{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:E2BFLPUBM4D6MQ3V2NDN5W7Y25","short_pith_number":"pith:E2BFLPUB","schema_version":"1.0","canonical_sha256":"268255be816707e64375d346dedbf8d777e002705fd12a53a3d6d1e6226f6071","source":{"kind":"arxiv","id":"1807.03516","version":1},"attestation_state":"computed","paper":{"title":"Gyrokinetic simulations of the influence of electron cyclotron current drive on tearing mode instabilities in tokamaks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Chijie Xiao, Dong Jian, Jingchun Li, Xiaogang Wang, Xiaoquan Ji, Zhihong Lin","submitted_at":"2018-07-10T08:07:29Z","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"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1807.03516","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-07-10T08:07:29Z","cross_cats_sorted":[],"title_canon_sha256":"392c98e91f14981bfaa43d58428afa0465254df42e277301162407fd57e4f98c","abstract_canon_sha256":"efc65e1baab6b786518f1f046e0c99ca1d5dac745a23f46832ae27baf33511c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:11:10.200126Z","signature_b64":"TCF+01SHY/rRrEhxisziCwznhsj65IGxxnbVT8JoxQRkOn3H3H743XkUqCvFTvhTWR7r4BuXeKr9SdaDgc3JAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"268255be816707e64375d346dedbf8d777e002705fd12a53a3d6d1e6226f6071","last_reissued_at":"2026-05-18T00:11:10.199404Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:11:10.199404Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gyrokinetic simulations of the influence of electron cyclotron current drive on tearing mode instabilities in tokamaks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Chijie Xiao, Dong Jian, Jingchun Li, Xiaogang Wang, Xiaoquan Ji, Zhihong Lin","submitted_at":"2018-07-10T08:07:29Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.03516","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1807.03516","created_at":"2026-05-18T00:11:10.199523+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.03516v1","created_at":"2026-05-18T00:11:10.199523+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.03516","created_at":"2026-05-18T00:11:10.199523+00:00"},{"alias_kind":"pith_short_12","alias_value":"E2BFLPUBM4D6","created_at":"2026-05-18T12:32:19.392346+00:00"},{"alias_kind":"pith_short_16","alias_value":"E2BFLPUBM4D6MQ3V","created_at":"2026-05-18T12:32:19.392346+00:00"},{"alias_kind":"pith_short_8","alias_value":"E2BFLPUB","created_at":"2026-05-18T12:32:19.392346+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25","json":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25.json","graph_json":"https://pith.science/api/pith-number/E2BFLPUBM4D6MQ3V2NDN5W7Y25/graph.json","events_json":"https://pith.science/api/pith-number/E2BFLPUBM4D6MQ3V2NDN5W7Y25/events.json","paper":"https://pith.science/paper/E2BFLPUB"},"agent_actions":{"view_html":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25","download_json":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25.json","view_paper":"https://pith.science/paper/E2BFLPUB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.03516&json=true","fetch_graph":"https://pith.science/api/pith-number/E2BFLPUBM4D6MQ3V2NDN5W7Y25/graph.json","fetch_events":"https://pith.science/api/pith-number/E2BFLPUBM4D6MQ3V2NDN5W7Y25/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25/action/storage_attestation","attest_author":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25/action/author_attestation","sign_citation":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25/action/citation_signature","submit_replication":"https://pith.science/pith/E2BFLPUBM4D6MQ3V2NDN5W7Y25/action/replication_record"}},"created_at":"2026-05-18T00:11:10.199523+00:00","updated_at":"2026-05-18T00:11:10.199523+00:00"}