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This fact opens the possibility of an accurate sum-rule extraction of $m_b$ by using $f_B$ as input. Combining precise lattice QCD determinations of $f_B$ with our sum-rule analysis based on the three-loop $O(\\alpha_s^2)$ heavy-light correlation function leads to $\\bar{m}_b(\\bar{m}_b)=(4.247\\pm0.034)\\;\\mbox{GeV}$."},"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":"1305.7099","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-30T13:18:57Z","cross_cats_sorted":[],"title_canon_sha256":"1e145f4ec5dc08a3a3687aae074ce88ab754237dbd14f9890c312dfabd9b138a","abstract_canon_sha256":"97e76bb03c1b3864ebcc1e91d7e835eabcec0ffec48e6791ed7e9f2b8b2f2d1e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:13:21.353454Z","signature_b64":"H96vkd66UWXgf8pYhZKpd+tu3OIFDxHc99O9s5UFC/MponeEFEQDvJTtT46mwVcjDhUgXX31jCGZrHW2t2UcDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1306fe9804192e11a1303c9b11c9322df7dd05b2cfadfb0b3cf834b2578f2b8b","last_reissued_at":"2026-05-18T03:13:21.352885Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:13:21.352885Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Accurate bottom-quark mass from Borel QCD sum rules for $f_B$ and $f_{B_s}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dmitri Melikhov, Silvano Simula, Wolfgang Lucha","submitted_at":"2013-05-30T13:18:57Z","abstract_excerpt":"We prove that Borel QCD sum rules for heavy-light currents yield very strong correlations between the $b$-quark mass $m_b$ and the $B$-meson decay constant $f_B$, namely, $\\delta f_B/f_B\\approx -8\\,\\delta m_b/m_b$. This fact opens the possibility of an accurate sum-rule extraction of $m_b$ by using $f_B$ as input. Combining precise lattice QCD determinations of $f_B$ with our sum-rule analysis based on the three-loop $O(\\alpha_s^2)$ heavy-light correlation function leads to $\\bar{m}_b(\\bar{m}_b)=(4.247\\pm0.034)\\;\\mbox{GeV}$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7099","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":"1305.7099","created_at":"2026-05-18T03:13:21.352963+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.7099v2","created_at":"2026-05-18T03:13:21.352963+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7099","created_at":"2026-05-18T03:13:21.352963+00:00"},{"alias_kind":"pith_short_12","alias_value":"CMDP5GAEDEXB","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_16","alias_value":"CMDP5GAEDEXBDIJQ","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_8","alias_value":"CMDP5GAE","created_at":"2026-05-18T12:27:40.988391+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"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":66,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX","json":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX.json","graph_json":"https://pith.science/api/pith-number/CMDP5GAEDEXBDIJQHSNRDSJSFX/graph.json","events_json":"https://pith.science/api/pith-number/CMDP5GAEDEXBDIJQHSNRDSJSFX/events.json","paper":"https://pith.science/paper/CMDP5GAE"},"agent_actions":{"view_html":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX","download_json":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX.json","view_paper":"https://pith.science/paper/CMDP5GAE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.7099&json=true","fetch_graph":"https://pith.science/api/pith-number/CMDP5GAEDEXBDIJQHSNRDSJSFX/graph.json","fetch_events":"https://pith.science/api/pith-number/CMDP5GAEDEXBDIJQHSNRDSJSFX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX/action/storage_attestation","attest_author":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX/action/author_attestation","sign_citation":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX/action/citation_signature","submit_replication":"https://pith.science/pith/CMDP5GAEDEXBDIJQHSNRDSJSFX/action/replication_record"}},"created_at":"2026-05-18T03:13:21.352963+00:00","updated_at":"2026-05-18T03:13:21.352963+00:00"}