{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:5NVF7FQOBDH7NCON2TNEUSFP3J","short_pith_number":"pith:5NVF7FQO","schema_version":"1.0","canonical_sha256":"eb6a5f960e08cff689cdd4da4a48afda53a0a76d8f4d4789c9df0c1308c34a7a","source":{"kind":"arxiv","id":"1812.08791","version":2},"attestation_state":"computed","paper":{"title":"SU(3)-breaking ratios for $D_{(s)}$ and $B_{(s)}$ mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Amarjit Soni, Andreas Juttner, Justus Tobias Tsang, Luigi Del Debbio, Nicolas Garron, Oliver Witzel (RBC/UKQCD collaboration), Peter A Boyle","submitted_at":"2018-12-20T18:48:36Z","abstract_excerpt":"We present results for the $SU(3)$ breaking ratios of decay constants $f_{D_s}/f_D$ and $f_{B_s}/f_B$ and - for the first time with physical pion masses - the ratio of bag parameters $B_{B_s}/B_{B_d}$, as well as the ratio $\\xi$, forming the ratio of the nonpeturbative contributions to neutral $B_{(s)}$ meson mixing. Our results are based on Lattice QCD simulations with chirally symmetric 2+1 dynamical flavors of domain wall fermions. Eight ensembles at three different lattice spacing in the range $a = 0.11 - 0.07\\,\\mathrm{fm}$ enter the analysis two of which feature physical light quark masse"},"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":"1812.08791","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-12-20T18:48:36Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"0da48a45f91aaa71c8106dae7cbbd83cf0cf543595f8d4aec437f26904c6eedd","abstract_canon_sha256":"da91c8eb5a99c602bd9e6a736e2ce6e1cebf552eb17ef5b461ef9322fd920003"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:11:22.136771Z","signature_b64":"9UkXgbjDemrUClhIv5oSG2PZesYm/brMcf72CwtzP/XvbPuxtqrveqUrX4JFyopeO8ZzffhFohy3cKIiCqMMDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb6a5f960e08cff689cdd4da4a48afda53a0a76d8f4d4789c9df0c1308c34a7a","last_reissued_at":"2026-07-05T01:11:22.136305Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:11:22.136305Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SU(3)-breaking ratios for $D_{(s)}$ and $B_{(s)}$ mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Amarjit Soni, Andreas Juttner, Justus Tobias Tsang, Luigi Del Debbio, Nicolas Garron, Oliver Witzel (RBC/UKQCD collaboration), Peter A Boyle","submitted_at":"2018-12-20T18:48:36Z","abstract_excerpt":"We present results for the $SU(3)$ breaking ratios of decay constants $f_{D_s}/f_D$ and $f_{B_s}/f_B$ and - for the first time with physical pion masses - the ratio of bag parameters $B_{B_s}/B_{B_d}$, as well as the ratio $\\xi$, forming the ratio of the nonpeturbative contributions to neutral $B_{(s)}$ meson mixing. Our results are based on Lattice QCD simulations with chirally symmetric 2+1 dynamical flavors of domain wall fermions. Eight ensembles at three different lattice spacing in the range $a = 0.11 - 0.07\\,\\mathrm{fm}$ enter the analysis two of which feature physical light quark masse"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.08791","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/1812.08791/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":"1812.08791","created_at":"2026-07-05T01:11:22.136367+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.08791v2","created_at":"2026-07-05T01:11:22.136367+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.08791","created_at":"2026-07-05T01:11:22.136367+00:00"},{"alias_kind":"pith_short_12","alias_value":"5NVF7FQOBDH7","created_at":"2026-07-05T01:11:22.136367+00:00"},{"alias_kind":"pith_short_16","alias_value":"5NVF7FQOBDH7NCON","created_at":"2026-07-05T01:11:22.136367+00:00"},{"alias_kind":"pith_short_8","alias_value":"5NVF7FQO","created_at":"2026-07-05T01:11:22.136367+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2607.00493","citing_title":"Gradient Flow Renormalization Schemes for Composite Fermion Operators","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2411.18639","citing_title":"Averages of $b$-hadron, $c$-hadron, and $\\tau$-lepton properties as of 2023","ref_index":174,"is_internal_anchor":false},{"citing_arxiv_id":"2411.04268","citing_title":"FLAG Review 2024","ref_index":76,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J","json":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J.json","graph_json":"https://pith.science/api/pith-number/5NVF7FQOBDH7NCON2TNEUSFP3J/graph.json","events_json":"https://pith.science/api/pith-number/5NVF7FQOBDH7NCON2TNEUSFP3J/events.json","paper":"https://pith.science/paper/5NVF7FQO"},"agent_actions":{"view_html":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J","download_json":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J.json","view_paper":"https://pith.science/paper/5NVF7FQO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.08791&json=true","fetch_graph":"https://pith.science/api/pith-number/5NVF7FQOBDH7NCON2TNEUSFP3J/graph.json","fetch_events":"https://pith.science/api/pith-number/5NVF7FQOBDH7NCON2TNEUSFP3J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J/action/storage_attestation","attest_author":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J/action/author_attestation","sign_citation":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J/action/citation_signature","submit_replication":"https://pith.science/pith/5NVF7FQOBDH7NCON2TNEUSFP3J/action/replication_record"}},"created_at":"2026-07-05T01:11:22.136367+00:00","updated_at":"2026-07-05T01:11:22.136367+00:00"}