{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:5E6RAEQ7XAETLAAQHSWQCQ3BST","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":"487b295feeeef4ee7f5fa4ee1352bac01f9ee7059086d723522eef05bfc1b142","cross_cats_sorted":["cond-mat.dis-nn","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-11-29T18:59:59Z","title_canon_sha256":"e64c0d4a35b91147945ae67de26eb83cd28b5d57b0032117534e7d7534cc8004"},"schema_version":"1.0","source":{"id":"2311.17920","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.17920","created_at":"2026-07-05T09:13:34Z"},{"alias_kind":"arxiv_version","alias_value":"2311.17920v1","created_at":"2026-07-05T09:13:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.17920","created_at":"2026-07-05T09:13:34Z"},{"alias_kind":"pith_short_12","alias_value":"5E6RAEQ7XAET","created_at":"2026-07-05T09:13:34Z"},{"alias_kind":"pith_short_16","alias_value":"5E6RAEQ7XAETLAAQ","created_at":"2026-07-05T09:13:34Z"},{"alias_kind":"pith_short_8","alias_value":"5E6RAEQ7","created_at":"2026-07-05T09:13:34Z"}],"graph_snapshots":[{"event_id":"sha256:310e69a43217a2d5a379953fc37b2a54f230016744285992642da328151124a9","target":"graph","created_at":"2026-07-05T09:13:34Z","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/2311.17920/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The single particle Green's function provides valuable information on the momentum and energy-resolved spectral properties for a strongly correlated system. In large-scale numerical calculations using quantum Monte Carlo (QMC), dynamical mean field theory (DMFT), including cluster-DMFT, one usually obtains the Green's function in imaginary-time $G(\\tau)$. The process of inverting a Laplace transform to obtain the spectral function $A(\\omega)$ in real-frequency is an ill-posed problem and forms the core of the analytic continuation problem. In this Letter, we propose to use a completely unsuper","authors_text":"Lauren Keyes, Maciej M. Maska, Maksymilian Kliczkowski, Mohit Randeria, Nandini Trivedi, Sayantan Roy, Thereza Paiva","cross_cats":["cond-mat.dis-nn","physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-11-29T18:59:59Z","title":"Autoencoder-based analytic continuation method for strongly correlated quantum systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.17920","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":"sha256:18faa393922555753f96d365b64cf8d9854e40cfa4ec9948f7ad9ab80dec9f89","target":"record","created_at":"2026-07-05T09:13:34Z","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":"487b295feeeef4ee7f5fa4ee1352bac01f9ee7059086d723522eef05bfc1b142","cross_cats_sorted":["cond-mat.dis-nn","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-11-29T18:59:59Z","title_canon_sha256":"e64c0d4a35b91147945ae67de26eb83cd28b5d57b0032117534e7d7534cc8004"},"schema_version":"1.0","source":{"id":"2311.17920","kind":"arxiv","version":1}},"canonical_sha256":"e93d10121fb8093580103cad01436194c4c2fd0d88a2c8cf1e861fa14982a514","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e93d10121fb8093580103cad01436194c4c2fd0d88a2c8cf1e861fa14982a514","first_computed_at":"2026-07-05T09:13:34.174006Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:13:34.174006Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MXiq7XOSMnfS4Yjy8hrEBT4YsZwV3F9DAmWlset1NkHAe2XWqMDaodYzk+d+oQJcNINKKqEAI5qz+3nW1rSrCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T09:13:34.174506Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.17920","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:18faa393922555753f96d365b64cf8d9854e40cfa4ec9948f7ad9ab80dec9f89","sha256:310e69a43217a2d5a379953fc37b2a54f230016744285992642da328151124a9"],"state_sha256":"cab4352ba7b447326aeda8b88ba6db6099908be91df646a7cdd26fe8e9b5661d"}