{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:VLJAULWGDQ5WQO75V6YCFUUG67","short_pith_number":"pith:VLJAULWG","schema_version":"1.0","canonical_sha256":"aad20a2ec61c3b683bfdafb022d286f7c1ea0510af6cb81ceaaba5d42e06a6b3","source":{"kind":"arxiv","id":"1703.08354","version":1},"attestation_state":"computed","paper":{"title":"Field-line localized destabilization of ballooning modes in 3D tokamaks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"B. Vanovac, C.C. Hegna, E. Strumberger, F. Mink, G. Birkenmeier, H. Zohm, L.C. Luhmann, M. Dunne, M. Willensdorfer, S.S. Denk, T.B. Cote, the ASDEX Upgrade Team, W. Suttrop","submitted_at":"2017-03-24T11:07:41Z","abstract_excerpt":"Field-line localized ballooning modes have been observed at the edge of high confinement mode plasmas in ASDEX Upgrade with rotating 3D perturbations induced by an externally applied n = 2 error field and during a moderate level of edge localized mode-mitigation. The observed ballooning modes are localized to the field-lines which experience one of the two zero-crossings of the radial flux surface displacement during one rotation period. The localization of the ballooning modes agrees very well with the localization of the largest growth rates from infinite-n ideal ballooning stability calcula"},"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":"1703.08354","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-03-24T11:07:41Z","cross_cats_sorted":[],"title_canon_sha256":"d370d295ee363d971021e98c62a5d1864b970ce9b7216230a137017178a4baae","abstract_canon_sha256":"4b5312ab37a8909f9425730983ef626df9a8ac1606f54abe154f3f91c5d7da24"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:09.021503Z","signature_b64":"SCNkuyeLU2pt4QUMMTdkqGj2qLDdD6rvc6mJcP7UEZZkbl1PriCmWi5ZrcVDZXZsrb3fknSdhmU4MNU0iwMRAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aad20a2ec61c3b683bfdafb022d286f7c1ea0510af6cb81ceaaba5d42e06a6b3","last_reissued_at":"2026-05-18T00:36:09.020781Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:09.020781Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Field-line localized destabilization of ballooning modes in 3D tokamaks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"B. Vanovac, C.C. Hegna, E. Strumberger, F. Mink, G. Birkenmeier, H. Zohm, L.C. Luhmann, M. Dunne, M. Willensdorfer, S.S. Denk, T.B. Cote, the ASDEX Upgrade Team, W. Suttrop","submitted_at":"2017-03-24T11:07:41Z","abstract_excerpt":"Field-line localized ballooning modes have been observed at the edge of high confinement mode plasmas in ASDEX Upgrade with rotating 3D perturbations induced by an externally applied n = 2 error field and during a moderate level of edge localized mode-mitigation. The observed ballooning modes are localized to the field-lines which experience one of the two zero-crossings of the radial flux surface displacement during one rotation period. The localization of the ballooning modes agrees very well with the localization of the largest growth rates from infinite-n ideal ballooning stability calcula"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.08354","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":"1703.08354","created_at":"2026-05-18T00:36:09.020899+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.08354v1","created_at":"2026-05-18T00:36:09.020899+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.08354","created_at":"2026-05-18T00:36:09.020899+00:00"},{"alias_kind":"pith_short_12","alias_value":"VLJAULWGDQ5W","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"VLJAULWGDQ5WQO75","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"VLJAULWG","created_at":"2026-05-18T12:31:49.984773+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/VLJAULWGDQ5WQO75V6YCFUUG67","json":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67.json","graph_json":"https://pith.science/api/pith-number/VLJAULWGDQ5WQO75V6YCFUUG67/graph.json","events_json":"https://pith.science/api/pith-number/VLJAULWGDQ5WQO75V6YCFUUG67/events.json","paper":"https://pith.science/paper/VLJAULWG"},"agent_actions":{"view_html":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67","download_json":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67.json","view_paper":"https://pith.science/paper/VLJAULWG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.08354&json=true","fetch_graph":"https://pith.science/api/pith-number/VLJAULWGDQ5WQO75V6YCFUUG67/graph.json","fetch_events":"https://pith.science/api/pith-number/VLJAULWGDQ5WQO75V6YCFUUG67/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67/action/storage_attestation","attest_author":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67/action/author_attestation","sign_citation":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67/action/citation_signature","submit_replication":"https://pith.science/pith/VLJAULWGDQ5WQO75V6YCFUUG67/action/replication_record"}},"created_at":"2026-05-18T00:36:09.020899+00:00","updated_at":"2026-05-18T00:36:09.020899+00:00"}