{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:N4SEPWEHJDVSXVVF3GLF52A7QY","short_pith_number":"pith:N4SEPWEH","canonical_record":{"source":{"id":"hep-lat/0508009","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-08-10T19:51:50Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"e86b753478559dcb2b63fb6550d7b42f79f36303f6bb2bcccbace691aa658e18","abstract_canon_sha256":"950720da39eebf2e2dbbf08618af9e39fd698c78e2b869e4e3c30d968303f3f5"},"schema_version":"1.0"},"canonical_sha256":"6f2447d88748eb2bd6a5d9965ee81f8625f34e84705c93bf5642f3994cf70359","source":{"kind":"arxiv","id":"hep-lat/0508009","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0508009","created_at":"2026-05-18T02:37:20Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0508009v2","created_at":"2026-05-18T02:37:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0508009","created_at":"2026-05-18T02:37:20Z"},{"alias_kind":"pith_short_12","alias_value":"N4SEPWEHJDVS","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"N4SEPWEHJDVSXVVF","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"N4SEPWEH","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:N4SEPWEHJDVSXVVF3GLF52A7QY","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0508009","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-08-10T19:51:50Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"e86b753478559dcb2b63fb6550d7b42f79f36303f6bb2bcccbace691aa658e18","abstract_canon_sha256":"950720da39eebf2e2dbbf08618af9e39fd698c78e2b869e4e3c30d968303f3f5"},"schema_version":"1.0"},"canonical_sha256":"6f2447d88748eb2bd6a5d9965ee81f8625f34e84705c93bf5642f3994cf70359","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:20.190223Z","signature_b64":"0yZZ/KCRMK5fZkB53T7cfMfKTjgTJ9fCVTiRFVCfpCJnX7tKn9WRlJe360HnLzH96AmQSmxfBQqBMN9lLJUWBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6f2447d88748eb2bd6a5d9965ee81f8625f34e84705c93bf5642f3994cf70359","last_reissued_at":"2026-05-18T02:37:20.189800Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:20.189800Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0508009","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":"2026-05-18T02:37:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wRFatAkNStvgErJpQBpidUh2QWXLRGazucBIAWhZYuIFunrZYDbfecgGc9OgZm/nLZ00TMHkzubV+t7kLqFIAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T15:39:57.439656Z"},"content_sha256":"4d084d67a275e9977ea1726a99f188b32e1bff40278e422cd9424e324d4610a1","schema_version":"1.0","event_id":"sha256:4d084d67a275e9977ea1726a99f188b32e1bff40278e422cd9424e324d4610a1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:N4SEPWEHJDVSXVVF3GLF52A7QY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Extrapolation Formulas for Neutron EDM Calculations in Lattice QCD","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Donal O'Connell, Martin J. Savage","submitted_at":"2005-08-10T19:51:50Z","abstract_excerpt":"Lattice QCD is rapidly progressing toward being able to reliably compute the electric dipole moment of the neutron as a function of the strong CP-violating parameter theta. Present day calculations are performed at unphysical values of the light quark masses, in volumes that are not exceptionally large and at lattice spacings that are not exceptionally small. We use chiral perturbation theory to determine the leading contributions to the neutron electric dipole moment at finite volume, and in partially-quenched calculations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0508009","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":"2026-05-18T02:37:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"x40YiwQs01bDKZzP74OQzZgpytTi+VPZiNBNirIoLIzpTva99i0vlEIeFCPQkvyr7E/Xp7qTEQDp25fRYCdIDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T15:39:57.440378Z"},"content_sha256":"2b2456027ca13a79029283670912a66c3633a351cfb986cdc940d43252458d5f","schema_version":"1.0","event_id":"sha256:2b2456027ca13a79029283670912a66c3633a351cfb986cdc940d43252458d5f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N4SEPWEHJDVSXVVF3GLF52A7QY/bundle.json","state_url":"https://pith.science/pith/