{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:B4PYEVFC7KQFKE5MVSLR3ODY7C","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":"8993fc9576fac5f6380cdb58475a8078a9ecce5672f9a3819943da6c8f3e5108","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2023-10-13T11:36:43Z","title_canon_sha256":"d5110ece87d547f3aaffb40fa4bface173a2729b0b91e2bc5ea2b7488a626790"},"schema_version":"1.0","source":{"id":"2310.09024","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2310.09024","created_at":"2026-07-05T07:00:38Z"},{"alias_kind":"arxiv_version","alias_value":"2310.09024v1","created_at":"2026-07-05T07:00:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.09024","created_at":"2026-07-05T07:00:38Z"},{"alias_kind":"pith_short_12","alias_value":"B4PYEVFC7KQF","created_at":"2026-07-05T07:00:38Z"},{"alias_kind":"pith_short_16","alias_value":"B4PYEVFC7KQFKE5M","created_at":"2026-07-05T07:00:38Z"},{"alias_kind":"pith_short_8","alias_value":"B4PYEVFC","created_at":"2026-07-05T07:00:38Z"}],"graph_snapshots":[{"event_id":"sha256:e837c74b6df25b3917b5abe69f8b71c43badda707a1450657d886c8d0758f883","target":"graph","created_at":"2026-07-05T07:00:38Z","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/2310.09024/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Model-based plasma scenario development lies at the heart of the design and operation of future fusion powerplants. Including turbulent transport in integrated models is essential for delivering a successful roadmap towards operation of ITER and the design of DEMO-class devices. Given the highly iterative nature of integrated models, fast machine-learning-based surrogates of turbulent transport are fundamental to fulfil the pressing need for faster simulations opening up pulse design, optimization, and flight simulator applications. A significant bottleneck is the generation of suitably large ","authors_text":"A. Ho, F. Casson, J. Barr, J. Buchanan, J. Citrin, JET contributors, L. Zanisi, S. Pamela, T. Madula, V. Gopakumar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2023-10-13T11:36:43Z","title":"Efficient training sets for surrogate models of tokamak turbulence with Active Deep Ensembles"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.09024","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":"sha256:3461144a21629b00b253db94e8b05c94c8fbd8596b3ea2f24eac63fa2da38084","target":"record","created_at":"2026-07-05T07:00:38Z","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":"8993fc9576fac5f6380cdb58475a8078a9ecce5672f9a3819943da6c8f3e5108","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2023-10-13T11:36:43Z","title_canon_sha256":"d5110ece87d547f3aaffb40fa4bface173a2729b0b91e2bc5ea2b7488a626790"},"schema_version":"1.0","source":{"id":"2310.09024","kind":"arxiv","version":1}},"canonical_sha256":"0f1f8254a2faa05513acac971db878f8ab7f9a6be7aee60a6ea6d8101332e6fe","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0f1f8254a2faa05513acac971db878f8ab7f9a6be7aee60a6ea6d8101332e6fe","first_computed_at":"2026-07-05T07:00:38.902421Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:00:38.902421Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"C22Z/MkdsZOU4iP8dhyd9ZOQGezcza1u5u+3qVd4veZkjSHJUd75UQRnPxGlwDAwTT/P1t9vQODZA3fEh6Y+BA==","signature_status":"signed_v1","signed_at":"2026-07-05T07:00:38.902866Z","signed_message":"canonical_sha256_bytes"},"source_id":"2310.09024","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3461144a21629b00b253db94e8b05c94c8fbd8596b3ea2f24eac63fa2da38084","sha256:e837c74b6df25b3917b5abe69f8b71c43badda707a1450657d886c8d0758f883"],"state_sha256":"0c525bf548c4da1aa0f0eaf38f6efee48575c38893aba184a84120ed9a3f383c"}