{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:ZYV5U4QYYRN4OMPHLSMSCQIXQ6","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":"b4cd39c88a2d74e53e0e27e190ef4a6b6b08a3fa32cf7b33746522dccf3b49c6","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2021-01-21T18:38:37Z","title_canon_sha256":"99a36a7c08d2b20962d16d9e8021888e65c3c24d68a519606435e76487c4bbbf"},"schema_version":"1.0","source":{"id":"2101.08766","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2101.08766","created_at":"2026-07-05T03:24:08Z"},{"alias_kind":"arxiv_version","alias_value":"2101.08766v4","created_at":"2026-07-05T03:24:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2101.08766","created_at":"2026-07-05T03:24:08Z"},{"alias_kind":"pith_short_12","alias_value":"ZYV5U4QYYRN4","created_at":"2026-07-05T03:24:08Z"},{"alias_kind":"pith_short_16","alias_value":"ZYV5U4QYYRN4OMPH","created_at":"2026-07-05T03:24:08Z"},{"alias_kind":"pith_short_8","alias_value":"ZYV5U4QY","created_at":"2026-07-05T03:24:08Z"}],"graph_snapshots":[{"event_id":"sha256:50a9ce83b08b972aa84baa11f66ba78f75537d8d96b5bf396f22a42b00a37837","target":"graph","created_at":"2026-07-05T03:24:08Z","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/2101.08766/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Stochastic phenomena are often described by Langevin equations, which serve as a mesoscopic model for microscopic dynamics. It is known since the work of Parisi and Sourlas that reversible (or equilibrium) dynamics present supersymmetries (SUSYs). These are revealed when the path-integral action is written as a function not only of the physical fields, but also of Grassmann fields representing a Jacobian arising from the noise distribution. SUSYs leave the action invariant upon a transformation of the fields that mixes the physical and the Grassmann ones. We show that, contrarily to the common","authors_text":"Bastien Marguet, Elisabeth Agoritsas, L\\'eonie Canet, Vivien Lecomte","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2021-01-21T18:38:37Z","title":"Supersymmetries in non-equilibrium Langevin dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2101.08766","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:a29f1990ac823b1d47c4931c01fecde247e5a8df7b1fce2b4291b879cf9f0b0f","target":"record","created_at":"2026-07-05T03:24:08Z","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":"b4cd39c88a2d74e53e0e27e190ef4a6b6b08a3fa32cf7b33746522dccf3b49c6","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2021-01-21T18:38:37Z","title_canon_sha256":"99a36a7c08d2b20962d16d9e8021888e65c3c24d68a519606435e76487c4bbbf"},"schema_version":"1.0","source":{"id":"2101.08766","kind":"arxiv","version":4}},"canonical_sha256":"ce2bda7218c45bc731e75c992141178782a31bdbac6615caf063fe7e09becbb8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ce2bda7218c45bc731e75c992141178782a31bdbac6615caf063fe7e09becbb8","first_computed_at":"2026-07-05T03:24:08.336709Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:24:08.336709Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QrzxA1Be6W+RIUMmqqJjh1L0ciEUAmtJ73IEsjgAXjOGOzUV1xay+MuOkWnpn6q62kyFQKH6D//jOiQJRN2xAw==","signature_status":"signed_v1","signed_at":"2026-07-05T03:24:08.337211Z","signed_message":"canonical_sha256_bytes"},"source_id":"2101.08766","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a29f1990ac823b1d47c4931c01fecde247e5a8df7b1fce2b4291b879cf9f0b0f","sha256:50a9ce83b08b972aa84baa11f66ba78f75537d8d96b5bf396f22a42b00a37837"],"state_sha256":"53ffc970f5806966fc18ff5f79bed49ebf13be8f94412215b054ad6e9aaaee4b"}