{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:VVBJ7ZDTWDFK5MARLNHAVLYJHY","short_pith_number":"pith:VVBJ7ZDT","schema_version":"1.0","canonical_sha256":"ad429fe473b0caaeb0115b4e0aaf093e03711f6268c96d3fb1b92dbda246f362","source":{"kind":"arxiv","id":"1710.10070","version":1},"attestation_state":"computed","paper":{"title":"Color dipole predictions for the exclusive vector meson photoproduction in $pp/pPb/PbPb$ collisions at Run 2 LHC energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"B. D. Moreira, F. S. Navarra, G. Sampaio dos Santos, M.V.T. Machado, V. P. Goncalves","submitted_at":"2017-10-27T10:51:04Z","abstract_excerpt":"In this paper we present a comprehensive analysis of exclusive vector meson photoproduction in $pp$, $pPb$ and $PbPb$ collisions at Run 2 LHC energies using the Color Dipole formalism. The rapidity distributions and total cross sections for the $\\rho$, $\\phi$, $J/\\Psi$, $\\Psi (2S)$ and $\\Upsilon$ production are estimated considering the more recent phenomenological models for the dipole - proton scattering amplitude, which are based on the Color Glass Condensate formalism and are able to describe the inclusive and exclusive $ep$ HERA data. Moreover, we also discuss the impact of the modelling "},"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":"1710.10070","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-27T10:51:04Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"76c3d40ffda58c9f890f820dcd2ee9c7358b4b0855af9b1deaf4990efc6d399c","abstract_canon_sha256":"b91ce68e396f13504dcbc3388940d2c2df91b1f2b853e835c09a7299c17fc0c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:41.792375Z","signature_b64":"Q29pg/Y6hwC9u4ujyprKS3Gyh0+5u8rcceJRAE+JGpJo8TkaiZn/WdNo+vwsGwUE1qnwt+WeWgTqBe64rlYqBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad429fe473b0caaeb0115b4e0aaf093e03711f6268c96d3fb1b92dbda246f362","last_reissued_at":"2026-05-18T00:28:41.791687Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:41.791687Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Color dipole predictions for the exclusive vector meson photoproduction in $pp/pPb/PbPb$ collisions at Run 2 LHC energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"B. D. Moreira, F. S. Navarra, G. Sampaio dos Santos, M.V.T. Machado, V. P. Goncalves","submitted_at":"2017-10-27T10:51:04Z","abstract_excerpt":"In this paper we present a comprehensive analysis of exclusive vector meson photoproduction in $pp$, $pPb$ and $PbPb$ collisions at Run 2 LHC energies using the Color Dipole formalism. The rapidity distributions and total cross sections for the $\\rho$, $\\phi$, $J/\\Psi$, $\\Psi (2S)$ and $\\Upsilon$ production are estimated considering the more recent phenomenological models for the dipole - proton scattering amplitude, which are based on the Color Glass Condensate formalism and are able to describe the inclusive and exclusive $ep$ HERA data. Moreover, we also discuss the impact of the modelling "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.10070","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":""},"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":"1710.10070","created_at":"2026-05-18T00:28:41.791792+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.10070v1","created_at":"2026-05-18T00:28:41.791792+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.10070","created_at":"2026-05-18T00:28:41.791792+00:00"},{"alias_kind":"pith_short_12","alias_value":"VVBJ7ZDTWDFK","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"VVBJ7ZDTWDFK5MAR","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"VVBJ7ZDT","created_at":"2026-05-18T12:31:49.984773+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"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":87,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY","json":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY.json","graph_json":"https://pith.science/api/pith-number/VVBJ7ZDTWDFK5MARLNHAVLYJHY/graph.json","events_json":"https://pith.science/api/pith-number/VVBJ7ZDTWDFK5MARLNHAVLYJHY/events.json","paper":"https://pith.science/paper/VVBJ7ZDT"},"agent_actions":{"view_html":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY","download_json":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY.json","view_paper":"https://pith.science/paper/VVBJ7ZDT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.10070&json=true","fetch_graph":"https://pith.science/api/pith-number/VVBJ7ZDTWDFK5MARLNHAVLYJHY/graph.json","fetch_events":"https://pith.science/api/pith-number/VVBJ7ZDTWDFK5MARLNHAVLYJHY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY/action/storage_attestation","attest_author":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY/action/author_attestation","sign_citation":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY/action/citation_signature","submit_replication":"https://pith.science/pith/VVBJ7ZDTWDFK5MARLNHAVLYJHY/action/replication_record"}},"created_at":"2026-05-18T00:28:41.791792+00:00","updated_at":"2026-05-18T00:28:41.791792+00:00"}