{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:63OCL5GNMKCNBPLU6HJHD7EBT3","short_pith_number":"pith:63OCL5GN","canonical_record":{"source":{"id":"2411.12521","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-11-19T14:10:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"d3950deb34270de6114cbb0c4332938c35b3df8a942f01c9e9ab3bd439bd1014","abstract_canon_sha256":"b39f70db947131e50a0b0a3c19fff0bd1a402379cf9f32d2e587bc4a5a3f5dc4"},"schema_version":"1.0"},"canonical_sha256":"f6dc25f4cd6284d0bd74f1d271fc819eebaddb617f6c109e53ad674d8196d334","source":{"kind":"arxiv","id":"2411.12521","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.12521","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"arxiv_version","alias_value":"2411.12521v3","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.12521","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"pith_short_12","alias_value":"63OCL5GNMKCN","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"pith_short_16","alias_value":"63OCL5GNMKCNBPLU","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"pith_short_8","alias_value":"63OCL5GN","created_at":"2026-07-05T10:27:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:63OCL5GNMKCNBPLU6HJHD7EBT3","target":"record","payload":{"canonical_record":{"source":{"id":"2411.12521","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-11-19T14:10:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"d3950deb34270de6114cbb0c4332938c35b3df8a942f01c9e9ab3bd439bd1014","abstract_canon_sha256":"b39f70db947131e50a0b0a3c19fff0bd1a402379cf9f32d2e587bc4a5a3f5dc4"},"schema_version":"1.0"},"canonical_sha256":"f6dc25f4cd6284d0bd74f1d271fc819eebaddb617f6c109e53ad674d8196d334","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:27:19.888622Z","signature_b64":"7xT8VwSHhxr4pZ0uKfhXfq7ffzW2k00O/xIjzEZi7h/QdslMS1tdHr97poOR/ecePc3on7VoYfdvvOl88rC8Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f6dc25f4cd6284d0bd74f1d271fc819eebaddb617f6c109e53ad674d8196d334","last_reissued_at":"2026-07-05T10:27:19.887868Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:27:19.887868Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.12521","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:27:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"58lMA4jMXNB20YuFXBLkjKGpFeEzIEPTkG/srrd5+OzLLE5B3fZ2kgRovmsVJGQgjQHOhQpjxbqgCOo3PB6pBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T00:57:31.991536Z"},"content_sha256":"942eb40bf0b158794386280ce9ed3dbca99b443ae44f462223eead48673b5273","schema_version":"1.0","event_id":"sha256:942eb40bf0b158794386280ce9ed3dbca99b443ae44f462223eead48673b5273"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:63OCL5GNMKCNBPLU6HJHD7EBT3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nucleon relativistic weak-neutral axial-vector four-current distributions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Yi Chen","submitted_at":"2024-11-19T14:10:00Z","abstract_excerpt":"Relativistic full weak-neutral axial-vector four-current distributions inside a general spin-$\\frac{1}{2}$ hadron are systematically studied for the first time, where the second-class current contribution associated with the induced pseudotensor form factor (FF) is included. We clearly demonstrate that the 3D axial charge distribution, being parity-odd in the Breit frame, is in fact related to the induced pseudotensor FF $G_T^Z(Q^2)$ rather than the axial FF $G_A^Z(Q^2)$. We study the frame-dependence of full axial-vector four-current distributions for a moving hadron, and compare them with th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.12521","kind":"arxiv","version":3},"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/2411.12521/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:27:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AQSH6sfN1EfRYUv01uvdMT91arq1/7kpqIY40gJ2VeQRZ71G+HoUVnR3ZP2qcLk1YqJyH9r7LKmsUa8bwWo4Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T00:57:31.991921Z"},"content_sha256":"391fbae3fd2703e5d31ae157f1b47bac6808419fabdf378d09d3b7418d1b7a69","schema_version":"1.0","event_id":"sha256:391fbae3fd2703e5d31ae157f1b47bac6808419fabdf378d09d3b7418d1b7a69"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/63OCL5GNMKCNBPLU6HJHD7EBT3/bundle.json","state_url":"https://pith.science/pith/63OCL5GNMKCNBPLU6HJHD7EBT3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/63OCL5GNMKCNBPLU6HJHD7EBT3/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":"2026-08-13T00:57:31Z","links":{"resolver":"https://pith.science/pith/63OCL5GNMKCNBPLU6HJHD7EBT3","bundle":"https://pith.science/pith/63OCL5GNMKCNBPLU6HJHD7EBT3/bundle.json","state":"https://pith.science/pith/63OCL5GNMKCNBPLU6HJHD7EBT3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/63OCL5GNMKCNBPLU6HJHD7EBT3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:63OCL5GNMKCNBPLU6HJHD7EBT3","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":"b39f70db947131e50a0b0a3c19fff0bd1a402379cf9f32d2e587bc4a5a3f5dc4","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-11-19T14:10:00Z","title_canon_sha256":"d3950deb34270de6114cbb0c4332938c35b3df8a942f01c9e9ab3bd439bd1014"},"schema_version":"1.0","source":{"id":"2411.12521","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.12521","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"arxiv_version","alias_value":"2411.12521v3","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.12521","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"pith_short_12","alias_value":"63OCL5GNMKCN","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"pith_short_16","alias_value":"63OCL5GNMKCNBPLU","created_at":"2026-07-05T10:27:19Z"},{"alias_kind":"pith_short_8","alias_value":"63OCL5GN","created_at":"2026-07-05T10:27:19Z"}],"graph_snapshots":[{"event_id":"sha256:391fbae3fd2703e5d31ae157f1b47bac6808419fabdf378d09d3b7418d1b7a69","target":"graph","created_at":"2026-07-05T10:27:19Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2411.12521/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Relativistic full weak-neutral axial-vector four-current distributions inside a general spin-$\\frac{1}{2}$ hadron are systematically studied for the first time, where the second-class current contribution associated with the induced pseudotensor form factor (FF) is included. We clearly demonstrate that the 3D axial charge distribution, being parity-odd in the Breit frame, is in fact related to the induced pseudotensor FF $G_T^Z(Q^2)$ rather than the axial FF $G_A^Z(Q^2)$. We study the frame-dependence of full axial-vector four-current distributions for a moving hadron, and compare them with th","authors_text":"Yi Chen","cross_cats":["nucl-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-11-19T14:10:00Z","title":"Nucleon relativistic weak-neutral axial-vector four-current distributions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.12521","kind":"arxiv","version":3},"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":"sha256:942eb40bf0b158794386280ce9ed3dbca99b443ae44f462223eead48673b5273","target":"record","created_at":"2026-07-05T10:27:19Z","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":"b39f70db947131e50a0b0a3c19fff0bd1a402379cf9f32d2e587bc4a5a3f5dc4","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-11-19T14:10:00Z","title_canon_sha256":"d3950deb34270de6114cbb0c4332938c35b3df8a942f01c9e9ab3bd439bd1014"},"schema_version":"1.0","source":{"id":"2411.12521","kind":"arxiv","version":3}},"canonical_sha256":"f6dc25f4cd6284d0bd74f1d271fc819eebaddb617f6c109e53ad674d8196d334","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f6dc25f4cd6284d0bd74f1d271fc819eebaddb617f6c109e53ad674d8196d334","first_computed_at":"2026-07-05T10:27:19.887868Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:27:19.887868Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7xT8VwSHhxr4pZ0uKfhXfq7ffzW2k00O/xIjzEZi7h/QdslMS1tdHr97poOR/ecePc3on7VoYfdvvOl88rC8Dw==","signature_status":"signed_v1","signed_at":"2026-07-05T10:27:19.888622Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.12521","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:942eb40bf0b158794386280ce9ed3dbca99b443ae44f462223eead48673b5273","sha256:391fbae3fd2703e5d31ae157f1b47bac6808419fabdf378d09d3b7418d1b7a69"],"state_sha256":"8ec5c4b9b8256076a4c195d8a3ebb591dc9988c28e9a49fe28c53a2d628fefcd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XMif3TggsJG00WweSeNMneglktZMn97RjVsNOq7cMIa+ixCM7NNLi/vnxdroRYj6yNnkYKj5MB7siLzZYcziBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T00:57:31.994803Z","bundle_sha256":"146f14aa36bfe1961cdcef61221e8fcc3f3d54a778c6ae35283a6982a00daee4"}}