{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:JV3NLJBQEEB5SO7CY2N6LZZYWH","short_pith_number":"pith:JV3NLJBQ","canonical_record":{"source":{"id":"1108.0964","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-08-04T00:25:09Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"40a6e9985213cdd6b82d3e2b320978dffcd0e471549c33e1d384521e2bca1a6d","abstract_canon_sha256":"a21cff7ea39e01059a5885f88cbb20eb7e02e2acef476106236fba7f687490f2"},"schema_version":"1.0"},"canonical_sha256":"4d76d5a4302103d93be2c69be5e738b1cb0e3322f2c8f4bb7d4154e3a87833b3","source":{"kind":"arxiv","id":"1108.0964","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.0964","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"arxiv_version","alias_value":"1108.0964v3","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.0964","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"pith_short_12","alias_value":"JV3NLJBQEEB5","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"JV3NLJBQEEB5SO7C","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"JV3NLJBQ","created_at":"2026-05-18T12:26:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:JV3NLJBQEEB5SO7CY2N6LZZYWH","target":"record","payload":{"canonical_record":{"source":{"id":"1108.0964","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-08-04T00:25:09Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"40a6e9985213cdd6b82d3e2b320978dffcd0e471549c33e1d384521e2bca1a6d","abstract_canon_sha256":"a21cff7ea39e01059a5885f88cbb20eb7e02e2acef476106236fba7f687490f2"},"schema_version":"1.0"},"canonical_sha256":"4d76d5a4302103d93be2c69be5e738b1cb0e3322f2c8f4bb7d4154e3a87833b3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:02.646385Z","signature_b64":"EPwSEaeWQy/W3eBF6bKqGjyzB1p4+27RDCPSAVIFiXhYI2A/s50isZWtgFx7r83YJfTw/a/JHEjtiREMTT+gDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d76d5a4302103d93be2c69be5e738b1cb0e3322f2c8f4bb7d4154e3a87833b3","last_reissued_at":"2026-05-18T03:23:02.645608Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:02.645608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1108.0964","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":"2026-05-18T03:23:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jr9fJLQ9waiRyIL5fDri32c/GkhLTjWO2pByEOmF8d0P5utIlWgDiv8j9QAQDyT0sbY65Tan3tyhLAnBTL75Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:36.398727Z"},"content_sha256":"54a9616640d19ae6492513ff6b819358f1bc39f3961f669a409d7ab92aa11a9c","schema_version":"1.0","event_id":"sha256:54a9616640d19ae6492513ff6b819358f1bc39f3961f669a409d7ab92aa11a9c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:JV3NLJBQEEB5SO7CY2N6LZZYWH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Residual Symmetries for Neutrino Mixing with a Large theta_13 and Nearly Maximal delta_D","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Duane A. Dicus, Shao-Feng Ge, Wayne W. Repko","submitted_at":"2011-08-04T00:25:09Z","abstract_excerpt":"The residual Z^s_2(k) and bar Z^s_2(k) symmetries induce a direct and unique phenomenological relation with theta_x (= theta_13) expressed in terms of the other two mixing angles, theta_s (= theta_12) and theta_a (= theta_23), and the Dirac CP phase delta_D. Z^s_2(k) predicts a theta_x probability distribution centered around 3^o ~ 6^o with an uncertainty of 2^o to 4^o while those from bar Z^s_2(k) are approximately a factor of two larger. Either result fits the T2K, MINOS and Double CHOOZ measurements. Alternately a prediction for the Dirac CP phase delta_D results in a peak at +-74^o (+-106^"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.0964","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":"2026-05-18T03:23:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IfMuYlnZDqOScqPrgHWCYr9kcfiypyhGYBBts5MyFxx4Zfa6Dq3F70s4PyCtA7ut/uMjvcQgUkYIIAitHMJKBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T23:05:36.399524Z"},"content_sha256":"01553422e4e8be654c483027d3b88e4186d648a28a41c3072e4b4e76d6c4edfc","schema_version":"1.0","event_id":"sha256:01553422e4e8be654c483027d3b88e4186d648a28a41c3072e4b4e76d6c4edfc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JV3NLJBQEEB5SO7CY2N6LZZYWH/bundle.json","state_url":"https://pith.science