{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:6D2L2KBX43IPPZAD3XX3KZ3EWU","short_pith_number":"pith:6D2L2KBX","canonical_record":{"source":{"id":"1312.6667","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-23T20:41:28Z","cross_cats_sorted":["astro-ph.CO","nucl-th","physics.atom-ph","physics.space-ph"],"title_canon_sha256":"6783f15f07c4efe3b4d4d00be541f4d05cf10cd755ccd2a2d9c44d8206043e1c","abstract_canon_sha256":"b97874653edfda7acf76aa4cf668202da3cf6e5efa1002160710aaf2d835dc8f"},"schema_version":"1.0"},"canonical_sha256":"f0f4bd2837e6d0f7e403ddefb56764b50749b38fc2ffd482073a9493b3abb14d","source":{"kind":"arxiv","id":"1312.6667","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.6667","created_at":"2026-05-18T02:26:13Z"},{"alias_kind":"arxiv_version","alias_value":"1312.6667v2","created_at":"2026-05-18T02:26:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.6667","created_at":"2026-05-18T02:26:13Z"},{"alias_kind":"pith_short_12","alias_value":"6D2L2KBX43IP","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"6D2L2KBX43IPPZAD","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"6D2L2KBX","created_at":"2026-05-18T12:27:36Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:6D2L2KBX43IPPZAD3XX3KZ3EWU","target":"record","payload":{"canonical_record":{"source":{"id":"1312.6667","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-23T20:41:28Z","cross_cats_sorted":["astro-ph.CO","nucl-th","physics.atom-ph","physics.space-ph"],"title_canon_sha256":"6783f15f07c4efe3b4d4d00be541f4d05cf10cd755ccd2a2d9c44d8206043e1c","abstract_canon_sha256":"b97874653edfda7acf76aa4cf668202da3cf6e5efa1002160710aaf2d835dc8f"},"schema_version":"1.0"},"canonical_sha256":"f0f4bd2837e6d0f7e403ddefb56764b50749b38fc2ffd482073a9493b3abb14d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:13.021081Z","signature_b64":"g1VDmLuqmiHIAImXtMDaCZAVVZRxbFJAXKG00AXLQINUzSR1wnmm7vRgy+jYOba/ILGBl/MoiwaqD8xpgrrJAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f0f4bd2837e6d0f7e403ddefb56764b50749b38fc2ffd482073a9493b3abb14d","last_reissued_at":"2026-05-18T02:26:13.020469Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:13.020469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.6667","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:26:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yDiIs9q6EL3cUbV2gAUhXSr/AVO2HgxtnHtfqukWnyKE8kSFKvphwpaPHJgjvG3jhmrDnrU0vHga/oVi4KK0BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:12:07.986242Z"},"content_sha256":"409c8dc7f8c2cc21d89610535ac5699b07a1d408743b907b0bc7dad94b3aa202","schema_version":"1.0","event_id":"sha256:409c8dc7f8c2cc21d89610535ac5699b07a1d408743b907b0bc7dad94b3aa202"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:6D2L2KBX43IPPZAD3XX3KZ3EWU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Axion-induced effects in atoms, molecules and nuclei: Parity nonconservation, anapole moments, electric dipole moments, and spin-gravity and spin-axion momentum couplings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","nucl-th","physics.atom-ph","physics.space-ph"],"primary_cat":"hep-ph","authors_text":"V. V. Flambaum, Y. V. Stadnik","submitted_at":"2013-12-23T20:41:28Z","abstract_excerpt":"We show that the interaction of an axion field, or in general a pseudoscalar field, with the axial-vector current generated by an electron through a derivative-type coupling can give rise to a time-dependent mixing of opposite-parity states in atomic and molecular systems. Likewise, the analogous interaction of an axion field with the axial-vector current generated by a nucleon can give rise to time-dependent mixing of opposite-parity states in nuclear systems. This mixing can induce oscillating electric dipole moments, oscillating parity non-conservation effects and oscillating anapole moment"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.6667","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:26:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T2P9+P6ziOJ8Sff4nWWRlT84kbxoNPepFI9/qBDtItiqbAlWVDPzBQk6CvfWAFYoKBRmU5/JPTdTr/FQnDq1Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:12:07.986683Z"},"content_sha256":"15cf99e32b852c6d149fec886fa9a207926f8f523b5ae00fb5c4ce4e1ba80536","schema_version":"1.0","event_id":"sha256:15cf99e32b852c6d149fec886fa9a207926f8f523b5ae00fb5c4ce4e1ba80536"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6D2L2KBX43IPPZAD3XX3KZ3EWU/bundle.json","state_url":"https://pith.science/pith/6D2L2KBX43IPPZAD3XX3KZ3EWU