{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:AJTRFS2KSWOXYJFLV64GMDQBH6","short_pith_number":"pith:AJTRFS2K","schema_version":"1.0","canonical_sha256":"026712cb4a959d7c24abafb8660e013f8633f154369a9f446c45aa2104b923bb","source":{"kind":"arxiv","id":"1109.3127","version":3},"attestation_state":"computed","paper":{"title":"Revisiting the Twist-3 Distribution Amplitudes of $K$ Meson within the QCD Background Field Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hai-Bing Fu, Hua-Yong Han, Qi-Li Liao, Tao Zhong, Xing-Gang Wu, Zhen-Yun Fang","submitted_at":"2011-09-14T16:28:21Z","abstract_excerpt":"In the present paper, we investigate the kaon twist-3 distribution amplitudes (DAs) $\\phi_{p,\\sigma}^K$ within the QCD background field approach. The $SU_f(3)$-breaking effects are studied in detail under a systematical way, especially the sum rules for the moments of $\\phi_{p,\\sigma}^K$ are obtained by keeping all the mass terms in the $s$-quark propagator consistently. After adding all the uncertainties in quadrature, the first two Gegenbauler moments of $\\phi_{p,\\sigma}^K$ are $a^1_{K,p}(1 {\\rm GeV}) = -0.376^{+0.103}_{-0.148}$, $a^2_{K,p}(1 {\\rm GeV}) = 0.701^{+0.481}_{-0.491}$, $a^1_{K,\\s"},"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":"1109.3127","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-09-14T16:28:21Z","cross_cats_sorted":[],"title_canon_sha256":"d0c5eabaaf2520113bfc2f718bd80c2d747c4eb8b1327591728ac9023ffff015","abstract_canon_sha256":"e909ae6fccf2e11a5b121f427816dc2ad9e46a62ab7b880eb21719990baea650"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:32.968091Z","signature_b64":"ums0qpRi8WiX+ofiJEELWVINIJgF+EqbBPR/NQ3PwpQM9UMTBcKsvS7Qd8FJUMfcBRTlra2fwhvjedkB0ev+AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"026712cb4a959d7c24abafb8660e013f8633f154369a9f446c45aa2104b923bb","last_reissued_at":"2026-05-18T02:00:32.967448Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:32.967448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revisiting the Twist-3 Distribution Amplitudes of $K$ Meson within the QCD Background Field Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hai-Bing Fu, Hua-Yong Han, Qi-Li Liao, Tao Zhong, Xing-Gang Wu, Zhen-Yun Fang","submitted_at":"2011-09-14T16:28:21Z","abstract_excerpt":"In the present paper, we investigate the kaon twist-3 distribution amplitudes (DAs) $\\phi_{p,\\sigma}^K$ within the QCD background field approach. The $SU_f(3)$-breaking effects are studied in detail under a systematical way, especially the sum rules for the moments of $\\phi_{p,\\sigma}^K$ are obtained by keeping all the mass terms in the $s$-quark propagator consistently. After adding all the uncertainties in quadrature, the first two Gegenbauler moments of $\\phi_{p,\\sigma}^K$ are $a^1_{K,p}(1 {\\rm GeV}) = -0.376^{+0.103}_{-0.148}$, $a^2_{K,p}(1 {\\rm GeV}) = 0.701^{+0.481}_{-0.491}$, $a^1_{K,\\s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.3127","kind":"arxiv","version":3},"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":"1109.3127","created_at":"2026-05-18T02:00:32.967554+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.3127v3","created_at":"2026-05-18T02:00:32.967554+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.3127","created_at":"2026-05-18T02:00:32.967554+00:00"},{"alias_kind":"pith_short_12","alias_value":"AJTRFS2KSWOX","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_16","alias_value":"AJTRFS2KSWOXYJFL","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_8","alias_value":"AJTRFS2K","created_at":"2026-05-18T12:26:24.575870+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/AJTRFS2KSWOXYJFLV64GMDQBH6","json":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6.json","graph_json":"https://pith.science/api/pith-number/AJTRFS2KSWOXYJFLV64GMDQBH6/graph.json","events_json":"https://pith.science/api/pith-number/AJTRFS2KSWOXYJFLV64GMDQBH6/events.json","paper":"https://pith.science/paper/AJTRFS2K"},"agent_actions":{"view_html":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6","download_json":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6.json","view_paper":"https://pith.science/paper/AJTRFS2K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.3127&json=true","fetch_graph":"https://pith.science/api/pith-number/AJTRFS2KSWOXYJFLV64GMDQBH6/graph.json","fetch_events":"https://pith.science/api/pith-number/AJTRFS2KSWOXYJFLV64GMDQBH6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6/action/storage_attestation","attest_author":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6/action/author_attestation","sign_citation":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6/action/citation_signature","submit_replication":"https://pith.science/pith/AJTRFS2KSWOXYJFLV64GMDQBH6/action/replication_record"}},"created_at":"2026-05-18T02:00:32.967554+00:00","updated_at":"2026-05-18T02:00:32.967554+00:00"}