{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:E4BRDTUT7DAWAUPYVV5BL7OYWW","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":"2026d42de40791fef77f6051bed3925eebe1cca6c560b940e3c2c405519022b8","cross_cats_sorted":["cs.CV","cs.LG"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-24T18:25:22Z","title_canon_sha256":"9b4c26fcf8eeb5ae89b137f0885ba4e3b1679b2564f3a28bd3b1ee19a0c3b01b"},"schema_version":"1.0","source":{"id":"2502.17397","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.17397","created_at":"2026-07-05T10:19:09Z"},{"alias_kind":"arxiv_version","alias_value":"2502.17397v1","created_at":"2026-07-05T10:19:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.17397","created_at":"2026-07-05T10:19:09Z"},{"alias_kind":"pith_short_12","alias_value":"E4BRDTUT7DAW","created_at":"2026-07-05T10:19:09Z"},{"alias_kind":"pith_short_16","alias_value":"E4BRDTUT7DAWAUPY","created_at":"2026-07-05T10:19:09Z"},{"alias_kind":"pith_short_8","alias_value":"E4BRDTUT","created_at":"2026-07-05T10:19:09Z"}],"graph_snapshots":[{"event_id":"sha256:9374eb0ea735dde469ade75244c4026dafbedfd2f338cbb43be612ca9c3d9dd4","target":"graph","created_at":"2026-07-05T10:19:09Z","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/2502.17397/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Maximizing fusion performance in tokamaks relies on high energy confinement, often achieved through distinct operating regimes. The automated labeling of these confinement states is crucial to enable large-scale analyses or for real-time control applications. While this task becomes difficult to automate near state transitions or in marginal scenarios, much success has been achieved with data-driven models. However, these methods generally provide predictions as point estimates, and cannot adequately deal with missing and/or broken input signals. To enable wide-range applicability, we develop ","authors_text":"Alessandro Pau, Cristina Venturini, Olivier Sauter, The TCV Team, the WPTE team, Vlado Menkovski, Yoeri Poels","cross_cats":["cs.CV","cs.LG"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-24T18:25:22Z","title":"Robust Confinement State Classification with Uncertainty Quantification through Ensembled Data-Driven Methods"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.17397","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":"sha256:874e84ba457a9b21a5ee981bc5f9883b6850be6d784bf66bfb8084bd717f4c52","target":"record","created_at":"2026-07-05T10:19:09Z","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":"2026d42de40791fef77f6051bed3925eebe1cca6c560b940e3c2c405519022b8","cross_cats_sorted":["cs.CV","cs.LG"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-24T18:25:22Z","title_canon_sha256":"9b4c26fcf8eeb5ae89b137f0885ba4e3b1679b2564f3a28bd3b1ee19a0c3b01b"},"schema_version":"1.0","source":{"id":"2502.17397","kind":"arxiv","version":1}},"canonical_sha256":"270311ce93f8c16051f8ad7a15fdd8b58324e200345f631c359543442576e558","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"270311ce93f8c16051f8ad7a15fdd8b58324e200345f631c359543442576e558","first_computed_at":"2026-07-05T10:19:09.704222Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:19:09.704222Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7+MeNYuiHLYwnUOuPDeF3KTCs2b0C7blt5c6Qv4JF8F8M6zzhaekB5Lo+s9rx/xJ3C/l/KFSQsY48b04qDj2Bg==","signature_status":"signed_v1","signed_at":"2026-07-05T10:19:09.704720Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.17397","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:874e84ba457a9b21a5ee981bc5f9883b6850be6d784bf66bfb8084bd717f4c52","sha256:9374eb0ea735dde469ade75244c4026dafbedfd2f338cbb43be612ca9c3d9dd4"],"state_sha256":"82da8be8f8d27a6728b3500bc56d0a432363b4e22ab5b95223d58442e1590929"}