{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:3TFPVGVDX2OFBC5GKHHBGVIGYC","short_pith_number":"pith:3TFPVGVD","schema_version":"1.0","canonical_sha256":"dccafa9aa3be9c508ba651ce135506c098aac1bf619c6d6a3c15c111d4711ef2","source":{"kind":"arxiv","id":"hep-ph/9806444","version":2},"attestation_state":"computed","paper":{"title":"Phenomenological prediction of the properties of the B_{C} system","license":"","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Lewis P. Fulcher (Bowling Green State University)","submitted_at":"1998-06-22T20:23:36Z","abstract_excerpt":"We present a comprehensive calculation of the energies, splittings and electromagnetic decay rates of the bottom charmed meson system. Our calculated result for the ground state lifetime is 0.38 \\pm 0.03 ps, in good agreement with the recent CDF measurement. In order to incorporate running coupling constant effects, we choose Richardson's potential for the central potential and take the spin-dependent potentials from the radiative one-loop expressions of Pantaleone, Tye and Ng. The effects of a nonperturbative spin-orbit potential are also included. Our parameters are determined from the low-l"},"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":"hep-ph/9806444","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-06-22T20:23:36Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"38258123738c8af6a863b35a1fe6ee4d76f8989499b1810cfdb5e9f2735e77f6","abstract_canon_sha256":"9fe3fd247f39a35b221840c92a8266b465d280acbd0be1559f61ae3501543bd1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:18.861374Z","signature_b64":"sPZrcqHbmDF8mB+7ZpvydsXpCFmiji5taZfNnqIqJ32iWP+ykAIv2KGBj6ODl/smpabr2M0qcx4tBDdNUYSgDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dccafa9aa3be9c508ba651ce135506c098aac1bf619c6d6a3c15c111d4711ef2","last_reissued_at":"2026-07-04T16:09:18.861021Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:18.861021Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phenomenological prediction of the properties of the B_{C} system","license":"","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Lewis P. Fulcher (Bowling Green State University)","submitted_at":"1998-06-22T20:23:36Z","abstract_excerpt":"We present a comprehensive calculation of the energies, splittings and electromagnetic decay rates of the bottom charmed meson system. Our calculated result for the ground state lifetime is 0.38 \\pm 0.03 ps, in good agreement with the recent CDF measurement. In order to incorporate running coupling constant effects, we choose Richardson's potential for the central potential and take the spin-dependent potentials from the radiative one-loop expressions of Pantaleone, Tye and Ng. The effects of a nonperturbative spin-orbit potential are also included. Our parameters are determined from the low-l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9806444","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/hep-ph/9806444/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":"hep-ph/9806444","created_at":"2026-07-04T16:09:18.861083+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9806444v2","created_at":"2026-07-04T16:09:18.861083+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9806444","created_at":"2026-07-04T16:09:18.861083+00:00"},{"alias_kind":"pith_short_12","alias_value":"3TFPVGVDX2OF","created_at":"2026-07-04T16:09:18.861083+00:00"},{"alias_kind":"pith_short_16","alias_value":"3TFPVGVDX2OFBC5G","created_at":"2026-07-04T16:09:18.861083+00:00"},{"alias_kind":"pith_short_8","alias_value":"3TFPVGVD","created_at":"2026-07-04T16:09:18.861083+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2607.00593","citing_title":"QCD sum-rule determination of the axial-vector mixing angle in the \\texorpdfstring{\\(B_c(1P)\\)}{Bc(1P)} sector","ref_index":7,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16228","citing_title":"Observation of a $B_c^{*+}$ meson with the ATLAS detector","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC","json":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC.json","graph_json":"https://pith.science/api/pith-number/3TFPVGVDX2OFBC5GKHHBGVIGYC/graph.json","events_json":"https://pith.science/api/pith-number/3TFPVGVDX2OFBC5GKHHBGVIGYC/events.json","paper":"https://pith.science/paper/3TFPVGVD"},"agent_actions":{"view_html":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC","download_json":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC.json","view_paper":"https://pith.science/paper/3TFPVGVD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9806444&json=true","fetch_graph":"https://pith.science/api/pith-number/3TFPVGVDX2OFBC5GKHHBGVIGYC/graph.json","fetch_events":"https://pith.science/api/pith-number/3TFPVGVDX2OFBC5GKHHBGVIGYC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC/action/storage_attestation","attest_author":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC/action/author_attestation","sign_citation":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC/action/citation_signature","submit_replication":"https://pith.science/pith/3TFPVGVDX2OFBC5GKHHBGVIGYC/action/replication_record"}},"created_at":"2026-07-04T16:09:18.861083+00:00","updated_at":"2026-07-04T16:09:18.861083+00:00"}