{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:ACRR2QMPZXPVMSPUD4D2XLT5X4","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":"ac34f1c3d9781d346d02ff2c8272bef9089932f65f801b386a936e385ca85e71","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2024-05-21T14:43:02Z","title_canon_sha256":"9213c56a647257ba7f352d56d5562d6179a193b307476c72175e058986a95cdc"},"schema_version":"1.0","source":{"id":"2405.13098","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2405.13098","created_at":"2026-07-05T10:37:26Z"},{"alias_kind":"arxiv_version","alias_value":"2405.13098v4","created_at":"2026-07-05T10:37:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.13098","created_at":"2026-07-05T10:37:26Z"},{"alias_kind":"pith_short_12","alias_value":"ACRR2QMPZXPV","created_at":"2026-07-05T10:37:26Z"},{"alias_kind":"pith_short_16","alias_value":"ACRR2QMPZXPVMSPU","created_at":"2026-07-05T10:37:26Z"},{"alias_kind":"pith_short_8","alias_value":"ACRR2QMP","created_at":"2026-07-05T10:37:26Z"}],"graph_snapshots":[{"event_id":"sha256:f36599b5292c6cd640af4e12e69decab08b75c2dcbefdfaf2398eb63654dc9c1","target":"graph","created_at":"2026-07-05T10:37:26Z","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/2405.13098/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Deep Neural Networks (DNNs) share important similarities with structural glasses. Both have many degrees of freedom, and their dynamics are governed by a high-dimensional, non-convex landscape representing either the loss or energy, respectively. Furthermore, both experience gradient descent dynamics subject to noise. In this work we investigate, by performing quantitative measurements on realistic networks trained on the MNIST and CIFAR-10 datasets, the extent to which this qualitative similarity gives rise to glass-like dynamics in neural networks. We demonstrate the existence of a Topology ","authors_text":"Liesbeth M. C. Janssen, Max Kerr Winter","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2024-05-21T14:43:02Z","title":"Glassy dynamics in deep neural networks: A structural comparison"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.13098","kind":"arxiv","version":4},"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":"sha256:4f7e0145c185da13d4c2bbf57050f70df203b3fefcb0ea0ae9aec25e04ecee78","target":"record","created_at":"2026-07-05T10:37:26Z","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":"ac34f1c3d9781d346d02ff2c8272bef9089932f65f801b386a936e385ca85e71","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2024-05-21T14:43:02Z","title_canon_sha256":"9213c56a647257ba7f352d56d5562d6179a193b307476c72175e058986a95cdc"},"schema_version":"1.0","source":{"id":"2405.13098","kind":"arxiv","version":4}},"canonical_sha256":"00a31d418fcddf5649f41f07abae7dbf17d05307e158e28471c892d839c609b2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"00a31d418fcddf5649f41f07abae7dbf17d05307e158e28471c892d839c609b2","first_computed_at":"2026-07-05T10:37:26.394574Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:37:26.394574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9dvnGQbUIGImlPY/SE3VFlDSmc+BbgV7Hu1nLFe4KipYlYoY6a/Fh86TZDExl96ID++tMSVbg7tpxQC/q676Bg==","signature_status":"signed_v1","signed_at":"2026-07-05T10:37:26.395190Z","signed_message":"canonical_sha256_bytes"},"source_id":"2405.13098","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4f7e0145c185da13d4c2bbf57050f70df203b3fefcb0ea0ae9aec25e04ecee78","sha256:f36599b5292c6cd640af4e12e69decab08b75c2dcbefdfaf2398eb63654dc9c1"],"state_sha256":"7f217184e4a00f254901cc0aec42c81cf843b6be7bce8fb59f134d4b7f423719"}