{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:OPNQTUX2DZGVEWTVJ6V6E4DP6O","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"0fee951c4a111fdd77edeae32e82dead9cc2cf7d8664c16c1f3e49347d1305f4","cross_cats_sorted":["nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-06-02T20:39:03Z","title_canon_sha256":"be5fbdbeffd3a04599c4ef6a4794bb2512ca9c2e663b0dd7363133f209ebba90"},"schema_version":"1.0","source":{"id":"1606.00866","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.00866","created_at":"2026-05-18T01:04:20Z"},{"alias_kind":"arxiv_version","alias_value":"1606.00866v1","created_at":"2026-05-18T01:04:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.00866","created_at":"2026-05-18T01:04:20Z"},{"alias_kind":"pith_short_12","alias_value":"OPNQTUX2DZGV","created_at":"2026-05-18T12:30:36Z"},{"alias_kind":"pith_short_16","alias_value":"OPNQTUX2DZGVEWTV","created_at":"2026-05-18T12:30:36Z"},{"alias_kind":"pith_short_8","alias_value":"OPNQTUX2","created_at":"2026-05-18T12:30:36Z"}],"graph_snapshots":[{"event_id":"sha256:ece15dbfc579f878f3f2aad09353324dc49a99c5a3b9596f39153c3e2ba60948","target":"graph","created_at":"2026-05-18T01:04:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"A statistical study of finite Larmor radius (FLR) effects on transport driven by electrostatic drift-waves is presented. The study is based on a reduced discrete Hamiltonian dynamical system known as the gyro-averaged standard map (GSM). In this system, FLR effects are incorporated through the gyro-averaging of a simplified weak-turbulence model of electrostatic fluctuations. Formally, the GSM is a modified version of the standard map in which the perturbation amplitude, $K_0$, becomes $K_0 J_0(\\hat{\\rho})$, where $J_0$ is the zeroth-order Bessel function and $\\hat{\\rho}$ is the Larmor radius.","authors_text":"D. del-Castillo-Negrete, I. L. Caldas, J. D. da Fonseca, . M. Sokolov","cross_cats":["nlin.CD"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-06-02T20:39:03Z","title":"A statistical study of gyro-averaging effects in a reduced model of drift-wave transport"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.00866","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:18befd639aa72686b9a1e84933f0f05de74beffb2391e1041bb4ee153d1eb1eb","target":"record","created_at":"2026-05-18T01:04:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"0fee951c4a111fdd77edeae32e82dead9cc2cf7d8664c16c1f3e49347d1305f4","cross_cats_sorted":["nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-06-02T20:39:03Z","title_canon_sha256":"be5fbdbeffd3a04599c4ef6a4794bb2512ca9c2e663b0dd7363133f209ebba90"},"schema_version":"1.0","source":{"id":"1606.00866","kind":"arxiv","version":1}},"canonical_sha256":"73db09d2fa1e4d525a754fabe2706ff3abc6baf62ba918bd2936e5b20d37f64b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"73db09d2fa1e4d525a754fabe2706ff3abc6baf62ba918bd2936e5b20d37f64b","first_computed_at":"2026-05-18T01:04:20.086311Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:04:20.086311Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gWo8l5bvLOGLoxb/XcL+D1yFbG4O7hpYZn8f9WCn6MhTmDVtXOrY779uXhlmP1vcgZTkl4HiL6VSNC/HNFoiBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:04:20.086862Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.00866","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:18befd639aa72686b9a1e84933f0f05de74beffb2391e1041bb4ee153d1eb1eb","sha256:ece15dbfc579f878f3f2aad09353324dc49a99c5a3b9596f39153c3e2ba60948"],"state_sha256":"f8f645d3b6fbc2d6695e249f970a895b5896e5635f0809eb29ed2b91ff8fa04d"}