{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:YJ77JN5F4DIEL2HY5E6CWT2WSZ","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":"2f5476dc4b8c0a3a7522bd82b93bc7f2b9bfee5262d628606c2a862e03019069","cross_cats_sorted":["physics.chem-ph","physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-08-29T15:55:14Z","title_canon_sha256":"1ba5abbb9df1fd2dc440c1abfe31210b1c756dac9cbc9ef255e35c9356a421bb"},"schema_version":"1.0","source":{"id":"2508.21729","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2508.21729","created_at":"2026-07-05T12:01:48Z"},{"alias_kind":"arxiv_version","alias_value":"2508.21729v1","created_at":"2026-07-05T12:01:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.21729","created_at":"2026-07-05T12:01:48Z"},{"alias_kind":"pith_short_12","alias_value":"YJ77JN5F4DIE","created_at":"2026-07-05T12:01:48Z"},{"alias_kind":"pith_short_16","alias_value":"YJ77JN5F4DIEL2HY","created_at":"2026-07-05T12:01:48Z"},{"alias_kind":"pith_short_8","alias_value":"YJ77JN5F","created_at":"2026-07-05T12:01:48Z"}],"graph_snapshots":[{"event_id":"sha256:275a10a57ed91696c8648a02e13b777e75803e1bfacc94adc95c51835475fdaa","target":"graph","created_at":"2026-07-05T12:01:48Z","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/2508.21729/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The quantum many-electron problem is not just at the heart of condensed matter phenomena, but also essential for first-principles simulation of chemical phenomena. Strong correlation in chemical systems are prevalent and present a formidable challenge in the simulation of these systems, while predictive phenomena in this domain often also requires a demanding level of accuracy to inform chemical behavior. Efficient representations of the many-electron states of chemical systems are therefore also being inspired by machine learning principles to provide an alternative to established approaches.","authors_text":"George H. Booth, Massimo Bortone, Yannic Rath","cross_cats":["physics.chem-ph","physics.comp-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-08-29T15:55:14Z","title":"Bayesian perspectives for quantum states and application to ab initio quantum chemistry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.21729","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":"sha256:563dc144739cfe42ef678aba87e72ecb210b3769759321ff205d48c973ae61c9","target":"record","created_at":"2026-07-05T12:01:48Z","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":"2f5476dc4b8c0a3a7522bd82b93bc7f2b9bfee5262d628606c2a862e03019069","cross_cats_sorted":["physics.chem-ph","physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-08-29T15:55:14Z","title_canon_sha256":"1ba5abbb9df1fd2dc440c1abfe31210b1c756dac9cbc9ef255e35c9356a421bb"},"schema_version":"1.0","source":{"id":"2508.21729","kind":"arxiv","version":1}},"canonical_sha256":"c27ff4b7a5e0d045e8f8e93c2b4f56964ee202ea439509aec6633aa3e4337303","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c27ff4b7a5e0d045e8f8e93c2b4f56964ee202ea439509aec6633aa3e4337303","first_computed_at":"2026-07-05T12:01:48.749976Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T12:01:48.749976Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ydOlZrhh+l2nMw8w99n26vHZX+j3OXevA1lC9WP+kUL9K+NMfy6MG8xx80OpdG+fusPV/RUXo+4NcblPg7CECw==","signature_status":"signed_v1","signed_at":"2026-07-05T12:01:48.750558Z","signed_message":"canonical_sha256_bytes"},"source_id":"2508.21729","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:563dc144739cfe42ef678aba87e72ecb210b3769759321ff205d48c973ae61c9","sha256:275a10a57ed91696c8648a02e13b777e75803e1bfacc94adc95c51835475fdaa"],"state_sha256":"48b6407a0bddf002dc1130c395b3ab189137ee2d8f085e5d5e31aa523b628c64"}