{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:EEJNAV7NGJZT3PNZ5A63RPLF4G","short_pith_number":"pith:EEJNAV7N","canonical_record":{"source":{"id":"hep-ph/0511160","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-11-14T00:59:43Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"e8b9f0e33478107786a73f9a045f2f69f163a4b46933e66f36f91f57908f2652","abstract_canon_sha256":"ceb8630c22c34adc30362247424de8fe1a414f46ccd9e77496513b3502218fec"},"schema_version":"1.0"},"canonical_sha256":"2112d057ed32733dbdb9e83db8bd65e1aaca61b880e7fbcb136b88f2ac4b6dfa","source":{"kind":"arxiv","id":"hep-ph/0511160","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0511160","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0511160v1","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0511160","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_12","alias_value":"EEJNAV7NGJZT","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_16","alias_value":"EEJNAV7NGJZT3PNZ","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_8","alias_value":"EEJNAV7N","created_at":"2026-07-04T15:19:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:EEJNAV7NGJZT3PNZ5A63RPLF4G","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0511160","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-11-14T00:59:43Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"e8b9f0e33478107786a73f9a045f2f69f163a4b46933e66f36f91f57908f2652","abstract_canon_sha256":"ceb8630c22c34adc30362247424de8fe1a414f46ccd9e77496513b3502218fec"},"schema_version":"1.0"},"canonical_sha256":"2112d057ed32733dbdb9e83db8bd65e1aaca61b880e7fbcb136b88f2ac4b6dfa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:19:47.017618Z","signature_b64":"7d/EhVn2Jsae8sBDGenQkPojJEBv3rPmLpHZPK1QyoWpa02MWsiJ+3zr7ec2Dh6q8g2Nc7bCkJWWpukUmdpIDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2112d057ed32733dbdb9e83db8bd65e1aaca61b880e7fbcb136b88f2ac4b6dfa","last_reissued_at":"2026-07-04T15:19:47.017240Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:19:47.017240Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0511160","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:19:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l50P2t0Tag9F3i0eVdX9K4M4fmWYbqiPPnxrhnTykUAdmPzeq/DUnezrIGgjloz3MrIPT1XqXJgDw2F/DpsoCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T16:28:03.198020Z"},"content_sha256":"602c52e6667bd068078fb290e0f34520d1d480dc1dc107a375bc40135ba7f221","schema_version":"1.0","event_id":"sha256:602c52e6667bd068078fb290e0f34520d1d480dc1dc107a375bc40135ba7f221"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:EEJNAV7NGJZT3PNZ5A63RPLF4G","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High-precision determination of the light-quark masses from realistic lattice QCD","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Christine T. H. Davies, G. Peter Lepage, Howard D. Trottier, Quentin Mason, Ron Horgan","submitted_at":"2005-11-14T00:59:43Z","abstract_excerpt":"Three-flavor lattice QCD simulations and two-loop perturbation theory are used to make the most precise determination to date of the strange-, up-, and down-quark masses, $m_s$, $m_u$, and $m_d$, respectively. Perturbative matching is required in order to connect the lattice-regularized bare- quark masses to the masses as defined in the \\msbar scheme, and this is done here for the first time at next-to-next-to leading (or two-loop) order. The bare-quark masses required as input come from simulations by the MILC collaboration of a highly-efficient formalism (using so-called ``staggered'' quarks"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0511160","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0511160/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:19:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2oF16VXeyZWtNH6Jrcu2rXpo99z9is7BajjMVvRoQY00djxi4pJXQ36Y5lKsoM07sGAN+HEQIO9JV8nIOClDDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T16:28:03.198718Z"},"content_sha256":"b50e7615367799f1dc0dd9f70e994160fe6fe7dc209ac1c7d308abc8f2338ef2","schema_version":"1.0","event_id":"sha256:b50e7615367799f1dc0dd9f70e994160fe6fe7dc209ac1c7d308abc8f2338ef2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EEJNAV7NGJZT3PNZ5A63RPLF4G/bundle.json","state_url":"https://pith.science/pith/EEJNAV7NGJZT3PNZ5A63RPLF4G/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EEJNAV7NGJZT3PNZ5A63RPLF4G/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":"2026-08-20T16:28:03Z","links":{"resolver":"https://pith.science/pith/EEJNAV7NGJZT3PNZ5A63RPLF4G","bundle":"https://pith.science/pith/EEJNAV7NGJZT3PNZ5A63RPLF4G/bundle.json","state":"https://pith.science/pith/EEJNAV7NGJZT3PNZ5A63RPLF4G/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EEJNAV7NGJZT3PNZ5A63RPLF4G/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:EEJNAV7NGJZT3PNZ5A63RPLF4G","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":"ceb8630c22c34adc30362247424de8fe1a414f46ccd9e77496513b3502218fec","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"2005-11-14T00:59:43Z","title_canon_sha256":"e8b9f0e33478107786a73f9a045f2f69f163a4b46933e66f36f91f57908f2652"},"schema_version":"1.0","source":{"id":"hep-ph/0511160","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0511160","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0511160v1","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0511160","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_12","alias_value":"EEJNAV7NGJZT","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_16","alias_value":"EEJNAV7NGJZT3PNZ","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_8","alias_value":"EEJNAV7N","created_at":"2026-07-04T15:19:47Z"}],"graph_snapshots":[{"event_id":"sha256:b50e7615367799f1dc0dd9f70e994160fe6fe7dc209ac1c7d308abc8f2338ef2","target":"graph","created_at":"2026-07-04T15:19:47Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/0511160/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Three-flavor lattice QCD simulations and two-loop perturbation theory are used to make the most precise determination to date of the strange-, up-, and down-quark masses, $m_s$, $m_u$, and $m_d$, respectively. Perturbative matching is required in order to connect the lattice-regularized bare- quark masses to the masses as defined in the \\msbar scheme, and this is done here for the first time at next-to-next-to leading (or two-loop) order. The bare-quark masses required as input come from simulations by the MILC collaboration of a highly-efficient formalism (using so-called ``staggered'' quarks","authors_text":"Christine T. H. Davies, G. Peter Lepage, Howard D. Trottier, Quentin Mason, Ron Horgan","cross_cats":["hep-lat"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2005-11-14T00:59:43Z","title":"High-precision determination of the light-quark masses from realistic lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0511160","kind":"arxiv","version":1},"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":"sha256:602c52e6667bd068078fb290e0f34520d1d480dc1dc107a375bc40135ba7f221","target":"record","created_at":"2026-07-04T15:19:47Z","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":"ceb8630c22c34adc30362247424de8fe1a414f46ccd9e77496513b3502218fec","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"2005-11-14T00:59:43Z","title_canon_sha256":"e8b9f0e33478107786a73f9a045f2f69f163a4b46933e66f36f91f57908f2652"},"schema_version":"1.0","source":{"id":"hep-ph/0511160","kind":"arxiv","version":1}},"canonical_sha256":"2112d057ed32733dbdb9e83db8bd65e1aaca61b880e7fbcb136b88f2ac4b6dfa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2112d057ed32733dbdb9e83db8bd65e1aaca61b880e7fbcb136b88f2ac4b6dfa","first_computed_at":"2026-07-04T15:19:47.017240Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:19:47.017240Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7d/EhVn2Jsae8sBDGenQkPojJEBv3rPmLpHZPK1QyoWpa02MWsiJ+3zr7ec2Dh6q8g2Nc7bCkJWWpukUmdpIDw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:19:47.017618Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0511160","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:602c52e6667bd068078fb290e0f34520d1d480dc1dc107a375bc40135ba7f221","sha256:b50e7615367799f1dc0dd9f70e994160fe6fe7dc209ac1c7d308abc8f2338ef2"],"state_sha256":"badaa6d3a917391273123ddade59c9f288958c742748e6b6f78f3960c51e5b38"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lO/BoXky6sUmAUpwzrKH4dDj7iEfOJQA4ZoqLyR40xwWxKRcpaFAMFytBSSrN9ZAP9yAl1vRxaHfXDrFHbEYDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-20T16:28:03.204189Z","bundle_sha256":"9d6ca9e6effa8b17436727f027034a09541c3550281fabc496415b1854d0adff"}}