{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:3IFZA7HKIG4YFSNPGMUOIO66CL","short_pith_number":"pith:3IFZA7HK","canonical_record":{"source":{"id":"1407.7044","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-25T20:07:48Z","cross_cats_sorted":[],"title_canon_sha256":"4f79eb55c6c3caf1cb6d4b461fcba295116661e86556494a02fbc528f81aaa82","abstract_canon_sha256":"d2e5f7127d72b4fcc6f6815ad8bedbca35336e5e6d0d9cc6a3d3491c13f3fd64"},"schema_version":"1.0"},"canonical_sha256":"da0b907cea41b982c9af3328e43bde12f5d37a51304c3cd7d2114d13a8016385","source":{"kind":"arxiv","id":"1407.7044","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.7044","created_at":"2026-05-18T02:31:11Z"},{"alias_kind":"arxiv_version","alias_value":"1407.7044v1","created_at":"2026-05-18T02:31:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.7044","created_at":"2026-05-18T02:31:11Z"},{"alias_kind":"pith_short_12","alias_value":"3IFZA7HKIG4Y","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"3IFZA7HKIG4YFSNP","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"3IFZA7HK","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:3IFZA7HKIG4YFSNPGMUOIO66CL","target":"record","payload":{"canonical_record":{"source":{"id":"1407.7044","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-25T20:07:48Z","cross_cats_sorted":[],"title_canon_sha256":"4f79eb55c6c3caf1cb6d4b461fcba295116661e86556494a02fbc528f81aaa82","abstract_canon_sha256":"d2e5f7127d72b4fcc6f6815ad8bedbca35336e5e6d0d9cc6a3d3491c13f3fd64"},"schema_version":"1.0"},"canonical_sha256":"da0b907cea41b982c9af3328e43bde12f5d37a51304c3cd7d2114d13a8016385","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:31:11.353030Z","signature_b64":"Lr+y+epn76qb4rZR9aSMYRfUEXn7QfXN0SH48zGdqnNolEvkeM7A/81LRPWBix6ymIilALiPTQxr3mk44pQFCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"da0b907cea41b982c9af3328e43bde12f5d37a51304c3cd7d2114d13a8016385","last_reissued_at":"2026-05-18T02:31:11.352419Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:31:11.352419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.7044","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:31:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8YGBowMsZkILBTKWL6giyne/JWViJxF5/HiwbQrn89sSC2JR36VEmJoq2K9eaoves3of8KgMvQPMopDSAMmjBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T14:36:27.653067Z"},"content_sha256":"cf2297fb5244cf38676572db275546957f315d99c3762c13977bff4c2f6a9368","schema_version":"1.0","event_id":"sha256:cf2297fb5244cf38676572db275546957f315d99c3762c13977bff4c2f6a9368"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:3IFZA7HKIG4YFSNPGMUOIO66CL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"$SU(2)\\times U(1)$ gauge invariance and the shape of new physics in rare $B$ decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Benjamin Grinstein, Jorge Martin Camalich, Rodrigo Alonso","submitted_at":"2014-07-25T20:07:48Z","abstract_excerpt":"New physics effects in $B$ decays are routinely modeled through operators invariant under the strong and electromagnetic gauge symmetries. Assuming the scale for new physics is well above the electro-weak scale, we further require invariance under the full Standard-Model gauge symmetry group. Retaining up to dimension-6 operators, we unveil new constraints between different new-physics operators that are assumed to be independent in the standard phenomenological analyses. We illustrate this approach by analyzing the constraints on new physics from rare $B_{q}$ (semi-)leptonic decays."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.7044","kind":"arxiv","version":1},"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":"2026-05-18T02:31:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HASwJyQ51e9EBd2MM75nsOqYU/8ZUH6vdOwD3O1Ut6CVqHJEZLbUdAP0XTNMyN297XVkHogXyVh8JlcLJPjLDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T14:36:27.653756Z"},"content_sha256":"cac6b84503f1367024c39dfa587f697db8125075deba6ebe1ad047580c7cfb47","schema_version":"1.0","event_id":"sha256:cac6b84503f1367024c39dfa587f697db8125075deba6ebe1ad047580c7cfb47"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3IFZA7HKIG4YFSNPGMUOIO66CL/bundle.json","state_url":"https://pith.science/pith