{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:EX6SY6RBWNYIJ3T6EMDLI2Z2GB","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":"73bf99773294abb9ce7223ce6f4be0241e0bea2c6c162ca0f5443fe786f3ba44","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-09-04T21:17:03Z","title_canon_sha256":"4f46d3e948f98080830c2268c609e2ab312b7fc9e5790cb5990c4b0cf6ec32b6"},"schema_version":"1.0","source":{"id":"1309.1189","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1309.1189","created_at":"2026-05-18T02:57:08Z"},{"alias_kind":"arxiv_version","alias_value":"1309.1189v2","created_at":"2026-05-18T02:57:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.1189","created_at":"2026-05-18T02:57:08Z"},{"alias_kind":"pith_short_12","alias_value":"EX6SY6RBWNYI","created_at":"2026-05-18T12:27:43Z"},{"alias_kind":"pith_short_16","alias_value":"EX6SY6RBWNYIJ3T6","created_at":"2026-05-18T12:27:43Z"},{"alias_kind":"pith_short_8","alias_value":"EX6SY6RB","created_at":"2026-05-18T12:27:43Z"}],"graph_snapshots":[{"event_id":"sha256:0c07792b5f042bb03c5d0ab90843e69a16a1d6c07bbdf650a036391c35d6bdb5","target":"graph","created_at":"2026-05-18T02:57:08Z","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":"The induced electric field in a tokamak drives a parallel electron current flow. In an inhomogeneous, finite beta plasma, when this electron flow is comparable to the ion thermal speed, the Alfven mode wave solutions of the electromagnetic gyrokinetic equation can become nearly purely growing kink modes. Using the new \"low-flow\" version of the gyrokinetic code GS2 developed for momentum transport studies [Barnes et al 2013 Phys. Rev. Lett. 111, 055005], we are able to model the effect of the induced parallel electric field on the electron distribution to study the destabilizing influence of cu","authors_text":"Felix I. Parra, Istv\\'an Pusztai, Michael Barnes, Peter J. Catto","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-09-04T21:17:03Z","title":"A current driven electromagnetic mode in sheared and toroidal configurations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.1189","kind":"arxiv","version":2},"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":"sha256:920b3899bc81899823f5eb71cd82b63f4927acfff3f16c764316ebfe824eb254","target":"record","created_at":"2026-05-18T02:57:08Z","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":"73bf99773294abb9ce7223ce6f4be0241e0bea2c6c162ca0f5443fe786f3ba44","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-09-04T21:17:03Z","title_canon_sha256":"4f46d3e948f98080830c2268c609e2ab312b7fc9e5790cb5990c4b0cf6ec32b6"},"schema_version":"1.0","source":{"id":"1309.1189","kind":"arxiv","version":2}},"canonical_sha256":"25fd2c7a21b37084ee7e2306b46b3a30452bf51705188782b9eed53d9ac36eb2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"25fd2c7a21b37084ee7e2306b46b3a30452bf51705188782b9eed53d9ac36eb2","first_computed_at":"2026-05-18T02:57:08.646391Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:57:08.646391Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9Z1j/uqUGEX6d+Dz20c1JgSaEdMdW6UiJ8KNLLDwnKEGENov8e8pXYwZrcE08jfg+Lr32WT7SQ1OF36+ZLrYCg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:57:08.646876Z","signed_message":"canonical_sha256_bytes"},"source_id":"1309.1189","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:920b3899bc81899823f5eb71cd82b63f4927acfff3f16c764316ebfe824eb254","sha256:0c07792b5f042bb03c5d0ab90843e69a16a1d6c07bbdf650a036391c35d6bdb5"],"state_sha256":"60ae2029bb4d4590fba49b85820a0cce340a50160424bc586f26a5e31252fa23"}