{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:YQ6KFDJBC3JGZQ2VXDEDXNPK4H","short_pith_number":"pith:YQ6KFDJB","schema_version":"1.0","canonical_sha256":"c43ca28d2116d26cc355b8c83bb5eae1ed6db41175184f13e50fa43fdbfabf22","source":{"kind":"arxiv","id":"1905.03259","version":2},"attestation_state":"computed","paper":{"title":"Revisiting the production of ALPs at B-factories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. Pobbe, L. Merlo, O. Sumensari, S. Rigolin","submitted_at":"2019-05-08T18:00:02Z","abstract_excerpt":"In this paper, the production of Axion-Like Particles (ALPs) at $B$-factories via the process $e^+e^- \\to \\gamma a$ is revisited. To this purpose, the relevant cross-section is computed via an effective Lagrangian with simultaneous ALP couplings to $b$-quarks and photons. The interplay between resonant and non-resonant contributions is shown to be relevant for experiments operating at $\\sqrt{s}=m_{\\Upsilon(nS)}$, with $n=1,2,3$, while the non-resonant one dominates at $\\Upsilon(4S)$. These effects imply that the experimental searches performed at different quarkonia resonances are sensitive to"},"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":"1905.03259","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-05-08T18:00:02Z","cross_cats_sorted":[],"title_canon_sha256":"3c92cba586894c0a7e2b67f76d40ac13340306edff6ce54181d64cb765031225","abstract_canon_sha256":"0bc81f72b0372a6f89eebe6fcf021eef7507b3a1f338ec6bf8d5291766d8c154"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:15.099114Z","signature_b64":"oU+AWrB4El2es/Yum1mkMFOruxtkk4+Qi2k6TWFXttnDURsvPLv3m1Xdhs4n+h5ZI9VsaOqqwklRl/Ws8foMBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c43ca28d2116d26cc355b8c83bb5eae1ed6db41175184f13e50fa43fdbfabf22","last_reissued_at":"2026-05-17T23:42:15.098446Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:15.098446Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revisiting the production of ALPs at B-factories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. Pobbe, L. Merlo, O. Sumensari, S. Rigolin","submitted_at":"2019-05-08T18:00:02Z","abstract_excerpt":"In this paper, the production of Axion-Like Particles (ALPs) at $B$-factories via the process $e^+e^- \\to \\gamma a$ is revisited. To this purpose, the relevant cross-section is computed via an effective Lagrangian with simultaneous ALP couplings to $b$-quarks and photons. The interplay between resonant and non-resonant contributions is shown to be relevant for experiments operating at $\\sqrt{s}=m_{\\Upsilon(nS)}$, with $n=1,2,3$, while the non-resonant one dominates at $\\Upsilon(4S)$. These effects imply that the experimental searches performed at different quarkonia resonances are sensitive to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.03259","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":"1905.03259","created_at":"2026-05-17T23:42:15.098548+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.03259v2","created_at":"2026-05-17T23:42:15.098548+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.03259","created_at":"2026-05-17T23:42:15.098548+00:00"},{"alias_kind":"pith_short_12","alias_value":"YQ6KFDJBC3JG","created_at":"2026-05-18T12:33:33.725879+00:00"},{"alias_kind":"pith_short_16","alias_value":"YQ6KFDJBC3JGZQ2V","created_at":"2026-05-18T12:33:33.725879+00:00"},{"alias_kind":"pith_short_8","alias_value":"YQ6KFDJB","created_at":"2026-05-18T12:33:33.725879+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.12298","citing_title":"The KSVZ Atlas: A Unified SMEFT-ALP Framework","ref_index":86,"is_internal_anchor":true},{"citing_arxiv_id":"2511.03786","citing_title":"Light new physics and the $\\tau$ lepton dipole moments","ref_index":173,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H","json":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H.json","graph_json":"https://pith.science/api/pith-number/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/graph.json","events_json":"https://pith.science/api/pith-number/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/events.json","paper":"https://pith.science/paper/YQ6KFDJB"},"agent_actions":{"view_html":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H","download_json":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H.json","view_paper":"https://pith.science/paper/YQ6KFDJB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.03259&json=true","fetch_graph":"https://pith.science/api/pith-number/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/graph.json","fetch_events":"https://pith.science/api/pith-number/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/action/storage_attestation","attest_author":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/action/author_attestation","sign_citation":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/action/citation_signature","submit_replication":"https://pith.science/pith/YQ6KFDJBC3JGZQ2VXDEDXNPK4H/action/replication_record"}},"created_at":"2026-05-17T23:42:15.098548+00:00","updated_at":"2026-05-17T23:42:15.098548+00:00"}