{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:SVC6VORYTFQN6X76MA5PYAHIXH","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":"4b8e411d607f5282568f8acbd166475fa061566f68d737430ecabb1c1374d63e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-05-16T09:11:17Z","title_canon_sha256":"d419fe24fab43695d4ed73757ef50c5f9c375dc8a15ed189bbe21a734a43e60f"},"schema_version":"1.0","source":{"id":"1305.3721","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.3721","created_at":"2026-05-18T03:25:34Z"},{"alias_kind":"arxiv_version","alias_value":"1305.3721v1","created_at":"2026-05-18T03:25:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.3721","created_at":"2026-05-18T03:25:34Z"},{"alias_kind":"pith_short_12","alias_value":"SVC6VORYTFQN","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_16","alias_value":"SVC6VORYTFQN6X76","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_8","alias_value":"SVC6VORY","created_at":"2026-05-18T12:27:59Z"}],"graph_snapshots":[{"event_id":"sha256:d3143b3d3bdf0dcf3bae8739491d82f87c388806457fd63af228b2513e15e4ad","target":"graph","created_at":"2026-05-18T03:25:34Z","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 non-linear interplay between the resistive wall mode (RWM) and the toroidal plasma flow is numerically investigated in a full toroidal geometry, by simultaneously solving the initial value problems for the n=1 RWM and the n=0 toroidal force balance equation. Here n is the toroidal mode number. The neoclassical toroidal viscous torque is identified as the major momentum sink that brakes the toroidal plasma flow during the non-linear evolution of the RWM. This holds for a mode that is initially either unstable or stable. For an initially stable RWM, the braking of the flow, and hence the eve","authors_text":"Youwen Sun, Yueqiang Liu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-05-16T09:11:17Z","title":"Toroidal modeling of interaction between resistive wall mode and plasma flow"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.3721","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":"sha256:0b05d47412613de97990e7529c1ba29507c5ae797431dd67dd197a46efaa3e1b","target":"record","created_at":"2026-05-18T03:25:34Z","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":"4b8e411d607f5282568f8acbd166475fa061566f68d737430ecabb1c1374d63e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-05-16T09:11:17Z","title_canon_sha256":"d419fe24fab43695d4ed73757ef50c5f9c375dc8a15ed189bbe21a734a43e60f"},"schema_version":"1.0","source":{"id":"1305.3721","kind":"arxiv","version":1}},"canonical_sha256":"9545eaba389960df5ffe603afc00e8b9fcc7cce4ef7bbaa7e9f1ac85151ff544","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9545eaba389960df5ffe603afc00e8b9fcc7cce4ef7bbaa7e9f1ac85151ff544","first_computed_at":"2026-05-18T03:25:34.116607Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:25:34.116607Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iGfqlryr/av28I4J9aJXNpsPgJJsEa/Dptypcj2a4/qpuEKQQuNmDI15hteF4dJG/ESyAqAZR1aQNqwJok4NCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:25:34.117330Z","signed_message":"canonical_sha256_bytes"},"source_id":"1305.3721","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0b05d47412613de97990e7529c1ba29507c5ae797431dd67dd197a46efaa3e1b","sha256:d3143b3d3bdf0dcf3bae8739491d82f87c388806457fd63af228b2513e15e4ad"],"state_sha256":"a3809d65ac75e3309dc34bffa59e466a3aae1a2ae693eb5e8ba13c1666fdad02"}