{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:SHLVQ66O64267A6GKYWAVLVII4","short_pith_number":"pith:SHLVQ66O","canonical_record":{"source":{"id":"1801.06377","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-19T12:06:39Z","cross_cats_sorted":[],"title_canon_sha256":"9d878ea543c993468b6c145a9d5b0f5b9333b0347c5592a2680f98b4f4c3dd67","abstract_canon_sha256":"d6b51018ea3ef2e11959bc476048260105cce46a54e8517340fbcdede9d700b6"},"schema_version":"1.0"},"canonical_sha256":"91d7587bcef735ef83c6562c0aaea847261fe8fc2290bb809c935ded1bc44eb1","source":{"kind":"arxiv","id":"1801.06377","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.06377","created_at":"2026-05-18T00:14:53Z"},{"alias_kind":"arxiv_version","alias_value":"1801.06377v2","created_at":"2026-05-18T00:14:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.06377","created_at":"2026-05-18T00:14:53Z"},{"alias_kind":"pith_short_12","alias_value":"SHLVQ66O6426","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_16","alias_value":"SHLVQ66O64267A6G","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_8","alias_value":"SHLVQ66O","created_at":"2026-05-18T12:32:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:SHLVQ66O64267A6GKYWAVLVII4","target":"record","payload":{"canonical_record":{"source":{"id":"1801.06377","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-19T12:06:39Z","cross_cats_sorted":[],"title_canon_sha256":"9d878ea543c993468b6c145a9d5b0f5b9333b0347c5592a2680f98b4f4c3dd67","abstract_canon_sha256":"d6b51018ea3ef2e11959bc476048260105cce46a54e8517340fbcdede9d700b6"},"schema_version":"1.0"},"canonical_sha256":"91d7587bcef735ef83c6562c0aaea847261fe8fc2290bb809c935ded1bc44eb1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:53.922144Z","signature_b64":"tOlpks08GhTyHTlxelxDW/buVuczg+4CTcOUhTIBbmKTDiqiwt4j+i6pBS1MZTX+qFobesrgRTD58QWjgPqRCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"91d7587bcef735ef83c6562c0aaea847261fe8fc2290bb809c935ded1bc44eb1","last_reissued_at":"2026-05-18T00:14:53.921478Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:53.921478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.06377","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":"2026-05-18T00:14:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XPlVh9goC4pJyrno/SwP8sVTE6ZqXZYrtajn3uVOpjtn7AWEdTp7LrLYLbftBQ+VoAKPlWXMLxmeV4MGFBoeAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T17:50:23.219012Z"},"content_sha256":"26024c36106b2cc448187bbd3ce1a30a060f7eeaead9cf9250542407f79ed8d1","schema_version":"1.0","event_id":"sha256:26024c36106b2cc448187bbd3ce1a30a060f7eeaead9cf9250542407f79ed8d1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:SHLVQ66O64267A6GKYWAVLVII4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Predictions for the Dirac CP-Violating Phase from Sum Rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander J. Stuart, Lisa L. Everett, Luis A. Delgadillo, Raymundo Ramos","submitted_at":"2018-01-19T12:06:39Z","abstract_excerpt":"We explore the implications of recent results relating the Dirac CP-violating phase to predicted and measured leptonic mixing angles within a standard set of theoretical scenarios in which charged lepton corrections are responsible for generating a non-zero value of the reactor mixing angle. We employ a full set of leptonic sum rules as required by the unitarity of the lepton mixing matrix, which can be reduced to predictions for the observable mixing angles and the Dirac CP-violating phase in terms of model parameters. These sum rules are investigated within a given set of theoretical scenari"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.06377","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":"2026-05-18T00:14:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LLpPAP5LmHmSv3ScCJeaKp0n6MaS4hxTj7RoQSsJkbdc8UX4lov79os/E75juEEgEE8xaUhzsF93DexfnDZDAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T17:50:23.219363Z"},"content_sha256":"6710902727e2c88025563e2caefc95df994cf388dd453909f3d5442943b0a941","schema_version":"1.0","event_id":"sha256:6710902727e2c88025563e2caefc95df994cf388dd453909f3d5442943b0a941"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SHLVQ66O64267A6GKYWAVLVII4/bundle.json","state_url":"https://pith.science