{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:ZW6BRLJOR37QC7TT4FILOL5NLK","short_pith_number":"pith:ZW6BRLJO","schema_version":"1.0","canonical_sha256":"cdbc18ad2e8eff017e73e150b72fad5abec3abdcfa9881d0565273cb3d7f6fc5","source":{"kind":"arxiv","id":"2004.13634","version":2},"attestation_state":"computed","paper":{"title":"Toroidal and slab ETG instability dominance in the linear spectrum of JET-ILW pedestals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Carine Giroud, Colin M. Roach, David R. Hatch, Felix I. Parra, Jason F. Parisi, JET contributors, Jon C. Hillesheim, Justin Ball, Michael Barnes, Nobuyuki Aiba, Plamen G. Ivanov, William Dorland","submitted_at":"2020-04-28T16:29:34Z","abstract_excerpt":"Local linear gyrokinetic simulations show that electron temperature gradient (ETG) instabilities are the fastest growing modes for $k_y \\rho_i \\gtrsim 0.1$ in the steep gradient region for a JET pedestal discharge (92174) where the electron temperature gradient is steeper than the ion temperature gradient. Here, $k_y$ is the wavenumber in the direction perpendicular to both the magnetic field and the radial direction, and $\\rho_i$ is the ion gyroradius. At $k_y \\rho_i \\gtrsim 1$, the fastest growing mode is often a novel type of toroidal ETG instability. This toroidal ETG mode is driven at sca"},"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":"2004.13634","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2020-04-28T16:29:34Z","cross_cats_sorted":[],"title_canon_sha256":"681769b55e28e81fb161aa7aedc613a5b9b1340ee02c1ca5847798ac89cdbdd7","abstract_canon_sha256":"642e28bac5a405f26c763ca84d07124923cd4b63c36cdb018cfe9e02b38a450e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:45:42.689339Z","signature_b64":"zR0BrfWjCmKYdj4ujgRW6/yYBa7abGnuyMxtAJPescp1cHmGibNrnHZxt14GTunzSDw4rNfV+8qpDc4ljQPIDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cdbc18ad2e8eff017e73e150b72fad5abec3abdcfa9881d0565273cb3d7f6fc5","last_reissued_at":"2026-07-05T01:45:42.688978Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:45:42.688978Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Toroidal and slab ETG instability dominance in the linear spectrum of JET-ILW pedestals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Carine Giroud, Colin M. Roach, David R. Hatch, Felix I. Parra, Jason F. Parisi, JET contributors, Jon C. Hillesheim, Justin Ball, Michael Barnes, Nobuyuki Aiba, Plamen G. Ivanov, William Dorland","submitted_at":"2020-04-28T16:29:34Z","abstract_excerpt":"Local linear gyrokinetic simulations show that electron temperature gradient (ETG) instabilities are the fastest growing modes for $k_y \\rho_i \\gtrsim 0.1$ in the steep gradient region for a JET pedestal discharge (92174) where the electron temperature gradient is steeper than the ion temperature gradient. Here, $k_y$ is the wavenumber in the direction perpendicular to both the magnetic field and the radial direction, and $\\rho_i$ is the ion gyroradius. At $k_y \\rho_i \\gtrsim 1$, the fastest growing mode is often a novel type of toroidal ETG instability. This toroidal ETG mode is driven at sca"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2004.13634","kind":"arxiv","version":2},"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/2004.13634/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":"2004.13634","created_at":"2026-07-05T01:45:42.689039+00:00"},{"alias_kind":"arxiv_version","alias_value":"2004.13634v2","created_at":"2026-07-05T01:45:42.689039+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2004.13634","created_at":"2026-07-05T01:45:42.689039+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZW6BRLJOR37Q","created_at":"2026-07-05T01:45:42.689039+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZW6BRLJOR37QC7TT","created_at":"2026-07-05T01:45:42.689039+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZW6BRLJO","created_at":"2026-07-05T01:45:42.689039+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/ZW6BRLJOR37QC7TT4FILOL5NLK","json":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK.json","graph_json":"https://pith.science/api/pith-number/ZW6BRLJOR37QC7TT4FILOL5NLK/graph.json","events_json":"https://pith.science/api/pith-number/ZW6BRLJOR37QC7TT4FILOL5NLK/events.json","paper":"https://pith.science/paper/ZW6BRLJO"},"agent_actions":{"view_html":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK","download_json":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK.json","view_paper":"https://pith.science/paper/ZW6BRLJO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2004.13634&json=true","fetch_graph":"https://pith.science/api/pith-number/ZW6BRLJOR37QC7TT4FILOL5NLK/graph.json","fetch_events":"https://pith.science/api/pith-number/ZW6BRLJOR37QC7TT4FILOL5NLK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK/action/storage_attestation","attest_author":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK/action/author_attestation","sign_citation":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK/action/citation_signature","submit_replication":"https://pith.science/pith/ZW6BRLJOR37QC7TT4FILOL5NLK/action/replication_record"}},"created_at":"2026-07-05T01:45:42.689039+00:00","updated_at":"2026-07-05T01:45:42.689039+00:00"}