{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:E2BFLPUBM4D6MQ3V2NDN5W7Y25","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":"efc65e1baab6b786518f1f046e0c99ca1d5dac745a23f46832ae27baf33511c4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-07-10T08:07:29Z","title_canon_sha256":"392c98e91f14981bfaa43d58428afa0465254df42e277301162407fd57e4f98c"},"schema_version":"1.0","source":{"id":"1807.03516","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.03516","created_at":"2026-05-18T00:11:10Z"},{"alias_kind":"arxiv_version","alias_value":"1807.03516v1","created_at":"2026-05-18T00:11:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.03516","created_at":"2026-05-18T00:11:10Z"},{"alias_kind":"pith_short_12","alias_value":"E2BFLPUBM4D6","created_at":"2026-05-18T12:32:19Z"},{"alias_kind":"pith_short_16","alias_value":"E2BFLPUBM4D6MQ3V","created_at":"2026-05-18T12:32:19Z"},{"alias_kind":"pith_short_8","alias_value":"E2BFLPUB","created_at":"2026-05-18T12:32:19Z"}],"graph_snapshots":[{"event_id":"sha256:03753d18480277c5702e5ff9dc99bfdacfdde85cfc6ef4afd354a02b7be49218","target":"graph","created_at":"2026-05-18T00:11:10Z","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"},"paper":{"abstract_excerpt":"A gyrokinetic simulation of the influence of electron cyclotron current drive and ion kinetic effect on the m/n=2/1 tearing mode (TM) instabilities is presented in HL-2A and DIII-D tokamak configurations. The TM evolution is calculated with a finite mass electron model and the rf current source is obtained by ray-tracing and the Fokker-Planck method. The TMs are found to be perfectly stabilized by a continuous 1MW 68GHz X2-mode in HL-2A tokamak, while instabilities in the DIII-D discharge (with lower value of CR=I_{rf}/I_{0}, where Irf is the wave driven current and I0 is the equilibrium plasm","authors_text":"Chijie Xiao, Dong Jian, Jingchun Li, Xiaogang Wang, Xiaoquan Ji, Zhihong Lin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-07-10T08:07:29Z","title":"Gyrokinetic simulations of the influence of electron cyclotron current drive on tearing mode instabilities in tokamaks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.03516","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":"sha256:3a2bbd5494d98b9f810360db622d36c63ed3f7c63e4d780c1a2d9bdcceaa79c2","target":"record","created_at":"2026-05-18T00:11:10Z","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":"efc65e1baab6b786518f1f046e0c99ca1d5dac745a23f46832ae27baf33511c4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-07-10T08:07:29Z","title_canon_sha256":"392c98e91f14981bfaa43d58428afa0465254df42e277301162407fd57e4f98c"},"schema_version":"1.0","source":{"id":"1807.03516","kind":"arxiv","version":1}},"canonical_sha256":"268255be816707e64375d346dedbf8d777e002705fd12a53a3d6d1e6226f6071","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"268255be816707e64375d346dedbf8d777e002705fd12a53a3d6d1e6226f6071","first_computed_at":"2026-05-18T00:11:10.199404Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:11:10.199404Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TCF+01SHY/rRrEhxisziCwznhsj65IGxxnbVT8JoxQRkOn3H3H743XkUqCvFTvhTWR7r4BuXeKr9SdaDgc3JAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:11:10.200126Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.03516","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3a2bbd5494d98b9f810360db622d36c63ed3f7c63e4d780c1a2d9bdcceaa79c2","sha256:03753d18480277c5702e5ff9dc99bfdacfdde85cfc6ef4afd354a02b7be49218"],"state_sha256":"d342dead5cd32b851d4d2dcbc6bef299184a7512c4e3866f149257a274528d1e"}