{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:TQM7TNHH3S3WIYBX2LLNORUPB6","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":"653aea899dda474563ab96c21bc89628c32ccaaed8723d643fc519b927464f0b","cross_cats_sorted":["cond-mat.supr-con","stat.AP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-08-07T13:08:40Z","title_canon_sha256":"9776301453118a1a2106f80f1fbf6a08ef29cc8a5e7c9b75e3a97da87ed60bb9"},"schema_version":"1.0","source":{"id":"2608.07194","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.07194","created_at":"2026-08-10T01:14:35Z"},{"alias_kind":"arxiv_version","alias_value":"2608.07194v1","created_at":"2026-08-10T01:14:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.07194","created_at":"2026-08-10T01:14:35Z"},{"alias_kind":"pith_short_12","alias_value":"TQM7TNHH3S3W","created_at":"2026-08-10T01:14:35Z"},{"alias_kind":"pith_short_16","alias_value":"TQM7TNHH3S3WIYBX","created_at":"2026-08-10T01:14:35Z"},{"alias_kind":"pith_short_8","alias_value":"TQM7TNHH","created_at":"2026-08-10T01:14:35Z"}],"graph_snapshots":[{"event_id":"sha256:0238f839f1e1fe22bdb9ba4cc619cc41842d5eab586bd82d97fdd7e5696a72b0","target":"graph","created_at":"2026-08-10T01:14:35Z","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/2608.07194/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In numerous physical, chemical, and biological systems the dynamics can be reduced to the motion of state variables in a complex potential landscape. In case the manifold is known, the motion and response of the embedded object can be described deterministically up to stochastic effects usually associated with a noise. In contrast, if the manifold is unknown, the static and dynamic response of the state variable may be used as a spectroscopic tool to characterize the potential landscape. Inspired by a seminal work of L.\\ Embon and co-workers, [Sci.\\ Rep.\\ \\textbf{5}, 7598 (2015)] we investigat","authors_text":"Luis Filsinger, Roland Willa","cross_cats":["cond-mat.supr-con","stat.AP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-08-07T13:08:40Z","title":"Statistical stability of random potentials to thermal and quantum activation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.07194","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:ecb27d150fbfe10f94bc77bd05c111beaaf44034da747384a920c414339b334d","target":"record","created_at":"2026-08-10T01:14:35Z","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":"653aea899dda474563ab96c21bc89628c32ccaaed8723d643fc519b927464f0b","cross_cats_sorted":["cond-mat.supr-con","stat.AP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-08-07T13:08:40Z","title_canon_sha256":"9776301453118a1a2106f80f1fbf6a08ef29cc8a5e7c9b75e3a97da87ed60bb9"},"schema_version":"1.0","source":{"id":"2608.07194","kind":"arxiv","version":1}},"canonical_sha256":"9c19f9b4e7dcb7646037d2d6d7468f0fa7fce6203b3ca5870ea3a0da78500187","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9c19f9b4e7dcb7646037d2d6d7468f0fa7fce6203b3ca5870ea3a0da78500187","first_computed_at":"2026-08-10T01:14:35.669392Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-08-10T01:14:35.669392Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YOqEbrdyM8E+YEJvmYNuSCwoHsLac8p7dRmt0d0MGV6lx2bEYHd8vVTt97sTj2HY/rnRZn6f0HWmubGE3I+2Bg==","signature_status":"signed_v1","signed_at":"2026-08-10T01:14:35.672097Z","signed_message":"canonical_sha256_bytes"},"source_id":"2608.07194","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ecb27d150fbfe10f94bc77bd05c111beaaf44034da747384a920c414339b334d","sha256:0238f839f1e1fe22bdb9ba4cc619cc41842d5eab586bd82d97fdd7e5696a72b0"],"state_sha256":"160f0501523e4cf346672b7714749dc2588c6148588881beebc7eeda5c295cec"}