{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:YZH5X4TBUEUUHZ7JN3PEOV7FBL","short_pith_number":"pith:YZH5X4TB","schema_version":"1.0","canonical_sha256":"c64fdbf261a12943e7e96ede4757e50ac7b84bf4a7270f9c1d22ab478293a6df","source":{"kind":"arxiv","id":"1701.04250","version":2},"attestation_state":"computed","paper":{"title":"The pseudoscalar meson electromagnetic form factor at high $Q^2$ from full lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. C. Zimermmane-Santos, A. T. Lytle, C. T. H. Davies, G. P. Lepage, J. Koponen","submitted_at":"2017-01-16T11:33:38Z","abstract_excerpt":"We give an accurate determination of the vector (electromagnetic) form factor, $F(Q^2)$, for a light pseudoscalar meson up to squared momentum transfer $Q^2$ values of 6 $\\mathrm{GeV}^2$ for the first time from full lattice QCD, including $u$, $d$, $s$ and $c$ quarks in the sea at multiple values of the lattice spacing. Our results show good control of lattice discretisation and sea quark mass effects. We study a pseudoscalar meson made of valence $s$ quarks but the qualitative picture obtained applies also to the $\\pi$ meson, relevant to upcoming experiments at Jefferson Lab. We find that $Q^"},"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":"1701.04250","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-01-16T11:33:38Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3acdd6a75532a46c58f25720c4e8a2fd79ee7cd483745e76a35baa664f78e529","abstract_canon_sha256":"3db15066fbf30f823115c5c1a073555e1ce368e969f0d9d39f478646480e00bf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:23.960468Z","signature_b64":"XCs3SFY8twj0a+uLNFwtGllo1CaRTtnyquyN06JIKDbHXpjXyQzwBpufx14II1Eq98EbI7la9LQBL+WV/hgQDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c64fdbf261a12943e7e96ede4757e50ac7b84bf4a7270f9c1d22ab478293a6df","last_reissued_at":"2026-05-18T00:35:23.960011Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:23.960011Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The pseudoscalar meson electromagnetic form factor at high $Q^2$ from full lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. C. Zimermmane-Santos, A. T. Lytle, C. T. H. Davies, G. P. Lepage, J. Koponen","submitted_at":"2017-01-16T11:33:38Z","abstract_excerpt":"We give an accurate determination of the vector (electromagnetic) form factor, $F(Q^2)$, for a light pseudoscalar meson up to squared momentum transfer $Q^2$ values of 6 $\\mathrm{GeV}^2$ for the first time from full lattice QCD, including $u$, $d$, $s$ and $c$ quarks in the sea at multiple values of the lattice spacing. Our results show good control of lattice discretisation and sea quark mass effects. We study a pseudoscalar meson made of valence $s$ quarks but the qualitative picture obtained applies also to the $\\pi$ meson, relevant to upcoming experiments at Jefferson Lab. We find that $Q^"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.04250","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":""},"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":"1701.04250","created_at":"2026-05-18T00:35:23.960074+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.04250v2","created_at":"2026-05-18T00:35:23.960074+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.04250","created_at":"2026-05-18T00:35:23.960074+00:00"},{"alias_kind":"pith_short_12","alias_value":"YZH5X4TBUEUU","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"YZH5X4TBUEUUHZ7J","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"YZH5X4TB","created_at":"2026-05-18T12:31:59.375834+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.06025","citing_title":"Mapping spatial distributions within pseudoscalar mesons","ref_index":95,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL","json":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL.json","graph_json":"https://pith.science/api/pith-number/YZH5X4TBUEUUHZ7JN3PEOV7FBL/graph.json","events_json":"https://pith.science/api/pith-number/YZH5X4TBUEUUHZ7JN3PEOV7FBL/events.json","paper":"https://pith.science/paper/YZH5X4TB"},"agent_actions":{"view_html":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL","download_json":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL.json","view_paper":"https://pith.science/paper/YZH5X4TB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.04250&json=true","fetch_graph":"https://pith.science/api/pith-number/YZH5X4TBUEUUHZ7JN3PEOV7FBL/graph.json","fetch_events":"https://pith.science/api/pith-number/YZH5X4TBUEUUHZ7JN3PEOV7FBL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL/action/storage_attestation","attest_author":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL/action/author_attestation","sign_citation":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL/action/citation_signature","submit_replication":"https://pith.science/pith/YZH5X4TBUEUUHZ7JN3PEOV7FBL/action/replication_record"}},"created_at":"2026-05-18T00:35:23.960074+00:00","updated_at":"2026-05-18T00:35:23.960074+00:00"}