{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:7ERK44FKDKSUIKWQSGYXZPUPDT","short_pith_number":"pith:7ERK44FK","canonical_record":{"source":{"id":"2207.08856","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-07-18T18:09:58Z","cross_cats_sorted":[],"title_canon_sha256":"9779293eac57f7d5e7d079a8e56211bf63ce904b0102cafb4565a5419898a6d6","abstract_canon_sha256":"a34cf56e31a279cb65f565e75e6774006675a370c5f46eb776816402f63dc504"},"schema_version":"1.0"},"canonical_sha256":"f922ae70aa1aa5442ad091b17cbe8f1cf48cabbbd9a28aafbebe7986819c0b28","source":{"kind":"arxiv","id":"2207.08856","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2207.08856","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"arxiv_version","alias_value":"2207.08856v2","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.08856","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"pith_short_12","alias_value":"7ERK44FKDKSU","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"pith_short_16","alias_value":"7ERK44FKDKSUIKWQ","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"pith_short_8","alias_value":"7ERK44FK","created_at":"2026-07-05T05:57:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:7ERK44FKDKSUIKWQSGYXZPUPDT","target":"record","payload":{"canonical_record":{"source":{"id":"2207.08856","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-07-18T18:09:58Z","cross_cats_sorted":[],"title_canon_sha256":"9779293eac57f7d5e7d079a8e56211bf63ce904b0102cafb4565a5419898a6d6","abstract_canon_sha256":"a34cf56e31a279cb65f565e75e6774006675a370c5f46eb776816402f63dc504"},"schema_version":"1.0"},"canonical_sha256":"f922ae70aa1aa5442ad091b17cbe8f1cf48cabbbd9a28aafbebe7986819c0b28","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:57:55.171212Z","signature_b64":"z1C2o/MITnrIaLL1BF9vyOO46cAdNtG0ZW6+wSPjNo96mp/fWjNaV6RnvwGjUa5UvnQHvJCsvWFHirbF07G9DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f922ae70aa1aa5442ad091b17cbe8f1cf48cabbbd9a28aafbebe7986819c0b28","last_reissued_at":"2026-07-05T05:57:55.170804Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:57:55.170804Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2207.08856","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":"2026-07-05T05:57:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rNq8+Lvn+ncc8iHztApFsgAbExLyHqzMtL6xq/cQFiGI/se1J4dJaVFnAyrPpUglCmpkef5+skAr7qLzuEFkDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T13:45:44.864785Z"},"content_sha256":"da092165e292f8348bc9a2645c4e0f1f866eb81abb16e3186033d4c51695b147","schema_version":"1.0","event_id":"sha256:da092165e292f8348bc9a2645c4e0f1f866eb81abb16e3186033d4c51695b147"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:7ERK44FKDKSUIKWQSGYXZPUPDT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dimension-8 SMEFT Matching Conditions for the Low-Energy Effective Field Theory","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David London, Jacky Kumar, Serge Hamoudou","submitted_at":"2022-07-18T18:09:58Z","abstract_excerpt":"In particle physics, the modern view is to categorize things in terms of effective field theories (EFTs). Above the weak scale, we have the SMEFT, formed when the heavy new physics (NP) is integrated out, and for which the Standard Model (SM) is the leading part. Below $M_W$, we have the LEFT (low-energy EFT), formed when the heavy SM particles ($W^\\pm$, $Z^0$, $H$, $t$) are also integrated out. In order to determine how low-energy measurements depend on the underlying NP, it is necessary to compute the matching conditions of LEFT operators to SMEFT operators. These matching conditions have be"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.08856","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/2207.08856/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":"2026-07-05T05:57:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jBgpVDiFbFTn02v2D4SkE9OsxYQZgjgL1/vVDlsrL9VkfZ/niEWtGlCsS/7NqtvYVk+i/N9Bf8+fV7P0HUhVBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T13:45:44.865295Z"},"content_sha256":"22f1159ccc38e5ecc4422088d531882126781d1dde2da9e4ba07a7335c979295","schema_version":"1.0","event_id":"sha256:22f1159ccc38e5ecc4422088d531882126781d1dde2da9e4ba07a7335c979295"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7ERK44FKDKSUIKWQSGYXZPUPDT/bundle.json","state_url":"https://pith.