{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:5L7HTLKR6HO3AYWHOVT7LRX7KA","short_pith_number":"pith:5L7HTLKR","canonical_record":{"source":{"id":"1612.09371","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-30T02:12:43Z","cross_cats_sorted":["nucl-th","physics.atom-ph"],"title_canon_sha256":"03fa54ec8e6fefe9c3662314424f3ba290c1629b2190d41b0c0dd0c6304c2321","abstract_canon_sha256":"61273896f692972ea81ac85b9da006bd52fb1978e8f2a35fafa05819197b3528"},"schema_version":"1.0"},"canonical_sha256":"eafe79ad51f1ddb062c77567f5c6ff502b0e13a395619015450800a65b4a0856","source":{"kind":"arxiv","id":"1612.09371","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.09371","created_at":"2026-05-18T00:52:08Z"},{"alias_kind":"arxiv_version","alias_value":"1612.09371v1","created_at":"2026-05-18T00:52:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.09371","created_at":"2026-05-18T00:52:08Z"},{"alias_kind":"pith_short_12","alias_value":"5L7HTLKR6HO3","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5L7HTLKR6HO3AYWH","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5L7HTLKR","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:5L7HTLKR6HO3AYWHOVT7LRX7KA","target":"record","payload":{"canonical_record":{"source":{"id":"1612.09371","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-30T02:12:43Z","cross_cats_sorted":["nucl-th","physics.atom-ph"],"title_canon_sha256":"03fa54ec8e6fefe9c3662314424f3ba290c1629b2190d41b0c0dd0c6304c2321","abstract_canon_sha256":"61273896f692972ea81ac85b9da006bd52fb1978e8f2a35fafa05819197b3528"},"schema_version":"1.0"},"canonical_sha256":"eafe79ad51f1ddb062c77567f5c6ff502b0e13a395619015450800a65b4a0856","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:52:08.905004Z","signature_b64":"uiWYQXC2X+rwTVORldqi5vhvQZfFnE3dm15SE33CsPEgX26S6CV8rhmme0js1hPZHzGsU4Z51bSwiDnAdOKdDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eafe79ad51f1ddb062c77567f5c6ff502b0e13a395619015450800a65b4a0856","last_reissued_at":"2026-05-18T00:52:08.904416Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:52:08.904416Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1612.09371","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:52:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jYq8G+KLMXSYS7noTG1fvEaszFLNeMtTAuxCia82OmiG5MeSgW0k+tVIsGG5tGq6hs4MiBKsHgLAotwyZm7rDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T15:46:36.193403Z"},"content_sha256":"7481e675a07bf3644ca65755044ca056c9ced16c9d46d3b91929e924eeb49cf0","schema_version":"1.0","event_id":"sha256:7481e675a07bf3644ca65755044ca056c9ced16c9d46d3b91929e924eeb49cf0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:5L7HTLKR6HO3AYWHOVT7LRX7KA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Improved limits on the hadronic and semi-hadronic CP violating parameters and role of a dark force carrier in the electric dipole moment of $^{199}$Hg","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th","physics.atom-ph"],"primary_cat":"hep-ph","authors_text":"B. K. Sahoo","submitted_at":"2016-12-30T02:12:43Z","abstract_excerpt":"Combining the recently reported electric dipole moment (EDM) of $^{199}$Hg atom due to breaking of parity and time-reversal symmetries with the improved relativistic atomic calculations, precise limits on the tensor-pseudotensor (T-PT) electron-nucleus (e-N) coupling coefficient and the nuclear Schiff moment (NSM) interactions are determined. Using these limits with the nuclear calculations, we infer limits on the EDMs of neutron and proton as $d_n < 2.2 \\times 10^{-26} |e| \\rm{cm}$ and $d_p < 2.1 \\times 10^{-25} |e| \\rm{cm}$, respectively, and on the quantum chromodynamics (QCD) parameter and"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.09371","kind":"arxiv","version":1},"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":"2026-05-18T00:52:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cfwPsAmrPwYrvZWrSRRqL9hplQSztRP1H4uUTTqNLaD/kMUzy5K6lnq0GvzztOR1h48e9Um5yr8Ip+gRN6QKDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T15:46:36.194045Z"},"content_sha256":"062e399fc472078c1a013da519565d88eac773e76b327e58139fbdf9c834b0c8","schema_version":"1.0","event_id":"sha256:062e399fc472078c1a013da519565d88eac773e76b327e58139fbdf9c834b0c8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5L7HTLKR6HO3AYWHOVT7LRX7KA/bundle.json","state_url":"https://pith.science