{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:GTRRO727SITXYGRNASZNZEEXND","short_pith_number":"pith:GTRRO727","canonical_record":{"source":{"id":"1312.6860","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-24T17:58:23Z","cross_cats_sorted":[],"title_canon_sha256":"bcdc8f55788efede6d2146d1a642369b789b23142d14f4fdc9cfd67103d5d979","abstract_canon_sha256":"d502980af521497370e41198185fe40f719733cc08d0795dde029dfda9b83943"},"schema_version":"1.0"},"canonical_sha256":"34e3177f5f92277c1a2d04b2dc909768e40b4c08ea2a9c68ead60f2205cb7496","source":{"kind":"arxiv","id":"1312.6860","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.6860","created_at":"2026-05-18T02:55:38Z"},{"alias_kind":"arxiv_version","alias_value":"1312.6860v3","created_at":"2026-05-18T02:55:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.6860","created_at":"2026-05-18T02:55:38Z"},{"alias_kind":"pith_short_12","alias_value":"GTRRO727SITX","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GTRRO727SITXYGRN","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GTRRO727","created_at":"2026-05-18T12:27:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:GTRRO727SITXYGRNASZNZEEXND","target":"record","payload":{"canonical_record":{"source":{"id":"1312.6860","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-24T17:58:23Z","cross_cats_sorted":[],"title_canon_sha256":"bcdc8f55788efede6d2146d1a642369b789b23142d14f4fdc9cfd67103d5d979","abstract_canon_sha256":"d502980af521497370e41198185fe40f719733cc08d0795dde029dfda9b83943"},"schema_version":"1.0"},"canonical_sha256":"34e3177f5f92277c1a2d04b2dc909768e40b4c08ea2a9c68ead60f2205cb7496","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:38.097856Z","signature_b64":"ZLYU5jcg1iVK3MaCI1cggoX7gLyyNdqOuzCk8NZH5hQIpWnG6WzZhSjtFNA0/KKqUnDoOwND67ucjch8mKfPCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"34e3177f5f92277c1a2d04b2dc909768e40b4c08ea2a9c68ead60f2205cb7496","last_reissued_at":"2026-05-18T02:55:38.097148Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:38.097148Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.6860","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":"2026-05-18T02:55:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QG9vwWiiAN0F3NWZTt3Mvo+HM58TMGGXeOukXlLffDDdp216hRqRupE/MNtPcJK8dMVbA2j6V94LxXCKSL6FDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:07:08.031283Z"},"content_sha256":"8dab8ad5e5ec4d4322b830064867f3e5a82dcd69a199024f6c1f3e150a4829b3","schema_version":"1.0","event_id":"sha256:8dab8ad5e5ec4d4322b830064867f3e5a82dcd69a199024f6c1f3e150a4829b3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:GTRRO727SITXYGRNASZNZEEXND","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Static weak dipole moments of the $\\tau$ lepton via renormalizable scalar leptoquark interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Bola\\~nos, A. Moyotl, G.Tavares-Velasco","submitted_at":"2013-12-24T17:58:23Z","abstract_excerpt":"The weak dipole moments of elementary fermions are calculated at the one-loop level in the framework of a renormalizable scalar leptoquark model that forbids baryon number violating processes and so is free from the strong constraints from experimental data. In this model there are two scalar leptoquarks accommodated in an $SU_L(2)\\times U_Y(1)$ doublet: one of such leptoquarks is non-chiral and has electric charge of $5/3e$, whereas the other one is chiral and has electric charge $2/3e$. In particular, a non-chiral leptoquark contributes to the weak properties of an up fermion via a chirality"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.6860","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":""},"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":"2026-05-18T02:55:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LIieh67SvhLMs0DlbiTLgPJOJw13yxUVoYYEfQ/AV6iybpyXKZzfs4flX+WRFo0uY8KtDbYVQTOy5IZNUqtEBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:07:08.031638Z"},"content_sha256":"1b58f909962ea73448ab6165e51f8e90b008eb9faab0e4d8359a5e9b6d06346b","schema_version":"1.0","event_id":"sha256:1b58f909962ea73448ab6165e51f8e90b008eb9faab0e4d8359a5e9b6d06346b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GTRRO727SITXYGRNASZNZEEXND/bundle.json","state_