{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:NTCOOKHDZAIHKSVFPLPYG5AHNQ","short_pith_number":"pith:NTCOOKHD","schema_version":"1.0","canonical_sha256":"6cc4e728e3c810754aa57adf8374076c115857334624b7c1aa284f47962ebd4c","source":{"kind":"arxiv","id":"hep-ph/0601194","version":1},"attestation_state":"computed","paper":{"title":"Extended Derivative Dispersion Relations","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.J. Menon, R.F. Avila","submitted_at":"2006-01-24T11:13:16Z","abstract_excerpt":"It is shown that, for a wide class of functions with physical interest as forward scattering amplitudes, integral dispersion relations can be replaced by derivative forms without any high-energy approximation. The applicability of these extended derivative relations, in the investigation of forward proton-proton and antiproton-proton elastic scattering, is exemplified by means of a Pomeron-Reggeon model with totally nondegenerate trajectories."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/0601194","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-01-24T11:13:16Z","cross_cats_sorted":[],"title_canon_sha256":"4de65297ebd6006c6792a6ac115d6ce2bf3d82fa78e0d72cac6b9d091255983d","abstract_canon_sha256":"fff860f69b9b5416c22e8449b6e20e298b0b927c09c3e044616c2aef48932f9e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:02.602978Z","signature_b64":"zr1KclKfA9OrF7DoHoiGva2z3onDrJf5RiTpLT7iU2PexK2qNwc47nk6hg/RNQ8gjvdG0K7xClojh2FgHE6WCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6cc4e728e3c810754aa57adf8374076c115857334624b7c1aa284f47962ebd4c","last_reissued_at":"2026-05-18T01:39:02.602235Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:02.602235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extended Derivative Dispersion Relations","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.J. Menon, R.F. Avila","submitted_at":"2006-01-24T11:13:16Z","abstract_excerpt":"It is shown that, for a wide class of functions with physical interest as forward scattering amplitudes, integral dispersion relations can be replaced by derivative forms without any high-energy approximation. The applicability of these extended derivative relations, in the investigation of forward proton-proton and antiproton-proton elastic scattering, is exemplified by means of a Pomeron-Reggeon model with totally nondegenerate trajectories."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0601194","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0601194","created_at":"2026-05-18T01:39:02.602360+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0601194v1","created_at":"2026-05-18T01:39:02.602360+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0601194","created_at":"2026-05-18T01:39:02.602360+00:00"},{"alias_kind":"pith_short_12","alias_value":"NTCOOKHDZAIH","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_16","alias_value":"NTCOOKHDZAIHKSVF","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_8","alias_value":"NTCOOKHD","created_at":"2026-05-18T12:25:54.717736+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ","json":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ.json","graph_json":"https://pith.science/api/pith-number/NTCOOKHDZAIHKSVFPLPYG5AHNQ/graph.json","events_json":"https://pith.science/api/pith-number/NTCOOKHDZAIHKSVFPLPYG5AHNQ/events.json","paper":"https://pith.science/paper/NTCOOKHD"},"agent_actions":{"view_html":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ","download_json":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ.json","view_paper":"https://pith.science/paper/NTCOOKHD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0601194&json=true","fetch_graph":"https://pith.science/api/pith-number/NTCOOKHDZAIHKSVFPLPYG5AHNQ/graph.json","fetch_events":"https://pith.science/api/pith-number/NTCOOKHDZAIHKSVFPLPYG5AHNQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ/action/storage_attestation","attest_author":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ/action/author_attestation","sign_citation":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ/action/citation_signature","submit_replication":"https://pith.science/pith/NTCOOKHDZAIHKSVFPLPYG5AHNQ/action/replication_record"}},"created_at":"2026-05-18T01:39:02.602360+00:00","updated_at":"2026-05-18T01:39:02.602360+00:00"}