{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:LPYLPP3ESOD3K5HHA4CBZB3VIN","short_pith_number":"pith:LPYLPP3E","canonical_record":{"source":{"id":"hep-ph/0403149","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-03-14T09:25:29Z","cross_cats_sorted":[],"title_canon_sha256":"5dd19a2c8331a53aed8af9e2b9d09607c2745242aebd52f48687c81efb8098e2","abstract_canon_sha256":"ac939582bf05947df4f6c52593f031ec4f08bb4a45b1ca00dcd2fe866020c21d"},"schema_version":"1.0"},"canonical_sha256":"5bf0b7bf649387b574e707041c87754378add64f486333381895bb0647529f10","source":{"kind":"arxiv","id":"hep-ph/0403149","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0403149","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0403149v1","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0403149","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"pith_short_12","alias_value":"LPYLPP3ESOD3","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"LPYLPP3ESOD3K5HH","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"LPYLPP3E","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:LPYLPP3ESOD3K5HHA4CBZB3VIN","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0403149","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-03-14T09:25:29Z","cross_cats_sorted":[],"title_canon_sha256":"5dd19a2c8331a53aed8af9e2b9d09607c2745242aebd52f48687c81efb8098e2","abstract_canon_sha256":"ac939582bf05947df4f6c52593f031ec4f08bb4a45b1ca00dcd2fe866020c21d"},"schema_version":"1.0"},"canonical_sha256":"5bf0b7bf649387b574e707041c87754378add64f486333381895bb0647529f10","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:48.728811Z","signature_b64":"l54KZU8PuEryaPZkbppwOrx4IB8ghmXXj4IdHM+q/GoDMOsrz1Yi6Zc9gpsKT1f7AE48fGD/gOQv4eBZwiJVAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5bf0b7bf649387b574e707041c87754378add64f486333381895bb0647529f10","last_reissued_at":"2026-05-18T04:15:48.728214Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:48.728214Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0403149","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:15:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gtB1CkhbKkEt31uXU2lXuoHm934cB0V2JhnGSI3mJroT6CcePRVH0l2loHCvV4pWNigGHhjA55r4PhB3mRP1AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:38:57.583893Z"},"content_sha256":"36068e5708b0e3b27884515f26076fa8a6f8998a4971455167ddd07eb8c9db3c","schema_version":"1.0","event_id":"sha256:36068e5708b0e3b27884515f26076fa8a6f8998a4971455167ddd07eb8c9db3c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:LPYLPP3ESOD3K5HHA4CBZB3VIN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Radiative Corrections to Neutrino-Nucleon Quasielastic Scattering","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Masataka Fukugita, Takahiro Kubota","submitted_at":"2004-03-14T09:25:29Z","abstract_excerpt":"Full one-loop radiative corrections are calculated for low energy neutrino-nucleon quasi-elastic scattering, $\\bar \\nu_{e}+p \\longrightarrow e^{+} + n$, which involves both Fermi and Gamow-Teller transitions, in the static limit of nucleons. The calculation is performed for both angular independent and dependent parts. We separate the corrections into the outer and inner parts {\\` a} la Sirlin. The outer part is infrared and ultraviolet finite, and involves the positron velocity. The calculation of the outer part is straightforward, but that of the inner part requires a scrutiny concerning the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0403149","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:15:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tKkydVAvnoOhQg28ieHHUHlJNwHHKdIcX69NOyAFAFV9qZUBB5S/3ScxBT3qvmOsaxv+fJ0ECvyotDfWRqJeDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:38:57.584350Z"},"content_sha256":"b6aea90daba8ef4c0afdb783addbf935de3a67eaffd29a01f9dadcfb86254c65","schema_version":"1.0","event_id":"sha256:b6aea90daba8ef4c0afdb783addbf935de3a67eaffd29a01f9dadcfb86254c65"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LPYLPP3ESOD3K5HHA4CBZB3VIN/bundle.json","state_url":"https://pith.science/pith/LPYLPP3ESOD3K5