{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:L4A22DRNSRG4DYYRD6MJ4HM7W6","short_pith_number":"pith:L4A22DRN","schema_version":"1.0","canonical_sha256":"5f01ad0e2d944dc1e3111f989e1d9fb7a93c66d40d6318cb593f22287a47b365","source":{"kind":"arxiv","id":"1702.07181","version":3},"attestation_state":"computed","paper":{"title":"Photoproduction of doubly heavy baryon at the LHeC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bi Huan-Yu, Li Xiao-Zhou, Ma Wen-Gan, Samuel Owusu, Xing-Gang Wu, Zhang Ren-You","submitted_at":"2017-02-23T11:43:50Z","abstract_excerpt":"The photoproduction of doubly heavy baryon, $\\Xi_{cc}$, $\\Xi_{bc}$ and $\\Xi_{bb}$, is predicted within the nonrelativistic QCD at the Large Hadron Electron Collider (LHeC). The $\\Xi_{QQ'}$ production via the photon-gluon fusing channel $\\gamma + g \\to \\langle{QQ'}\\rangle[n] +\\bar{Q} +\\bar{Q'}$ and the extrinsic heavy quark channel $\\gamma + Q \\to \\langle{QQ'}\\rangle[n]+\\bar{Q'}$ have been considered, where $Q$ or $Q'$ stand for heavy $c$ or $b$ quark and $\\langle{QQ'}\\rangle[n]$ stands for a $QQ'$ diquark with given spin- and color- configurations $[n]$. The diquark shall fragmentate into $\\Xi"},"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":"1702.07181","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-23T11:43:50Z","cross_cats_sorted":[],"title_canon_sha256":"42094ba44a3677d62779b1acf2cc97f581e3fd786fdbbdc387af66e4646fe09e","abstract_canon_sha256":"486e2f18b82843373bcf77ef9645531445a08ffeea0144c3dcc05d7cdd92efb3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:28.557089Z","signature_b64":"9u7EOtq1R5XJYeAlUIwTVC+abUhX+WbaLBv+ThIzouIhp2Xvcslk8RcpJhEEnZ4j1NC5HTrrNkns18BmKjohCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f01ad0e2d944dc1e3111f989e1d9fb7a93c66d40d6318cb593f22287a47b365","last_reissued_at":"2026-05-18T00:40:28.556534Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:28.556534Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Photoproduction of doubly heavy baryon at the LHeC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bi Huan-Yu, Li Xiao-Zhou, Ma Wen-Gan, Samuel Owusu, Xing-Gang Wu, Zhang Ren-You","submitted_at":"2017-02-23T11:43:50Z","abstract_excerpt":"The photoproduction of doubly heavy baryon, $\\Xi_{cc}$, $\\Xi_{bc}$ and $\\Xi_{bb}$, is predicted within the nonrelativistic QCD at the Large Hadron Electron Collider (LHeC). The $\\Xi_{QQ'}$ production via the photon-gluon fusing channel $\\gamma + g \\to \\langle{QQ'}\\rangle[n] +\\bar{Q} +\\bar{Q'}$ and the extrinsic heavy quark channel $\\gamma + Q \\to \\langle{QQ'}\\rangle[n]+\\bar{Q'}$ have been considered, where $Q$ or $Q'$ stand for heavy $c$ or $b$ quark and $\\langle{QQ'}\\rangle[n]$ stands for a $QQ'$ diquark with given spin- and color- configurations $[n]$. The diquark shall fragmentate into $\\Xi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.07181","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":""},"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":"1702.07181","created_at":"2026-05-18T00:40:28.556616+00:00"},{"alias_kind":"arxiv_version","alias_value":"1702.07181v3","created_at":"2026-05-18T00:40:28.556616+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.07181","created_at":"2026-05-18T00:40:28.556616+00:00"},{"alias_kind":"pith_short_12","alias_value":"L4A22DRNSRG4","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"L4A22DRNSRG4DYYR","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"L4A22DRN","created_at":"2026-05-18T12:31:28.150371+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.05348","citing_title":"Resolved photoproduction of the $B_c$ meson in electron-proton collisions","ref_index":51,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6","json":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6.json","graph_json":"https://pith.science/api/pith-number/L4A22DRNSRG4DYYRD6MJ4HM7W6/graph.json","events_json":"https://pith.science/api/pith-number/L4A22DRNSRG4DYYRD6MJ4HM7W6/events.json","paper":"https://pith.science/paper/L4A22DRN"},"agent_actions":{"view_html":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6","download_json":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6.json","view_paper":"https://pith.science/paper/L4A22DRN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1702.07181&json=true","fetch_graph":"https://pith.science/api/pith-number/L4A22DRNSRG4DYYRD6MJ4HM7W6/graph.json","fetch_events":"https://pith.science/api/pith-number/L4A22DRNSRG4DYYRD6MJ4HM7W6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6/action/storage_attestation","attest_author":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6/action/author_attestation","sign_citation":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6/action/citation_signature","submit_replication":"https://pith.science/pith/L4A22DRNSRG4DYYRD6MJ4HM7W6/action/replication_record"}},"created_at":"2026-05-18T00:40:28.556616+00:00","updated_at":"2026-05-18T00:40:28.556616+00:00"}