{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:55RXOEQK6GASHGT77AXEQO2KMP","short_pith_number":"pith:55RXOEQK","canonical_record":{"source":{"id":"1404.4670","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2014-04-17T23:47:53Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"bf2999586d32cfec6307b4272271b28fd5b37b715fc4416b1ee0222d63fe07e3","abstract_canon_sha256":"a8e6cc4c36b199be3910f78f9eabd7b1311fd5a9e92f4b476b71bc78bb303b52"},"schema_version":"1.0"},"canonical_sha256":"ef6377120af181239a7ff82e483b4a63d5e26d1799664d02d6819b072b1b4caf","source":{"kind":"arxiv","id":"1404.4670","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.4670","created_at":"2026-05-18T02:22:29Z"},{"alias_kind":"arxiv_version","alias_value":"1404.4670v2","created_at":"2026-05-18T02:22:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.4670","created_at":"2026-05-18T02:22:29Z"},{"alias_kind":"pith_short_12","alias_value":"55RXOEQK6GAS","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"55RXOEQK6GASHGT7","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"55RXOEQK","created_at":"2026-05-18T12:28:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:55RXOEQK6GASHGT77AXEQO2KMP","target":"record","payload":{"canonical_record":{"source":{"id":"1404.4670","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2014-04-17T23:47:53Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"bf2999586d32cfec6307b4272271b28fd5b37b715fc4416b1ee0222d63fe07e3","abstract_canon_sha256":"a8e6cc4c36b199be3910f78f9eabd7b1311fd5a9e92f4b476b71bc78bb303b52"},"schema_version":"1.0"},"canonical_sha256":"ef6377120af181239a7ff82e483b4a63d5e26d1799664d02d6819b072b1b4caf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:29.922007Z","signature_b64":"08AA60iyse/geuqfCRAZiJx3NjSvIXA/s0JIkQy0xzWCc/YhvtqFgXYF8xoIPq3g1PKBedzDI1lO5ZZnamBjDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef6377120af181239a7ff82e483b4a63d5e26d1799664d02d6819b072b1b4caf","last_reissued_at":"2026-05-18T02:22:29.921561Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:29.921561Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1404.4670","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:22:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OSk3Q6Sb0TOBeGtgMd1AIRal0sz1nNvBDaGb12ApnoUYWng836PU6QOpzJ5S3k8FjMKXQdBVEcCKg9MKnIS+BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:07:52.040898Z"},"content_sha256":"8f0740f5e60f83036447845549275c929c81f434ab784ab389e4d624080775d9","schema_version":"1.0","event_id":"sha256:8f0740f5e60f83036447845549275c929c81f434ab784ab389e4d624080775d9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:55RXOEQK6GASHGT77AXEQO2KMP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"B-meson decay constants from 2+1-flavor lattice QCD with domain-wall light quarks and relativistic heavy quarks","license":"http://creativecommons.org/licenses/publicdomain/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Amarjit Soni, Christoph Lehner, Jonathan M. Flynn, Norman H.Christ, Oliver Witzel, Ruth S. Van de Water, Taichi Kawanai, Taku Izubuchi","submitted_at":"2014-04-17T23:47:53Z","abstract_excerpt":"We calculate the B-meson decay constants f_B, f_Bs, and their ratio in unquenched lattice QCD using domain-wall light quarks and relativistic b-quarks. We use gauge-field ensembles generated by the RBC and UKQCD collaborations using the domain-wall fermion action and Iwasaki gauge action with three flavors of light dynamical quarks. We analyze data at two lattice spacings of a ~ 0.11, 0.086 fm with unitary pion masses as light as M_pi ~ 290 MeV; this enables us to control the extrapolation to the physical light-quark masses and continuum. For the b-quarks we use the anisotropic clover action