{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:NVMRBIQVVFLLDNNYYZNY6XKMFE","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":"f0c8cd479e3ac43236e4d1fb3509d389cd6d830551f0c0f597f3934374e647e8","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-09-22T18:22:56Z","title_canon_sha256":"69ad323e432d962d7ba61d5b578b1da4ce7290a2219df499bc043d51e0d81af9"},"schema_version":"1.0","source":{"id":"2309.13126","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2309.13126","created_at":"2026-07-05T07:47:05Z"},{"alias_kind":"arxiv_version","alias_value":"2309.13126v2","created_at":"2026-07-05T07:47:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.13126","created_at":"2026-07-05T07:47:05Z"},{"alias_kind":"pith_short_12","alias_value":"NVMRBIQVVFLL","created_at":"2026-07-05T07:47:05Z"},{"alias_kind":"pith_short_16","alias_value":"NVMRBIQVVFLLDNNY","created_at":"2026-07-05T07:47:05Z"},{"alias_kind":"pith_short_8","alias_value":"NVMRBIQV","created_at":"2026-07-05T07:47:05Z"}],"graph_snapshots":[{"event_id":"sha256:120c65b5aa05f8b817602c53dddaa236cc95526b18364e15385c89884fd4208b","target":"graph","created_at":"2026-07-05T07:47:05Z","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/2309.13126/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Stretched-exponential relaxation is a widely observed phenomenon found in ordered ferromagnets as well as glassy systems. One modeling approach connects this behavior to a droplet dynamics described by an effective Langevin equation for the droplet radius with a $r^{2/3}$ potential. Here, we study a Brownian particle under the influence of a general confining, albeit weak, potential field that grows with distance as a sub-linear power law. We find that for this memoryless model, observables display stretched-exponential relaxation. The probability density function of the system is studied usin","authors_text":"David A. Kessler, Eli Barkai, Lucianno Defaveri","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-09-22T18:22:56Z","title":"Stretched-exponential relaxation in weakly-confined Brownian systems through large deviation theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.13126","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":"sha256:4b7f23ddef6a458022125a57fec0537bfaa109e4d3f6a46be91fa9529340a10a","target":"record","created_at":"2026-07-05T07:47:05Z","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":"f0c8cd479e3ac43236e4d1fb3509d389cd6d830551f0c0f597f3934374e647e8","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-09-22T18:22:56Z","title_canon_sha256":"69ad323e432d962d7ba61d5b578b1da4ce7290a2219df499bc043d51e0d81af9"},"schema_version":"1.0","source":{"id":"2309.13126","kind":"arxiv","version":2}},"canonical_sha256":"6d5910a215a956b1b5b8c65b8f5d4c291995cd4a3634038be9ee28b8514c8c1f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6d5910a215a956b1b5b8c65b8f5d4c291995cd4a3634038be9ee28b8514c8c1f","first_computed_at":"2026-07-05T07:47:05.074631Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:47:05.074631Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vS3ciNoKtZCxoaf0bun5oKEUNF6DDEtZ8c385/aw7D7yn7YtgSFApAIEDa+X+oISw+imx509WXJ82/GMGRgPBA==","signature_status":"signed_v1","signed_at":"2026-07-05T07:47:05.075091Z","signed_message":"canonical_sha256_bytes"},"source_id":"2309.13126","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4b7f23ddef6a458022125a57fec0537bfaa109e4d3f6a46be91fa9529340a10a","sha256:120c65b5aa05f8b817602c53dddaa236cc95526b18364e15385c89884fd4208b"],"state_sha256":"aed08da11dc5e7edf5a81cb1dcfbe526771d969da36452a2cb47bd1bee88c79e"}