{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:U3SVJSSICIB5VUR5T4PJDZAOY4","short_pith_number":"pith:U3SVJSSI","schema_version":"1.0","canonical_sha256":"a6e554ca481203dad23d9f1e91e40ec705c49521f0951b669fdc1955f5323fa6","source":{"kind":"arxiv","id":"hep-ph/0609302","version":1},"attestation_state":"computed","paper":{"title":"$e^+e^- \\to \\gamma X(3872)$ near the $D^* {\\bar D}^*$ threshold","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.B. Voloshin, S. Dubynskiy","submitted_at":"2006-09-28T19:36:54Z","abstract_excerpt":"We evaluate the cross section of the process $e^+e^- \\to \\gamma X(3872)$ in terms of the content of the $D^{*0} {\\bar D}^0$ `molecular' component in the wave function of the resonance X(3872). If this component is dominating, the cross section of the reaction $e^+e^- \\to \\gamma X(3872)$ can reach up to about $10^{-3}$ of that for $e^+e^- \\to D^* {\\bar D}^*$ at energy slightly above the $D^* {\\bar D}^*$ threshold, and the considered process can be a realistic source of the X(3872) particles for the studies of this resonance."},"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":"hep-ph/0609302","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-09-28T19:36:54Z","cross_cats_sorted":[],"title_canon_sha256":"99811512674964a86a345c7ed8ae8c72b0e9b249e37ff82e71ec6f68125f546b","abstract_canon_sha256":"7a43619132b8f6867a72998edd6a71d5b73a0c85ca0b4fe578d317c1371a70e2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:34.176469Z","signature_b64":"Mnv0ASyFxqVFPLq6K42QBABpLMYh5YmfVdNjpdn6oYcfohPx5u2CYc7ptG4zGJEex4TD3aa9dSa00pApc+QMAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a6e554ca481203dad23d9f1e91e40ec705c49521f0951b669fdc1955f5323fa6","last_reissued_at":"2026-07-04T15:22:34.175295Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:34.175295Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$e^+e^- \\to \\gamma X(3872)$ near the $D^* {\\bar D}^*$ threshold","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.B. Voloshin, S. Dubynskiy","submitted_at":"2006-09-28T19:36:54Z","abstract_excerpt":"We evaluate the cross section of the process $e^+e^- \\to \\gamma X(3872)$ in terms of the content of the $D^{*0} {\\bar D}^0$ `molecular' component in the wave function of the resonance X(3872). If this component is dominating, the cross section of the reaction $e^+e^- \\to \\gamma X(3872)$ can reach up to about $10^{-3}$ of that for $e^+e^- \\to D^* {\\bar D}^*$ at energy slightly above the $D^* {\\bar D}^*$ threshold, and the considered process can be a realistic source of the X(3872) particles for the studies of this resonance."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0609302","kind":"arxiv","version":1},"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/hep-ph/0609302/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":"hep-ph/0609302","created_at":"2026-07-04T15:22:34.176062+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0609302v1","created_at":"2026-07-04T15:22:34.176062+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0609302","created_at":"2026-07-04T15:22:34.176062+00:00"},{"alias_kind":"pith_short_12","alias_value":"U3SVJSSICIB5","created_at":"2026-07-04T15:22:34.176062+00:00"},{"alias_kind":"pith_short_16","alias_value":"U3SVJSSICIB5VUR5","created_at":"2026-07-04T15:22:34.176062+00:00"},{"alias_kind":"pith_short_8","alias_value":"U3SVJSSI","created_at":"2026-07-04T15:22:34.176062+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1909.03901","citing_title":"Production of $X(3872)$ and a Photon in $e^+e^-$ Annihilation","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4","json":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4.json","graph_json":"https://pith.science/api/pith-number/U3SVJSSICIB5VUR5T4PJDZAOY4/graph.json","events_json":"https://pith.science/api/pith-number/U3SVJSSICIB5VUR5T4PJDZAOY4/events.json","paper":"https://pith.science/paper/U3SVJSSI"},"agent_actions":{"view_html":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4","download_json":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4.json","view_paper":"https://pith.science/paper/U3SVJSSI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0609302&json=true","fetch_graph":"https://pith.science/api/pith-number/U3SVJSSICIB5VUR5T4PJDZAOY4/graph.json","fetch_events":"https://pith.science/api/pith-number/U3SVJSSICIB5VUR5T4PJDZAOY4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4/action/storage_attestation","attest_author":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4/action/author_attestation","sign_citation":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4/action/citation_signature","submit_replication":"https://pith.science/pith/U3SVJSSICIB5VUR5T4PJDZAOY4/action/replication_record"}},"created_at":"2026-07-04T15:22:34.176062+00:00","updated_at":"2026-07-04T15:22:34.176062+00:00"}