{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:N4BKXVFAGPJSK3B5JMDINSFUVA","short_pith_number":"pith:N4BKXVFA","canonical_record":{"source":{"id":"1612.08090","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-23T21:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"ea8e22af27ed28ed189a66f41da2d55ed76f0fb000600c204b30286864ddc86a","abstract_canon_sha256":"986f200b5db1d5a346a3b32e6a5f0bc4fef5b67c8da8c240c481c0b2fe9defef"},"schema_version":"1.0"},"canonical_sha256":"6f02abd4a033d3256c3d4b0686c8b4a803d344e0bb3b0b3b46abd72ab87b33ff","source":{"kind":"arxiv","id":"1612.08090","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.08090","created_at":"2026-05-18T00:35:35Z"},{"alias_kind":"arxiv_version","alias_value":"1612.08090v2","created_at":"2026-05-18T00:35:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.08090","created_at":"2026-05-18T00:35:35Z"},{"alias_kind":"pith_short_12","alias_value":"N4BKXVFAGPJS","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"N4BKXVFAGPJSK3B5","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"N4BKXVFA","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:N4BKXVFAGPJSK3B5JMDINSFUVA","target":"record","payload":{"canonical_record":{"source":{"id":"1612.08090","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-23T21:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"ea8e22af27ed28ed189a66f41da2d55ed76f0fb000600c204b30286864ddc86a","abstract_canon_sha256":"986f200b5db1d5a346a3b32e6a5f0bc4fef5b67c8da8c240c481c0b2fe9defef"},"schema_version":"1.0"},"canonical_sha256":"6f02abd4a033d3256c3d4b0686c8b4a803d344e0bb3b0b3b46abd72ab87b33ff","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:35.094824Z","signature_b64":"cf1FpKv9y8hTgz7VfCApLhqG+XrPfylWYs+NG6Ej+ccRjIikD/7NqJrwE3R7Jhzzt7hkz3cfm5B+MyF0VYvqAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6f02abd4a033d3256c3d4b0686c8b4a803d344e0bb3b0b3b46abd72ab87b33ff","last_reissued_at":"2026-05-18T00:35:35.094171Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:35.094171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1612.08090","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":"2026-05-18T00:35:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Eo7M1OQB3s0ApUoZLGdXL8DyXh3uUW/43drvjVe0GZCdskIp0te/dy2Oomgu1qUS7/nMwwy6eL31z6LkCr6+CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T17:25:07.461734Z"},"content_sha256":"9bf731734c35cb21a5249cbff51cd00b7905bb162409d2b999470768c8e3e76f","schema_version":"1.0","event_id":"sha256:9bf731734c35cb21a5249cbff51cd00b7905bb162409d2b999470768c8e3e76f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:N4BKXVFAGPJSK3B5JMDINSFUVA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electric Dipole Moments in Natural Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matthew Reece, Yuichiro Nakai","submitted_at":"2016-12-23T21:00:00Z","abstract_excerpt":"We discuss electric dipole moments (EDMs) in the framework of CP-violating natural supersymmetry (SUSY). Recent experimental results have significantly tightened constraints on the EDMs of electrons and of mercury, and substantial further progress is expected in the near future. We assess how these results constrain the parameter space of natural SUSY. In addition to our discussion of SUSY, we provide a set of general formulas for two-loop fermion EDMs, which can be applied to a wide range of models of new physics. In the SUSY context, the two-loop effects of stops and charginos respectively c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.08090","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":""},"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":"2026-05-18T00:35:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t+9E3ra3sxtqxqRTF0+gd4CvL4DwK+7aItk64XeVnJJkp/FWokzAIVaIxzeGJYWgTyk8HVRO3Funtk4US48PDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T17:25:07.462280Z"},"content_sha256":"eaa01a53bd9d6579687a3d79da009e5f7db0c858229b81592722a4f4d0451b6a","schema_version":"1.0","event_id":"sha256:eaa01a53bd9d6579687a3d79da009e5f7db0c858229b81592722a4f4d0451b6a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N4BKXVFAGPJSK3B5JMDINSFUVA/bundle.json","state_url