/pith/5L7HTLKR6HO3AYWHOVT7LRX7KA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5L7HTLKR6HO3AYWHOVT7LRX7KA/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":"2026-05-24T15:46:36Z","links":{"resolver":"https://pith.science/pith/5L7HTLKR6HO3AYWHOVT7LRX7KA","bundle":"https://pith.science/pith/5L7HTLKR6HO3AYWHOVT7LRX7KA/bundle.json","state":"https://pith.science/pith/5L7HTLKR6HO3AYWHOVT7LRX7KA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5L7HTLKR6HO3AYWHOVT7LRX7KA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:5L7HTLKR6HO3AYWHOVT7LRX7KA","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":"61273896f692972ea81ac85b9da006bd52fb1978e8f2a35fafa05819197b3528","cross_cats_sorted":["nucl-th","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-30T02:12:43Z","title_canon_sha256":"03fa54ec8e6fefe9c3662314424f3ba290c1629b2190d41b0c0dd0c6304c2321"},"schema_version":"1.0","source":{"id":"1612.09371","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.09371","created_at":"2026-05-18T00:52:08Z"},{"alias_kind":"arxiv_version","alias_value":"1612.09371v1","created_at":"2026-05-18T00:52:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.09371","created_at":"2026-05-18T00:52:08Z"},{"alias_kind":"pith_short_12","alias_value":"5L7HTLKR6HO3","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5L7HTLKR6HO3AYWH","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5L7HTLKR","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:062e399fc472078c1a013da519565d88eac773e76b327e58139fbdf9c834b0c8","target":"graph","created_at":"2026-05-18T00:52:08Z","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":"Combining the recently reported electric dipole moment (EDM) of $^{199}$Hg atom due to breaking of parity and time-reversal symmetries with the improved relativistic atomic calculations, precise limits on the tensor-pseudotensor (T-PT) electron-nucleus (e-N) coupling coefficient and the nuclear Schiff moment (NSM) interactions are determined. Using these limits with the nuclear calculations, we infer limits on the EDMs of neutron and proton as $d_n < 2.2 \\times 10^{-26} |e| \\rm{cm}$ and $d_p < 2.1 \\times 10^{-25} |e| \\rm{cm}$, respectively, and on the quantum chromodynamics (QCD) parameter and","authors_text":"B. K. Sahoo","cross_cats":["nucl-th","physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-30T02:12:43Z","title":"Improved limits on the hadronic and semi-hadronic CP violating parameters and role of a dark force carrier in the electric dipole moment of $^{199}$Hg"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.09371","kind":"arxiv","version":1},"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":"sha256:7481e675a07bf3644ca65755044ca056c9ced16c9d46d3b91929e924eeb49cf0","target":"record","created_at":"2026-05-18T00:52:08Z","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":"61273896f692972ea81ac85b9da006bd52fb1978e8f2a35fafa05819197b3528","cross_cats_sorted":["nucl-th","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-12-30T02:12:43Z","title_canon_sha256":"03fa54ec8e6fefe9c3662314424f3ba290c1629b2190d41b0c0dd0c6304c2321"},"schema_version":"1.0","source":{"id":"1612.09371","kind":"arxiv","version":1}},"canonical_sha256":"eafe79ad51f1ddb062c77567f5c6ff502b0e13a395619015450800a65b4a0856","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"eafe79ad51f1ddb062c77567f5c6ff502b0e13a395619015450800a65b4a0856","first_computed_at":"2026-05-18T00:52:08.904416Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:52:08.904416Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uiWYQXC2X+rwTVORldqi5vhvQZfFnE3dm15SE33CsPEgX26S6CV8rhmme0js1hPZHzGsU4Z51bSwiDnAdOKdDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:52:08.905004Z","signed_message":"canonical_sha256_bytes"},"source_id":"1612.09371","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7481e675a07bf3644ca65755044ca056c9ced16c9d46d3b91929e924eeb49cf0","sha256:062e399fc472078c1a013da519565d88eac773e76b327e58139fbdf9c834b0c8"],"state_sha256":"2c967e14e5986cf75f0afd1c79069743b6f891651cbf4ef115b48f4aba69bb5c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u0JB5MPCzOPiuIjShyko726HRi/eyB/Sozwjb1gCxPUkMBOslHRNydykyCyJUbPK/dW4hXGmOUMThnGJEB27Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T15:46:36.197753Z","bundle_sha256":"9dd14c0de88c9aa2e4f6c35b0f7223affe8ec0185928a851b2aa896779a2b7a4"}}