/pith/SHLVQ66O64267A6GKYWAVLVII4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SHLVQ66O64267A6GKYWAVLVII4/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":"2026-06-03T17:50:23Z","links":{"resolver":"https://pith.science/pith/SHLVQ66O64267A6GKYWAVLVII4","bundle":"https://pith.science/pith/SHLVQ66O64267A6GKYWAVLVII4/bundle.json","state":"https://pith.science/pith/SHLVQ66O64267A6GKYWAVLVII4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SHLVQ66O64267A6GKYWAVLVII4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:SHLVQ66O64267A6GKYWAVLVII4","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":"d6b51018ea3ef2e11959bc476048260105cce46a54e8517340fbcdede9d700b6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-19T12:06:39Z","title_canon_sha256":"9d878ea543c993468b6c145a9d5b0f5b9333b0347c5592a2680f98b4f4c3dd67"},"schema_version":"1.0","source":{"id":"1801.06377","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.06377","created_at":"2026-05-18T00:14:53Z"},{"alias_kind":"arxiv_version","alias_value":"1801.06377v2","created_at":"2026-05-18T00:14:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.06377","created_at":"2026-05-18T00:14:53Z"},{"alias_kind":"pith_short_12","alias_value":"SHLVQ66O6426","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_16","alias_value":"SHLVQ66O64267A6G","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_8","alias_value":"SHLVQ66O","created_at":"2026-05-18T12:32:53Z"}],"graph_snapshots":[{"event_id":"sha256:6710902727e2c88025563e2caefc95df994cf388dd453909f3d5442943b0a941","target":"graph","created_at":"2026-05-18T00:14:53Z","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 explore the implications of recent results relating the Dirac CP-violating phase to predicted and measured leptonic mixing angles within a standard set of theoretical scenarios in which charged lepton corrections are responsible for generating a non-zero value of the reactor mixing angle. We employ a full set of leptonic sum rules as required by the unitarity of the lepton mixing matrix, which can be reduced to predictions for the observable mixing angles and the Dirac CP-violating phase in terms of model parameters. These sum rules are investigated within a given set of theoretical scenari","authors_text":"Alexander J. Stuart, Lisa L. Everett, Luis A. Delgadillo, Raymundo Ramos","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-19T12:06:39Z","title":"Predictions for the Dirac CP-Violating Phase from Sum Rules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.06377","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":"sha256:26024c36106b2cc448187bbd3ce1a30a060f7eeaead9cf9250542407f79ed8d1","target":"record","created_at":"2026-05-18T00:14:53Z","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":"d6b51018ea3ef2e11959bc476048260105cce46a54e8517340fbcdede9d700b6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-19T12:06:39Z","title_canon_sha256":"9d878ea543c993468b6c145a9d5b0f5b9333b0347c5592a2680f98b4f4c3dd67"},"schema_version":"1.0","source":{"id":"1801.06377","kind":"arxiv","version":2}},"canonical_sha256":"91d7587bcef735ef83c6562c0aaea847261fe8fc2290bb809c935ded1bc44eb1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"91d7587bcef735ef83c6562c0aaea847261fe8fc2290bb809c935ded1bc44eb1","first_computed_at":"2026-05-18T00:14:53.921478Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:14:53.921478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tOlpks08GhTyHTlxelxDW/buVuczg+4CTcOUhTIBbmKTDiqiwt4j+i6pBS1MZTX+qFobesrgRTD58QWjgPqRCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:14:53.922144Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.06377","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:26024c36106b2cc448187bbd3ce1a30a060f7eeaead9cf9250542407f79ed8d1","sha256:6710902727e2c88025563e2caefc95df994cf388dd453909f3d5442943b0a941"],"state_sha256":"fee963a92a66d6997f0335e6275ce22b87a3098486e33c3baa8ae648fe709c80"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uB/3c8wO1FmDyz8x8AgjHn0Ku9QIqZUiuBrQ5/9tM1x75ljDtdGZpwmt73LAeHbkxdQY4RO79xHGgpDPsJVODQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T17:50:23.221250Z","bundle_sha256":"97307e1d8093f7fa160436767d3f32b39c70a4c384bc051bd93891828f8e17e6"}}