{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:QE7H2CDGTSWWRUNTTAHEJR562N","short_pith_number":"pith:QE7H2CDG","canonical_record":{"source":{"id":"hep-ph/0203175","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-03-18T17:46:00Z","cross_cats_sorted":[],"title_canon_sha256":"b6c194a12f72b5df4661105361370bad876ac40c37ef49086f85a4340c0dc67c","abstract_canon_sha256":"468dcc9b8cd4d4b4b64ce0796f228ce6fbe4bb36be72604628d2a230867461ca"},"schema_version":"1.0"},"canonical_sha256":"813e7d08669cad68d1b3980e44c7bed3605ac1d876767634c41f953f0140bd5b","source":{"kind":"arxiv","id":"hep-ph/0203175","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0203175","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0203175v1","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0203175","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"pith_short_12","alias_value":"QE7H2CDGTSWW","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"QE7H2CDGTSWWRUNT","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"QE7H2CDG","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:QE7H2CDGTSWWRUNTTAHEJR562N","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0203175","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-03-18T17:46:00Z","cross_cats_sorted":[],"title_canon_sha256":"b6c194a12f72b5df4661105361370bad876ac40c37ef49086f85a4340c0dc67c","abstract_canon_sha256":"468dcc9b8cd4d4b4b64ce0796f228ce6fbe4bb36be72604628d2a230867461ca"},"schema_version":"1.0"},"canonical_sha256":"813e7d08669cad68d1b3980e44c7bed3605ac1d876767634c41f953f0140bd5b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:25.913586Z","signature_b64":"PhqvuUbRsBySPkrbjOx7/5AjYgmYdF2qJ9QgCD2ORORZvvH8h/BAdp7W1sW1EFeExCfepWCsS6RCOJweIuXSBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"813e7d08669cad68d1b3980e44c7bed3605ac1d876767634c41f953f0140bd5b","last_reissued_at":"2026-05-18T04:13:25.913061Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:25.913061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0203175","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":"2026-05-18T04:13:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nBRcMe8kxC5M2k3cPaog4KIFWFD0//Osstp4k5uS4Bi32l4UuQIcGvVApYxsBlOjgB28LG9j97Pr+5jAX3IoAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T21:24:29.355746Z"},"content_sha256":"ff52744d6a70ddd907d3ed4fd43224008a467f0a44d0183c03ee7fef5ed55e47","schema_version":"1.0","event_id":"sha256:ff52744d6a70ddd907d3ed4fd43224008a467f0a44d0183c03ee7fef5ed55e47"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:QE7H2CDGTSWWRUNTTAHEJR562N","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Asymptotic conditions for electromagnetic form factors of hadrons represented by VMD model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Z. Dubnickova, C. Adamuscin, P. Weisenpacher, R. Pekarik, S. Dubnicka","submitted_at":"2002-03-18T17:46:00Z","abstract_excerpt":"A system of linear homogeneous algebraic equations for coupling constant ratios of vector-mesons to hadrons is derived by imposing an asymptotic behaviuor upon the VMD pole parametrization of an hadron electromagnetic form factor. A similar system of equations with a simpler structure of coefficients, taken as even powers of vector-meson masses, is derived by means of integral superconvergent sum rules for the imaginary part of the considered from factor using its appropriate delta function approximation. Although both systems have been derived starting from different properties of the electro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0203175","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":"2026-05-18T04:13:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lRLbdT3wqn1hqRvdHIXBX5zRQQUrqZbQqDxMMVqe0ETucAN7KK1oCFDL22l/19AEhZlpX2SlAWwn5AbeKCriAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T21:24:29.356089Z"},"content_sha256":"b4a680ccb5b5c97af69b8e68039e4047385bf7823ea2221061aaef70f8220776","schema_version":"1.0","event_id":"sha256:b4a680ccb5b5c97af69b8e68039e4047385bf7823ea2221061aaef70f8220776"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QE7H2CDGTSWWRUNTTAHEJR562N/bundle.json","state_url":"https://pith.science/pith/QE7H2CDGTSWWRUNTTAHEJR562N/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QE7H2CDGTSWWRUNTTAHEJR562N/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":"2026-05-31T21:24:29Z","links":{"resolver":"https://pith.science/pith/QE7H2CDGTSWWRUNTTAHEJR562N","bundle":"https://pith.science/pith/QE7H2CDGTSWWRUNTTAHEJR562N/bundle.json","state":"https://pith.science/pith/QE7H2CDGTSWWRUNTTAHEJR562N/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QE7H2CDGTSWWRUNTTAHEJR562N/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:QE7H2CDGTSWWRUNTTAHEJR562N","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":"468dcc9b8cd4d4b4b64ce0796f228ce6fbe4bb36be72604628d2a230867461ca","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2002-03-18T17:46:00Z","title_canon_sha256":"b6c194a12f72b5df4661105361370bad876ac40c37ef49086f85a4340c0dc67c"},"schema_version":"1.0","source":{"id":"hep-ph/0203175","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0203175","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0203175v1","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0203175","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"pith_short_12","alias_value":"QE7H2CDGTSWW","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"QE7H2CDGTSWWRUNT","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"QE7H2CDG","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:b4a680ccb5b5c97af69b8e68039e4047385bf7823ea2221061aaef70f8220776","target":"graph","created_at":"2026-05-18T04:13:25Z","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":"A system of linear homogeneous algebraic equations for coupling constant ratios of vector-mesons to hadrons is derived by imposing an asymptotic behaviuor upon the VMD pole parametrization of an hadron electromagnetic form factor. A similar system of equations with a simpler structure of coefficients, taken as even powers of vector-meson masses, is derived by means of integral superconvergent sum rules for the imaginary part of the considered from factor using its appropriate delta function approximation. Although both systems have been derived starting from different properties of the electro","authors_text":"A.Z. Dubnickova, C. Adamuscin, P. Weisenpacher, R. Pekarik, S. Dubnicka","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2002-03-18T17:46:00Z","title":"Asymptotic conditions for electromagnetic form factors of hadrons represented by VMD model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0203175","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:ff52744d6a70ddd907d3ed4fd43224008a467f0a44d0183c03ee7fef5ed55e47","target":"record","created_at":"2026-05-18T04:13:25Z","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":"468dcc9b8cd4d4b4b64ce0796f228ce6fbe4bb36be72604628d2a230867461ca","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2002-03-18T17:46:00Z","title_canon_sha256":"b6c194a12f72b5df4661105361370bad876ac40c37ef49086f85a4340c0dc67c"},"schema_version":"1.0","source":{"id":"hep-ph/0203175","kind":"arxiv","version":1}},"canonical_sha256":"813e7d08669cad68d1b3980e44c7bed3605ac1d876767634c41f953f0140bd5b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"813e7d08669cad68d1b3980e44c7bed3605ac1d876767634c41f953f0140bd5b","first_computed_at":"2026-05-18T04:13:25.913061Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:13:25.913061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PhqvuUbRsBySPkrbjOx7/5AjYgmYdF2qJ9QgCD2ORORZvvH8h/BAdp7W1sW1EFeExCfepWCsS6RCOJweIuXSBw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:13:25.913586Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0203175","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ff52744d6a70ddd907d3ed4fd43224008a467f0a44d0183c03ee7fef5ed55e47","sha256:b4a680ccb5b5c97af69b8e68039e4047385bf7823ea2221061aaef70f8220776"],"state_sha256":"c03d891bad0f425ac51bf6e025779aa5c074b44e5d91e26625dccb22124d4b37"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WlI5kszldsdW1Ji6vIrM5RDIAKtUt9P475nAL1VdAqtml6ubQeyJuyakSgGkFtnUMYWDmoSSs15oYfBTLmfyCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T21:24:29.358019Z","bundle_sha256":"0988fa77a7ecd154712bc665f7492e5ddce8ae9c77279de79aae4ae2e43df950"}}