w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.4670","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:22:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U08Rtb9o+A8dYwPdEsxBUC4sr9piFaW0XbGL4YnEOaoMIet+8FRU9jqfm3ZGi4c4vNOzUpQPhYBXUexoxKABBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:07:52.041447Z"},"content_sha256":"6c3156bdb489ece3ef666ce35b5d3fb5b8ac500cc9ab04d7b41957386de54169","schema_version":"1.0","event_id":"sha256:6c3156bdb489ece3ef666ce35b5d3fb5b8ac500cc9ab04d7b41957386de54169"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/55RXOEQK6GASHGT77AXEQO2KMP/bundle.json","state_url":"https://pith.science/pith/55RXOEQK6GASHGT77AXEQO2KMP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/55RXOEQK6GASHGT77AXEQO2KMP/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-27T20:07:52Z","links":{"resolver":"https://pith.science/pith/55RXOEQK6GASHGT77AXEQO2KMP","bundle":"https://pith.science/pith/55RXOEQK6GASHGT77AXEQO2KMP/bundle.json","state":"https://pith.science/pith/55RXOEQK6GASHGT77AXEQO2KMP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/55RXOEQK6GASHGT77AXEQO2KMP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:55RXOEQK6GASHGT77AXEQO2KMP","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"a8e6cc4c36b199be3910f78f9eabd7b1311fd5a9e92f4b476b71bc78bb303b52","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2014-04-17T23:47:53Z","title_canon_sha256":"bf2999586d32cfec6307b4272271b28fd5b37b715fc4416b1ee0222d63fe07e3"},"schema_version":"1.0","source":{"id":"1404.4670","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.4670","created_at":"2026-05-18T02:22:29Z"},{"alias_kind":"arxiv_version","alias_value":"1404.4670v2","created_at":"2026-05-18T02:22:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.4670","created_at":"2026-05-18T02:22:29Z"},{"alias_kind":"pith_short_12","alias_value":"55RXOEQK6GAS","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"55RXOEQK6GASHGT7","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"55RXOEQK","created_at":"2026-05-18T12:28:14Z"}],"graph_snapshots":[{"event_id":"sha256:6c3156bdb489ece3ef666ce35b5d3fb5b8ac500cc9ab04d7b41957386de54169","target":"graph","created_at":"2026-05-18T02:22:29Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We calculate the B-meson decay constants f_B, f_Bs, and their ratio in unquenched lattice QCD using domain-wall light quarks and relativistic b-quarks. We use gauge-field ensembles generated by the RBC and UKQCD collaborations using the domain-wall fermion action and Iwasaki gauge action with three flavors of light dynamical quarks. We analyze data at two lattice spacings of a ~ 0.11, 0.086 fm with unitary pion masses as light as M_pi ~ 290 MeV; this enables us to control the extrapolation to the physical light-quark masses and continuum. For the b-quarks we use the anisotropic clover action w","authors_text":"Amarjit Soni, Christoph Lehner, Jonathan M. Flynn, Norman H.Christ, Oliver Witzel, Ruth S. Van de Water, Taichi Kawanai, Taku Izubuchi","cross_cats":["hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2014-04-17T23:47:53Z","title":"B-meson decay constants from 2+1-flavor lattice QCD with domain-wall light quarks and relativistic heavy quarks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.4670","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:8f0740f5e60f83036447845549275c929c81f434ab784ab389e4d624080775d9","target":"record","created_at":"2026-05-18T02:22:29Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"a8e6cc4c36b199be3910f78f9eabd7b1311fd5a9e92f4b476b71bc78bb303b52","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/publicdomain/","primary_cat":"hep-lat","submitted_at":"2014-04-17T23:47:53Z","title_canon_sha256":"bf2999586d32cfec6307b4272271b28fd5b37b715fc4416b1ee0222d63fe07e3"},"schema_version":"1.0","source":{"id":"1404.4670","kind":"arxiv","version":2}},"canonical_sha256":"ef6377120af181239a7ff82e483b4a63d5e26d1799664d02d6819b072b1b4caf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ef6377120af181239a7ff82e483b4a63d5e26d1799664d02d6819b072b1b4caf","first_computed_at":"2026-05-18T02:22:29.921561Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:22:29.921561Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"08AA60iyse/geuqfCRAZiJx3NjSvIXA/s0JIkQy0xzWCc/YhvtqFgXYF8xoIPq3g1PKBedzDI1lO5ZZnamBjDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:22:29.922007Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.4670","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8f0740f5e60f83036447845549275c929c81f434ab784ab389e4d624080775d9","sha256:6c3156bdb489ece3ef666ce35b5d3fb5b8ac500cc9ab04d7b41957386de54169"],"state_sha256":"7d3b17e067a44ae7575e62433a7beaa0fd1145ebf29a9266e8cf15241b8a5251"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UfwMHHHwIumV5+8D/XOpWL171vnxu9qIYghI5Ie3vFYaWZ7YU15my3Eumlm6KSpC/42MPRboA8NExUcGy+34AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T20:07:52.044441Z","bundle_sha256":"9dbfe4f973a0c5159bbf508edfe7c199580ac7d31a966361201ca52226be0734"}}