{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:D3RHLKNUURZIB3FUZIAUPJUJV3","short_pith_number":"pith:D3RHLKNU","schema_version":"1.0","canonical_sha256":"1ee275a9b4a47280ecb4ca0147a689aece2dcf0605654a7f83c7d1c42b32e8fa","source":{"kind":"arxiv","id":"1602.03560","version":2},"attestation_state":"computed","paper":{"title":"$B^0_{(s)}$-mixing matrix elements from lattice QCD for the Standard Model and beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, A. S. Kronfeld, A. X. El-Khadra, C. Bernard, C. C. Chang, C. DeTar, C. M. Bouchard, Daping Du, D. Toussaint, E. D. Freeland, E. Gamiz, E. T. Neil, J. Laiho, J. Simone, P. B. Mackenzie, Ran Zhou, R. Sugar, R. S. Van de Water, Steven Gottlieb, U. M. Heller","submitted_at":"2016-02-10T22:27:30Z","abstract_excerpt":"We calculate---for the first time in three-flavor lattice QCD---the hadronic matrix elements of all five local operators that contribute to neutral $B^0$- and $B_s$-meson mixing in and beyond the Standard Model. We present a complete error budget for each matrix element and also provide the full set of correlations among the matrix elements. We also present the corresponding bag parameters and their correlations, as well as specific combinations of the mixing matrix elements that enter the expression for the neutral $B$-meson width difference. We obtain the most precise determination to date o"},"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":"1602.03560","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-02-10T22:27:30Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"f7ac776e851f9784bfb981b9bbcc53cbe9ca6e0f9c77537e0032077054120a20","abstract_canon_sha256":"788dd4e97136a84091cd2e2392876816b993423d46f71348facbe57028267266"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:31.572063Z","signature_b64":"/Gp1r9Dpr53w/+kmQyorbbiVVlPc/9NR1H29dHHtobsYJytvTazgiqlFuTv+2Fgu3QvoG3T040p1LoJnYX6FAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1ee275a9b4a47280ecb4ca0147a689aece2dcf0605654a7f83c7d1c42b32e8fa","last_reissued_at":"2026-05-18T01:11:31.571715Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:31.571715Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$B^0_{(s)}$-mixing matrix elements from lattice QCD for the Standard Model and beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, A. S. Kronfeld, A. X. El-Khadra, C. Bernard, C. C. Chang, C. DeTar, C. M. Bouchard, Daping Du, D. Toussaint, E. D. Freeland, E. Gamiz, E. T. Neil, J. Laiho, J. Simone, P. B. Mackenzie, Ran Zhou, R. Sugar, R. S. Van de Water, Steven Gottlieb, U. M. Heller","submitted_at":"2016-02-10T22:27:30Z","abstract_excerpt":"We calculate---for the first time in three-flavor lattice QCD---the hadronic matrix elements of all five local operators that contribute to neutral $B^0$- and $B_s$-meson mixing in and beyond the Standard Model. We present a complete error budget for each matrix element and also provide the full set of correlations among the matrix elements. We also present the corresponding bag parameters and their correlations, as well as specific combinations of the mixing matrix elements that enter the expression for the neutral $B$-meson width difference. We obtain the most precise determination to date o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.03560","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":"1602.03560","created_at":"2026-05-18T01:11:31.571772+00:00"},{"alias_kind":"arxiv_version","alias_value":"1602.03560v2","created_at":"2026-05-18T01:11:31.571772+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.03560","created_at":"2026-05-18T01:11:31.571772+00:00"},{"alias_kind":"pith_short_12","alias_value":"D3RHLKNUURZI","created_at":"2026-05-18T12:30:09.641336+00:00"},{"alias_kind":"pith_short_16","alias_value":"D3RHLKNUURZIB3FU","created_at":"2026-05-18T12:30:09.641336+00:00"},{"alias_kind":"pith_short_8","alias_value":"D3RHLKNU","created_at":"2026-05-18T12:30:09.641336+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2411.18639","citing_title":"Averages of $b$-hadron, $c$-hadron, and $\\tau$-lepton properties as of 2023","ref_index":172,"is_internal_anchor":true},{"citing_arxiv_id":"2411.04268","citing_title":"FLAG Review 2024","ref_index":79,"is_internal_anchor":true},{"citing_arxiv_id":"2604.25998","citing_title":"New insights into the $b\\rightarrow c \\bar{u}q$ puzzle through Top-Bottom synergies","ref_index":65,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3","json":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3.json","graph_json":"https://pith.science/api/pith-number/D3RHLKNUURZIB3FUZIAUPJUJV3/graph.json","events_json":"https://pith.science/api/pith-number/D3RHLKNUURZIB3FUZIAUPJUJV3/events.json","paper":"https://pith.science/paper/D3RHLKNU"},"agent_actions":{"view_html":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3","download_json":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3.json","view_paper":"https://pith.science/paper/D3RHLKNU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1602.03560&json=true","fetch_graph":"https://pith.science/api/pith-number/D3RHLKNUURZIB3FUZIAUPJUJV3/graph.json","fetch_events":"https://pith.science/api/pith-number/D3RHLKNUURZIB3FUZIAUPJUJV3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3/action/storage_attestation","attest_author":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3/action/author_attestation","sign_citation":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3/action/citation_signature","submit_replication":"https://pith.science/pith/D3RHLKNUURZIB3FUZIAUPJUJV3/action/replication_record"}},"created_at":"2026-05-18T01:11:31.571772+00:00","updated_at":"2026-05-18T01:11:31.571772+00:00"}