{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:3P7CC7LKUI6KPSZ4M6JYE7OLRE","short_pith_number":"pith:3P7CC7LK","canonical_record":{"source":{"id":"hep-lat/0511004","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-11-01T16:05:00Z","cross_cats_sorted":[],"title_canon_sha256":"cbd12cfe99b5b6894693dd3148cb6a6037694486f41d700d608f21284d6ef60f","abstract_canon_sha256":"6a5ebfa858ddad73b4faa84b0e74a8f1ebc40e3c4a9ef213bef319274476d85e"},"schema_version":"1.0"},"canonical_sha256":"dbfe217d6aa23ca7cb3c6793827dcb890662a3a514d365efb949519e5a342300","source":{"kind":"arxiv","id":"hep-lat/0511004","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0511004","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0511004v1","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0511004","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"pith_short_12","alias_value":"3P7CC7LKUI6K","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"pith_short_16","alias_value":"3P7CC7LKUI6KPSZ4","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"pith_short_8","alias_value":"3P7CC7LK","created_at":"2026-07-04T17:21:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:3P7CC7LKUI6KPSZ4M6JYE7OLRE","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0511004","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-11-01T16:05:00Z","cross_cats_sorted":[],"title_canon_sha256":"cbd12cfe99b5b6894693dd3148cb6a6037694486f41d700d608f21284d6ef60f","abstract_canon_sha256":"6a5ebfa858ddad73b4faa84b0e74a8f1ebc40e3c4a9ef213bef319274476d85e"},"schema_version":"1.0"},"canonical_sha256":"dbfe217d6aa23ca7cb3c6793827dcb890662a3a514d365efb949519e5a342300","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:21:52.806379Z","signature_b64":"Xa3aiP3bGJDG+o4R4vtTaVSZRYHUXQy/it7E81u+6dJBGKq955wLgdcPlJy9cOdoJbnJJc65VFC9McPHIpeBBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dbfe217d6aa23ca7cb3c6793827dcb890662a3a514d365efb949519e5a342300","last_reissued_at":"2026-07-04T17:21:52.805968Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:21:52.805968Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0511004","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":"2026-07-04T17:21:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tJPIuJZa6PlZq3EGVWPZV74xzqZAIw3KzNo83WxmmEHSPiKKN10GHKcc1MMSOUghEoXnFTwBk4bvtoSjzmUGAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:23:19.229480Z"},"content_sha256":"82ba776b78b44e67deca2d9322dc651f093e5bff67073c5e1c7d2eeac0ab065e","schema_version":"1.0","event_id":"sha256:82ba776b78b44e67deca2d9322dc651f093e5bff67073c5e1c7d2eeac0ab065e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:3P7CC7LKUI6KPSZ4M6JYE7OLRE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chiral and Continuum Extrapolation of Partially-Quenched Hadron Masses","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. W. Thomas, C. R. Allton, D. B. Leinweber, R. D. Young, W. Armour","submitted_at":"2005-11-01T16:05:00Z","abstract_excerpt":"Using the finite-range regularisation (FRR) of chiral effective field theory, the chiral extrapolation formula for the vector meson mass is derived for the case of partially-quenched QCD. We re-analyse the dynamical fermion QCD data for the vector meson mass from the CP-PACS collaboration. A global fit, including finite lattice spacing effects, of all 16 of their ensembles is performed. We study the FRR method together with a naive polynomial approach and find excellent agreement ~1% with the experimental value of M_rho from the former approach. These results are extended to the case of the nu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0511004","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-lat/0511004/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":"2026-07-04T17:21:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fn3PhS9rmtdI3uBAgPJ3E/ATdXDpfaYg6oJ9f9UY1KuMEMIA1D+dlR+51gOCi3n0Okttp/AvZGjWYPvgi2nyBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:23:19.229986Z"},"content_sha256":"e030da46ac81361b5be4d78c012e58f6f3f6128f4b044eb4d9c96f4728a9e13f","schema_version":"1.0","event_id":"sha256:e030da46ac81361b5be4d78c012e58f6f3f6128f4b044eb4d9c96f4728a9e13f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3P7CC7LKUI6KPSZ4M6JYE7OLRE/bundle.json","state_url":"https://pith.science/pith/3P7CC7LKUI