{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:DD6TL4CNIQQKLZJKV42QCE6JM6","short_pith_number":"pith:DD6TL4CN","canonical_record":{"source":{"id":"2409.00398","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-31T09:16:08Z","cross_cats_sorted":[],"title_canon_sha256":"d6dff29b7ac40740906bdf458cb2e9b9963b51f40b35da110ccfb4378f62a077","abstract_canon_sha256":"0610afdd4498d5521b2f2e7973cfca00f0d40dd335c45022585cba574863d62a"},"schema_version":"1.0"},"canonical_sha256":"18fd35f04d4420a5e52aaf350113c9679764906492f97182713e4b29329f6ac4","source":{"kind":"arxiv","id":"2409.00398","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.00398","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"arxiv_version","alias_value":"2409.00398v2","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.00398","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"pith_short_12","alias_value":"DD6TL4CNIQQK","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"pith_short_16","alias_value":"DD6TL4CNIQQKLZJK","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"pith_short_8","alias_value":"DD6TL4CN","created_at":"2026-07-05T11:55:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:DD6TL4CNIQQKLZJKV42QCE6JM6","target":"record","payload":{"canonical_record":{"source":{"id":"2409.00398","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-31T09:16:08Z","cross_cats_sorted":[],"title_canon_sha256":"d6dff29b7ac40740906bdf458cb2e9b9963b51f40b35da110ccfb4378f62a077","abstract_canon_sha256":"0610afdd4498d5521b2f2e7973cfca00f0d40dd335c45022585cba574863d62a"},"schema_version":"1.0"},"canonical_sha256":"18fd35f04d4420a5e52aaf350113c9679764906492f97182713e4b29329f6ac4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:55:14.696625Z","signature_b64":"wC/jlSWlQNdmrjOlEB0hLB8dFH09iIU4f/d09n8WiabvXbQurtWoJ73ALG2taDYDJ2ngs3qeSMCz3z2pSGtnCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18fd35f04d4420a5e52aaf350113c9679764906492f97182713e4b29329f6ac4","last_reissued_at":"2026-07-05T11:55:14.696175Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:55:14.696175Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2409.00398","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:55:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GgUnVIiDfTTTGz3J90tW5ZxLD19UC4JRMYJhXRc2I7fALw0hNQYbX4XEFBDad+35FzgmlM14qiO52TDArpJjAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T15:15:11.569984Z"},"content_sha256":"d81744f0f515180a0c9e351b0d9515f8c817ba342857704af4c25c512c87e443","schema_version":"1.0","event_id":"sha256:d81744f0f515180a0c9e351b0d9515f8c817ba342857704af4c25c512c87e443"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:DD6TL4CNIQQKLZJKV42QCE6JM6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Variational Monte Carlo with Neural Network Quantum States for Yang-Mills Matrix Model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Enrico Rinaldi, Masanori Hanada, Norbert Bodendorfer, Onur Oktay, Vaibhav Gautam","submitted_at":"2024-08-31T09:16:08Z","abstract_excerpt":"We apply the variational Monte Carlo method based on neural network quantum states, using a neural autoregressive flow architecture as our ansatz, to determine the ground state wave function of the bosonic SU($N$) Yang-Mills-type two-matrix model at strong coupling. Previous literature hinted at the inaccuracy of such an approach at strong coupling. In this work, the accuracy of the results is tested using lattice Monte Carlo simulations: we benchmark the expectation value of the energy of the ground state for system sizes $N$ that are beyond brute-force exact diagonalization methods. We obser"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.00398","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2409.00398/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:55:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vdpaI6ufZ2gJYfzSt0+VddSniQLyIiCZ5oKDauh/Q0nJAixJ1xC185GW27K4LA6IYl/lorcjJoph2SwlWT6QCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T15:15:11.570562Z"},"content_sha256":"835f6ff427da8b1e94593e04dae1e81ad01a3e96055b9c87cbaaa5cd88c0ef00","schema_version":"1.0","event_id":"sha256:835f6ff427da8b1e94593e04dae1e81ad01a3e96055b9c87cbaaa5cd88c0ef00"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DD6TL4CNIQQKLZJKV42QCE6JM6/bundle.json","state_url":"https://pith.science/pith/DD6TL4CNIQQKLZJKV42QCE6JM6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DD6TL4CNIQQKLZJKV42QCE6JM6/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-03T15:15:11Z","links":{"resolver":"https://pith.science/pith/DD6TL4CNIQQKLZJKV42QCE6JM6","bundle":"https://pith.science/pith/DD6TL4CNIQQKLZJKV42QCE6JM6/bundle.json","state":"https://pith.science/pith/DD6TL4CNIQQKLZJKV42QCE6JM6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DD6TL4CNIQQKLZJKV42QCE6JM6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:DD6TL4CNIQQKLZJKV42QCE6JM6","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":"0610afdd4498d5521b2f2e7973cfca00f0d40dd335c45022585cba574863d62a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-31T09:16:08Z","title_canon_sha256":"d6dff29b7ac40740906bdf458cb2e9b9963b51f40b35da110ccfb4378f62a077"},"schema_version":"1.0","source":{"id":"2409.00398","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.00398","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"arxiv_version","alias_value":"2409.00398v2","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.00398","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"pith_short_12","alias_value":"DD6TL4CNIQQK","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"pith_short_16","alias_value":"DD6TL4CNIQQKLZJK","created_at":"2026-07-05T11:55:14Z"},{"alias_kind":"pith_short_8","alias_value":"DD6TL4CN","created_at":"2026-07-05T11:55:14Z"}],"graph_snapshots":[{"event_id":"sha256:835f6ff427da8b1e94593e04dae1e81ad01a3e96055b9c87cbaaa5cd88c0ef00","target":"graph","created_at":"2026-07-05T11:55:14Z","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/2409.00398/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We apply the variational Monte Carlo method based on neural network quantum states, using a neural autoregressive flow architecture as our ansatz, to determine the ground state wave function of the bosonic SU($N$) Yang-Mills-type two-matrix model at strong coupling. Previous literature hinted at the inaccuracy of such an approach at strong coupling. In this work, the accuracy of the results is tested using lattice Monte Carlo simulations: we benchmark the expectation value of the energy of the ground state for system sizes $N$ that are beyond brute-force exact diagonalization methods. We obser","authors_text":"Enrico Rinaldi, Masanori Hanada, Norbert Bodendorfer, Onur Oktay, Vaibhav Gautam","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-31T09:16:08Z","title":"Variational Monte Carlo with Neural Network Quantum States for Yang-Mills Matrix Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.00398","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:d81744f0f515180a0c9e351b0d9515f8c817ba342857704af4c25c512c87e443","target":"record","created_at":"2026-07-05T11:55:14Z","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":"0610afdd4498d5521b2f2e7973cfca00f0d40dd335c45022585cba574863d62a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-31T09:16:08Z","title_canon_sha256":"d6dff29b7ac40740906bdf458cb2e9b9963b51f40b35da110ccfb4378f62a077"},"schema_version":"1.0","source":{"id":"2409.00398","kind":"arxiv","version":2}},"canonical_sha256":"18fd35f04d4420a5e52aaf350113c9679764906492f97182713e4b29329f6ac4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"18fd35f04d4420a5e52aaf350113c9679764906492f97182713e4b29329f6ac4","first_computed_at":"2026-07-05T11:55:14.696175Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:55:14.696175Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wC/jlSWlQNdmrjOlEB0hLB8dFH09iIU4f/d09n8WiabvXbQurtWoJ73ALG2taDYDJ2ngs3qeSMCz3z2pSGtnCA==","signature_status":"signed_v1","signed_at":"2026-07-05T11:55:14.696625Z","signed_message":"canonical_sha256_bytes"},"source_id":"2409.00398","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d81744f0f515180a0c9e351b0d9515f8c817ba342857704af4c25c512c87e443","sha256:835f6ff427da8b1e94593e04dae1e81ad01a3e96055b9c87cbaaa5cd88c0ef00"],"state_sha256":"7c3cde08198554ca54f9e448f7edbd03e372caea846e8c2a590cf4ae923ffe25"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2kE9/EJOgp5TDdcPTjDkWMBinVOvMbCHndhVN0lvPpyQjgVNTziSy9c1hy4ztxIiuvgZevwTxD+Ix/MsctE/AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T15:15:11.576203Z","bundle_sha256":"3b3f6d641f6b91da043ff2f6e96a17ad08c540a86f5c6cb7ff3cd4a82e715491"}}