{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:UYJHLR632DZNHSP67RRIO66EHP","short_pith_number":"pith:UYJHLR63","schema_version":"1.0","canonical_sha256":"a61275c7dbd0f2d3c9fefc62877bc43bff3f2d17f30f12ffaa62a621843a42ba","source":{"kind":"arxiv","id":"hep-ph/9604217","version":1},"attestation_state":"computed","paper":{"title":"Scattering Lengths and Medium and High Energy $\\pi\\pi$ Scattering","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Ananthanarayan, P. B\\\"uttiker","submitted_at":"1996-04-02T13:36:31Z","abstract_excerpt":"Medium and high energy absorptive parts contribute to dispersive expressions for D- wave scattering lengths, $a^0_2$ and $a^2_2$. For the model employed by Basdevant, Frogatt and Peterson we find the D- wave driving term contributions to the D- wave scattering lengths are $1.8\\cdot 10^{-4}$ to $a^0_2$ and $0.4\\cdot 10^{-4}$ to $a^2_2$, roughly $10\\%$ and $30\\%$ of their respective\n central experimental values. Inequivalent sets of sum rules are used as a compelling test of the consistency of the model for which crossing symmetry is not guaranteed. Results for the F- wave scattering length $a^1"},"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/9604217","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-04-02T13:36:31Z","cross_cats_sorted":[],"title_canon_sha256":"9427defd622954a117711f375c6733f71d81e3fe75e50acf7aaa7f925152305b","abstract_canon_sha256":"303d113ec5e00bcd62d731d3a6821b2ea4ee7ae304fd4faa3dcb2899e6b7aac6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:29.705723Z","signature_b64":"k6lQndNR6aAVvmCo3QBhlb8P3naDgVptL6jbtxSEG1oFXCOVCnp+/yMyzDzieViKPNZxwilG1kmAtNrb76R8Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a61275c7dbd0f2d3c9fefc62877bc43bff3f2d17f30f12ffaa62a621843a42ba","last_reissued_at":"2026-05-18T01:06:29.705101Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:29.705101Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scattering Lengths and Medium and High Energy $\\pi\\pi$ Scattering","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Ananthanarayan, P. B\\\"uttiker","submitted_at":"1996-04-02T13:36:31Z","abstract_excerpt":"Medium and high energy absorptive parts contribute to dispersive expressions for D- wave scattering lengths, $a^0_2$ and $a^2_2$. For the model employed by Basdevant, Frogatt and Peterson we find the D- wave driving term contributions to the D- wave scattering lengths are $1.8\\cdot 10^{-4}$ to $a^0_2$ and $0.4\\cdot 10^{-4}$ to $a^2_2$, roughly $10\\%$ and $30\\%$ of their respective\n central experimental values. Inequivalent sets of sum rules are used as a compelling test of the consistency of the model for which crossing symmetry is not guaranteed. Results for the F- wave scattering length $a^1"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9604217","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/9604217","created_at":"2026-05-18T01:06:29.705197+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9604217v1","created_at":"2026-05-18T01:06:29.705197+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9604217","created_at":"2026-05-18T01:06:29.705197+00:00"},{"alias_kind":"pith_short_12","alias_value":"UYJHLR632DZN","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"UYJHLR632DZNHSP6","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"UYJHLR63","created_at":"2026-05-18T12:25:48.327863+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/UYJHLR632DZNHSP67RRIO66EHP","json":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP.json","graph_json":"https://pith.science/api/pith-number/UYJHLR632DZNHSP67RRIO66EHP/graph.json","events_json":"https://pith.science/api/pith-number/UYJHLR632DZNHSP67RRIO66EHP/events.json","paper":"https://pith.science/paper/UYJHLR63"},"agent_actions":{"view_html":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP","download_json":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP.json","view_paper":"https://pith.science/paper/UYJHLR63","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9604217&json=true","fetch_graph":"https://pith.science/api/pith-number/UYJHLR632DZNHSP67RRIO66EHP/graph.json","fetch_events":"https://pith.science/api/pith-number/UYJHLR632DZNHSP67RRIO66EHP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP/action/storage_attestation","attest_author":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP/action/author_attestation","sign_citation":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP/action/citation_signature","submit_replication":"https://pith.science/pith/UYJHLR632DZNHSP67RRIO66EHP/action/replication_record"}},"created_at":"2026-05-18T01:06:29.705197+00:00","updated_at":"2026-05-18T01:06:29.705197+00:00"}