{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:ILRDNBWBDB3Y7FHANUKWCQ4TFY","short_pith_number":"pith:ILRDNBWB","canonical_record":{"source":{"id":"2109.15085","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-09-30T12:54:22Z","cross_cats_sorted":[],"title_canon_sha256":"753a27ac14c3ea91b3538a05c4f8706fc4b2fbfe47945f05e7cd1010deb66e24","abstract_canon_sha256":"fff0882bb3e377596e2aecb08f4f68bd2d9f048cf6d4a98a59d63b4139844faa"},"schema_version":"1.0"},"canonical_sha256":"42e23686c118778f94e06d156143932e3acfb6fbcdbd8cb070acc74b77a967fa","source":{"kind":"arxiv","id":"2109.15085","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2109.15085","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"arxiv_version","alias_value":"2109.15085v3","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2109.15085","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"pith_short_12","alias_value":"ILRDNBWBDB3Y","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"ILRDNBWBDB3Y7FHA","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"ILRDNBWB","created_at":"2026-07-05T05:32:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:ILRDNBWBDB3Y7FHANUKWCQ4TFY","target":"record","payload":{"canonical_record":{"source":{"id":"2109.15085","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-09-30T12:54:22Z","cross_cats_sorted":[],"title_canon_sha256":"753a27ac14c3ea91b3538a05c4f8706fc4b2fbfe47945f05e7cd1010deb66e24","abstract_canon_sha256":"fff0882bb3e377596e2aecb08f4f68bd2d9f048cf6d4a98a59d63b4139844faa"},"schema_version":"1.0"},"canonical_sha256":"42e23686c118778f94e06d156143932e3acfb6fbcdbd8cb070acc74b77a967fa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:32:43.142493Z","signature_b64":"buhmUWX7nMpa951qZOaHvapjr2sfm+sYCREpxEYDnbk8zYcFjc3B2IGIKNn9P71bjYAF68LxtKi/NpfefaSODQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42e23686c118778f94e06d156143932e3acfb6fbcdbd8cb070acc74b77a967fa","last_reissued_at":"2026-07-05T05:32:43.141993Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:32:43.141993Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2109.15085","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":"2026-07-05T05:32:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nHazVZt9xh0G5CLvAuAoRAAnpriPk23JwxZjqRuoC9UYnusYnfhiu8VM6BM5BOgc7Yznvh2cvSiRhzrsZ8DsCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T19:59:44.628339Z"},"content_sha256":"b96ced9f87d8374aba245816ad2ab8c7fcac26bf5680a6fd2bd93c7841b46eab","schema_version":"1.0","event_id":"sha256:b96ced9f87d8374aba245816ad2ab8c7fcac26bf5680a6fd2bd93c7841b46eab"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:ILRDNBWBDB3Y7FHANUKWCQ4TFY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electric dipole moments at one-loop in the dimension-6 SMEFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andreas Weiler, Elena Venturini, Jonathan Kley, Tobias Theil","submitted_at":"2021-09-30T12:54:22Z","abstract_excerpt":"In this paper we present the complete expressions of the lepton and neutron electric dipole moments (EDMs) in the Standard Model Effective Field Theory (SMEFT), up to 1-loop and dimension-6 level and including both RG running contributions and finite corrections. The latter play a fundamental role in the cases of operators that do not renormalize the dipoles, but there are also classes of operators for which they provide an important fraction, $10-20\\%$, of the total 1-loop contribution, if the new physics scale is around $\\Lambda=5$ TeV. We present the full set of bounds on each individual Wi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2109.15085","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2109.15085/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":"2026-07-05T05:32:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Fjd3Y7plIlf7wiTD3BO3nLZAZmX5Du5JO0u8Hk/6/kA4H0MNfGVBpS9OPtcC+xQHfm1jVjBSjbSi2c4hrf/AAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T19:59:44.629249Z"},"content_sha256":"d01e8f1fa4fef8e8fd092e31a4454c4426a8d1f6c6b5bf1347611b2492ea97c0","schema_version":"1.0","event_id":"sha256:d01e8f1fa4fef8e8fd092e31a4454c4426a8d1f6c6b5bf1347611b2492ea97c0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ILRDNBWBDB3Y7FHANUKWCQ4TFY/bundle.json","state_url":"https://pith.science/pith/ILRDNBWBDB3Y7FHANUKWCQ4TFY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ILRDNBWBDB3Y7FHANUKWCQ4TFY/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":"2026-08-11T19:59:44Z","links":{"resolver":"https://pith.science/pith/ILRDNBWBDB3Y7FHANUKWCQ4TFY","bundle":"https://pith.science/pith/ILRDNBWBDB3Y7FHANUKWCQ4TFY/bundle.json","state":"https://pith.science/pith/ILRDNBWBDB3Y7FHANUKWCQ4TFY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ILRDNBWBDB3Y7FHANUKWCQ4TFY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:ILRDNBWBDB3Y7FHANUKWCQ4TFY","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":"fff0882bb3e377596e2aecb08f4f68bd2d9f048cf6d4a98a59d63b4139844faa","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-09-30T12:54:22Z","title_canon_sha256":"753a27ac14c3ea91b3538a05c4f8706fc4b2fbfe47945f05e7cd1010deb66e24"},"schema_version":"1.0","source":{"id":"2109.15085","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2109.15085","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"arxiv_version","alias_value":"2109.15085v3","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2109.15085","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"pith_short_12","alias_value":"ILRDNBWBDB3Y","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"ILRDNBWBDB3Y7FHA","created_at":"2026-07-05T05:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"ILRDNBWB","created_at":"2026-07-05T05:32:43Z"}],"graph_snapshots":[{"event_id":"sha256:d01e8f1fa4fef8e8fd092e31a4454c4426a8d1f6c6b5bf1347611b2492ea97c0","target":"graph","created_at":"2026-07-05T05:32:43Z","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/2109.15085/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this paper we present the complete expressions of the lepton and neutron electric dipole moments (EDMs) in the Standard Model Effective Field Theory (SMEFT), up to 1-loop and dimension-6 level and including both RG running contributions and finite corrections. The latter play a fundamental role in the cases of operators that do not renormalize the dipoles, but there are also classes of operators for which they provide an important fraction, $10-20\\%$, of the total 1-loop contribution, if the new physics scale is around $\\Lambda=5$ TeV. We present the full set of bounds on each individual Wi","authors_text":"Andreas Weiler, Elena Venturini, Jonathan Kley, Tobias Theil","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-09-30T12:54:22Z","title":"Electric dipole moments at one-loop in the dimension-6 SMEFT"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2109.15085","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:b96ced9f87d8374aba245816ad2ab8c7fcac26bf5680a6fd2bd93c7841b46eab","target":"record","created_at":"2026-07-05T05:32:43Z","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":"fff0882bb3e377596e2aecb08f4f68bd2d9f048cf6d4a98a59d63b4139844faa","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-09-30T12:54:22Z","title_canon_sha256":"753a27ac14c3ea91b3538a05c4f8706fc4b2fbfe47945f05e7cd1010deb66e24"},"schema_version":"1.0","source":{"id":"2109.15085","kind":"arxiv","version":3}},"canonical_sha256":"42e23686c118778f94e06d156143932e3acfb6fbcdbd8cb070acc74b77a967fa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"42e23686c118778f94e06d156143932e3acfb6fbcdbd8cb070acc74b77a967fa","first_computed_at":"2026-07-05T05:32:43.141993Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:32:43.141993Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"buhmUWX7nMpa951qZOaHvapjr2sfm+sYCREpxEYDnbk8zYcFjc3B2IGIKNn9P71bjYAF68LxtKi/NpfefaSODQ==","signature_status":"signed_v1","signed_at":"2026-07-05T05:32:43.142493Z","signed_message":"canonical_sha256_bytes"},"source_id":"2109.15085","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b96ced9f87d8374aba245816ad2ab8c7fcac26bf5680a6fd2bd93c7841b46eab","sha256:d01e8f1fa4fef8e8fd092e31a4454c4426a8d1f6c6b5bf1347611b2492ea97c0"],"state_sha256":"ba2f6a3dec8344e57c3e3ea1a1cdd2786ff3390fa688b5d262e02dc1988fd25d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"whD+PFS7ziLUKE/6RiVjEbR4iQKOgF8dKrKZs/nEFeZaAdjqdR6v1qxYE4FgZhsxgMAxCNytctBwEbE0KLrIDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T19:59:44.654757Z","bundle_sha256":"f81e9a4d70a91d2435eacc7d0fd763cbf70077f134ecaeb59cda799eba5b6fdc"}}