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As an important sequential work, we make a further discussion on the production of the more complicated $P$-wave excited $(c\\bar{b})$-quarkonium states, i.e. $|(c\\bar{b})_{\\bf 1}[^1P_1]>$ and $|(c\\bar{b})_{\\bf 1}[^3P_J]>$ (with $J=(1,2,3)$). More over, we also calculate the channel with the two color-octet quarkonium states $|(c\\bar{b})_{\\bf 8}[^1S_0]g>$ and $|(c\\bar{b})_{\\bf 8}["},"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":"1011.5961","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-27T09:48:59Z","cross_cats_sorted":[],"title_canon_sha256":"2806b49abde0dfb6c348115e8afb5e335fcc065c1212bcec05760f3465b04241","abstract_canon_sha256":"aa178ab6ccfe51348a9e15dc1e983869c011ba903d909af23c399fe4177c71f8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:48.982397Z","signature_b64":"n/wrxWOhYcBgv1cwdevkxgFPMzCML3EFMDY6jdrRtE/S7DnKzW+CvqXsth5HgwrdVhUHLLNgrLdqqG/HM5VcCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58002cdf53c65782523d21d043df5749cd3aefd6e4e1d4ab71d3b3149db7a04b","last_reissued_at":"2026-05-18T04:25:48.981743Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:48.981743Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Production of the $P$-Wave Excited $B_c$-States through the $Z^0$ Boson Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Gu Chen, Jia-wei Zhang, Li-Cheng Deng, Xing-Gang Wu, Zhi Yang","submitted_at":"2010-11-27T09:48:59Z","abstract_excerpt":"In Ref.[7],we have dealt with the production of the two color-singlet $S$-wave $(c\\bar{b})$-quarkonium states $B_c(|(c\\bar{b})_{\\bf 1}[^1S_0]>)$ and $B^*_c(|(c\\bar{b})_{\\bf 1}[^3S_1]>)$ through the $Z^0$ boson decays. As an important sequential work, we make a further discussion on the production of the more complicated $P$-wave excited $(c\\bar{b})$-quarkonium states, i.e. $|(c\\bar{b})_{\\bf 1}[^1P_1]>$ and $|(c\\bar{b})_{\\bf 1}[^3P_J]>$ (with $J=(1,2,3)$). More over, we also calculate the channel with the two color-octet quarkonium states $|(c\\bar{b})_{\\bf 8}[^1S_0]g>$ and $|(c\\bar{b})_{\\bf 8}["},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.5961","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":""},"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":"1011.5961","created_at":"2026-05-18T04:25:48.981859+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.5961v2","created_at":"2026-05-18T04:25:48.981859+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.5961","created_at":"2026-05-18T04:25:48.981859+00:00"},{"alias_kind":"pith_short_12","alias_value":"LAACZX2TYZLY","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_16","alias_value":"LAACZX2TYZLYEUR5","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_8","alias_value":"LAACZX2T","created_at":"2026-05-18T12:26:10.704358+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":44,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH","json":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH.json","graph_json":"https://pith.science/api/pith-number/LAACZX2TYZLYEUR5EHIEHX2XJH/graph.json","events_json":"https://pith.science/api/pith-number/LAACZX2TYZLYEUR5EHIEHX2XJH/events.json","paper":"https://pith.science/paper/LAACZX2T"},"agent_actions":{"view_html":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH","download_json":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH.json","view_paper":"https://pith.science/paper/LAACZX2T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.5961&json=true","fetch_graph":"https://pith.science/api/pith-number/LAACZX2TYZLYEUR5EHIEHX2XJH/graph.json","fetch_events":"https://pith.science/api/pith-number/LAACZX2TYZLYEUR5EHIEHX2XJH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH/action/storage_attestation","attest_author":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH/action/author_attestation","sign_citation":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH/action/citation_signature","submit_replication":"https://pith.science/pith/LAACZX2TYZLYEUR5EHIEHX2XJH/action/replication_record"}},"created_at":"2026-05-18T04:25:48.981859+00:00","updated_at":"2026-05-18T04:25:48.981859+00:00"}