{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:AECAMBRIKCQ722MI7ULWK5OPCD","short_pith_number":"pith:AECAMBRI","canonical_record":{"source":{"id":"2203.11224","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-03-21T18:00:01Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"c8bf156120bc5e5782b515e65c13907826c84840e5bc46979e6525c1686538bb","abstract_canon_sha256":"0faa1ae842ac158e9cfd0fe5c4179e6a34654b4970b1b2b4cb3db7f8e2620aeb"},"schema_version":"1.0"},"canonical_sha256":"010406062850a1fd6988fd176575cf10e4aa4226d34ba4b5c3d9ed8e6014c4a8","source":{"kind":"arxiv","id":"2203.11224","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2203.11224","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"arxiv_version","alias_value":"2203.11224v2","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.11224","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"pith_short_12","alias_value":"AECAMBRIKCQ7","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"pith_short_16","alias_value":"AECAMBRIKCQ722MI","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"pith_short_8","alias_value":"AECAMBRI","created_at":"2026-07-05T04:48:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:AECAMBRIKCQ722MI7ULWK5OPCD","target":"record","payload":{"canonical_record":{"source":{"id":"2203.11224","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-03-21T18:00:01Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"c8bf156120bc5e5782b515e65c13907826c84840e5bc46979e6525c1686538bb","abstract_canon_sha256":"0faa1ae842ac158e9cfd0fe5c4179e6a34654b4970b1b2b4cb3db7f8e2620aeb"},"schema_version":"1.0"},"canonical_sha256":"010406062850a1fd6988fd176575cf10e4aa4226d34ba4b5c3d9ed8e6014c4a8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:48:45.149985Z","signature_b64":"yp2t4geuuW4yLVsG0986H3XF2h1sPgyb/UBnz52Kz+VBtAW4IMyZGudlVYV+xEE0omWKhI4D/oHRTWAw8u6NDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"010406062850a1fd6988fd176575cf10e4aa4226d34ba4b5c3d9ed8e6014c4a8","last_reissued_at":"2026-07-05T04:48:45.149577Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:48:45.149577Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2203.11224","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":"2026-07-05T04:48:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rKHhlc3Ggzng4ERdclDX4BB5RsPaQpVRMflI9bbMZ6xnjg3jnt1vm6eV9j0qD3Rlsyeblhv6+BsBS2c8vwDNAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T04:54:00.360602Z"},"content_sha256":"b91d6447d37b6755fe0c9825a23592f39550ce3e8105038f521f5801ffad36f9","schema_version":"1.0","event_id":"sha256:b91d6447d37b6755fe0c9825a23592f39550ce3e8105038f521f5801ffad36f9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:AECAMBRIKCQ722MI7ULWK5OPCD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"NLO QCD Renormalization Group Evolution for Non-Leptonic $\\Delta F=2$ Transitions in the SMEFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Andrzej J. Buras, Jacky Kumar, Jason Aebischer","submitted_at":"2022-03-21T18:00:01Z","abstract_excerpt":"We present for the first time NLO QCD Renormalization Group (RG) evolution matrices for non-leptonic $\\Delta F=2$ transitions in the Standard Model Effective Field Theory (SMEFT). To this end we transform first the known two-loop QCD anomalous dimension matrices (ADMs) of the BSM operators in the so-called BMU basis into the ones in the common Weak Effective Theory (WET) basis (the so-called JMS basis) for which tree-level and one-loop matching to the SMEFT are already known. This allows us subsequently to find the two-loop QCD ADMs for the SMEFT non-leptonic $\\Delta F=2$ operators in the Wars"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.11224","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2203.11224/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T04:48:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eT5QgRQojpyQE8HbuZmd/0Hg0FLe/hyV2Z1uNa/eJHz4+1YjsZvuqm66CEGtpSX3p9i0nY7ynxDGMle11awuCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T04:54:00.360978Z"},"content_sha256":"bf56ebedd1c4c02fe26e5560f815b380423dfce3f2cd88b105349dc501eb13f0","schema_version":"1.0","event_id":"sha256:bf56ebedd1c4c02fe26e5560f815b380423dfce3f2cd88b105349dc501eb13f0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AECAMBRIKCQ722MI7ULWK5OPCD/bundle.json","state_url":"https://pith.science/pith/AECAMBRIKCQ722MI7ULWK5OPCD