N4SEPWEHJDVSXVVF3GLF52A7QY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N4SEPWEHJDVSXVVF3GLF52A7QY/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":"2026-06-08T15:39:57Z","links":{"resolver":"https://pith.science/pith/N4SEPWEHJDVSXVVF3GLF52A7QY","bundle":"https://pith.science/pith/N4SEPWEHJDVSXVVF3GLF52A7QY/bundle.json","state":"https://pith.science/pith/N4SEPWEHJDVSXVVF3GLF52A7QY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N4SEPWEHJDVSXVVF3GLF52A7QY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:N4SEPWEHJDVSXVVF3GLF52A7QY","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":"950720da39eebf2e2dbbf08618af9e39fd698c78e2b869e4e3c30d968303f3f5","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2005-08-10T19:51:50Z","title_canon_sha256":"e86b753478559dcb2b63fb6550d7b42f79f36303f6bb2bcccbace691aa658e18"},"schema_version":"1.0","source":{"id":"hep-lat/0508009","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0508009","created_at":"2026-05-18T02:37:20Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0508009v2","created_at":"2026-05-18T02:37:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0508009","created_at":"2026-05-18T02:37:20Z"},{"alias_kind":"pith_short_12","alias_value":"N4SEPWEHJDVS","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"N4SEPWEHJDVSXVVF","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"N4SEPWEH","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:2b2456027ca13a79029283670912a66c3633a351cfb986cdc940d43252458d5f","target":"graph","created_at":"2026-05-18T02:37:20Z","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":"Lattice QCD is rapidly progressing toward being able to reliably compute the electric dipole moment of the neutron as a function of the strong CP-violating parameter theta. Present day calculations are performed at unphysical values of the light quark masses, in volumes that are not exceptionally large and at lattice spacings that are not exceptionally small. We use chiral perturbation theory to determine the leading contributions to the neutron electric dipole moment at finite volume, and in partially-quenched calculations.","authors_text":"Donal O'Connell, Martin J. Savage","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2005-08-10T19:51:50Z","title":"Extrapolation Formulas for Neutron EDM Calculations in Lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0508009","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":"sha256:4d084d67a275e9977ea1726a99f188b32e1bff40278e422cd9424e324d4610a1","target":"record","created_at":"2026-05-18T02:37:20Z","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":"950720da39eebf2e2dbbf08618af9e39fd698c78e2b869e4e3c30d968303f3f5","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2005-08-10T19:51:50Z","title_canon_sha256":"e86b753478559dcb2b63fb6550d7b42f79f36303f6bb2bcccbace691aa658e18"},"schema_version":"1.0","source":{"id":"hep-lat/0508009","kind":"arxiv","version":2}},"canonical_sha256":"6f2447d88748eb2bd6a5d9965ee81f8625f34e84705c93bf5642f3994cf70359","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6f2447d88748eb2bd6a5d9965ee81f8625f34e84705c93bf5642f3994cf70359","first_computed_at":"2026-05-18T02:37:20.189800Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:37:20.189800Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0yZZ/KCRMK5fZkB53T7cfMfKTjgTJ9fCVTiRFVCfpCJnX7tKn9WRlJe360HnLzH96AmQSmxfBQqBMN9lLJUWBw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:37:20.190223Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0508009","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4d084d67a275e9977ea1726a99f188b32e1bff40278e422cd9424e324d4610a1","sha256:2b2456027ca13a79029283670912a66c3633a351cfb986cdc940d43252458d5f"],"state_sha256":"e3f10f128409b294be3b72e71f83a283d368bf64974f1ba535d7bfa39716c03f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LZ9ILC29aiOxc5AGW3RkofckBQWILOXcwd7Pq6wjkZObrjEXMORRNC0X+rHYGwMk9aidq11k81v2hmpFB2R+Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T15:39:57.444284Z","bundle_sha256":"38f8d65750aaa4b879ceab6f7c51da1a6bee32f41ac1e36c566bac9c8013db94"}}