{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:A3GOEKZ4WFKCORVIAZA4L2ZITT","short_pith_number":"pith:A3GOEKZ4","schema_version":"1.0","canonical_sha256":"06cce22b3cb1542746a80641c5eb289cee9a80baaff7ad6eeb4b339a10181113","source":{"kind":"arxiv","id":"2304.08416","version":1},"attestation_state":"computed","paper":{"title":"Simulation of the TAEs saturation phase in Large Helical Device device: MHD burst","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"D. A. Spong, J. Ortiz, J. Varela, L. Garcia, R. Seki, Y. Ghai, Y. Todo","submitted_at":"2023-04-17T16:34:06Z","abstract_excerpt":"The aim of the present study is to analyze the saturation regime of the Toroidal Alfven Eigenmodes (TAE) in the LHD plasma, particularly the MHD burst. The linear and nonlinear evolution of the TAEs are simulated by the FAR3d code that uses a reduced MHD model for the thermal plasma coupled with a gyrofluid model for the energetic particles (EP) species. The linear simulations indicate the overlapping of 1/2-1/1, 2/3-2/4 and 3/5-3/6 TAEs in the inner-middle plasma region and frequency range of 45-75 kHz, triggered by EPs with an energy of Tf = 45 keV and EP beta = 0.022. The nonlinear simulati"},"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":"2304.08416","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2023-04-17T16:34:06Z","cross_cats_sorted":[],"title_canon_sha256":"f0a14c195561fa78c41ccf4513dd0fbeb2d9aeac42f417db336273c4a4f6851e","abstract_canon_sha256":"6b200ec4e2ca8cf55c182af250b9b9e60c807c387ff090df7c667e434365190b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:01:52.158802Z","signature_b64":"evdiJd1KY+ekkWBpYsWNKzrKvpGiEAqtV0aoxTOVf14w17TKIGP3DjPKLaerYZMacEdY0U1c+5n3SAkY2vCNCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"06cce22b3cb1542746a80641c5eb289cee9a80baaff7ad6eeb4b339a10181113","last_reissued_at":"2026-07-05T06:01:52.158354Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:01:52.158354Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulation of the TAEs saturation phase in Large Helical Device device: MHD burst","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"D. A. Spong, J. Ortiz, J. Varela, L. Garcia, R. Seki, Y. Ghai, Y. Todo","submitted_at":"2023-04-17T16:34:06Z","abstract_excerpt":"The aim of the present study is to analyze the saturation regime of the Toroidal Alfven Eigenmodes (TAE) in the LHD plasma, particularly the MHD burst. The linear and nonlinear evolution of the TAEs are simulated by the FAR3d code that uses a reduced MHD model for the thermal plasma coupled with a gyrofluid model for the energetic particles (EP) species. The linear simulations indicate the overlapping of 1/2-1/1, 2/3-2/4 and 3/5-3/6 TAEs in the inner-middle plasma region and frequency range of 45-75 kHz, triggered by EPs with an energy of Tf = 45 keV and EP beta = 0.022. The nonlinear simulati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2304.08416","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2304.08416/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2304.08416","created_at":"2026-07-05T06:01:52.158418+00:00"},{"alias_kind":"arxiv_version","alias_value":"2304.08416v1","created_at":"2026-07-05T06:01:52.158418+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2304.08416","created_at":"2026-07-05T06:01:52.158418+00:00"},{"alias_kind":"pith_short_12","alias_value":"A3GOEKZ4WFKC","created_at":"2026-07-05T06:01:52.158418+00:00"},{"alias_kind":"pith_short_16","alias_value":"A3GOEKZ4WFKCORVI","created_at":"2026-07-05T06:01:52.158418+00:00"},{"alias_kind":"pith_short_8","alias_value":"A3GOEKZ4","created_at":"2026-07-05T06:01:52.158418+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/A3GOEKZ4WFKCORVIAZA4L2ZITT","json":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT.json","graph_json":"https://pith.science/api/pith-number/A3GOEKZ4WFKCORVIAZA4L2ZITT/graph.json","events_json":"https://pith.science/api/pith-number/A3GOEKZ4WFKCORVIAZA4L2ZITT/events.json","paper":"https://pith.science/paper/A3GOEKZ4"},"agent_actions":{"view_html":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT","download_json":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT.json","view_paper":"https://pith.science/paper/A3GOEKZ4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2304.08416&json=true","fetch_graph":"https://pith.science/api/pith-number/A3GOEKZ4WFKCORVIAZA4L2ZITT/graph.json","fetch_events":"https://pith.science/api/pith-number/A3GOEKZ4WFKCORVIAZA4L2ZITT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT/action/storage_attestation","attest_author":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT/action/author_attestation","sign_citation":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT/action/citation_signature","submit_replication":"https://pith.science/pith/A3GOEKZ4WFKCORVIAZA4L2ZITT/action/replication_record"}},"created_at":"2026-07-05T06:01:52.158418+00:00","updated_at":"2026-07-05T06:01:52.158418+00:00"}