{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:DE5HV5UQBC4IL3JCUCW3TTGT57","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":"c6aa4393d10a4a48f2ec6081e7c093530ff6f9dd02c6e5ca6098d80b37efde1c","cross_cats_sorted":["hep-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-10-17T15:29:32Z","title_canon_sha256":"84f9325b066467eb82f88b7e6704ed245371a1964b5d9c43f6697a89ef50109e"},"schema_version":"1.0","source":{"id":"2410.13670","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.13670","created_at":"2026-07-05T09:22:04Z"},{"alias_kind":"arxiv_version","alias_value":"2410.13670v1","created_at":"2026-07-05T09:22:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.13670","created_at":"2026-07-05T09:22:04Z"},{"alias_kind":"pith_short_12","alias_value":"DE5HV5UQBC4I","created_at":"2026-07-05T09:22:04Z"},{"alias_kind":"pith_short_16","alias_value":"DE5HV5UQBC4IL3JC","created_at":"2026-07-05T09:22:04Z"},{"alias_kind":"pith_short_8","alias_value":"DE5HV5UQ","created_at":"2026-07-05T09:22:04Z"}],"graph_snapshots":[{"event_id":"sha256:4e27bcfc80780cfe8091e555d6c215f7e881129198348cd5e4bca65549274516","target":"graph","created_at":"2026-07-05T09:22:04Z","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/2410.13670/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a systematic study of the nucleon-electron tensor-pseudotensor (Ne-TPT) interaction in candidate molecules for next-generation experimental searches for new sources of charge-parity violation. The considered molecules are all amenable to assembly from laser-cooled atoms, with the francium-silver (FrAg) molecule previously shown to be the most sensitive to the Schiff moment interaction in this set. Interelectron correlation effects are treated through relativistic general-excitation-rank configuration-interaction theory in the framework of the Dirac-Coulomb Hamiltonian. We find in Fr","authors_text":"Aur\\'elien Marc, Timo Fleig","cross_cats":["hep-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-10-17T15:29:32Z","title":"Semi-Hadronic Charge-Parity Violation Interaction Constants in CsAg, FrLi and FrAg molecules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.13670","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":"sha256:0d6140c26306d4f2cbc9e0eec2bc7b4e2d5dd1560e263669333ef5b11b0cd2ec","target":"record","created_at":"2026-07-05T09:22:04Z","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":"c6aa4393d10a4a48f2ec6081e7c093530ff6f9dd02c6e5ca6098d80b37efde1c","cross_cats_sorted":["hep-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-10-17T15:29:32Z","title_canon_sha256":"84f9325b066467eb82f88b7e6704ed245371a1964b5d9c43f6697a89ef50109e"},"schema_version":"1.0","source":{"id":"2410.13670","kind":"arxiv","version":1}},"canonical_sha256":"193a7af69008b885ed22a0adb9ccd3effde07f4cdfbed01ade5820f39df50680","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"193a7af69008b885ed22a0adb9ccd3effde07f4cdfbed01ade5820f39df50680","first_computed_at":"2026-07-05T09:22:04.224694Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:22:04.224694Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"he2FBQ2NWWGUF7By/hpJ1d+tusd6J6ksdZOJvROcb2BsSVu6PBTjUikUW1UlyZYBl39ZOGXSknlnUcmck1nYCw==","signature_status":"signed_v1","signed_at":"2026-07-05T09:22:04.225137Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.13670","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0d6140c26306d4f2cbc9e0eec2bc7b4e2d5dd1560e263669333ef5b11b0cd2ec","sha256:4e27bcfc80780cfe8091e555d6c215f7e881129198348cd5e4bca65549274516"],"state_sha256":"3572a3e233c0b49ef781830b4dca899c38d538581e46e0d42d42e7be71c67bac"}