HHA4CBZB3VIN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LPYLPP3ESOD3K5HHA4CBZB3VIN/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-30T08:38:57Z","links":{"resolver":"https://pith.science/pith/LPYLPP3ESOD3K5HHA4CBZB3VIN","bundle":"https://pith.science/pith/LPYLPP3ESOD3K5HHA4CBZB3VIN/bundle.json","state":"https://pith.science/pith/LPYLPP3ESOD3K5HHA4CBZB3VIN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LPYLPP3ESOD3K5HHA4CBZB3VIN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:LPYLPP3ESOD3K5HHA4CBZB3VIN","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"ac939582bf05947df4f6c52593f031ec4f08bb4a45b1ca00dcd2fe866020c21d","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2004-03-14T09:25:29Z","title_canon_sha256":"5dd19a2c8331a53aed8af9e2b9d09607c2745242aebd52f48687c81efb8098e2"},"schema_version":"1.0","source":{"id":"hep-ph/0403149","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0403149","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0403149v1","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0403149","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"pith_short_12","alias_value":"LPYLPP3ESOD3","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"LPYLPP3ESOD3K5HH","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"LPYLPP3E","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:b6aea90daba8ef4c0afdb783addbf935de3a67eaffd29a01f9dadcfb86254c65","target":"graph","created_at":"2026-05-18T04:15:48Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Full one-loop radiative corrections are calculated for low energy neutrino-nucleon quasi-elastic scattering, $\\bar \\nu_{e}+p \\longrightarrow e^{+} + n$, which involves both Fermi and Gamow-Teller transitions, in the static limit of nucleons. The calculation is performed for both angular independent and dependent parts. We separate the corrections into the outer and inner parts {\\` a} la Sirlin. The outer part is infrared and ultraviolet finite, and involves the positron velocity. The calculation of the outer part is straightforward, but that of the inner part requires a scrutiny concerning the","authors_text":"Masataka Fukugita, Takahiro Kubota","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2004-03-14T09:25:29Z","title":"Radiative Corrections to Neutrino-Nucleon Quasielastic Scattering"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0403149","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:36068e5708b0e3b27884515f26076fa8a6f8998a4971455167ddd07eb8c9db3c","target":"record","created_at":"2026-05-18T04:15:48Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"ac939582bf05947df4f6c52593f031ec4f08bb4a45b1ca00dcd2fe866020c21d","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2004-03-14T09:25:29Z","title_canon_sha256":"5dd19a2c8331a53aed8af9e2b9d09607c2745242aebd52f48687c81efb8098e2"},"schema_version":"1.0","source":{"id":"hep-ph/0403149","kind":"arxiv","version":1}},"canonical_sha256":"5bf0b7bf649387b574e707041c87754378add64f486333381895bb0647529f10","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5bf0b7bf649387b574e707041c87754378add64f486333381895bb0647529f10","first_computed_at":"2026-05-18T04:15:48.728214Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:15:48.728214Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"l54KZU8PuEryaPZkbppwOrx4IB8ghmXXj4IdHM+q/GoDMOsrz1Yi6Zc9gpsKT1f7AE48fGD/gOQv4eBZwiJVAg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:15:48.728811Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0403149","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:36068e5708b0e3b27884515f26076fa8a6f8998a4971455167ddd07eb8c9db3c","sha256:b6aea90daba8ef4c0afdb783addbf935de3a67eaffd29a01f9dadcfb86254c65"],"state_sha256":"045d38b44b4dd206e074c66c7eb8a5ba1d2c8f651075a1f69309aabb184d98cb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TgQZtPySrxAH+3D9i6fXxCcTbwZA1oTOYRKwb2ej0mNekF9AL+2ioSO21AyHYM1LYDY5nccgSJgi2kl6zLpHBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T08:38:57.587213Z","bundle_sha256":"91675e597c81d5a6ec8cd55b74c12992a153f75f25522f613adea4fb3fefbeb5"}}