{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:SVC6VORYTFQN6X76MA5PYAHIXH","short_pith_number":"pith:SVC6VORY","schema_version":"1.0","canonical_sha256":"9545eaba389960df5ffe603afc00e8b9fcc7cce4ef7bbaa7e9f1ac85151ff544","source":{"kind":"arxiv","id":"1305.3721","version":1},"attestation_state":"computed","paper":{"title":"Toroidal modeling of interaction between resistive wall mode and plasma flow","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Youwen Sun, Yueqiang Liu","submitted_at":"2013-05-16T09:11:17Z","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"},"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":"1305.3721","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-05-16T09:11:17Z","cross_cats_sorted":[],"title_canon_sha256":"d419fe24fab43695d4ed73757ef50c5f9c375dc8a15ed189bbe21a734a43e60f","abstract_canon_sha256":"4b8e411d607f5282568f8acbd166475fa061566f68d737430ecabb1c1374d63e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:25:34.117330Z","signature_b64":"iGfqlryr/av28I4J9aJXNpsPgJJsEa/Dptypcj2a4/qpuEKQQuNmDI15hteF4dJG/ESyAqAZR1aQNqwJok4NCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9545eaba389960df5ffe603afc00e8b9fcc7cce4ef7bbaa7e9f1ac85151ff544","last_reissued_at":"2026-05-18T03:25:34.116607Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:25:34.116607Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Toroidal modeling of interaction between resistive wall mode and plasma flow","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Youwen Sun, Yueqiang Liu","submitted_at":"2013-05-16T09:11:17Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.3721","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":"1305.3721","created_at":"2026-05-18T03:25:34.116732+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.3721v1","created_at":"2026-05-18T03:25:34.116732+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.3721","created_at":"2026-05-18T03:25:34.116732+00:00"},{"alias_kind":"pith_short_12","alias_value":"SVC6VORYTFQN","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_16","alias_value":"SVC6VORYTFQN6X76","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_8","alias_value":"SVC6VORY","created_at":"2026-05-18T12:27:59.945178+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/SVC6VORYTFQN6X76MA5PYAHIXH","json":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH.json","graph_json":"https://pith.science/api/pith-number/SVC6VORYTFQN6X76MA5PYAHIXH/graph.json","events_json":"https://pith.science/api/pith-number/SVC6VORYTFQN6X76MA5PYAHIXH/events.json","paper":"https://pith.science/paper/SVC6VORY"},"agent_actions":{"view_html":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH","download_json":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH.json","view_paper":"https://pith.science/paper/SVC6VORY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.3721&json=true","fetch_graph":"https://pith.science/api/pith-number/SVC6VORYTFQN6X76MA5PYAHIXH/graph.json","fetch_events":"https://pith.science/api/pith-number/SVC6VORYTFQN6X76MA5PYAHIXH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH/action/storage_attestation","attest_author":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH/action/author_attestation","sign_citation":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH/action/citation_signature","submit_replication":"https://pith.science/pith/SVC6VORYTFQN6X76MA5PYAHIXH/action/replication_record"}},"created_at":"2026-05-18T03:25:34.116732+00:00","updated_at":"2026-05-18T03:25:34.116732+00:00"}