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6D2L2KBX43IPPZAD3XX3KZ3EWU/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":"2026-05-25T23:12:07Z","links":{"resolver":"https://pith.science/pith/6D2L2KBX43IPPZAD3XX3KZ3EWU","bundle":"https://pith.science/pith/6D2L2KBX43IPPZAD3XX3KZ3EWU/bundle.json","state":"https://pith.science/pith/6D2L2KBX43IPPZAD3XX3KZ3EWU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6D2L2KBX43IPPZAD3XX3KZ3EWU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:6D2L2KBX43IPPZAD3XX3KZ3EWU","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":"b97874653edfda7acf76aa4cf668202da3cf6e5efa1002160710aaf2d835dc8f","cross_cats_sorted":["astro-ph.CO","nucl-th","physics.atom-ph","physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-23T20:41:28Z","title_canon_sha256":"6783f15f07c4efe3b4d4d00be541f4d05cf10cd755ccd2a2d9c44d8206043e1c"},"schema_version":"1.0","source":{"id":"1312.6667","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.6667","created_at":"2026-05-18T02:26:13Z"},{"alias_kind":"arxiv_version","alias_value":"1312.6667v2","created_at":"2026-05-18T02:26:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.6667","created_at":"2026-05-18T02:26:13Z"},{"alias_kind":"pith_short_12","alias_value":"6D2L2KBX43IP","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"6D2L2KBX43IPPZAD","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"6D2L2KBX","created_at":"2026-05-18T12:27:36Z"}],"graph_snapshots":[{"event_id":"sha256:15cf99e32b852c6d149fec886fa9a207926f8f523b5ae00fb5c4ce4e1ba80536","target":"graph","created_at":"2026-05-18T02:26:13Z","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":"We show that the interaction of an axion field, or in general a pseudoscalar field, with the axial-vector current generated by an electron through a derivative-type coupling can give rise to a time-dependent mixing of opposite-parity states in atomic and molecular systems. Likewise, the analogous interaction of an axion field with the axial-vector current generated by a nucleon can give rise to time-dependent mixing of opposite-parity states in nuclear systems. This mixing can induce oscillating electric dipole moments, oscillating parity non-conservation effects and oscillating anapole moment","authors_text":"V. V. Flambaum, Y. V. Stadnik","cross_cats":["astro-ph.CO","nucl-th","physics.atom-ph","physics.space-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-23T20:41:28Z","title":"Axion-induced effects in atoms, molecules and nuclei: Parity nonconservation, anapole moments, electric dipole moments, and spin-gravity and spin-axion momentum couplings"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.6667","kind":"arxiv","version":2},"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":"sha256:409c8dc7f8c2cc21d89610535ac5699b07a1d408743b907b0bc7dad94b3aa202","target":"record","created_at":"2026-05-18T02:26:13Z","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":"b97874653edfda7acf76aa4cf668202da3cf6e5efa1002160710aaf2d835dc8f","cross_cats_sorted":["astro-ph.CO","nucl-th","physics.atom-ph","physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-23T20:41:28Z","title_canon_sha256":"6783f15f07c4efe3b4d4d00be541f4d05cf10cd755ccd2a2d9c44d8206043e1c"},"schema_version":"1.0","source":{"id":"1312.6667","kind":"arxiv","version":2}},"canonical_sha256":"f0f4bd2837e6d0f7e403ddefb56764b50749b38fc2ffd482073a9493b3abb14d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f0f4bd2837e6d0f7e403ddefb56764b50749b38fc2ffd482073a9493b3abb14d","first_computed_at":"2026-05-18T02:26:13.020469Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:26:13.020469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"g1VDmLuqmiHIAImXtMDaCZAVVZRxbFJAXKG00AXLQINUzSR1wnmm7vRgy+jYOba/ILGBl/MoiwaqD8xpgrrJAg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:26:13.021081Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.6667","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:409c8dc7f8c2cc21d89610535ac5699b07a1d408743b907b0bc7dad94b3aa202","sha256:15cf99e32b852c6d149fec886fa9a207926f8f523b5ae00fb5c4ce4e1ba80536"],"state_sha256":"2bede6d1a2d18df2f155035c4e8cb7b718e13013044bce130ef8a4b928809d69"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2cVZ/Gz+7+qTyZ0pdYkw9eMqyLAajRPiTzZkr8zR1toIh1u3FHY6Kr8bb4MhDFQtpW/GVDactpHv/9cPSIykDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T23:12:07.990186Z","bundle_sha256":"50ffc9b7e489bdf43c59373037b026b3e5a463044c297a77bc89de202953697b"}}