{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:SGKISKTAJLU5EDPY7ATJ62I5XT","short_pith_number":"pith:SGKISKTA","schema_version":"1.0","canonical_sha256":"9194892a604ae9d20df8f8269f691dbcc15f362ff7d16cfa9c89b06e47b8faf8","source":{"kind":"arxiv","id":"0903.1994","version":1},"attestation_state":"computed","paper":{"title":"Pion Form Factor in the NLC QCD SR approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.P. Bakulev, A.V. Pimikov, N.G. Stefanis","submitted_at":"2009-03-11T15:28:30Z","abstract_excerpt":"We present results of a calculation of the electromagnetic pion form factor within a framework of QCD Sum Rules with nonlocal condensates and using a perturbative spectral density which includes \\mathcal{O}(\\alpha_s) contributions."},"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":"0903.1994","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-11T15:28:30Z","cross_cats_sorted":[],"title_canon_sha256":"6419eb93614f053a4ef023de42d52832dd333ea8ad5c7f257b57f47711ccad1e","abstract_canon_sha256":"9bdb4185d0b381a9f3d0f6ffbc68c5a6946a3f448ddc3dee9a5de9035f01c473"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:00.490787Z","signature_b64":"F9D/vuTVVpt9VKYbEshllo6gL8JOukGNk6t3ZMW7DM7/MOA8CxG/aqCf83lyzf1Z02d8/7z2sKgpushma6SPDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9194892a604ae9d20df8f8269f691dbcc15f362ff7d16cfa9c89b06e47b8faf8","last_reissued_at":"2026-05-18T02:35:00.490380Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:00.490380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pion Form Factor in the NLC QCD SR approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.P. Bakulev, A.V. Pimikov, N.G. Stefanis","submitted_at":"2009-03-11T15:28:30Z","abstract_excerpt":"We present results of a calculation of the electromagnetic pion form factor within a framework of QCD Sum Rules with nonlocal condensates and using a perturbative spectral density which includes \\mathcal{O}(\\alpha_s) contributions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.1994","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":"0903.1994","created_at":"2026-05-18T02:35:00.490445+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.1994v1","created_at":"2026-05-18T02:35:00.490445+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.1994","created_at":"2026-05-18T02:35:00.490445+00:00"},{"alias_kind":"pith_short_12","alias_value":"SGKISKTAJLU5","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"SGKISKTAJLU5EDPY","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"SGKISKTA","created_at":"2026-05-18T12:26:01.383474+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/SGKISKTAJLU5EDPY7ATJ62I5XT","json":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT.json","graph_json":"https://pith.science/api/pith-number/SGKISKTAJLU5EDPY7ATJ62I5XT/graph.json","events_json":"https://pith.science/api/pith-number/SGKISKTAJLU5EDPY7ATJ62I5XT/events.json","paper":"https://pith.science/paper/SGKISKTA"},"agent_actions":{"view_html":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT","download_json":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT.json","view_paper":"https://pith.science/paper/SGKISKTA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.1994&json=true","fetch_graph":"https://pith.science/api/pith-number/SGKISKTAJLU5EDPY7ATJ62I5XT/graph.json","fetch_events":"https://pith.science/api/pith-number/SGKISKTAJLU5EDPY7ATJ62I5XT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT/action/storage_attestation","attest_author":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT/action/author_attestation","sign_citation":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT/action/citation_signature","submit_replication":"https://pith.science/pith/SGKISKTAJLU5EDPY7ATJ62I5XT/action/replication_record"}},"created_at":"2026-05-18T02:35:00.490445+00:00","updated_at":"2026-05-18T02:35:00.490445+00:00"}