{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:G6YB6BXTMKDYLQHCL3RUAW3KW4","short_pith_number":"pith:G6YB6BXT","schema_version":"1.0","canonical_sha256":"37b01f06f3628785c0e25ee3405b6ab726ea96ef06099fc92319e74de7dae7dc","source":{"kind":"arxiv","id":"1906.03322","version":2},"attestation_state":"computed","paper":{"title":"Production of $\\Lambda_\\mathrm{c}^+$ baryons in proton-proton and lead-lead collisions at $\\sqrt{s_\\mathrm{NN}} =$ 5.02 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2019-06-07T20:26:06Z","abstract_excerpt":"The differential cross sections of $\\Lambda_\\mathrm{c}^+$ baryon production are measured via the exclusive decay channel $\\Lambda_\\mathrm{c}^+$ $\\to$ pK$^-\\pi^+$ using the CMS detector at the LHC. Spectra are measured as a function of transverse momentum ($p_\\mathrm{T}$) in proton-proton (pp) and lead-lead (PbPb) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV. The measurement is performed within the $\\Lambda_\\mathrm{c}^+$ rapidity interval $|y|$ $<$ 1.0 in the $p_\\mathrm{T}$ range of 5-20 GeV/$c$ in pp and 10-20 GeV/$c$ in PbPb collisions. The observed yields of $\\Lambda_\\ma"},"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":"1906.03322","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-06-07T20:26:06Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"18a11fa449ddb3517170b8448c24816a580b07d0a2278aac2cf0c7e48bfd0672","abstract_canon_sha256":"b2d1b294f706e829d769992dcfb92a6fe926247fbc5f76746614f1e0f2da1989"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:44:38.574141Z","signature_b64":"7dlLSoZ6U8l2GKFgWplyKYFAS6C2XrEmvt5Uw5kYdOxmJ1wWRWs6c81ijcvR2ys0zbuzG6TjQwGO1/x0uRKQCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"37b01f06f3628785c0e25ee3405b6ab726ea96ef06099fc92319e74de7dae7dc","last_reissued_at":"2026-07-05T00:44:38.573732Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:44:38.573732Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Production of $\\Lambda_\\mathrm{c}^+$ baryons in proton-proton and lead-lead collisions at $\\sqrt{s_\\mathrm{NN}} =$ 5.02 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2019-06-07T20:26:06Z","abstract_excerpt":"The differential cross sections of $\\Lambda_\\mathrm{c}^+$ baryon production are measured via the exclusive decay channel $\\Lambda_\\mathrm{c}^+$ $\\to$ pK$^-\\pi^+$ using the CMS detector at the LHC. Spectra are measured as a function of transverse momentum ($p_\\mathrm{T}$) in proton-proton (pp) and lead-lead (PbPb) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV. The measurement is performed within the $\\Lambda_\\mathrm{c}^+$ rapidity interval $|y|$ $<$ 1.0 in the $p_\\mathrm{T}$ range of 5-20 GeV/$c$ in pp and 10-20 GeV/$c$ in PbPb collisions. The observed yields of $\\Lambda_\\ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.03322","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/1906.03322/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":"1906.03322","created_at":"2026-07-05T00:44:38.573788+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.03322v2","created_at":"2026-07-05T00:44:38.573788+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.03322","created_at":"2026-07-05T00:44:38.573788+00:00"},{"alias_kind":"pith_short_12","alias_value":"G6YB6BXTMKDY","created_at":"2026-07-05T00:44:38.573788+00:00"},{"alias_kind":"pith_short_16","alias_value":"G6YB6BXTMKDYLQHC","created_at":"2026-07-05T00:44:38.573788+00:00"},{"alias_kind":"pith_short_8","alias_value":"G6YB6BXT","created_at":"2026-07-05T00:44:38.573788+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2506.22616","citing_title":"A novel phenomenological approach to total charm cross-section measurements at the LHC","ref_index":27,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4","json":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4.json","graph_json":"https://pith.science/api/pith-number/G6YB6BXTMKDYLQHCL3RUAW3KW4/graph.json","events_json":"https://pith.science/api/pith-number/G6YB6BXTMKDYLQHCL3RUAW3KW4/events.json","paper":"https://pith.science/paper/G6YB6BXT"},"agent_actions":{"view_html":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4","download_json":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4.json","view_paper":"https://pith.science/paper/G6YB6BXT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.03322&json=true","fetch_graph":"https://pith.science/api/pith-number/G6YB6BXTMKDYLQHCL3RUAW3KW4/graph.json","fetch_events":"https://pith.science/api/pith-number/G6YB6BXTMKDYLQHCL3RUAW3KW4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4/action/storage_attestation","attest_author":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4/action/author_attestation","sign_citation":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4/action/citation_signature","submit_replication":"https://pith.science/pith/G6YB6BXTMKDYLQHCL3RUAW3KW4/action/replication_record"}},"created_at":"2026-07-05T00:44:38.573788+00:00","updated_at":"2026-07-05T00:44:38.573788+00:00"}