{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:ELUGVFJCOEK2O55H6VUFGKGPYK","short_pith_number":"pith:ELUGVFJC","schema_version":"1.0","canonical_sha256":"22e86a95227115a777a7f5685328cfc2957c516b20e6b5b7895c2f189b1c4621","source":{"kind":"arxiv","id":"1607.02898","version":2},"attestation_state":"computed","paper":{"title":"Phase dependent advection-diffusion in drift wave - zonal flow turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.AO"],"primary_cat":"physics.plasm-ph","authors_text":"Johan Anderson, Sara Moradi","submitted_at":"2016-07-11T10:57:08Z","abstract_excerpt":"In plasma turbulence theory, due to the complexity of the system with many non-linearly interacting waves, the dynamics of the phases is often disregarded and the so-called random-phase approximation (RPA) is used assuming the existence of a Chirikov-like criterion for the onset of wave stochasticity. The dynamical amplitudes are represented as complex numbers, $\\psi = \\psi_r + i\\psi_i = ae^{i\\theta}$, with the amplitudes slowly varying whereas the phases are rapidly varying and, in particular, distributed uniformly over the interval $[0;2\\pi)$. However, one could expect that the phase dynamic"},"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":"1607.02898","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-07-11T10:57:08Z","cross_cats_sorted":["nlin.AO"],"title_canon_sha256":"23131f49b3c0fce0a641f5140049fb4552fa789a156f6a7c8c90f691a72b4923","abstract_canon_sha256":"d35eee0a6498d5d19296832fce7af33a3ec5797834492acc94ea3584abfa41e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:09.726414Z","signature_b64":"8zP9CU3tyU498YbbR15D8rZpXweDbx7fzZd+orgxz2GqppX7qtXO08rzgPZseXszxQ4H4vis7UpbTxy/GV4rAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22e86a95227115a777a7f5685328cfc2957c516b20e6b5b7895c2f189b1c4621","last_reissued_at":"2026-05-18T01:11:09.725579Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:09.725579Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase dependent advection-diffusion in drift wave - zonal flow turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.AO"],"primary_cat":"physics.plasm-ph","authors_text":"Johan Anderson, Sara Moradi","submitted_at":"2016-07-11T10:57:08Z","abstract_excerpt":"In plasma turbulence theory, due to the complexity of the system with many non-linearly interacting waves, the dynamics of the phases is often disregarded and the so-called random-phase approximation (RPA) is used assuming the existence of a Chirikov-like criterion for the onset of wave stochasticity. The dynamical amplitudes are represented as complex numbers, $\\psi = \\psi_r + i\\psi_i = ae^{i\\theta}$, with the amplitudes slowly varying whereas the phases are rapidly varying and, in particular, distributed uniformly over the interval $[0;2\\pi)$. However, one could expect that the phase dynamic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.02898","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":"1607.02898","created_at":"2026-05-18T01:11:09.725656+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.02898v2","created_at":"2026-05-18T01:11:09.725656+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.02898","created_at":"2026-05-18T01:11:09.725656+00:00"},{"alias_kind":"pith_short_12","alias_value":"ELUGVFJCOEK2","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_16","alias_value":"ELUGVFJCOEK2O55H","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_8","alias_value":"ELUGVFJC","created_at":"2026-05-18T12:30:12.583610+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/ELUGVFJCOEK2O55H6VUFGKGPYK","json":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK.json","graph_json":"https://pith.science/api/pith-number/ELUGVFJCOEK2O55H6VUFGKGPYK/graph.json","events_json":"https://pith.science/api/pith-number/ELUGVFJCOEK2O55H6VUFGKGPYK/events.json","paper":"https://pith.science/paper/ELUGVFJC"},"agent_actions":{"view_html":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK","download_json":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK.json","view_paper":"https://pith.science/paper/ELUGVFJC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.02898&json=true","fetch_graph":"https://pith.science/api/pith-number/ELUGVFJCOEK2O55H6VUFGKGPYK/graph.json","fetch_events":"https://pith.science/api/pith-number/ELUGVFJCOEK2O55H6VUFGKGPYK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK/action/storage_attestation","attest_author":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK/action/author_attestation","sign_citation":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK/action/citation_signature","submit_replication":"https://pith.science/pith/ELUGVFJCOEK2O55H6VUFGKGPYK/action/replication_record"}},"created_at":"2026-05-18T01:11:09.725656+00:00","updated_at":"2026-05-18T01:11:09.725656+00:00"}