{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:ZX2MOASEZVSR4PKP4GZPZ3EFBL","short_pith_number":"pith:ZX2MOASE","schema_version":"1.0","canonical_sha256":"cdf4c70244cd651e3d4fe1b2fcec850aee82139a33f4f4b7305f581e1dd8e6de","source":{"kind":"arxiv","id":"1310.7372","version":1},"attestation_state":"computed","paper":{"title":"Beyond the Standard Model B-parameters with improved staggered fermions in $N_f=2+1$ QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Boram Yoon, Chulwoo Jung, Hwancheol Jeong, Hyung-Jin Kim, Jaehoon Leem, Jangho Kim, Jongjeong Kim, Kwangwoo Kim, Seonghee Kim, Stephen R. Sharpe, Taegil Bae, Weonjong Lee, Yong-Chull Jang","submitted_at":"2013-10-28T10:44:31Z","abstract_excerpt":"We calculate the kaon mixing B-parameters for operators arising generically in theories of physics beyond the standard model. We use HYP-smeared improved staggered fermions on the $N_f = 2+1$ MILC asqtad lattices. Operator matching is done perturbatively at one-loop order. Chiral extrapolations are done using \"golden combinations\" in which one-loop chiral logarithms are absent. For the combined sea-quark mass and continuum extrapolation, we use three lattice spacings: $a \\approx 0.045, 0.06$ and $0.09 \\text{fm}$. Our results have a total error of 5-6%, which is dominated by the systematic erro"},"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":"1310.7372","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-10-28T10:44:31Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"59657d51351af3ff33782e4c05a0ecec20c0201258f6dc5dd46ae9768de943b7","abstract_canon_sha256":"fb08fb4d8b907646908c3b612b211e4500493387459cd4565b15ac935bdf66a3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:08:45.539666Z","signature_b64":"f0E5lw8kCS32RA4FwaUg3gOlZ3xMVkjLKvLItk3dcLWPN//T49KSzvtavTauhTb3GQKOcyPxPK8rUqBU3s0iBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cdf4c70244cd651e3d4fe1b2fcec850aee82139a33f4f4b7305f581e1dd8e6de","last_reissued_at":"2026-05-18T03:08:45.539197Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:08:45.539197Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Beyond the Standard Model B-parameters with improved staggered fermions in $N_f=2+1$ QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Boram Yoon, Chulwoo Jung, Hwancheol Jeong, Hyung-Jin Kim, Jaehoon Leem, Jangho Kim, Jongjeong Kim, Kwangwoo Kim, Seonghee Kim, Stephen R. Sharpe, Taegil Bae, Weonjong Lee, Yong-Chull Jang","submitted_at":"2013-10-28T10:44:31Z","abstract_excerpt":"We calculate the kaon mixing B-parameters for operators arising generically in theories of physics beyond the standard model. We use HYP-smeared improved staggered fermions on the $N_f = 2+1$ MILC asqtad lattices. Operator matching is done perturbatively at one-loop order. Chiral extrapolations are done using \"golden combinations\" in which one-loop chiral logarithms are absent. For the combined sea-quark mass and continuum extrapolation, we use three lattice spacings: $a \\approx 0.045, 0.06$ and $0.09 \\text{fm}$. Our results have a total error of 5-6%, which is dominated by the systematic erro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.7372","kind":"arxiv","version":1},"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":"1310.7372","created_at":"2026-05-18T03:08:45.539277+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.7372v1","created_at":"2026-05-18T03:08:45.539277+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.7372","created_at":"2026-05-18T03:08:45.539277+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZX2MOASEZVSR","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZX2MOASEZVSR4PKP","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZX2MOASE","created_at":"2026-05-18T12:28:09.283467+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL","json":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL.json","graph_json":"https://pith.science/api/pith-number/ZX2MOASEZVSR4PKP4GZPZ3EFBL/graph.json","events_json":"https://pith.science/api/pith-number/ZX2MOASEZVSR4PKP4GZPZ3EFBL/events.json","paper":"https://pith.science/paper/ZX2MOASE"},"agent_actions":{"view_html":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL","download_json":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL.json","view_paper":"https://pith.science/paper/ZX2MOASE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.7372&json=true","fetch_graph":"https://pith.science/api/pith-number/ZX2MOASEZVSR4PKP4GZPZ3EFBL/graph.json","fetch_events":"https://pith.science/api/pith-number/ZX2MOASEZVSR4PKP4GZPZ3EFBL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL/action/storage_attestation","attest_author":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL/action/author_attestation","sign_citation":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL/action/citation_signature","submit_replication":"https://pith.science/pith/ZX2MOASEZVSR4PKP4GZPZ3EFBL/action/replication_record"}},"created_at":"2026-05-18T03:08:45.539277+00:00","updated_at":"2026-05-18T03:08:45.539277+00:00"}