{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:JPDBAVPONWWGH4EQTZFVE5DIZV","short_pith_number":"pith:JPDBAVPO","schema_version":"1.0","canonical_sha256":"4bc61055ee6dac63f0909e4b527468cd4e3c3ddf32729968bd9281c58eb96330","source":{"kind":"arxiv","id":"2211.06211","version":2},"attestation_state":"computed","paper":{"title":"$K_0^\\ast(1430)$ Twist-2 Distribution Amplitude and $B_s,D_s \\to K_0^\\ast(1430)$ Transition Form Factors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dong Huang, Hai-Bing Fu, Hong Tong, Tao Zhong, Xing-Gang Wu, Zai-Hui Wu","submitted_at":"2022-11-11T14:04:00Z","abstract_excerpt":"Based on the scenario that the $K_0^\\ast(1430)$ is viewed as the ground state of $s\\bar{q}$ or $q\\bar{s}$, we study the $K_0^\\ast(1430)$ leading-twist distribution amplitude (DA) $\\phi_{2;K_0^\\ast}(x,\\mu)$ with the QCD sum rules in the framework of background field theory. A more reasonable sum rule formula for $\\xi$-moments $\\langle\\xi^n\\rangle_{2;K_0^\\ast}$ is suggested, which eliminates the influence brought by the fact that the sum rule of $\\langle\\xi^0_p\\rangle_{3;K_0^\\ast}$ cannot be normalized in whole Borel region. More accurate values of the first ten $\\xi$-moments, $\\langle\\xi^n\\rang"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2211.06211","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-11-11T14:04:00Z","cross_cats_sorted":[],"title_canon_sha256":"6dcd1118ef3021c058183e1a2f66acddc0eb86ba67c63628daa8d9488c9eca53","abstract_canon_sha256":"4eb3fc661f66e8394721f8954a5811ab09b52099afc9cc2d8a67928c37810218"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:36:24.741269Z","signature_b64":"CM2pcpgiuIa66FExOZerCnFwAi6fiveu5CQyeZbdPXLr6xvL8+AdDuzX0EzsPAp7OG2X7X/K+lK7MLOCa9m1CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4bc61055ee6dac63f0909e4b527468cd4e3c3ddf32729968bd9281c58eb96330","last_reissued_at":"2026-07-05T06:36:24.740776Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:36:24.740776Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$K_0^\\ast(1430)$ Twist-2 Distribution Amplitude and $B_s,D_s \\to K_0^\\ast(1430)$ Transition Form Factors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dong Huang, Hai-Bing Fu, Hong Tong, Tao Zhong, Xing-Gang Wu, Zai-Hui Wu","submitted_at":"2022-11-11T14:04:00Z","abstract_excerpt":"Based on the scenario that the $K_0^\\ast(1430)$ is viewed as the ground state of $s\\bar{q}$ or $q\\bar{s}$, we study the $K_0^\\ast(1430)$ leading-twist distribution amplitude (DA) $\\phi_{2;K_0^\\ast}(x,\\mu)$ with the QCD sum rules in the framework of background field theory. A more reasonable sum rule formula for $\\xi$-moments $\\langle\\xi^n\\rangle_{2;K_0^\\ast}$ is suggested, which eliminates the influence brought by the fact that the sum rule of $\\langle\\xi^0_p\\rangle_{3;K_0^\\ast}$ cannot be normalized in whole Borel region. More accurate values of the first ten $\\xi$-moments, $\\langle\\xi^n\\rang"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.06211","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/2211.06211/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":"2211.06211","created_at":"2026-07-05T06:36:24.740834+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.06211v2","created_at":"2026-07-05T06:36:24.740834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.06211","created_at":"2026-07-05T06:36:24.740834+00:00"},{"alias_kind":"pith_short_12","alias_value":"JPDBAVPONWWG","created_at":"2026-07-05T06:36:24.740834+00:00"},{"alias_kind":"pith_short_16","alias_value":"JPDBAVPONWWGH4EQ","created_at":"2026-07-05T06:36:24.740834+00:00"},{"alias_kind":"pith_short_8","alias_value":"JPDBAVPO","created_at":"2026-07-05T06:36:24.740834+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2511.14165","citing_title":"Systematic analysis of $D_{(s)}$ meson semi-leptonic decays in the covariant light-front quark model","ref_index":64,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV","json":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV.json","graph_json":"https://pith.science/api/pith-number/JPDBAVPONWWGH4EQTZFVE5DIZV/graph.json","events_json":"https://pith.science/api/pith-number/JPDBAVPONWWGH4EQTZFVE5DIZV/events.json","paper":"https://pith.science/paper/JPDBAVPO"},"agent_actions":{"view_html":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV","download_json":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV.json","view_paper":"https://pith.science/paper/JPDBAVPO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.06211&json=true","fetch_graph":"https://pith.science/api/pith-number/JPDBAVPONWWGH4EQTZFVE5DIZV/graph.json","fetch_events":"https://pith.science/api/pith-number/JPDBAVPONWWGH4EQTZFVE5DIZV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV/action/storage_attestation","attest_author":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV/action/author_attestation","sign_citation":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV/action/citation_signature","submit_replication":"https://pith.science/pith/JPDBAVPONWWGH4EQTZFVE5DIZV/action/replication_record"}},"created_at":"2026-07-05T06:36:24.740834+00:00","updated_at":"2026-07-05T06:36:24.740834+00:00"}