{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:NZUYHOOMENYQICMBVTE336PTLP","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":"b1cda59ba8bcb43b8fbfce8b5e5af84cb30709c71ade98fe78869e1333da765b","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2021-03-17T07:33:22Z","title_canon_sha256":"eff4d9563cc31fa7e49cd3f93b95b11a18874a76f104a778c747e75137501b3f"},"schema_version":"1.0","source":{"id":"2103.09482","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2103.09482","created_at":"2026-07-05T02:24:04Z"},{"alias_kind":"arxiv_version","alias_value":"2103.09482v1","created_at":"2026-07-05T02:24:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.09482","created_at":"2026-07-05T02:24:04Z"},{"alias_kind":"pith_short_12","alias_value":"NZUYHOOMENYQ","created_at":"2026-07-05T02:24:04Z"},{"alias_kind":"pith_short_16","alias_value":"NZUYHOOMENYQICMB","created_at":"2026-07-05T02:24:04Z"},{"alias_kind":"pith_short_8","alias_value":"NZUYHOOM","created_at":"2026-07-05T02:24:04Z"}],"graph_snapshots":[{"event_id":"sha256:06dd61918d88326a62b4b4f4183c4b0c184e67cb670dae7cd01c1d5c0eeabc63","target":"graph","created_at":"2026-07-05T02:24:04Z","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/2103.09482/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We propose a Restricted Boltzmann Machine (RBM) neural network using a quantum thermodynamics formalism and the maximization of entropy as the cost function for the optimization problem. We verify the possibility of using an entropy maximization approach for modeling physical systems by applying it to the Inverse Ising Problem, which describes a system of interacting spins. The temperature-dependent behaviors of physical quantities, such as magnetization and Gibbs energy, were calculated from the Ising Hamiltonian whose coefficients were obtained through entropy maximization and were found to ","authors_text":"Eleanor Watson, Roshawn Terrell, Timofey Golubev","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2021-03-17T07:33:22Z","title":"Developing a Maximum-Entropy Restricted Boltzmann Machine with a Quantum Thermodynamics Formalism"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.09482","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":"sha256:2d46a8a7c50f644885d1259c8c7218da3f86deaa830e7cfb862fa0313b29bffd","target":"record","created_at":"2026-07-05T02:24:04Z","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":"b1cda59ba8bcb43b8fbfce8b5e5af84cb30709c71ade98fe78869e1333da765b","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2021-03-17T07:33:22Z","title_canon_sha256":"eff4d9563cc31fa7e49cd3f93b95b11a18874a76f104a778c747e75137501b3f"},"schema_version":"1.0","source":{"id":"2103.09482","kind":"arxiv","version":1}},"canonical_sha256":"6e6983b9cc2371040981acc9bdf9f35bc5b374920107e9573678244e300eda9f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6e6983b9cc2371040981acc9bdf9f35bc5b374920107e9573678244e300eda9f","first_computed_at":"2026-07-05T02:24:04.203038Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:24:04.203038Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"atv3HxfdCGUOTkYk5ewh4J9EdL8PBx8eoJASAk1SZG9A81QuS35k+RY4mBxF+EBOe0HAC8zkFoTaTiM3KnOiCg==","signature_status":"signed_v1","signed_at":"2026-07-05T02:24:04.203503Z","signed_message":"canonical_sha256_bytes"},"source_id":"2103.09482","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2d46a8a7c50f644885d1259c8c7218da3f86deaa830e7cfb862fa0313b29bffd","sha256:06dd61918d88326a62b4b4f4183c4b0c184e67cb670dae7cd01c1d5c0eeabc63"],"state_sha256":"8225b50023e37e349be75280c921babf2839dda41e222b30e8be6dfa2d576af1"}