{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:GRUBRL2IXX4VU6I3CNGLWLYLS3","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":"06bf4c73021b0a4e60b6e7384e4fe71e47a7499dd26081d893189fb845dab17d","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2021-03-14T22:18:51Z","title_canon_sha256":"62ca4e26372998f43cc8935cf22444b65180da38c211a4940717c38064fe5a9e"},"schema_version":"1.0","source":{"id":"2103.08054","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2103.08054","created_at":"2026-07-05T04:13:22Z"},{"alias_kind":"arxiv_version","alias_value":"2103.08054v1","created_at":"2026-07-05T04:13:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.08054","created_at":"2026-07-05T04:13:22Z"},{"alias_kind":"pith_short_12","alias_value":"GRUBRL2IXX4V","created_at":"2026-07-05T04:13:22Z"},{"alias_kind":"pith_short_16","alias_value":"GRUBRL2IXX4VU6I3","created_at":"2026-07-05T04:13:22Z"},{"alias_kind":"pith_short_8","alias_value":"GRUBRL2I","created_at":"2026-07-05T04:13:22Z"}],"graph_snapshots":[{"event_id":"sha256:bb5be5e19d1f354a2591fb064a1580f70329dff97182e77efaba1992a4b258f3","target":"graph","created_at":"2026-07-05T04:13:22Z","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/2103.08054/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We introduce a method of exploring potential energy contours in complex dynamical systems based on potentiostatic kinematics wherein the systems are evolved with minimal changes to their potential energy. We construct a simple iterative algorithm for performing potentiostatic kinematics, which uses an estimate curvature to predict new configurations space coordinates on the potential energy contour and a potentiostat term component to correct for errors in prediction. Our methods are then applied to atomic structure models using an interatomic potential for energy and force evaluations as woul","authors_text":"James M. Rondinelli, Michael J. Waters","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2021-03-14T22:18:51Z","title":"Contour Exploration with Potentiostatic Kinematics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.08054","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":"sha256:1cfdd2dc7faf407c7001e79d01b601c1a453993790aa44ad96e1b1a1c72b662d","target":"record","created_at":"2026-07-05T04:13:22Z","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":"06bf4c73021b0a4e60b6e7384e4fe71e47a7499dd26081d893189fb845dab17d","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2021-03-14T22:18:51Z","title_canon_sha256":"62ca4e26372998f43cc8935cf22444b65180da38c211a4940717c38064fe5a9e"},"schema_version":"1.0","source":{"id":"2103.08054","kind":"arxiv","version":1}},"canonical_sha256":"346818af48bdf95a791b134cbb2f0b96cd652be810fc0cc7339962453dd2b82c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"346818af48bdf95a791b134cbb2f0b96cd652be810fc0cc7339962453dd2b82c","first_computed_at":"2026-07-05T04:13:22.564018Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:13:22.564018Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1reC4h3BqNF0vzuVbANmCmYqBX2HP3nVg6HqQEL6tcKbVCNOL0SVpIkF6WYCKy9ozzU43zNPUO8qVuJTuZlRCg==","signature_status":"signed_v1","signed_at":"2026-07-05T04:13:22.564454Z","signed_message":"canonical_sha256_bytes"},"source_id":"2103.08054","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1cfdd2dc7faf407c7001e79d01b601c1a453993790aa44ad96e1b1a1c72b662d","sha256:bb5be5e19d1f354a2591fb064a1580f70329dff97182e77efaba1992a4b258f3"],"state_sha256":"f8f124ac5488c8b1b85b9b3ddaa3dccdaf4efd64ac2fce019b1225fd3d5100e7"}