g5kEetxvMFa9EjuupqEzlzG/5Sp1qCvsXZUMHXwlnLQUtCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2e21e288825b66157c8ae393f96c1cb91d60b28ef4fbd3173497684aa10860d2","last_reissued_at":"2026-07-05T11:14:34.753682Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:14:34.753682Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Investigating the inclusive $D^0$ photoproduction in ultraperipheral $PbPb$ collisions at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Luana Santana, Victor P. Goncalves, Wolfgang Sch\\\"afer","submitted_at":"2025-06-02T20:06:35Z","abstract_excerpt":"The inclusive $D^0$ photoproduction in $PbPb$ collisions at the center - of - mass energies of the Large Hadron Collider (LHC) is investigated considering the color dipole $S$ - matrix approach. The analytical expressions for the differential distributions are derived in the impact parameter and transverse momentum spaces and predictions for the rapidity and transverse momentum distributions are presented considering three distinct models for the unintegrated gluon distribution of the nuclear target. In particular, we compare the predictions derived assuming a linear dynamics, with and without"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.02223","kind":"arxiv","version":1},"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/2506.02223/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":"2506.02223","created_at":"2026-07-05T11:14:34.753750+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.02223v1","created_at":"2026-07-05T11:14:34.753750+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.02223","created_at":"2026-07-05T11:14:34.753750+00:00"},{"alias_kind":"pith_short_12","alias_value":"FYQ6FCECLNTB","created_at":"2026-07-05T11:14:34.753750+00:00"},{"alias_kind":"pith_short_16","alias_value":"FYQ6FCECLNTBK7EK","created_at":"2026-07-05T11:14:34.753750+00:00"},{"alias_kind":"pith_short_8","alias_value":"FYQ6FCEC","created_at":"2026-07-05T11:14:34.753750+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2508.18438","citing_title":"Evaluating the ratio of the exclusive vector meson photoproduction to inclusive hadron/jet production cross section in ultraperipheral heavy ion collisions","ref_index":82,"is_internal_anchor":false},{"citing_arxiv_id":"2509.02115","citing_title":"Probing nuclear structure with the Balitsky-Kovchegov equation in full impact-parameter dependence","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE","json":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE.json","graph_json":"https://pith.science/api/pith-number/FYQ6FCECLNTBK7EK4OJ7S3A4XE/graph.json","events_json":"https://pith.science/api/pith-number/FYQ6FCECLNTBK7EK4OJ7S3A4XE/events.json","paper":"https://pith.science/paper/FYQ6FCEC"},"agent_actions":{"view_html":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE","download_json":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE.json","view_paper":"https://pith.science/paper/FYQ6FCEC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.02223&json=true","fetch_graph":"https://pith.science/api/pith-number/FYQ6FCECLNTBK7EK4OJ7S3A4XE/graph.json","fetch_events":"https://pith.science/api/pith-number/FYQ6FCECLNTBK7EK4OJ7S3A4XE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE/action/storage_attestation","attest_author":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE/action/author_attestation","sign_citation":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE/action/citation_signature","submit_replication":"https://pith.science/pith/FYQ6FCECLNTBK7EK4OJ7S3A4XE/action/replication_record"}},"created_at":"2026-07-05T11:14:34.753750+00:00","updated_at":"2026-07-05T11:14:34.753750+00:00"}