{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:XWN73RHPVO6A2XEIGFZR7OMC6A","short_pith_number":"pith:XWN73RHP","schema_version":"1.0","canonical_sha256":"bd9bfdc4efabbc0d5c8831731fb982f0035b13f7bea7c932a78c47991142174a","source":{"kind":"arxiv","id":"1712.09262","version":4},"attestation_state":"computed","paper":{"title":"$B$- and $D$-meson leptonic decay constants from four-flavor lattice QCD","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. DeTar, D. Toussaint, E. G\\'amiz, E.T. Neil, J. Komijani, J. Laiho, J.N. Simone, N. Brown, P.B. Mackenzie, R.L. Sugar, R.S. Van de Water, Steven Gottlieb, U.M. Heller","submitted_at":"2017-12-26T13:08:41Z","abstract_excerpt":"We calculate the leptonic decay constants of heavy-light pseudoscalar mesons with charm and bottom quarks in lattice quantum chromodynamics on four-flavor QCD gauge-field configurations with dynamical $u$, $d$, $s$, and $c$ quarks. We analyze over twenty isospin-symmetric ensembles with six lattice spacings down to $a\\approx 0.03$~fm and several values of the light-quark mass down to the physical value $\\frac{1}{2}(m_u+m_d)$. We employ the highly-improved staggered-quark (HISQ) action for the sea and valence quarks; on the finest lattice spacings, discretization errors are sufficiently small t"},"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":"1712.09262","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-12-26T13:08:41Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"dfb2cf28d44201ff5cbba9434681b7ed388545a5489c91ed710336b90bc7933a","abstract_canon_sha256":"e520cb11336a7016b1fedcc32cc4c61b11935ac2d5d8e28892fafecb050e18cf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:00:49.334102Z","signature_b64":"mRh6Z92BYPGjuijqcfYssIqirX8lUoOaPTlG5e7gy24pRPbj93Noi458nm6uh/E+Elk6GAnt/Mzgp+ANwdJfDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd9bfdc4efabbc0d5c8831731fb982f0035b13f7bea7c932a78c47991142174a","last_reissued_at":"2026-07-05T00:00:49.333559Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:00:49.333559Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$B$- and $D$-meson leptonic decay constants from four-flavor lattice QCD","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. DeTar, D. Toussaint, E. G\\'amiz, E.T. Neil, J. Komijani, J. Laiho, J.N. Simone, N. Brown, P.B. Mackenzie, R.L. Sugar, R.S. Van de Water, Steven Gottlieb, U.M. Heller","submitted_at":"2017-12-26T13:08:41Z","abstract_excerpt":"We calculate the leptonic decay constants of heavy-light pseudoscalar mesons with charm and bottom quarks in lattice quantum chromodynamics on four-flavor QCD gauge-field configurations with dynamical $u$, $d$, $s$, and $c$ quarks. We analyze over twenty isospin-symmetric ensembles with six lattice spacings down to $a\\approx 0.03$~fm and several values of the light-quark mass down to the physical value $\\frac{1}{2}(m_u+m_d)$. We employ the highly-improved staggered-quark (HISQ) action for the sea and valence quarks; on the finest lattice spacings, discretization errors are sufficiently small t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.09262","kind":"arxiv","version":4},"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/1712.09262/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":"1712.09262","created_at":"2026-07-05T00:00:49.333623+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.09262v4","created_at":"2026-07-05T00:00:49.333623+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.09262","created_at":"2026-07-05T00:00:49.333623+00:00"},{"alias_kind":"pith_short_12","alias_value":"XWN73RHPVO6A","created_at":"2026-07-05T00:00:49.333623+00:00"},{"alias_kind":"pith_short_16","alias_value":"XWN73RHPVO6A2XEI","created_at":"2026-07-05T00:00:49.333623+00:00"},{"alias_kind":"pith_short_8","alias_value":"XWN73RHP","created_at":"2026-07-05T00:00:49.333623+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":9,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2209.05289","citing_title":"Semileptonic weak Hamiltonian to $\\mathcal{O}(\\alpha \\alpha_s(\\mu_{\\mathrm{Lattice}}))$ in momentum-space subtraction schemes","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2307.14585","citing_title":"Improved measurement of the branching fraction of $D_s^+\\to\\mu^+\\nu_\\mu$","ref_index":14,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21908","citing_title":"Semileptonic sum rules in heavy-to-light charm decays","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2508.02862","citing_title":"New high-precision $b$, $c$, and $s$ masses from pseudoscalar-pseudoscalar correlators in $n_f=4$ lattice QCD","ref_index":30,"is_internal_anchor":false},{"citing_arxiv_id":"2411.04268","citing_title":"FLAG Review 2024","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06560","citing_title":"$F_K/F_\\pi$ as a precision test of a new four flavor Domain Wall Fermion action","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00989","citing_title":"$CP$ violation in neutral kaon mixing in $D^0\\rightarrow K_SK_S$","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2604.04715","citing_title":"A Precision Test of First Row CKM Unitarity from Lattice QCD","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20644","citing_title":"Review of experimental studies of charmed meson decays at BESIII","ref_index":78,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A","json":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A.json","graph_json":"https://pith.science/api/pith-number/XWN73RHPVO6A2XEIGFZR7OMC6A/graph.json","events_json":"https://pith.science/api/pith-number/XWN73RHPVO6A2XEIGFZR7OMC6A/events.json","paper":"https://pith.science/paper/XWN73RHP"},"agent_actions":{"view_html":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A","download_json":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A.json","view_paper":"https://pith.science/paper/XWN73RHP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.09262&json=true","fetch_graph":"https://pith.science/api/pith-number/XWN73RHPVO6A2XEIGFZR7OMC6A/graph.json","fetch_events":"https://pith.science/api/pith-number/XWN73RHPVO6A2XEIGFZR7OMC6A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A/action/storage_attestation","attest_author":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A/action/author_attestation","sign_citation":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A/action/citation_signature","submit_replication":"https://pith.science/pith/XWN73RHPVO6A2XEIGFZR7OMC6A/action/replication_record"}},"created_at":"2026-07-05T00:00:49.333623+00:00","updated_at":"2026-07-05T00:00:49.333623+00:00"}