{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:XYJCCJOFUULMLZX3BOKGO3W37M","short_pith_number":"pith:XYJCCJOF","schema_version":"1.0","canonical_sha256":"be122125c5a516c5e6fb0b94676edbfb03afe6dc4c0ff50a369ca7ff41838d31","source":{"kind":"arxiv","id":"1201.4382","version":1},"attestation_state":"computed","paper":{"title":"Top-quark production at hadron colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Ferroglia, R. Bonciani","submitted_at":"2012-01-20T20:45:36Z","abstract_excerpt":"The current theoretical predictions for the observables related to the top-quark pair and the single-top productions at hadron colliders are briefly reviewed. The theoretical predictions are compared to the experimental measurements carried out at the Tevatron and the LHC."},"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":"1201.4382","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-01-20T20:45:36Z","cross_cats_sorted":[],"title_canon_sha256":"b38ca8d67f0f74b0ddb4ad17210b3db1f0aa29473a524e907a340f7e1b17fff0","abstract_canon_sha256":"7c96e2316e5569ca03bebaff5dc98cde74b94d68351697cd0c231e67d324590a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:04:07.300451Z","signature_b64":"ao3VKsr11lPMZRa2hrsIkV4DixiW/OJLt2jtNlhVYDeU+ilBRS8Xmyuhm3D+XheSdOATP30z68NNWxtzgPiRBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"be122125c5a516c5e6fb0b94676edbfb03afe6dc4c0ff50a369ca7ff41838d31","last_reissued_at":"2026-05-18T04:04:07.299855Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:04:07.299855Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Top-quark production at hadron colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Ferroglia, R. Bonciani","submitted_at":"2012-01-20T20:45:36Z","abstract_excerpt":"The current theoretical predictions for the observables related to the top-quark pair and the single-top productions at hadron colliders are briefly reviewed. The theoretical predictions are compared to the experimental measurements carried out at the Tevatron and the LHC."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.4382","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":"1201.4382","created_at":"2026-05-18T04:04:07.299959+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.4382v1","created_at":"2026-05-18T04:04:07.299959+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.4382","created_at":"2026-05-18T04:04:07.299959+00:00"},{"alias_kind":"pith_short_12","alias_value":"XYJCCJOFUULM","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_16","alias_value":"XYJCCJOFUULMLZX3","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_8","alias_value":"XYJCCJOF","created_at":"2026-05-18T12:27:27.928770+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M","json":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M.json","graph_json":"https://pith.science/api/pith-number/XYJCCJOFUULMLZX3BOKGO3W37M/graph.json","events_json":"https://pith.science/api/pith-number/XYJCCJOFUULMLZX3BOKGO3W37M/events.json","paper":"https://pith.science/paper/XYJCCJOF"},"agent_actions":{"view_html":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M","download_json":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M.json","view_paper":"https://pith.science/paper/XYJCCJOF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.4382&json=true","fetch_graph":"https://pith.science/api/pith-number/XYJCCJOFUULMLZX3BOKGO3W37M/graph.json","fetch_events":"https://pith.science/api/pith-number/XYJCCJOFUULMLZX3BOKGO3W37M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M/action/storage_attestation","attest_author":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M/action/author_attestation","sign_citation":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M/action/citation_signature","submit_replication":"https://pith.science/pith/XYJCCJOFUULMLZX3BOKGO3W37M/action/replication_record"}},"created_at":"2026-05-18T04:04:07.299959+00:00","updated_at":"2026-05-18T04:04:07.299959+00:00"}