{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:WCZQUYPHA6KPWIJFLWUDQ773CL","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":"846fcc2fccd9279def724b355c1fa5b29cb7b332b8b7d6dbe51d0af13c49139b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-07-13T05:23:40Z","title_canon_sha256":"537e6cef31bb3a85199e2ff54ab2fc70db90719da4325e8e107bb53081f9bb7f"},"schema_version":"1.0","source":{"id":"2607.11103","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.11103","created_at":"2026-07-14T01:22:16Z"},{"alias_kind":"arxiv_version","alias_value":"2607.11103v1","created_at":"2026-07-14T01:22:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.11103","created_at":"2026-07-14T01:22:16Z"},{"alias_kind":"pith_short_12","alias_value":"WCZQUYPHA6KP","created_at":"2026-07-14T01:22:16Z"},{"alias_kind":"pith_short_16","alias_value":"WCZQUYPHA6KPWIJF","created_at":"2026-07-14T01:22:16Z"},{"alias_kind":"pith_short_8","alias_value":"WCZQUYPH","created_at":"2026-07-14T01:22:16Z"}],"graph_snapshots":[{"event_id":"sha256:352a8d30b9269272c8d50ea76d3136a0175ff7c15cedd54236618f6f67464614","target":"graph","created_at":"2026-07-14T01:22:16Z","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/2607.11103/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A local neoclassical transport module has been developed and validated in the semi-Lagrangian gyrokinetic code NLT for multi-species collisional plasmas. The module incorporates a linearized multi-species Sugama collision operator and provides two complementary solution strategies. In the initial-value formulation, a composite substep source-integration scheme is introduced to accurately evaluate the neoclassical drive along unperturbed particle trajectories while retaining large macroscopic time steps. A direct steady-state solver is also implemented to obtain the stationary neoclassical resp","authors_text":"Chengkang Pan, Dandan Liao, Guoxu Wang, Lei Ye, Nong Xiang, Qilong Ren, Wei Zhang, Xiaotao Xiao","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-07-13T05:23:40Z","title":"Development and validation of a local neoclassical transport module in NLT with applications to EAST-relevant impurity transport and trapped-electron-mode stability"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.11103","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":"sha256:694b15c48d98d82b258fe047cd25a35414badf08a5dc5bd9e49c152506a04b0e","target":"record","created_at":"2026-07-14T01:22:16Z","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":"846fcc2fccd9279def724b355c1fa5b29cb7b332b8b7d6dbe51d0af13c49139b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-07-13T05:23:40Z","title_canon_sha256":"537e6cef31bb3a85199e2ff54ab2fc70db90719da4325e8e107bb53081f9bb7f"},"schema_version":"1.0","source":{"id":"2607.11103","kind":"arxiv","version":1}},"canonical_sha256":"b0b30a61e70794fb21255da8387ffb12d8303dfec8f4cb58aec8e37312b856fa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b0b30a61e70794fb21255da8387ffb12d8303dfec8f4cb58aec8e37312b856fa","first_computed_at":"2026-07-14T01:22:16.521713Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-14T01:22:16.521713Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NUFpFw+qCSgF00bYPpNsSFuld+6dhwraXD+w1EQ2jVApLXBojUFiVXeBIME7DbkDk0cyfKmgj2C5KUE4OIu/Cg==","signature_status":"signed_v1","signed_at":"2026-07-14T01:22:16.522654Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.11103","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:694b15c48d98d82b258fe047cd25a35414badf08a5dc5bd9e49c152506a04b0e","sha256:352a8d30b9269272c8d50ea76d3136a0175ff7c15cedd54236618f6f67464614"],"state_sha256":"64156dfe23fa31fce90dca480e5c760b562df69e4af5b65e5737a1f099c6c800"}