{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:FBEN35V2XISJEQNF7ZRNX5PM5I","short_pith_number":"pith:FBEN35V2","schema_version":"1.0","canonical_sha256":"2848ddf6baba249241a5fe62dbf5ecea0f21e8a3a85ef16329bc5a437f547f39","source":{"kind":"arxiv","id":"hep-ph/0108204","version":1},"attestation_state":"computed","paper":{"title":"Implications of $\\bar{\\nu}_{e}e^{-}\\to W^{-}\\gamma$ for high-energy $\\bar{\\nu}_e$ observation","license":"","headline":"","cross_cats":["astro-ph"],"primary_cat":"hep-ph","authors_text":"Guey-Lin Lin (NCTU), H. Athar (NCTS, NCTU)","submitted_at":"2001-08-24T11:43:13Z","abstract_excerpt":"Absorption of high-energy $\\bar{\\nu}_e$ over electrons above the W boson production threshold is reexamined. It is pointed out that, in the case of photon emissions along the direction of incident high-energy $\\bar{\\nu}_e$, the kinematically allowed average energy carried by the final state hard photon can be $\\leq 1%$ of the incident $\\bar{\\nu}_e$ energy above the W boson production threshold. The differential energy spectrum for the final state hard photon is calculated. We also discuss implications of our results for the prospective search of high-energy $\\bar{\\nu}_e$ through this final sta"},"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/0108204","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-08-24T11:43:13Z","cross_cats_sorted":["astro-ph"],"title_canon_sha256":"aa9e9f09c41803cfa1f2b23c35212a00835ea5372c421e24e9194f5d0d706cf3","abstract_canon_sha256":"d74fa914d1b251dad1fbc8d813752deafc59b7c96153a096fb7ea9f821e57f3b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:21:31.702392Z","signature_b64":"uKE/A1BR6YsrBlwF55ZgN5Mh2P6kY2NygqgHb8zE5gwc1/5uqCu0Kv8ebNtDoOx42BVptZi0bzi2cC6Mbe9EAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2848ddf6baba249241a5fe62dbf5ecea0f21e8a3a85ef16329bc5a437f547f39","last_reissued_at":"2026-05-18T04:21:31.701903Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:21:31.701903Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Implications of $\\bar{\\nu}_{e}e^{-}\\to W^{-}\\gamma$ for high-energy $\\bar{\\nu}_e$ observation","license":"","headline":"","cross_cats":["astro-ph"],"primary_cat":"hep-ph","authors_text":"Guey-Lin Lin (NCTU), H. Athar (NCTS, NCTU)","submitted_at":"2001-08-24T11:43:13Z","abstract_excerpt":"Absorption of high-energy $\\bar{\\nu}_e$ over electrons above the W boson production threshold is reexamined. It is pointed out that, in the case of photon emissions along the direction of incident high-energy $\\bar{\\nu}_e$, the kinematically allowed average energy carried by the final state hard photon can be $\\leq 1%$ of the incident $\\bar{\\nu}_e$ energy above the W boson production threshold. The differential energy spectrum for the final state hard photon is calculated. We also discuss implications of our results for the prospective search of high-energy $\\bar{\\nu}_e$ through this final sta"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0108204","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":""},"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/0108204","created_at":"2026-05-18T04:21:31.701973+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0108204v1","created_at":"2026-05-18T04:21:31.701973+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0108204","created_at":"2026-05-18T04:21:31.701973+00:00"},{"alias_kind":"pith_short_12","alias_value":"FBEN35V2XISJ","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"FBEN35V2XISJEQNF","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"FBEN35V2","created_at":"2026-05-18T12:25:50.254431+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/FBEN35V2XISJEQNF7ZRNX5PM5I","json":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I.json","graph_json":"https://pith.science/api/pith-number/FBEN35V2XISJEQNF7ZRNX5PM5I/graph.json","events_json":"https://pith.science/api/pith-number/FBEN35V2XISJEQNF7ZRNX5PM5I/events.json","paper":"https://pith.science/paper/FBEN35V2"},"agent_actions":{"view_html":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I","download_json":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I.json","view_paper":"https://pith.science/paper/FBEN35V2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0108204&json=true","fetch_graph":"https://pith.science/api/pith-number/FBEN35V2XISJEQNF7ZRNX5PM5I/graph.json","fetch_events":"https://pith.science/api/pith-number/FBEN35V2XISJEQNF7ZRNX5PM5I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I/action/storage_attestation","attest_author":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I/action/author_attestation","sign_citation":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I/action/citation_signature","submit_replication":"https://pith.science/pith/FBEN35V2XISJEQNF7ZRNX5PM5I/action/replication_record"}},"created_at":"2026-05-18T04:21:31.701973+00:00","updated_at":"2026-05-18T04:21:31.701973+00:00"}