{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:TOM2LMMDITEIGQY6JR5PNJ347F","short_pith_number":"pith:TOM2LMMD","schema_version":"1.0","canonical_sha256":"9b99a5b18344c883431e4c7af6a77cf95571d29c83abbc11aa5c30cb29e05291","source":{"kind":"arxiv","id":"1911.02845","version":2},"attestation_state":"computed","paper":{"title":"Form factor $\\pi^0 \\gamma^* \\gamma$ in lightcone sum rules combined with renormalization-group summation vs experimental data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. V. Pimikov, C. Ayala, N. G. Stefanis, S. V. Mikhailov","submitted_at":"2019-11-07T10:56:56Z","abstract_excerpt":"We consider the lightcone sum-rule (LCSR) description of the pion-photon transition form factor in combination with the renormalization group of QCD. The emerging scheme represents a certain version of Fractional Analytic Perturbation Theory and significantly extends the applicability domain of perturbation theory towards lower momenta $Q^2\\lesssim 1$ GeV$^2$. We show that the predictions calculated herewith agree very well with the released preliminary data of the BESIII experiment, which have very small errors just in this region, while the agreement with other data at higher $Q^2$ is compat"},"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":"1911.02845","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-11-07T10:56:56Z","cross_cats_sorted":[],"title_canon_sha256":"56a7200b46ebb117068eb1b685e914c4ba07bc0815fab6ee82fa0479890ddb32","abstract_canon_sha256":"c509ea75fa36220a1c0baf0366cba9976701f3d06dd28d1e89f6c9d958f533d2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:20:44.674899Z","signature_b64":"si5iSM1u8nWwqVGGlCOnB6kPbAFdlV/Slmg5tcl35EH+mr2GDlCW2DRgWidks+IJKMhzfpgqWMjKFlvCsakcBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b99a5b18344c883431e4c7af6a77cf95571d29c83abbc11aa5c30cb29e05291","last_reissued_at":"2026-07-05T00:20:44.674552Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:20:44.674552Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Form factor $\\pi^0 \\gamma^* \\gamma$ in lightcone sum rules combined with renormalization-group summation vs experimental data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. V. Pimikov, C. Ayala, N. G. Stefanis, S. V. Mikhailov","submitted_at":"2019-11-07T10:56:56Z","abstract_excerpt":"We consider the lightcone sum-rule (LCSR) description of the pion-photon transition form factor in combination with the renormalization group of QCD. The emerging scheme represents a certain version of Fractional Analytic Perturbation Theory and significantly extends the applicability domain of perturbation theory towards lower momenta $Q^2\\lesssim 1$ GeV$^2$. We show that the predictions calculated herewith agree very well with the released preliminary data of the BESIII experiment, which have very small errors just in this region, while the agreement with other data at higher $Q^2$ is compat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.02845","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1911.02845/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1911.02845","created_at":"2026-07-05T00:20:44.674601+00:00"},{"alias_kind":"arxiv_version","alias_value":"1911.02845v2","created_at":"2026-07-05T00:20:44.674601+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.02845","created_at":"2026-07-05T00:20:44.674601+00:00"},{"alias_kind":"pith_short_12","alias_value":"TOM2LMMDITEI","created_at":"2026-07-05T00:20:44.674601+00:00"},{"alias_kind":"pith_short_16","alias_value":"TOM2LMMDITEIGQY6","created_at":"2026-07-05T00:20:44.674601+00:00"},{"alias_kind":"pith_short_8","alias_value":"TOM2LMMD","created_at":"2026-07-05T00:20:44.674601+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/TOM2LMMDITEIGQY6JR5PNJ347F","json":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F.json","graph_json":"https://pith.science/api/pith-number/TOM2LMMDITEIGQY6JR5PNJ347F/graph.json","events_json":"https://pith.science/api/pith-number/TOM2LMMDITEIGQY6JR5PNJ347F/events.json","paper":"https://pith.science/paper/TOM2LMMD"},"agent_actions":{"view_html":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F","download_json":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F.json","view_paper":"https://pith.science/paper/TOM2LMMD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1911.02845&json=true","fetch_graph":"https://pith.science/api/pith-number/TOM2LMMDITEIGQY6JR5PNJ347F/graph.json","fetch_events":"https://pith.science/api/pith-number/TOM2LMMDITEIGQY6JR5PNJ347F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F/action/storage_attestation","attest_author":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F/action/author_attestation","sign_citation":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F/action/citation_signature","submit_replication":"https://pith.science/pith/TOM2LMMDITEIGQY6JR5PNJ347F/action/replication_record"}},"created_at":"2026-07-05T00:20:44.674601+00:00","updated_at":"2026-07-05T00:20:44.674601+00:00"}