/3IFZA7HKIG4YFSNPGMUOIO66CL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3IFZA7HKIG4YFSNPGMUOIO66CL/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":"2026-05-24T14:36:27Z","links":{"resolver":"https://pith.science/pith/3IFZA7HKIG4YFSNPGMUOIO66CL","bundle":"https://pith.science/pith/3IFZA7HKIG4YFSNPGMUOIO66CL/bundle.json","state":"https://pith.science/pith/3IFZA7HKIG4YFSNPGMUOIO66CL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3IFZA7HKIG4YFSNPGMUOIO66CL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:3IFZA7HKIG4YFSNPGMUOIO66CL","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":"d2e5f7127d72b4fcc6f6815ad8bedbca35336e5e6d0d9cc6a3d3491c13f3fd64","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-25T20:07:48Z","title_canon_sha256":"4f79eb55c6c3caf1cb6d4b461fcba295116661e86556494a02fbc528f81aaa82"},"schema_version":"1.0","source":{"id":"1407.7044","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.7044","created_at":"2026-05-18T02:31:11Z"},{"alias_kind":"arxiv_version","alias_value":"1407.7044v1","created_at":"2026-05-18T02:31:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.7044","created_at":"2026-05-18T02:31:11Z"},{"alias_kind":"pith_short_12","alias_value":"3IFZA7HKIG4Y","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"3IFZA7HKIG4YFSNP","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"3IFZA7HK","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:cac6b84503f1367024c39dfa587f697db8125075deba6ebe1ad047580c7cfb47","target":"graph","created_at":"2026-05-18T02:31:11Z","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":"New physics effects in $B$ decays are routinely modeled through operators invariant under the strong and electromagnetic gauge symmetries. Assuming the scale for new physics is well above the electro-weak scale, we further require invariance under the full Standard-Model gauge symmetry group. Retaining up to dimension-6 operators, we unveil new constraints between different new-physics operators that are assumed to be independent in the standard phenomenological analyses. We illustrate this approach by analyzing the constraints on new physics from rare $B_{q}$ (semi-)leptonic decays.","authors_text":"Benjamin Grinstein, Jorge Martin Camalich, Rodrigo Alonso","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-25T20:07:48Z","title":"$SU(2)\\times U(1)$ gauge invariance and the shape of new physics in rare $B$ decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.7044","kind":"arxiv","version":1},"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:cf2297fb5244cf38676572db275546957f315d99c3762c13977bff4c2f6a9368","target":"record","created_at":"2026-05-18T02:31:11Z","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":"d2e5f7127d72b4fcc6f6815ad8bedbca35336e5e6d0d9cc6a3d3491c13f3fd64","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-25T20:07:48Z","title_canon_sha256":"4f79eb55c6c3caf1cb6d4b461fcba295116661e86556494a02fbc528f81aaa82"},"schema_version":"1.0","source":{"id":"1407.7044","kind":"arxiv","version":1}},"canonical_sha256":"da0b907cea41b982c9af3328e43bde12f5d37a51304c3cd7d2114d13a8016385","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"da0b907cea41b982c9af3328e43bde12f5d37a51304c3cd7d2114d13a8016385","first_computed_at":"2026-05-18T02:31:11.352419Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:31:11.352419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Lr+y+epn76qb4rZR9aSMYRfUEXn7QfXN0SH48zGdqnNolEvkeM7A/81LRPWBix6ymIilALiPTQxr3mk44pQFCg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:31:11.353030Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.7044","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cf2297fb5244cf38676572db275546957f315d99c3762c13977bff4c2f6a9368","sha256:cac6b84503f1367024c39dfa587f697db8125075deba6ebe1ad047580c7cfb47"],"state_sha256":"56baee56ad073dd86ae4b415bc8c2b05cbb598cf4667f6d936863728311c261e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3tg/2TOxLLiYd1YyD517tFgOfLEEWBT0TJGSoVSsw9iqgjeC70fWZrcVv6oBVldECK8AJKgWbnSj9p5jlY1iDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T14:36:27.657109Z","bundle_sha256":"002a3b6b8753597729359f03b12f066684d11809c2eb1cf6de8550f020463e52"}}