science/pith/7ERK44FKDKSUIKWQSGYXZPUPDT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7ERK44FKDKSUIKWQSGYXZPUPDT/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":"2026-08-05T13:45:44Z","links":{"resolver":"https://pith.science/pith/7ERK44FKDKSUIKWQSGYXZPUPDT","bundle":"https://pith.science/pith/7ERK44FKDKSUIKWQSGYXZPUPDT/bundle.json","state":"https://pith.science/pith/7ERK44FKDKSUIKWQSGYXZPUPDT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7ERK44FKDKSUIKWQSGYXZPUPDT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:7ERK44FKDKSUIKWQSGYXZPUPDT","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":"a34cf56e31a279cb65f565e75e6774006675a370c5f46eb776816402f63dc504","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-07-18T18:09:58Z","title_canon_sha256":"9779293eac57f7d5e7d079a8e56211bf63ce904b0102cafb4565a5419898a6d6"},"schema_version":"1.0","source":{"id":"2207.08856","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2207.08856","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"arxiv_version","alias_value":"2207.08856v2","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.08856","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"pith_short_12","alias_value":"7ERK44FKDKSU","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"pith_short_16","alias_value":"7ERK44FKDKSUIKWQ","created_at":"2026-07-05T05:57:55Z"},{"alias_kind":"pith_short_8","alias_value":"7ERK44FK","created_at":"2026-07-05T05:57:55Z"}],"graph_snapshots":[{"event_id":"sha256:22f1159ccc38e5ecc4422088d531882126781d1dde2da9e4ba07a7335c979295","target":"graph","created_at":"2026-07-05T05:57:55Z","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/2207.08856/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In particle physics, the modern view is to categorize things in terms of effective field theories (EFTs). Above the weak scale, we have the SMEFT, formed when the heavy new physics (NP) is integrated out, and for which the Standard Model (SM) is the leading part. Below $M_W$, we have the LEFT (low-energy EFT), formed when the heavy SM particles ($W^\\pm$, $Z^0$, $H$, $t$) are also integrated out. In order to determine how low-energy measurements depend on the underlying NP, it is necessary to compute the matching conditions of LEFT operators to SMEFT operators. These matching conditions have be","authors_text":"David London, Jacky Kumar, Serge Hamoudou","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-07-18T18:09:58Z","title":"Dimension-8 SMEFT Matching Conditions for the Low-Energy Effective Field Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.08856","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:da092165e292f8348bc9a2645c4e0f1f866eb81abb16e3186033d4c51695b147","target":"record","created_at":"2026-07-05T05:57:55Z","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":"a34cf56e31a279cb65f565e75e6774006675a370c5f46eb776816402f63dc504","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-07-18T18:09:58Z","title_canon_sha256":"9779293eac57f7d5e7d079a8e56211bf63ce904b0102cafb4565a5419898a6d6"},"schema_version":"1.0","source":{"id":"2207.08856","kind":"arxiv","version":2}},"canonical_sha256":"f922ae70aa1aa5442ad091b17cbe8f1cf48cabbbd9a28aafbebe7986819c0b28","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f922ae70aa1aa5442ad091b17cbe8f1cf48cabbbd9a28aafbebe7986819c0b28","first_computed_at":"2026-07-05T05:57:55.170804Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:57:55.170804Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"z1C2o/MITnrIaLL1BF9vyOO46cAdNtG0ZW6+wSPjNo96mp/fWjNaV6RnvwGjUa5UvnQHvJCsvWFHirbF07G9DQ==","signature_status":"signed_v1","signed_at":"2026-07-05T05:57:55.171212Z","signed_message":"canonical_sha256_bytes"},"source_id":"2207.08856","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:da092165e292f8348bc9a2645c4e0f1f866eb81abb16e3186033d4c51695b147","sha256:22f1159ccc38e5ecc4422088d531882126781d1dde2da9e4ba07a7335c979295"],"state_sha256":"62a479e8706277a34127fc88fbc4a2bde525eb35f23bb5d9c1baa481b2adc2fb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NrnfmvzFzLDwjkPHGe5zgTE/GD6fAABCG36PLkGVSDvPl6UNCnoijQBw1AWu8S3NRbjwntuUuVqcw/ly9/ExDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T13:45:44.869225Z","bundle_sha256":"53e6623fd44f97ca5ac05b4a2d1ad7140f1de394cf21bbcae1b42c17d0b5be7f"}}