":"https://pith.science/pith/N4BKXVFAGPJSK3B5JMDINSFUVA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N4BKXVFAGPJSK3B5JMDINSFUVA/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":"2026-08-09T17:25:07Z","links":{"resolver":"https://pith.science/pith/N4BKXVFAGPJSK3B5JMDINSFUVA","bundle":"https://pith.science/pith/N4BKXVFAGPJSK3B5JMDINSFUVA/bundle.json","state":"https://pith.science/pith/N4BKXVFAGPJSK3B5JMDINSFUVA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N4BKXVFAGPJSK3B5JMDINSFUVA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:N4BKXVFAGPJSK3B5JMDINSFUVA","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":"986f200b5db1d5a346a3b32e6a5f0bc4fef5b67c8da8c240c481c0b2fe9defef","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-23T21:00:00Z","title_canon_sha256":"ea8e22af27ed28ed189a66f41da2d55ed76f0fb000600c204b30286864ddc86a"},"schema_version":"1.0","source":{"id":"1612.08090","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.08090","created_at":"2026-05-18T00:35:35Z"},{"alias_kind":"arxiv_version","alias_value":"1612.08090v2","created_at":"2026-05-18T00:35:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.08090","created_at":"2026-05-18T00:35:35Z"},{"alias_kind":"pith_short_12","alias_value":"N4BKXVFAGPJS","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"N4BKXVFAGPJSK3B5","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"N4BKXVFA","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:eaa01a53bd9d6579687a3d79da009e5f7db0c858229b81592722a4f4d0451b6a","target":"graph","created_at":"2026-05-18T00:35:35Z","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 discuss electric dipole moments (EDMs) in the framework of CP-violating natural supersymmetry (SUSY). Recent experimental results have significantly tightened constraints on the EDMs of electrons and of mercury, and substantial further progress is expected in the near future. We assess how these results constrain the parameter space of natural SUSY. In addition to our discussion of SUSY, we provide a set of general formulas for two-loop fermion EDMs, which can be applied to a wide range of models of new physics. In the SUSY context, the two-loop effects of stops and charginos respectively c","authors_text":"Matthew Reece, Yuichiro Nakai","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-23T21:00:00Z","title":"Electric Dipole Moments in Natural Supersymmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.08090","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":"sha256:9bf731734c35cb21a5249cbff51cd00b7905bb162409d2b999470768c8e3e76f","target":"record","created_at":"2026-05-18T00:35:35Z","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":"986f200b5db1d5a346a3b32e6a5f0bc4fef5b67c8da8c240c481c0b2fe9defef","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-23T21:00:00Z","title_canon_sha256":"ea8e22af27ed28ed189a66f41da2d55ed76f0fb000600c204b30286864ddc86a"},"schema_version":"1.0","source":{"id":"1612.08090","kind":"arxiv","version":2}},"canonical_sha256":"6f02abd4a033d3256c3d4b0686c8b4a803d344e0bb3b0b3b46abd72ab87b33ff","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6f02abd4a033d3256c3d4b0686c8b4a803d344e0bb3b0b3b46abd72ab87b33ff","first_computed_at":"2026-05-18T00:35:35.094171Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:35.094171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cf1FpKv9y8hTgz7VfCApLhqG+XrPfylWYs+NG6Ej+ccRjIikD/7NqJrwE3R7Jhzzt7hkz3cfm5B+MyF0VYvqAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:35.094824Z","signed_message":"canonical_sha256_bytes"},"source_id":"1612.08090","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9bf731734c35cb21a5249cbff51cd00b7905bb162409d2b999470768c8e3e76f","sha256:eaa01a53bd9d6579687a3d79da009e5f7db0c858229b81592722a4f4d0451b6a"],"state_sha256":"a0193f851c86b5182b98c8bf7da9d21af007b970382f1ffc3b72986499c7eb57"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3Gh9o6RpnbubcWSDaMcGTFshYE1z+EG62PAirT/Oue+Ay/Z0UsXjP5tbYDBq+mQC8eR/s14yqR0mzNvEUKhPBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T17:25:07.465617Z","bundle_sha256":"d7711ced89ae78118a926efdf933e48c00abab1fb4c326a0d3916c4571ff4e4b"}}