{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:ERCTSWYFTH7G6HD6KNUFLCZ2EG","short_pith_number":"pith:ERCTSWYF","schema_version":"1.0","canonical_sha256":"2445395b0599fe6f1c7e5368558b3a21b06ca9e8a3de8e3c92300bd45f2d2948","source":{"kind":"arxiv","id":"1108.6327","version":2},"attestation_state":"computed","paper":{"title":"Gyrokinetic Equations for Strong-Gradient Regions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Andris M. Dimits","submitted_at":"2011-08-31T19:21:51Z","abstract_excerpt":"A gyrokinetic theory is developed under a set of orderings applicable to the edge region of tokamaks and other magnetic confinement devices, as well as to internal transport barriers. The result is a practical set equations that is valid for large perturbation amplitudes [q{\\delta}{\\psi}/T = O(1), where {\\delta}{\\psi} = {\\delta}{\\phi} - v_par {\\delta}A_par/c], which is straightforward to implement numerically, and which has straightforward expressions for its conservation properties. Here, q is the particle charge, {\\delta}{\\phi} and {\\delta}A_par are the perturbed electrostatic and parallel m"},"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":"1108.6327","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2011-08-31T19:21:51Z","cross_cats_sorted":[],"title_canon_sha256":"14303d33845b0a45d3a08ac5d7eeb6d63649216d3f3d31db072e62e5c85e7a98","abstract_canon_sha256":"21360f2a45ceb1a110d3f6728450c365ef1f7ad589f3570625e05b40a39593eb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:43.809887Z","signature_b64":"TO7sljHp7ttfSSMxFuEVvK1Q/AINxXfL5WJR7P62DkBnGoBVGXtY4HVVT1thuoiuTlV+sZCG8md+JOTSh4MnAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2445395b0599fe6f1c7e5368558b3a21b06ca9e8a3de8e3c92300bd45f2d2948","last_reissued_at":"2026-05-18T02:00:43.809215Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:43.809215Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gyrokinetic Equations for Strong-Gradient Regions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Andris M. Dimits","submitted_at":"2011-08-31T19:21:51Z","abstract_excerpt":"A gyrokinetic theory is developed under a set of orderings applicable to the edge region of tokamaks and other magnetic confinement devices, as well as to internal transport barriers. The result is a practical set equations that is valid for large perturbation amplitudes [q{\\delta}{\\psi}/T = O(1), where {\\delta}{\\psi} = {\\delta}{\\phi} - v_par {\\delta}A_par/c], which is straightforward to implement numerically, and which has straightforward expressions for its conservation properties. Here, q is the particle charge, {\\delta}{\\phi} and {\\delta}A_par are the perturbed electrostatic and parallel m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.6327","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":""},"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":"1108.6327","created_at":"2026-05-18T02:00:43.809327+00:00"},{"alias_kind":"arxiv_version","alias_value":"1108.6327v2","created_at":"2026-05-18T02:00:43.809327+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.6327","created_at":"2026-05-18T02:00:43.809327+00:00"},{"alias_kind":"pith_short_12","alias_value":"ERCTSWYFTH7G","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_16","alias_value":"ERCTSWYFTH7G6HD6","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_8","alias_value":"ERCTSWYF","created_at":"2026-05-18T12:26:28.662955+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/ERCTSWYFTH7G6HD6KNUFLCZ2EG","json":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG.json","graph_json":"https://pith.science/api/pith-number/ERCTSWYFTH7G6HD6KNUFLCZ2EG/graph.json","events_json":"https://pith.science/api/pith-number/ERCTSWYFTH7G6HD6KNUFLCZ2EG/events.json","paper":"https://pith.science/paper/ERCTSWYF"},"agent_actions":{"view_html":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG","download_json":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG.json","view_paper":"https://pith.science/paper/ERCTSWYF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1108.6327&json=true","fetch_graph":"https://pith.science/api/pith-number/ERCTSWYFTH7G6HD6KNUFLCZ2EG/graph.json","fetch_events":"https://pith.science/api/pith-number/ERCTSWYFTH7G6HD6KNUFLCZ2EG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG/action/storage_attestation","attest_author":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG/action/author_attestation","sign_citation":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG/action/citation_signature","submit_replication":"https://pith.science/pith/ERCTSWYFTH7G6HD6KNUFLCZ2EG/action/replication_record"}},"created_at":"2026-05-18T02:00:43.809327+00:00","updated_at":"2026-05-18T02:00:43.809327+00:00"}