{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:AAAAD2SVZCBJPFBGOSTGM6IWJE","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":"a7f70812d4419e8fbe18d44bd9021076375824b89333c8ffc13d5e4f38c46bc7","cross_cats_sorted":["physics.data-an","stat.ML"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-07-28T09:40:44Z","title_canon_sha256":"44bc6345b2cd62065d7e5f04bc2893fe7832e7defab61771b4942eaf3f1c9a13"},"schema_version":"1.0","source":{"id":"1607.08379","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.08379","created_at":"2026-05-18T01:00:34Z"},{"alias_kind":"arxiv_version","alias_value":"1607.08379v1","created_at":"2026-05-18T01:00:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.08379","created_at":"2026-05-18T01:00:34Z"},{"alias_kind":"pith_short_12","alias_value":"AAAAD2SVZCBJ","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"AAAAD2SVZCBJPFBG","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"AAAAD2SV","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:3bc58a86c13acb8abfb8505039e7dfbc64f224ed617fc1eea8d14ed6210fef62","target":"graph","created_at":"2026-05-18T01:00:34Z","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"},"paper":{"abstract_excerpt":"We describe and analyze some novel approaches for studying the dynamics of Ising spin glass models. We first briefly consider the variational approach based on minimizing the Kullback-Leibler divergence between independent trajectories and the real ones and note that this approach only coincides with the mean field equations from the saddle point approximation to the generating functional when the dynamics is defined through a logistic link function, which is the case for the kinetic Ising model with parallel update. We then spend the rest of the paper developing two ways of going beyond the s","authors_text":"Claudia Battistin, Ludovica Bachschmid-Romano, Manfred Opper, Yasser Roudi","cross_cats":["physics.data-an","stat.ML"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-07-28T09:40:44Z","title":"Variational perturbation and extended Plefka approaches to dynamics on random networks: the case of the kinetic Ising model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.08379","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:e804d3e8f392ced1d8bca4c1885188c7e05ab27539a85470f8f87ac63030a660","target":"record","created_at":"2026-05-18T01:00:34Z","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":"a7f70812d4419e8fbe18d44bd9021076375824b89333c8ffc13d5e4f38c46bc7","cross_cats_sorted":["physics.data-an","stat.ML"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-07-28T09:40:44Z","title_canon_sha256":"44bc6345b2cd62065d7e5f04bc2893fe7832e7defab61771b4942eaf3f1c9a13"},"schema_version":"1.0","source":{"id":"1607.08379","kind":"arxiv","version":1}},"canonical_sha256":"000001ea55c88297942674a6667916490d50713f9e0357e0168029bf3edd8c42","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"000001ea55c88297942674a6667916490d50713f9e0357e0168029bf3edd8c42","first_computed_at":"2026-05-18T01:00:33.999982Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:00:33.999982Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3gSfx4f6Tw3SSi0rIiUdDDjWLPyAA8OGNDstEqY4sxUwal71kG95B02KZkszyO2LG2nIZedtxuOWbb1wIohlAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:00:34.000608Z","signed_message":"canonical_sha256_bytes"},"source_id":"1607.08379","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e804d3e8f392ced1d8bca4c1885188c7e05ab27539a85470f8f87ac63030a660","sha256:3bc58a86c13acb8abfb8505039e7dfbc64f224ed617fc1eea8d14ed6210fef62"],"state_sha256":"7a44c36fee678db2ba026a0eba3b12f3dcb716c6dea409bbb6febb5b3e4e73be"}