{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:D3VDKDVZEEIQZOUL4OA2IZYO5N","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":"46cc2bbd50b4a6a4a44e74421204bfaf2512e5896f197b0ad8383cd93455adaf","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-06-10T17:50:56Z","title_canon_sha256":"4ff8c0ff4819ceead7b3ed5b97df11685d8ef0b0ef3ed444cc8ad51896f39980"},"schema_version":"1.0","source":{"id":"2406.06511","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.06511","created_at":"2026-07-05T08:31:16Z"},{"alias_kind":"arxiv_version","alias_value":"2406.06511v2","created_at":"2026-07-05T08:31:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.06511","created_at":"2026-07-05T08:31:16Z"},{"alias_kind":"pith_short_12","alias_value":"D3VDKDVZEEIQ","created_at":"2026-07-05T08:31:16Z"},{"alias_kind":"pith_short_16","alias_value":"D3VDKDVZEEIQZOUL","created_at":"2026-07-05T08:31:16Z"},{"alias_kind":"pith_short_8","alias_value":"D3VDKDVZ","created_at":"2026-07-05T08:31:16Z"}],"graph_snapshots":[{"event_id":"sha256:3bd1ee1e0c730b08df1d3de361664dc0e8482655e78f5575e237ecb76bd74159","target":"graph","created_at":"2026-07-05T08:31:16Z","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/2406.06511/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Understanding the physics of strongly correlated materials is one of the grand challenge problems for physics today. A large class of scientifically interesting materials, from high-$T_c$ superconductors to spin liquids, involve medium to strong correlations, and building a holistic understanding of these materials is critical. Doing so is hindered by the competition between the kinetic energy and Coulomb repulsion, which renders both analytic and numerical methods unsatisfactory for describing interacting materials. Fault-tolerant quantum computers have been proposed as a path forward to over","authors_text":"Alexander F. Kemper, Anjali A. Agrawal, Athena Caesura, Joshua Job, Josh Y. Mutus, Justin E. Elenewski, Kaitlyn J. Morrell, Mark J. Hodson, Peter D. Johnson, S. N. Saadatmand, Tyler L. Wilson","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-06-10T17:50:56Z","title":"Quantifying fault tolerant simulation of strongly correlated systems using the Fermi-Hubbard model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.06511","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:fbaca7416e00ec85a3bc49f8f054a76e0790776b929369ea349da106110dfdc9","target":"record","created_at":"2026-07-05T08:31:16Z","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":"46cc2bbd50b4a6a4a44e74421204bfaf2512e5896f197b0ad8383cd93455adaf","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-06-10T17:50:56Z","title_canon_sha256":"4ff8c0ff4819ceead7b3ed5b97df11685d8ef0b0ef3ed444cc8ad51896f39980"},"schema_version":"1.0","source":{"id":"2406.06511","kind":"arxiv","version":2}},"canonical_sha256":"1eea350eb921110cba8be381a4670eeb44420196b9b92539b9dd347efc3ac949","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1eea350eb921110cba8be381a4670eeb44420196b9b92539b9dd347efc3ac949","first_computed_at":"2026-07-05T08:31:16.525645Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:31:16.525645Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qlfJimhfo9JU2QPsFo+meI186GLGqIV8kNl9L7vVpnHCXZfdLunfEeWmI8zV+i5LohTr3mZvHE3xFrfNsf5aDA==","signature_status":"signed_v1","signed_at":"2026-07-05T08:31:16.526149Z","signed_message":"canonical_sha256_bytes"},"source_id":"2406.06511","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fbaca7416e00ec85a3bc49f8f054a76e0790776b929369ea349da106110dfdc9","sha256:3bd1ee1e0c730b08df1d3de361664dc0e8482655e78f5575e237ecb76bd74159"],"state_sha256":"ccde8e19639a004be4b595f698a9a87f2121fa433a78d72b17e030dfb7dfa759"}