{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:6I5AOPL6MXOIQRLZQE2RKTA43H","short_pith_number":"pith:6I5AOPL6","canonical_record":{"source":{"id":"hep-lat/0501021","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-01-24T00:24:30Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"2ad4c93c490438ea46deab304fa58c2645d426814b3fa5c17372a5e67188f723","abstract_canon_sha256":"50d2c88420739a623e4ba31588cca3639370627be52b52926fbfd70c7168ac88"},"schema_version":"1.0"},"canonical_sha256":"f23a073d7e65dc8845798135154c1cd9cf53802ce8a1beeee34916f9f9c9f7a7","source":{"kind":"arxiv","id":"hep-lat/0501021","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0501021","created_at":"2026-05-18T04:28:37Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0501021v1","created_at":"2026-05-18T04:28:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0501021","created_at":"2026-05-18T04:28:37Z"},{"alias_kind":"pith_short_12","alias_value":"6I5AOPL6MXOI","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"6I5AOPL6MXOIQRLZ","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"6I5AOPL6","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:6I5AOPL6MXOIQRLZQE2RKTA43H","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0501021","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-01-24T00:24:30Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"2ad4c93c490438ea46deab304fa58c2645d426814b3fa5c17372a5e67188f723","abstract_canon_sha256":"50d2c88420739a623e4ba31588cca3639370627be52b52926fbfd70c7168ac88"},"schema_version":"1.0"},"canonical_sha256":"f23a073d7e65dc8845798135154c1cd9cf53802ce8a1beeee34916f9f9c9f7a7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:37.827915Z","signature_b64":"4oba7ZrAKVfAsrLiI9GiyUJfTFMdOd8Hac4oRIqUqTFt9kZWJKdciJO5oZwwQEVqYCZhISMpDjkHrPWIKyPQCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f23a073d7e65dc8845798135154c1cd9cf53802ce8a1beeee34916f9f9c9f7a7","last_reissued_at":"2026-05-18T04:28:37.827473Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:37.827473Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0501021","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":"2026-05-18T04:28:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rjWXcEuOursf01rIiG1trhZkB2KMYwQ6sSW+Q/Zhvz3jdRgYf1B3AAEUnYHAKW/jX1uXp9oWRLzzbWBKIdhjCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T21:33:17.475851Z"},"content_sha256":"de3f05746e0119c65e6374a151f448068dc12c945fc13a3b6a50c0ba1602a51e","schema_version":"1.0","event_id":"sha256:de3f05746e0119c65e6374a151f448068dc12c945fc13a3b6a50c0ba1602a51e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:6I5AOPL6MXOIQRLZQE2RKTA43H","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Baryon Masses in Lattice QCD with Exact Chiral Symmetry","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Ting-Wai Chiu, Tung-Han Hsieh","submitted_at":"2005-01-24T00:24:30Z","abstract_excerpt":"We investigate the baryon mass spectrum in quenched lattice QCD with exact chiral symmetry. For 100 gauge configurations generated with Wilson gauge action at $ \\beta = 6.1 $ on the $ 20^3 \\times 40 $ lattice, we compute (point-to-point) quark propagators for 30 quark masses in the range $ 67 {MeV} \\le m_q \\le 1790 {MeV} $. For baryons only composed of strange and charm quarks, their masses are extracted directly from the time correlation functions, while for those containing $ u (d) $ light quarks, their masses are obtained by chiral extrapolation to $ m_\\pi = 135 $ MeV. Our results of baryon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0501021","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:28:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"S9qiMK8Fr34de5KzirbSCZJZQCThLBgyemM5Gl7RKhAxEW30Cd9GjH/F7q9/mskvcq9w2vPfVacnfibvj2XFAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T21:33:17.476576Z"},"content_sha256":"60c2e086f75e0c645b4f5236c8b62cfd6e95aeae9324d04806549f5165d8f83a","schema_version":"1.0","event_id":"sha256:60c2e086f75e0c645b4f5236c8b62cfd6e95aeae9324d04806549f5165d8f83a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6I5AOPL6MXOIQRLZQE2RKTA43H/bundle.json","state_url":"https://pith.science/pith/6I5AOPL6MXOIQRLZQE2RKTA43H/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6I5AOPL6MXOIQRLZQE2RKTA43H/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":"2026-05-29T21:33:17Z","links":{"resolver":"https://pith.science/pith/6I5AOPL6MXOIQRLZQE2RKTA43H","bundle":"https://pith.science/pith/6I5AOPL6MXOIQRLZQE2RKTA43H/bundle.json","state":"https://pith.science/pith/6I5AOPL6MXOIQRLZQE2RKTA43H/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6I5AOPL6MXOIQRLZQE2RKTA43H/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:6I5AOPL6MXOIQRLZQE2RKTA43H","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":"50d2c88420739a623e4ba31588cca3639370627be52b52926fbfd70c7168ac88","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2005-01-24T00:24:30Z","title_canon_sha256":"2ad4c93c490438ea46deab304fa58c2645d426814b3fa5c17372a5e67188f723"},"schema_version":"1.0","source":{"id":"hep-lat/0501021","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0501021","created_at":"2026-05-18T04:28:37Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0501021v1","created_at":"2026-05-18T04:28:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0501021","created_at":"2026-05-18T04:28:37Z"},{"alias_kind":"pith_short_12","alias_value":"6I5AOPL6MXOI","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"6I5AOPL6MXOIQRLZ","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"6I5AOPL6","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:60c2e086f75e0c645b4f5236c8b62cfd6e95aeae9324d04806549f5165d8f83a","target":"graph","created_at":"2026-05-18T04:28:37Z","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 investigate the baryon mass spectrum in quenched lattice QCD with exact chiral symmetry. For 100 gauge configurations generated with Wilson gauge action at $ \\beta = 6.1 $ on the $ 20^3 \\times 40 $ lattice, we compute (point-to-point) quark propagators for 30 quark masses in the range $ 67 {MeV} \\le m_q \\le 1790 {MeV} $. For baryons only composed of strange and charm quarks, their masses are extracted directly from the time correlation functions, while for those containing $ u (d) $ light quarks, their masses are obtained by chiral extrapolation to $ m_\\pi = 135 $ MeV. Our results of baryon","authors_text":"Ting-Wai Chiu, Tung-Han Hsieh","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2005-01-24T00:24:30Z","title":"Baryon Masses in Lattice QCD with Exact Chiral Symmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0501021","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:de3f05746e0119c65e6374a151f448068dc12c945fc13a3b6a50c0ba1602a51e","target":"record","created_at":"2026-05-18T04:28:37Z","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":"50d2c88420739a623e4ba31588cca3639370627be52b52926fbfd70c7168ac88","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2005-01-24T00:24:30Z","title_canon_sha256":"2ad4c93c490438ea46deab304fa58c2645d426814b3fa5c17372a5e67188f723"},"schema_version":"1.0","source":{"id":"hep-lat/0501021","kind":"arxiv","version":1}},"canonical_sha256":"f23a073d7e65dc8845798135154c1cd9cf53802ce8a1beeee34916f9f9c9f7a7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f23a073d7e65dc8845798135154c1cd9cf53802ce8a1beeee34916f9f9c9f7a7","first_computed_at":"2026-05-18T04:28:37.827473Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:28:37.827473Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4oba7ZrAKVfAsrLiI9GiyUJfTFMdOd8Hac4oRIqUqTFt9kZWJKdciJO5oZwwQEVqYCZhISMpDjkHrPWIKyPQCg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:28:37.827915Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0501021","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:de3f05746e0119c65e6374a151f448068dc12c945fc13a3b6a50c0ba1602a51e","sha256:60c2e086f75e0c645b4f5236c8b62cfd6e95aeae9324d04806549f5165d8f83a"],"state_sha256":"a42859368c789fae0cb3d7de33438357238b0091413bfa83c506629188dd09c6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P8U/Mq7LW29ufBrQQ91pF6joCffMzd1SDlGHNno62gIPUYX5OQKdkqU01vfqiB6ju1ta+4AmXCE+dE7p8Sq6Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T21:33:17.481052Z","bundle_sha256":"1c4b22c271555e642098967b1ff09be43c930dc8c66cddefd84e418c1e4f47cb"}}