{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:L5MAFEDUX5Z2A5J3BBYJ6Z5CVP","short_pith_number":"pith:L5MAFEDU","canonical_record":{"source":{"id":"1311.4704","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-19T11:40:45Z","cross_cats_sorted":[],"title_canon_sha256":"c743c54732e61952ac5204fd310a99fdebc999ace077464909c11834795f6822","abstract_canon_sha256":"1b612de0710f28c0dd82426a69db4d37d5d696b462ba4c8d388cac572f751a2b"},"schema_version":"1.0"},"canonical_sha256":"5f58029074bf73a0753b08709f67a2abd83dd0882e4f8b3559cb3e4663388fa3","source":{"kind":"arxiv","id":"1311.4704","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.4704","created_at":"2026-05-18T01:16:33Z"},{"alias_kind":"arxiv_version","alias_value":"1311.4704v3","created_at":"2026-05-18T01:16:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.4704","created_at":"2026-05-18T01:16:33Z"},{"alias_kind":"pith_short_12","alias_value":"L5MAFEDUX5Z2","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"L5MAFEDUX5Z2A5J3","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"L5MAFEDU","created_at":"2026-05-18T12:27:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:L5MAFEDUX5Z2A5J3BBYJ6Z5CVP","target":"record","payload":{"canonical_record":{"source":{"id":"1311.4704","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-19T11:40:45Z","cross_cats_sorted":[],"title_canon_sha256":"c743c54732e61952ac5204fd310a99fdebc999ace077464909c11834795f6822","abstract_canon_sha256":"1b612de0710f28c0dd82426a69db4d37d5d696b462ba4c8d388cac572f751a2b"},"schema_version":"1.0"},"canonical_sha256":"5f58029074bf73a0753b08709f67a2abd83dd0882e4f8b3559cb3e4663388fa3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:33.641419Z","signature_b64":"4357vqBzUHryD0t2EGcdXLb7XCvDssSrJL8Ezmm7zJg1qMieQbt6nUiQnwcrD4Fmb33o5nKhrBDahrQGa66fCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f58029074bf73a0753b08709f67a2abd83dd0882e4f8b3559cb3e4663388fa3","last_reissued_at":"2026-05-18T01:16:33.640790Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:33.640790Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1311.4704","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":"2026-05-18T01:16:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"m84AyEPlDVjZU5Y1v7oZclXzlItwfMI3deNcZ0fvNWWdjWfpA0hH6iZbPkX/mQbVby0KB1TCDdkP4lGEdJusCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T20:50:49.912873Z"},"content_sha256":"6de400c26dfa1305bc1034b74653beddf87ebd12d08d69f043f7e459edc9ac52","schema_version":"1.0","event_id":"sha256:6de400c26dfa1305bc1034b74653beddf87ebd12d08d69f043f7e459edc9ac52"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:L5MAFEDUX5Z2A5J3BBYJ6Z5CVP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gauge invariant Barr-Zee type contributions to fermionic EDMs in the two-Higgs doublet models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Junji Hisano, Kohsaku Tobioka, Teppei Kitahara, Tomohiro Abe","submitted_at":"2013-11-19T11:40:45Z","abstract_excerpt":"We calculate all gauge invariant Barr-Zee type contributions to fermionic electric dipole moments (EDMs) in the two-Higgs doublet models (2HDM) with softly broken Z2 symmetry. We start by studying the tensor structure of h to VV' part in the Barr-Zee diagrams, and we calculate the effective couplings in a gauge invariant way by using the pinch technique. Then we calculate all Barr-Zee diagrams relevant for electron and neutron EDMs. We make bounds on the parameter space in type-I, type-II, type-X, and type-Y 2HDMs. The electron and neutron EDMs are complementary to each other in discrimination"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.4704","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":"2026-05-18T01:16:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/btlo6yBIw94j73B3jDezcSzQ6SSV90xaaJqxdKinLgeZS6YzD0nch7BRLvccHfvN92EbwDBxU5sigvfTOMTDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T20:50:49.913549Z"},"content_sha256":"d8598d63f57a9007006636221ded160a8d2ad757aff008dd766613eed37bcd9f","schema_version":"1.0","event_id":"sha256:d8598d63f57a9007006636221ded160a8d2ad757aff008dd766613eed37bcd9f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/L5MAFEDUX5Z2A5J3BBYJ6Z5CVP/bundle.json","state_url":"https://pith.science/