{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:DOQQCT4YVM4AJIYB63MVNFSMCF","short_pith_number":"pith:DOQQCT4Y","canonical_record":{"source":{"id":"hep-ph/0603196","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-23T18:28:08Z","cross_cats_sorted":[],"title_canon_sha256":"ab2c7a0dc6abc324df85ad69210fb95bc4e92c8dfd931bc59a9ed24c56a722ee","abstract_canon_sha256":"1a49487cdcc27cba1378f14d574b68eff5f525e0cd659483e51183f6abed2def"},"schema_version":"1.0"},"canonical_sha256":"1ba1014f98ab3804a301f6d956964c1179e777f316e153138eaae52240537feb","source":{"kind":"arxiv","id":"hep-ph/0603196","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0603196","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0603196v1","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0603196","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"pith_short_12","alias_value":"DOQQCT4YVM4A","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"pith_short_16","alias_value":"DOQQCT4YVM4AJIYB","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"pith_short_8","alias_value":"DOQQCT4Y","created_at":"2026-07-04T17:01:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:DOQQCT4YVM4AJIYB63MVNFSMCF","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0603196","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-23T18:28:08Z","cross_cats_sorted":[],"title_canon_sha256":"ab2c7a0dc6abc324df85ad69210fb95bc4e92c8dfd931bc59a9ed24c56a722ee","abstract_canon_sha256":"1a49487cdcc27cba1378f14d574b68eff5f525e0cd659483e51183f6abed2def"},"schema_version":"1.0"},"canonical_sha256":"1ba1014f98ab3804a301f6d956964c1179e777f316e153138eaae52240537feb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:01:42.233773Z","signature_b64":"mybRpypshVy3Lm95QKA+JPhXGl4h+W/9NXv/KooBq0yNtGYuVI/f9yvqcW+Yo9b9oiOtoxVooA7TQ5/Cvg7pDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1ba1014f98ab3804a301f6d956964c1179e777f316e153138eaae52240537feb","last_reissued_at":"2026-07-04T17:01:42.233429Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:01:42.233429Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0603196","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":"2026-07-04T17:01:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"j1FlfpnQ5Y6hKkbaK7yp6N0bKulPo8lZuRKR7/KsuJRf0YrJqJnqHShmpe/qyQnKqE3lAgu7hjVrzVYX01sgDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T14:41:08.594125Z"},"content_sha256":"05dc6814d4ab90353b711cb09cb2b6c906318290c747412fd14dd3ab7e157e1c","schema_version":"1.0","event_id":"sha256:05dc6814d4ab90353b711cb09cb2b6c906318290c747412fd14dd3ab7e157e1c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:DOQQCT4YVM4AJIYB63MVNFSMCF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Constituent Quark Masses and the Electroweak Standard Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Rupp, M.D. Scadron, R. Delbourgo","submitted_at":"2006-03-23T18:28:08Z","abstract_excerpt":"Constituent quark masses can be determined quite well from experimental data in several ways and one can obtain fairly accurate values for all six $m_q$. The strong quark-meson coupling $g=2\\pi /\\sqrt{3}$ arises from the quark-level linear $\\sigma$ model, whereas $e$ and $\\sin\\theta_w$ arise from weak interactions when the heavy $M_W$ and $M_Z$ are regarded as resonances in analogy with the strong KSFR relation. The Higgs boson mass, tied to null expectation value of charged Higgs components, is found to be around 317 GeV. Finally, the experimental CPV phase angle $\\delta$ and the three CKM an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0603196","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/0603196/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":"2026-07-04T17:01:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sDPwz68rTsDJFahTaPtbbNFfalhyAg0I+lRTX6hiamgrMa23nknJ57E3qdxiQi3TsedJLcyovKTlirB2zlfEBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T14:41:08.594642Z"},"content_sha256":"bc53ced43d575ece3e452bb4d1f056c40f42c9fb4bcff22cd6813b6ea09b2e57","schema_version":"1.0","event_id":"sha256:bc53ced43d575ece3e452bb4d1f056c40f42c9fb4bcff22cd6813b6ea09b2e57"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DOQQCT4YVM4AJIYB63MVNFSMCF/bundle.json","state_url":"https://pith.science/pith/DOQQCT4YVM4AJIYB63MVNFSMCF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DOQQCT4YVM4AJIYB63MVNFSMCF/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":"2026-08-16T14:41:08Z","links":{"resolver":"https://pith.science/pith/DOQQCT4YVM4AJIYB63MVNFSMCF","bundle":"https://pith.science/pith/DOQQCT4YVM4AJIYB63MVNFSMCF/bundle.json","state":"https://pith.science/pith/DOQQCT4YVM4AJIYB63MVNFSMCF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DOQQCT4YVM4AJIYB63MVNFSMCF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:DOQQCT4YVM4AJIYB63MVNFSMCF","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":"1a49487cdcc27cba1378f14d574b68eff5f525e0cd659483e51183f6abed2def","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-23T18:28:08Z","title_canon_sha256":"ab2c7a0dc6abc324df85ad69210fb95bc4e92c8dfd931bc59a9ed24c56a722ee"},"schema_version":"1.0","source":{"id":"hep-ph/0603196","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0603196","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0603196v1","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0603196","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"pith_short_12","alias_value":"DOQQCT4YVM4A","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"pith_short_16","alias_value":"DOQQCT4YVM4AJIYB","created_at":"2026-07-04T17:01:42Z"},{"alias_kind":"pith_short_8","alias_value":"DOQQCT4Y","created_at":"2026-07-04T17:01:42Z"}],"graph_snapshots":[{"event_id":"sha256:bc53ced43d575ece3e452bb4d1f056c40f42c9fb4bcff22cd6813b6ea09b2e57","target":"graph","created_at":"2026-07-04T17:01:42Z","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/0603196/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Constituent quark masses can be determined quite well from experimental data in several ways and one can obtain fairly accurate values for all six $m_q$. The strong quark-meson coupling $g=2\\pi /\\sqrt{3}$ arises from the quark-level linear $\\sigma$ model, whereas $e$ and $\\sin\\theta_w$ arise from weak interactions when the heavy $M_W$ and $M_Z$ are regarded as resonances in analogy with the strong KSFR relation. The Higgs boson mass, tied to null expectation value of charged Higgs components, is found to be around 317 GeV. Finally, the experimental CPV phase angle $\\delta$ and the three CKM an","authors_text":"G. Rupp, M.D. Scadron, R. Delbourgo","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2006-03-23T18:28:08Z","title":"Constituent Quark Masses and the Electroweak Standard Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0603196","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":"sha256:05dc6814d4ab90353b711cb09cb2b6c906318290c747412fd14dd3ab7e157e1c","target":"record","created_at":"2026-07-04T17:01:42Z","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":"1a49487cdcc27cba1378f14d574b68eff5f525e0cd659483e51183f6abed2def","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-23T18:28:08Z","title_canon_sha256":"ab2c7a0dc6abc324df85ad69210fb95bc4e92c8dfd931bc59a9ed24c56a722ee"},"schema_version":"1.0","source":{"id":"hep-ph/0603196","kind":"arxiv","version":1}},"canonical_sha256":"1ba1014f98ab3804a301f6d956964c1179e777f316e153138eaae52240537feb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1ba1014f98ab3804a301f6d956964c1179e777f316e153138eaae52240537feb","first_computed_at":"2026-07-04T17:01:42.233429Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:01:42.233429Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mybRpypshVy3Lm95QKA+JPhXGl4h+W/9NXv/KooBq0yNtGYuVI/f9yvqcW+Yo9b9oiOtoxVooA7TQ5/Cvg7pDA==","signature_status":"signed_v1","signed_at":"2026-07-04T17:01:42.233773Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0603196","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:05dc6814d4ab90353b711cb09cb2b6c906318290c747412fd14dd3ab7e157e1c","sha256:bc53ced43d575ece3e452bb4d1f056c40f42c9fb4bcff22cd6813b6ea09b2e57"],"state_sha256":"3b391b898b8d796eb0b88009ba211f0cdc1e85c388e7920cf1528b7ba0101440"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gE++AWvzkydwh2VKMOxCucELJVB2UbYdtpRD0g2hxQkC7yFXfNq1mTw/xt70q0PMrR+nWOGHoR9nzMqDnUwtAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T14:41:08.600334Z","bundle_sha256":"6630ea027dbf50949a2701685b9301970394ba69a1dc0a636d54e79af77940df"}}