/pith/JV3NLJBQEEB5SO7CY2N6LZZYWH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JV3NLJBQEEB5SO7CY2N6LZZYWH/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":"2026-08-04T23:05:36Z","links":{"resolver":"https://pith.science/pith/JV3NLJBQEEB5SO7CY2N6LZZYWH","bundle":"https://pith.science/pith/JV3NLJBQEEB5SO7CY2N6LZZYWH/bundle.json","state":"https://pith.science/pith/JV3NLJBQEEB5SO7CY2N6LZZYWH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JV3NLJBQEEB5SO7CY2N6LZZYWH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:JV3NLJBQEEB5SO7CY2N6LZZYWH","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":"a21cff7ea39e01059a5885f88cbb20eb7e02e2acef476106236fba7f687490f2","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-08-04T00:25:09Z","title_canon_sha256":"40a6e9985213cdd6b82d3e2b320978dffcd0e471549c33e1d384521e2bca1a6d"},"schema_version":"1.0","source":{"id":"1108.0964","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.0964","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"arxiv_version","alias_value":"1108.0964v3","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.0964","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"pith_short_12","alias_value":"JV3NLJBQEEB5","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"JV3NLJBQEEB5SO7C","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"JV3NLJBQ","created_at":"2026-05-18T12:26:32Z"}],"graph_snapshots":[{"event_id":"sha256:01553422e4e8be654c483027d3b88e4186d648a28a41c3072e4b4e76d6c4edfc","target":"graph","created_at":"2026-05-18T03:23:02Z","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 residual Z^s_2(k) and bar Z^s_2(k) symmetries induce a direct and unique phenomenological relation with theta_x (= theta_13) expressed in terms of the other two mixing angles, theta_s (= theta_12) and theta_a (= theta_23), and the Dirac CP phase delta_D. Z^s_2(k) predicts a theta_x probability distribution centered around 3^o ~ 6^o with an uncertainty of 2^o to 4^o while those from bar Z^s_2(k) are approximately a factor of two larger. Either result fits the T2K, MINOS and Double CHOOZ measurements. Alternately a prediction for the Dirac CP phase delta_D results in a peak at +-74^o (+-106^","authors_text":"Duane A. Dicus, Shao-Feng Ge, Wayne W. Repko","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-08-04T00:25:09Z","title":"Residual Symmetries for Neutrino Mixing with a Large theta_13 and Nearly Maximal delta_D"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.0964","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":"sha256:54a9616640d19ae6492513ff6b819358f1bc39f3961f669a409d7ab92aa11a9c","target":"record","created_at":"2026-05-18T03:23:02Z","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":"a21cff7ea39e01059a5885f88cbb20eb7e02e2acef476106236fba7f687490f2","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-08-04T00:25:09Z","title_canon_sha256":"40a6e9985213cdd6b82d3e2b320978dffcd0e471549c33e1d384521e2bca1a6d"},"schema_version":"1.0","source":{"id":"1108.0964","kind":"arxiv","version":3}},"canonical_sha256":"4d76d5a4302103d93be2c69be5e738b1cb0e3322f2c8f4bb7d4154e3a87833b3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4d76d5a4302103d93be2c69be5e738b1cb0e3322f2c8f4bb7d4154e3a87833b3","first_computed_at":"2026-05-18T03:23:02.645608Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:23:02.645608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EPwSEaeWQy/W3eBF6bKqGjyzB1p4+27RDCPSAVIFiXhYI2A/s50isZWtgFx7r83YJfTw/a/JHEjtiREMTT+gDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:23:02.646385Z","signed_message":"canonical_sha256_bytes"},"source_id":"1108.0964","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:54a9616640d19ae6492513ff6b819358f1bc39f3961f669a409d7ab92aa11a9c","sha256:01553422e4e8be654c483027d3b88e4186d648a28a41c3072e4b4e76d6c4edfc"],"state_sha256":"abb7512ef107f91ce06e8a9d627aef4a29de5314a90aacdf23d60e63c9b2dedb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lY5oFpu2sWMotMb2eb3nITLBxgMG+zE4H+qx9R5PITv0RmoF+LW9S3f2jhMOhSOmt4NXdBB/BkJHAXjUMGcDBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T23:05:36.406487Z","bundle_sha256":"15d585ec8bec8cb9506e5672c038c668e5b63d1590c164edb7b42dc039dd0d29"}}