6KPSZ4M6JYE7OLRE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3P7CC7LKUI6KPSZ4M6JYE7OLRE/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":"2026-08-11T10:23:19Z","links":{"resolver":"https://pith.science/pith/3P7CC7LKUI6KPSZ4M6JYE7OLRE","bundle":"https://pith.science/pith/3P7CC7LKUI6KPSZ4M6JYE7OLRE/bundle.json","state":"https://pith.science/pith/3P7CC7LKUI6KPSZ4M6JYE7OLRE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3P7CC7LKUI6KPSZ4M6JYE7OLRE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:3P7CC7LKUI6KPSZ4M6JYE7OLRE","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":"6a5ebfa858ddad73b4faa84b0e74a8f1ebc40e3c4a9ef213bef319274476d85e","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2005-11-01T16:05:00Z","title_canon_sha256":"cbd12cfe99b5b6894693dd3148cb6a6037694486f41d700d608f21284d6ef60f"},"schema_version":"1.0","source":{"id":"hep-lat/0511004","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0511004","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0511004v1","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0511004","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"pith_short_12","alias_value":"3P7CC7LKUI6K","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"pith_short_16","alias_value":"3P7CC7LKUI6KPSZ4","created_at":"2026-07-04T17:21:52Z"},{"alias_kind":"pith_short_8","alias_value":"3P7CC7LK","created_at":"2026-07-04T17:21:52Z"}],"graph_snapshots":[{"event_id":"sha256:e030da46ac81361b5be4d78c012e58f6f3f6128f4b044eb4d9c96f4728a9e13f","target":"graph","created_at":"2026-07-04T17:21:52Z","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-lat/0511004/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Using the finite-range regularisation (FRR) of chiral effective field theory, the chiral extrapolation formula for the vector meson mass is derived for the case of partially-quenched QCD. We re-analyse the dynamical fermion QCD data for the vector meson mass from the CP-PACS collaboration. A global fit, including finite lattice spacing effects, of all 16 of their ensembles is performed. We study the FRR method together with a naive polynomial approach and find excellent agreement ~1% with the experimental value of M_rho from the former approach. These results are extended to the case of the nu","authors_text":"A. W. Thomas, C. R. Allton, D. B. Leinweber, R. D. Young, W. Armour","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2005-11-01T16:05:00Z","title":"Chiral and Continuum Extrapolation of Partially-Quenched Hadron Masses"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0511004","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":"sha256:82ba776b78b44e67deca2d9322dc651f093e5bff67073c5e1c7d2eeac0ab065e","target":"record","created_at":"2026-07-04T17:21:52Z","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":"6a5ebfa858ddad73b4faa84b0e74a8f1ebc40e3c4a9ef213bef319274476d85e","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2005-11-01T16:05:00Z","title_canon_sha256":"cbd12cfe99b5b6894693dd3148cb6a6037694486f41d700d608f21284d6ef60f"},"schema_version":"1.0","source":{"id":"hep-lat/0511004","kind":"arxiv","version":1}},"canonical_sha256":"dbfe217d6aa23ca7cb3c6793827dcb890662a3a514d365efb949519e5a342300","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dbfe217d6aa23ca7cb3c6793827dcb890662a3a514d365efb949519e5a342300","first_computed_at":"2026-07-04T17:21:52.805968Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:21:52.805968Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Xa3aiP3bGJDG+o4R4vtTaVSZRYHUXQy/it7E81u+6dJBGKq955wLgdcPlJy9cOdoJbnJJc65VFC9McPHIpeBBQ==","signature_status":"signed_v1","signed_at":"2026-07-04T17:21:52.806379Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0511004","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:82ba776b78b44e67deca2d9322dc651f093e5bff67073c5e1c7d2eeac0ab065e","sha256:e030da46ac81361b5be4d78c012e58f6f3f6128f4b044eb4d9c96f4728a9e13f"],"state_sha256":"6ffb7a5811b09d83251bc5f66932cb3842219ec46b045eec1e2640f19bebbe6c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2jLch+wc8T/VIRPibTFG8TKcQWPVhxB0canQVVINpquf/IOm0bNedtaFSF2hZaGsmPBma7HW4cJjKEbaiSgFBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T10:23:19.234393Z","bundle_sha256":"c378bea9cdda9dd96d754565e578c5f63fa05f41fe3c0d3c73833426031e7f99"}}