{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:KU6DWLGZW7AVORLOOQUQ3EU6ZQ","short_pith_number":"pith:KU6DWLGZ","canonical_record":{"source":{"id":"1210.5887","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-22T13:14:32Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"2f772092923600415c81c65d82b6568a9da34bc159c79ac9cc96f9ae10c6b681","abstract_canon_sha256":"7644154315765de99689547563d6494b76dbecd99bdfb23ea269011d1c6bbcc3"},"schema_version":"1.0"},"canonical_sha256":"553c3b2cd9b7c157456e74290d929ecc296848f02a729692af7517012d83510e","source":{"kind":"arxiv","id":"1210.5887","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.5887","created_at":"2026-05-18T03:37:52Z"},{"alias_kind":"arxiv_version","alias_value":"1210.5887v3","created_at":"2026-05-18T03:37:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.5887","created_at":"2026-05-18T03:37:52Z"},{"alias_kind":"pith_short_12","alias_value":"KU6DWLGZW7AV","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KU6DWLGZW7AVORLO","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KU6DWLGZ","created_at":"2026-05-18T12:27:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:KU6DWLGZW7AVORLOOQUQ3EU6ZQ","target":"record","payload":{"canonical_record":{"source":{"id":"1210.5887","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-22T13:14:32Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"2f772092923600415c81c65d82b6568a9da34bc159c79ac9cc96f9ae10c6b681","abstract_canon_sha256":"7644154315765de99689547563d6494b76dbecd99bdfb23ea269011d1c6bbcc3"},"schema_version":"1.0"},"canonical_sha256":"553c3b2cd9b7c157456e74290d929ecc296848f02a729692af7517012d83510e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:37:52.344641Z","signature_b64":"MGEHq4yCWhivWKP8AvrZi1C5m+zk4PjmDF0i4PbGmCAIAN1potarPiGQPTIgVxE3wAgZ/Oe3fgxqFd4lBXUqDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"553c3b2cd9b7c157456e74290d929ecc296848f02a729692af7517012d83510e","last_reissued_at":"2026-05-18T03:37:52.343891Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:37:52.343891Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.5887","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:37:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gmXk588SScTTTNmQ/Y4YDLLJ9H3OiGiCekuPs6B9qIQZAzOxiudFH+Cerjz3z/EeDLIURa+R9HCKbOPxTnx5CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:55:30.383011Z"},"content_sha256":"8b3ee1ce56b02b59b7c4273263502c15d804c53a7386f2fedb0f73a77baf8a2f","schema_version":"1.0","event_id":"sha256:8b3ee1ce56b02b59b7c4273263502c15d804c53a7386f2fedb0f73a77baf8a2f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:KU6DWLGZW7AVORLOOQUQ3EU6ZQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Baryon electric dipole moments from strong CP violation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Feng-Kun Guo, Ulf-G. Mei{\\ss}ner","submitted_at":"2012-10-22T13:14:32Z","abstract_excerpt":"The electric dipole form factors and moments of the ground state baryons are calculated in chiral perturbation theory at next-to-leading order. We show that the baryon electric dipole form factors at this order depend only on two combinations of low-energy constants. We also derive various relations that are free of unknown low-energy constants. We use recent lattice QCD data to calculate all baryon EDMs. In particular, we find d_n = -2.9\\pm 0.9 and d_p = 1.1\\pm 1.1 in units of 10^{-16} e \\theta_0 cm. Finite volume corrections to the moments are also worked out. We show that for a precision ex"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.5887","kind":"arxiv","version":3},"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":"2026-05-18T03:37:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3mvEW/bwKSVshc52ObAcfFEjxNstp7CrwrWrG3sJDopdjYqG78FFftaWHS8kY5165dvN+doOf2e+mRsyVQBhCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:55:30.383744Z"},"content_sha256":"1798124781ebd3e0fff4774ccae03140f84d893d0a8b47e8b102016c29a77268","schema_version":"1.0","event_id":"sha256:1798124781ebd3e0fff4774ccae03140f84d893d0a8b47e8b102016c29a77268"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KU6DWLGZW7AVORLOOQUQ3EU6ZQ/bundle.json","state_url":"https://pith.science/pith/KU6DWLGZW7AVORLOOQUQ3EU6ZQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KU6DWLGZW7AVORLOOQUQ3EU6ZQ/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":"2026-05-25T18:55:30Z","links":{"resolver":"https://pith.science/pith/KU6DWLGZW7AVORLOOQUQ3EU6ZQ","bundle":"https://pith.science/pith/KU6DWLGZW7AVORLOOQUQ3EU6ZQ/bundle.json","state":"https://pith.science/pith/KU6DWLGZW7AVORLOOQUQ3EU6ZQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KU6DWLGZW7AVORLOOQUQ3EU6ZQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:KU6DWLGZW7AVORLOOQUQ3EU6ZQ","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":"7644154315765de99689547563d6494b76dbecd99bdfb23ea269011d1c6bbcc3","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-22T13:14:32Z","title_canon_sha256":"2f772092923600415c81c65d82b6568a9da34bc159c79ac9cc96f9ae10c6b681"},"schema_version":"1.0","source":{"id":"1210.5887","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.5887","created_at":"2026-05-18T03:37:52Z"},{"alias_kind":"arxiv_version","alias_value":"1210.5887v3","created_at":"2026-05-18T03:37:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.5887","created_at":"2026-05-18T03:37:52Z"},{"alias_kind":"pith_short_12","alias_value":"KU6DWLGZW7AV","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KU6DWLGZW7AVORLO","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KU6DWLGZ","created_at":"2026-05-18T12:27:11Z"}],"graph_snapshots":[{"event_id":"sha256:1798124781ebd3e0fff4774ccae03140f84d893d0a8b47e8b102016c29a77268","target":"graph","created_at":"2026-05-18T03:37:52Z","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"},"paper":{"abstract_excerpt":"The electric dipole form factors and moments of the ground state baryons are calculated in chiral perturbation theory at next-to-leading order. We show that the baryon electric dipole form factors at this order depend only on two combinations of low-energy constants. We also derive various relations that are free of unknown low-energy constants. We use recent lattice QCD data to calculate all baryon EDMs. In particular, we find d_n = -2.9\\pm 0.9 and d_p = 1.1\\pm 1.1 in units of 10^{-16} e \\theta_0 cm. Finite volume corrections to the moments are also worked out. We show that for a precision ex","authors_text":"Feng-Kun Guo, Ulf-G. Mei{\\ss}ner","cross_cats":["hep-lat","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-22T13:14:32Z","title":"Baryon electric dipole moments from strong CP violation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.5887","kind":"arxiv","version":3},"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":"sha256:8b3ee1ce56b02b59b7c4273263502c15d804c53a7386f2fedb0f73a77baf8a2f","target":"record","created_at":"2026-05-18T03:37:52Z","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":"7644154315765de99689547563d6494b76dbecd99bdfb23ea269011d1c6bbcc3","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-22T13:14:32Z","title_canon_sha256":"2f772092923600415c81c65d82b6568a9da34bc159c79ac9cc96f9ae10c6b681"},"schema_version":"1.0","source":{"id":"1210.5887","kind":"arxiv","version":3}},"canonical_sha256":"553c3b2cd9b7c157456e74290d929ecc296848f02a729692af7517012d83510e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"553c3b2cd9b7c157456e74290d929ecc296848f02a729692af7517012d83510e","first_computed_at":"2026-05-18T03:37:52.343891Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:37:52.343891Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MGEHq4yCWhivWKP8AvrZi1C5m+zk4PjmDF0i4PbGmCAIAN1potarPiGQPTIgVxE3wAgZ/Oe3fgxqFd4lBXUqDg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:37:52.344641Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.5887","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8b3ee1ce56b02b59b7c4273263502c15d804c53a7386f2fedb0f73a77baf8a2f","sha256:1798124781ebd3e0fff4774ccae03140f84d893d0a8b47e8b102016c29a77268"],"state_sha256":"a0c1e65484ba59305206abd4e6cd8efb1c01da71384d958c67f57bcc3808a086"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"p25vfmTYT1gwaLxtfYBVcmJvFGBCpaIgaP7H49d+DmgiL5I1GmLIGIff4MCJmJMIK49wTmueB9mY7P76y0LXCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:55:30.387851Z","bundle_sha256":"875322e501af19ecfd2c9271395d511eb6d2c7dbec548517edbbf571acb69193"}}