pith/L5MAFEDUX5Z2A5J3BBYJ6Z5CVP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/L5MAFEDUX5Z2A5J3BBYJ6Z5CVP/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":"2026-06-05T20:50:49Z","links":{"resolver":"https://pith.science/pith/L5MAFEDUX5Z2A5J3BBYJ6Z5CVP","bundle":"https://pith.science/pith/L5MAFEDUX5Z2A5J3BBYJ6Z5CVP/bundle.json","state":"https://pith.science/pith/L5MAFEDUX5Z2A5J3BBYJ6Z5CVP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/L5MAFEDUX5Z2A5J3BBYJ6Z5CVP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:L5MAFEDUX5Z2A5J3BBYJ6Z5CVP","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":"1b612de0710f28c0dd82426a69db4d37d5d696b462ba4c8d388cac572f751a2b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-19T11:40:45Z","title_canon_sha256":"c743c54732e61952ac5204fd310a99fdebc999ace077464909c11834795f6822"},"schema_version":"1.0","source":{"id":"1311.4704","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.4704","created_at":"2026-05-18T01:16:33Z"},{"alias_kind":"arxiv_version","alias_value":"1311.4704v3","created_at":"2026-05-18T01:16:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.4704","created_at":"2026-05-18T01:16:33Z"},{"alias_kind":"pith_short_12","alias_value":"L5MAFEDUX5Z2","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"L5MAFEDUX5Z2A5J3","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"L5MAFEDU","created_at":"2026-05-18T12:27:51Z"}],"graph_snapshots":[{"event_id":"sha256:d8598d63f57a9007006636221ded160a8d2ad757aff008dd766613eed37bcd9f","target":"graph","created_at":"2026-05-18T01:16:33Z","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":"We calculate all gauge invariant Barr-Zee type contributions to fermionic electric dipole moments (EDMs) in the two-Higgs doublet models (2HDM) with softly broken Z2 symmetry. We start by studying the tensor structure of h to VV' part in the Barr-Zee diagrams, and we calculate the effective couplings in a gauge invariant way by using the pinch technique. Then we calculate all Barr-Zee diagrams relevant for electron and neutron EDMs. We make bounds on the parameter space in type-I, type-II, type-X, and type-Y 2HDMs. The electron and neutron EDMs are complementary to each other in discrimination","authors_text":"Junji Hisano, Kohsaku Tobioka, Teppei Kitahara, Tomohiro Abe","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-19T11:40:45Z","title":"Gauge invariant Barr-Zee type contributions to fermionic EDMs in the two-Higgs doublet models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.4704","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":"sha256:6de400c26dfa1305bc1034b74653beddf87ebd12d08d69f043f7e459edc9ac52","target":"record","created_at":"2026-05-18T01:16:33Z","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":"1b612de0710f28c0dd82426a69db4d37d5d696b462ba4c8d388cac572f751a2b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-19T11:40:45Z","title_canon_sha256":"c743c54732e61952ac5204fd310a99fdebc999ace077464909c11834795f6822"},"schema_version":"1.0","source":{"id":"1311.4704","kind":"arxiv","version":3}},"canonical_sha256":"5f58029074bf73a0753b08709f67a2abd83dd0882e4f8b3559cb3e4663388fa3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5f58029074bf73a0753b08709f67a2abd83dd0882e4f8b3559cb3e4663388fa3","first_computed_at":"2026-05-18T01:16:33.640790Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:16:33.640790Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4357vqBzUHryD0t2EGcdXLb7XCvDssSrJL8Ezmm7zJg1qMieQbt6nUiQnwcrD4Fmb33o5nKhrBDahrQGa66fCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:16:33.641419Z","signed_message":"canonical_sha256_bytes"},"source_id":"1311.4704","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6de400c26dfa1305bc1034b74653beddf87ebd12d08d69f043f7e459edc9ac52","sha256:d8598d63f57a9007006636221ded160a8d2ad757aff008dd766613eed37bcd9f"],"state_sha256":"ac22ff5181d17c40a655fd9231c49a03df64d67d6083b08857d69cddff53a076"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/q5OOt3WSAYw+GN1Q21gDO+2JMwj6oajoZQ4Iazm9jkIKXuIDYqxviOBqp3UW5cgFdTfT2v6vyYWitt60sZECA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T20:50:49.917305Z","bundle_sha256":"5b3749e216c7c69199ebdc8776382f6c9e4c70f37e4c6d014c6786fd025ea1dd"}}