{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:CDO5HLBHCW6BDPKSRBGLMEG3MY","short_pith_number":"pith:CDO5HLBH","schema_version":"1.0","canonical_sha256":"10ddd3ac2715bc11bd52884cb610db66371e32a6448c2e33522e9c687096b169","source":{"kind":"arxiv","id":"1705.01504","version":3},"attestation_state":"computed","paper":{"title":"Leading components in forward elastic hadron scattering: Derivative dispersion relations and asymptotic uniqueness","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"D.A. Fagundes, M.J. Menon, P.V.R.G. Silva","submitted_at":"2017-05-03T16:42:45Z","abstract_excerpt":"Forward amplitude analyses constitute an important approach in the investigation of the energy dependence of the total hadronic cross-section $\\sigma_{tot}$ and the $\\rho$ parameter. The standard picture indicates for $\\sigma_{tot}$ a leading log-squared dependence at the highest c.m. energies, in accordance with the Froissart-Lukaszuk-Martin bound. Beyond this log-squared (L2) leading dependence, other amplitude analyses have considered a log-raised-to-gamma form (L$\\gamma$), with $\\gamma$ as a real free fit parameter. In this case, analytic connections with $\\rho$ can be obtained either thro"},"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":"1705.01504","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-03T16:42:45Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"96a5049f1092e1aee39304b9483549fecbd26b1b35f21eca535d00df7ee08622","abstract_canon_sha256":"00443fc0a70869d7cedcfb75af75e451bc5cc4f6857a7f5cebe3442420afcd91"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:45.002694Z","signature_b64":"bcU+t71c3U+nTN33u/Cbhc4VjTa7imB/Yy8Ush5LzqbuUxw7nJdZ3TRlmUadDEysSJzYx73835nuOVxIppazBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"10ddd3ac2715bc11bd52884cb610db66371e32a6448c2e33522e9c687096b169","last_reissued_at":"2026-05-18T00:30:45.002163Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:45.002163Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Leading components in forward elastic hadron scattering: Derivative dispersion relations and asymptotic uniqueness","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"D.A. Fagundes, M.J. Menon, P.V.R.G. Silva","submitted_at":"2017-05-03T16:42:45Z","abstract_excerpt":"Forward amplitude analyses constitute an important approach in the investigation of the energy dependence of the total hadronic cross-section $\\sigma_{tot}$ and the $\\rho$ parameter. The standard picture indicates for $\\sigma_{tot}$ a leading log-squared dependence at the highest c.m. energies, in accordance with the Froissart-Lukaszuk-Martin bound. Beyond this log-squared (L2) leading dependence, other amplitude analyses have considered a log-raised-to-gamma form (L$\\gamma$), with $\\gamma$ as a real free fit parameter. In this case, analytic connections with $\\rho$ can be obtained either thro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.01504","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1705.01504","created_at":"2026-05-18T00:30:45.002252+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.01504v3","created_at":"2026-05-18T00:30:45.002252+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.01504","created_at":"2026-05-18T00:30:45.002252+00:00"},{"alias_kind":"pith_short_12","alias_value":"CDO5HLBHCW6B","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_16","alias_value":"CDO5HLBHCW6BDPKS","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_8","alias_value":"CDO5HLBH","created_at":"2026-05-18T12:31:10.602751+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/CDO5HLBHCW6BDPKSRBGLMEG3MY","json":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY.json","graph_json":"https://pith.science/api/pith-number/CDO5HLBHCW6BDPKSRBGLMEG3MY/graph.json","events_json":"https://pith.science/api/pith-number/CDO5HLBHCW6BDPKSRBGLMEG3MY/events.json","paper":"https://pith.science/paper/CDO5HLBH"},"agent_actions":{"view_html":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY","download_json":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY.json","view_paper":"https://pith.science/paper/CDO5HLBH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.01504&json=true","fetch_graph":"https://pith.science/api/pith-number/CDO5HLBHCW6BDPKSRBGLMEG3MY/graph.json","fetch_events":"https://pith.science/api/pith-number/CDO5HLBHCW6BDPKSRBGLMEG3MY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY/action/storage_attestation","attest_author":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY/action/author_attestation","sign_citation":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY/action/citation_signature","submit_replication":"https://pith.science/pith/CDO5HLBHCW6BDPKSRBGLMEG3MY/action/replication_record"}},"created_at":"2026-05-18T00:30:45.002252+00:00","updated_at":"2026-05-18T00:30:45.002252+00:00"}