url":"https://pith.science/pith/GTRRO727SITXYGRNASZNZEEXND/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GTRRO727SITXYGRNASZNZEEXND/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":"2026-06-02T12:07:08Z","links":{"resolver":"https://pith.science/pith/GTRRO727SITXYGRNASZNZEEXND","bundle":"https://pith.science/pith/GTRRO727SITXYGRNASZNZEEXND/bundle.json","state":"https://pith.science/pith/GTRRO727SITXYGRNASZNZEEXND/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GTRRO727SITXYGRNASZNZEEXND/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:GTRRO727SITXYGRNASZNZEEXND","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":"d502980af521497370e41198185fe40f719733cc08d0795dde029dfda9b83943","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-24T17:58:23Z","title_canon_sha256":"bcdc8f55788efede6d2146d1a642369b789b23142d14f4fdc9cfd67103d5d979"},"schema_version":"1.0","source":{"id":"1312.6860","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.6860","created_at":"2026-05-18T02:55:38Z"},{"alias_kind":"arxiv_version","alias_value":"1312.6860v3","created_at":"2026-05-18T02:55:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.6860","created_at":"2026-05-18T02:55:38Z"},{"alias_kind":"pith_short_12","alias_value":"GTRRO727SITX","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GTRRO727SITXYGRN","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GTRRO727","created_at":"2026-05-18T12:27:45Z"}],"graph_snapshots":[{"event_id":"sha256:1b58f909962ea73448ab6165e51f8e90b008eb9faab0e4d8359a5e9b6d06346b","target":"graph","created_at":"2026-05-18T02:55:38Z","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":"The weak dipole moments of elementary fermions are calculated at the one-loop level in the framework of a renormalizable scalar leptoquark model that forbids baryon number violating processes and so is free from the strong constraints from experimental data. In this model there are two scalar leptoquarks accommodated in an $SU_L(2)\\times U_Y(1)$ doublet: one of such leptoquarks is non-chiral and has electric charge of $5/3e$, whereas the other one is chiral and has electric charge $2/3e$. In particular, a non-chiral leptoquark contributes to the weak properties of an up fermion via a chirality","authors_text":"A. Bola\\~nos, A. Moyotl, G.Tavares-Velasco","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-24T17:58:23Z","title":"Static weak dipole moments of the $\\tau$ lepton via renormalizable scalar leptoquark interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.6860","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":"sha256:8dab8ad5e5ec4d4322b830064867f3e5a82dcd69a199024f6c1f3e150a4829b3","target":"record","created_at":"2026-05-18T02:55:38Z","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":"d502980af521497370e41198185fe40f719733cc08d0795dde029dfda9b83943","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-24T17:58:23Z","title_canon_sha256":"bcdc8f55788efede6d2146d1a642369b789b23142d14f4fdc9cfd67103d5d979"},"schema_version":"1.0","source":{"id":"1312.6860","kind":"arxiv","version":3}},"canonical_sha256":"34e3177f5f92277c1a2d04b2dc909768e40b4c08ea2a9c68ead60f2205cb7496","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"34e3177f5f92277c1a2d04b2dc909768e40b4c08ea2a9c68ead60f2205cb7496","first_computed_at":"2026-05-18T02:55:38.097148Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:55:38.097148Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZLYU5jcg1iVK3MaCI1cggoX7gLyyNdqOuzCk8NZH5hQIpWnG6WzZhSjtFNA0/KKqUnDoOwND67ucjch8mKfPCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:55:38.097856Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.6860","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8dab8ad5e5ec4d4322b830064867f3e5a82dcd69a199024f6c1f3e150a4829b3","sha256:1b58f909962ea73448ab6165e51f8e90b008eb9faab0e4d8359a5e9b6d06346b"],"state_sha256":"8af8b9cfa1dea2b069ec02b53c665c9720c458c8797236fc26dc1fd9d31daa8b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NuynTq9M9M0r7rLcym9F7UtYm/wQpj1tBh/PhG3LNFjfHDlTol4ZNhhjXkObI7wS0g8on73P2VtjV+M5UVk/DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T12:07:08.033489Z","bundle_sha256":"6e8a5f88078f0e701c175ccaacc9e9bc919d351c88ab8de86ee9ec65bfbeb988"}}