{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:DEMTUIMUCEUBA3KQ35OFFFK6VQ","short_pith_number":"pith:DEMTUIMU","schema_version":"1.0","canonical_sha256":"19193a21941128106d50df5c52955eac1f2b4572f3d3ff1e36fa7bdaec9f4ddb","source":{"kind":"arxiv","id":"1012.2733","version":2},"attestation_state":"computed","paper":{"title":"Pion mass dependence of the $K_{l3}$ semileptonic scalar form factor within finite volume","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Abolfazl Mirjalili, Karim Ghorbani, Mohammad.M. Yazdanpanah","submitted_at":"2010-12-13T14:21:40Z","abstract_excerpt":"We calculate the scalar semileptonic kaon decay in finite volume at the momentum transfer $t_{m} = (m_{K} - m_{\\pi})^2$, using chiral perturbation theory. At first we obtain the hadronic matrix element to be calculated in finite volume. We then evaluate the finite size effects for two volumes with $L = 1.83 fm$ and $L= 2.73 fm$ and find that the difference between the finite volume corrections of the two volumes are larger than the difference as quoted in \\cite{Boyle2007a}. It appears then that the pion masses used for the scalar form factor in ChPT are large which result in large finite volum"},"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":"1012.2733","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-12-13T14:21:40Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"6b16b638d90bc0c836f117ceaf76b083c80a13e6403d3b028783303deefb573e","abstract_canon_sha256":"c64aa59281acbf6142c0cf14bce0815977c23c92e97df6ef6eb467bfb16f9253"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:27.609331Z","signature_b64":"WyXl5vZ5YuXbB0sweCg0UDQtA4Dqhy8/IbsKu5IXa6u+LEHtCP1l4LBBxcEuvoKiL8OKiALsu5t96ENgQlTiBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"19193a21941128106d50df5c52955eac1f2b4572f3d3ff1e36fa7bdaec9f4ddb","last_reissued_at":"2026-05-18T02:04:27.608645Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:27.608645Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pion mass dependence of the $K_{l3}$ semileptonic scalar form factor within finite volume","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Abolfazl Mirjalili, Karim Ghorbani, Mohammad.M. Yazdanpanah","submitted_at":"2010-12-13T14:21:40Z","abstract_excerpt":"We calculate the scalar semileptonic kaon decay in finite volume at the momentum transfer $t_{m} = (m_{K} - m_{\\pi})^2$, using chiral perturbation theory. At first we obtain the hadronic matrix element to be calculated in finite volume. We then evaluate the finite size effects for two volumes with $L = 1.83 fm$ and $L= 2.73 fm$ and find that the difference between the finite volume corrections of the two volumes are larger than the difference as quoted in \\cite{Boyle2007a}. It appears then that the pion masses used for the scalar form factor in ChPT are large which result in large finite volum"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.2733","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":"1012.2733","created_at":"2026-05-18T02:04:27.608755+00:00"},{"alias_kind":"arxiv_version","alias_value":"1012.2733v2","created_at":"2026-05-18T02:04:27.608755+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.2733","created_at":"2026-05-18T02:04:27.608755+00:00"},{"alias_kind":"pith_short_12","alias_value":"DEMTUIMUCEUB","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"DEMTUIMUCEUBA3KQ","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"DEMTUIMU","created_at":"2026-05-18T12:26:06.534383+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/DEMTUIMUCEUBA3KQ35OFFFK6VQ","json":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ.json","graph_json":"https://pith.science/api/pith-number/DEMTUIMUCEUBA3KQ35OFFFK6VQ/graph.json","events_json":"https://pith.science/api/pith-number/DEMTUIMUCEUBA3KQ35OFFFK6VQ/events.json","paper":"https://pith.science/paper/DEMTUIMU"},"agent_actions":{"view_html":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ","download_json":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ.json","view_paper":"https://pith.science/paper/DEMTUIMU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1012.2733&json=true","fetch_graph":"https://pith.science/api/pith-number/DEMTUIMUCEUBA3KQ35OFFFK6VQ/graph.json","fetch_events":"https://pith.science/api/pith-number/DEMTUIMUCEUBA3KQ35OFFFK6VQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ/action/storage_attestation","attest_author":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ/action/author_attestation","sign_citation":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ/action/citation_signature","submit_replication":"https://pith.science/pith/DEMTUIMUCEUBA3KQ35OFFFK6VQ/action/replication_record"}},"created_at":"2026-05-18T02:04:27.608755+00:00","updated_at":"2026-05-18T02:04:27.608755+00:00"}