{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:RTTLSN6PWLTGOS5SOKELKX4BW6","short_pith_number":"pith:RTTLSN6P","schema_version":"1.0","canonical_sha256":"8ce6b937cfb2e6674bb27288b55f81b78e0df382b80778599af1de0286551aea","source":{"kind":"arxiv","id":"1409.3053","version":2},"attestation_state":"computed","paper":{"title":"The $\\rho$-meson longitudinal leading-twist distribution amplitude","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hai-Bing Fu, Huan-Yu Bi, Hua-Yong Han, Xing-Gang Wu, Yang Ma","submitted_at":"2014-09-10T13:06:58Z","abstract_excerpt":"In the present paper, we suggest a convenient model for the vector $\\rho$-meson longitudinal leading-twist distribution amplitude $\\phi_{2;\\rho}^\\|$, whose distribution is controlled by a single parameter $B^\\|_{2;\\rho}$. By choosing proper chiral current in the correlator, we obtain new light-cone sum rules (LCSR) for the $B\\to\\rho$ TFFs $A_1$, $A_2$ and $V$, in which the $\\delta^1$-order $\\phi_{2;\\rho}^\\|$ provides dominant contributions. Then we make a detailed discussion on the $\\phi_{2;\\rho}^\\|$ properties via those $B\\to\\rho$ TFFs. A proper choice of $B^\\|_{2;\\rho}$ can make all the TFFs"},"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":"1409.3053","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-10T13:06:58Z","cross_cats_sorted":[],"title_canon_sha256":"4124e95824b7866112269b75054ece097843f848dcaf361c8614485088bc8840","abstract_canon_sha256":"e99c71654416d9ac6b498f63608d099c18662ba188f9827429a2421ab62f916d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:03.238893Z","signature_b64":"26GkshwoIBEXzd5gAaUvkap0Om2DW8ML6fDVmmY/V1Tixrh0l4E6lSVTLbqG88M26/4ZSiML4AemWPyLJppyAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8ce6b937cfb2e6674bb27288b55f81b78e0df382b80778599af1de0286551aea","last_reissued_at":"2026-05-18T02:41:03.238434Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:03.238434Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The $\\rho$-meson longitudinal leading-twist distribution amplitude","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hai-Bing Fu, Huan-Yu Bi, Hua-Yong Han, Xing-Gang Wu, Yang Ma","submitted_at":"2014-09-10T13:06:58Z","abstract_excerpt":"In the present paper, we suggest a convenient model for the vector $\\rho$-meson longitudinal leading-twist distribution amplitude $\\phi_{2;\\rho}^\\|$, whose distribution is controlled by a single parameter $B^\\|_{2;\\rho}$. By choosing proper chiral current in the correlator, we obtain new light-cone sum rules (LCSR) for the $B\\to\\rho$ TFFs $A_1$, $A_2$ and $V$, in which the $\\delta^1$-order $\\phi_{2;\\rho}^\\|$ provides dominant contributions. Then we make a detailed discussion on the $\\phi_{2;\\rho}^\\|$ properties via those $B\\to\\rho$ TFFs. A proper choice of $B^\\|_{2;\\rho}$ can make all the TFFs"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.3053","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":"1409.3053","created_at":"2026-05-18T02:41:03.238503+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.3053v2","created_at":"2026-05-18T02:41:03.238503+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.3053","created_at":"2026-05-18T02:41:03.238503+00:00"},{"alias_kind":"pith_short_12","alias_value":"RTTLSN6PWLTG","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"RTTLSN6PWLTGOS5S","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"RTTLSN6P","created_at":"2026-05-18T12:28:46.137349+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/RTTLSN6PWLTGOS5SOKELKX4BW6","json":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6.json","graph_json":"https://pith.science/api/pith-number/RTTLSN6PWLTGOS5SOKELKX4BW6/graph.json","events_json":"https://pith.science/api/pith-number/RTTLSN6PWLTGOS5SOKELKX4BW6/events.json","paper":"https://pith.science/paper/RTTLSN6P"},"agent_actions":{"view_html":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6","download_json":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6.json","view_paper":"https://pith.science/paper/RTTLSN6P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.3053&json=true","fetch_graph":"https://pith.science/api/pith-number/RTTLSN6PWLTGOS5SOKELKX4BW6/graph.json","fetch_events":"https://pith.science/api/pith-number/RTTLSN6PWLTGOS5SOKELKX4BW6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6/action/storage_attestation","attest_author":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6/action/author_attestation","sign_citation":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6/action/citation_signature","submit_replication":"https://pith.science/pith/RTTLSN6PWLTGOS5SOKELKX4BW6/action/replication_record"}},"created_at":"2026-05-18T02:41:03.238503+00:00","updated_at":"2026-05-18T02:41:03.238503+00:00"}