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AECAMBRIKCQ722MI7ULWK5OPCD/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":"2026-07-09T04:54:00Z","links":{"resolver":"https://pith.science/pith/AECAMBRIKCQ722MI7ULWK5OPCD","bundle":"https://pith.science/pith/AECAMBRIKCQ722MI7ULWK5OPCD/bundle.json","state":"https://pith.science/pith/AECAMBRIKCQ722MI7ULWK5OPCD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AECAMBRIKCQ722MI7ULWK5OPCD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:AECAMBRIKCQ722MI7ULWK5OPCD","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":"0faa1ae842ac158e9cfd0fe5c4179e6a34654b4970b1b2b4cb3db7f8e2620aeb","cross_cats_sorted":["hep-ex","hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-03-21T18:00:01Z","title_canon_sha256":"c8bf156120bc5e5782b515e65c13907826c84840e5bc46979e6525c1686538bb"},"schema_version":"1.0","source":{"id":"2203.11224","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2203.11224","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"arxiv_version","alias_value":"2203.11224v2","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.11224","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"pith_short_12","alias_value":"AECAMBRIKCQ7","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"pith_short_16","alias_value":"AECAMBRIKCQ722MI","created_at":"2026-07-05T04:48:45Z"},{"alias_kind":"pith_short_8","alias_value":"AECAMBRI","created_at":"2026-07-05T04:48:45Z"}],"graph_snapshots":[{"event_id":"sha256:bf56ebedd1c4c02fe26e5560f815b380423dfce3f2cd88b105349dc501eb13f0","target":"graph","created_at":"2026-07-05T04:48:45Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2203.11224/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present for the first time NLO QCD Renormalization Group (RG) evolution matrices for non-leptonic $\\Delta F=2$ transitions in the Standard Model Effective Field Theory (SMEFT). To this end we transform first the known two-loop QCD anomalous dimension matrices (ADMs) of the BSM operators in the so-called BMU basis into the ones in the common Weak Effective Theory (WET) basis (the so-called JMS basis) for which tree-level and one-loop matching to the SMEFT are already known. This allows us subsequently to find the two-loop QCD ADMs for the SMEFT non-leptonic $\\Delta F=2$ operators in the Wars","authors_text":"Andrzej J. Buras, Jacky Kumar, Jason Aebischer","cross_cats":["hep-ex","hep-lat"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-03-21T18:00:01Z","title":"NLO QCD Renormalization Group Evolution for Non-Leptonic $\\Delta F=2$ Transitions in the SMEFT"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.11224","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:b91d6447d37b6755fe0c9825a23592f39550ce3e8105038f521f5801ffad36f9","target":"record","created_at":"2026-07-05T04:48:45Z","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":"0faa1ae842ac158e9cfd0fe5c4179e6a34654b4970b1b2b4cb3db7f8e2620aeb","cross_cats_sorted":["hep-ex","hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-03-21T18:00:01Z","title_canon_sha256":"c8bf156120bc5e5782b515e65c13907826c84840e5bc46979e6525c1686538bb"},"schema_version":"1.0","source":{"id":"2203.11224","kind":"arxiv","version":2}},"canonical_sha256":"010406062850a1fd6988fd176575cf10e4aa4226d34ba4b5c3d9ed8e6014c4a8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"010406062850a1fd6988fd176575cf10e4aa4226d34ba4b5c3d9ed8e6014c4a8","first_computed_at":"2026-07-05T04:48:45.149577Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:48:45.149577Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yp2t4geuuW4yLVsG0986H3XF2h1sPgyb/UBnz52Kz+VBtAW4IMyZGudlVYV+xEE0omWKhI4D/oHRTWAw8u6NDg==","signature_status":"signed_v1","signed_at":"2026-07-05T04:48:45.149985Z","signed_message":"canonical_sha256_bytes"},"source_id":"2203.11224","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b91d6447d37b6755fe0c9825a23592f39550ce3e8105038f521f5801ffad36f9","sha256:bf56ebedd1c4c02fe26e5560f815b380423dfce3f2cd88b105349dc501eb13f0"],"state_sha256":"2bd812cc341836aa40b32571ea2a389da26d73ef12ebb1c058ac995b6ba756ba"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PB6mPBc50cepqCxiIsNwmwXtFa20BiqsdywqNXXl0C4Q/xbUS2OpvfuJ4KxMfdfcia6WRQYW8bYhgNiSQk9oDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-09T04:54:00.363018Z","bundle_sha256":"c5d6d1dd352dbb9e8ef834d6cc204471b03434a161500e13cd19f41e3ed7e933"}}