{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:H2IGSN6TNXFNIZQDERIJPEB6AB","short_pith_number":"pith:H2IGSN6T","canonical_record":{"source":{"id":"1608.05373","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-08-18T18:51:18Z","cross_cats_sorted":["physics.ao-ph"],"title_canon_sha256":"70a44f8ee1a12f9edd032f33dcbd21236138861c1f748335af007113403a8d44","abstract_canon_sha256":"45b697084a5d2186dd5a76d0b1631547f28aaacec964dcc38673a2e3d4a45fba"},"schema_version":"1.0"},"canonical_sha256":"3e906937d36dcad46603245097903e005feb511de0899f0caac046b390af1a70","source":{"kind":"arxiv","id":"1608.05373","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.05373","created_at":"2026-05-18T00:54:47Z"},{"alias_kind":"arxiv_version","alias_value":"1608.05373v2","created_at":"2026-05-18T00:54:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.05373","created_at":"2026-05-18T00:54:47Z"},{"alias_kind":"pith_short_12","alias_value":"H2IGSN6TNXFN","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_16","alias_value":"H2IGSN6TNXFNIZQD","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_8","alias_value":"H2IGSN6T","created_at":"2026-05-18T12:30:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:H2IGSN6TNXFNIZQDERIJPEB6AB","target":"record","payload":{"canonical_record":{"source":{"id":"1608.05373","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-08-18T18:51:18Z","cross_cats_sorted":["physics.ao-ph"],"title_canon_sha256":"70a44f8ee1a12f9edd032f33dcbd21236138861c1f748335af007113403a8d44","abstract_canon_sha256":"45b697084a5d2186dd5a76d0b1631547f28aaacec964dcc38673a2e3d4a45fba"},"schema_version":"1.0"},"canonical_sha256":"3e906937d36dcad46603245097903e005feb511de0899f0caac046b390af1a70","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:47.440626Z","signature_b64":"FGDvhCizvJMnY75fKL5PJz8Qn7cLLEoVxUIjx9B1ms9fRBDLNgQmTT567qXDNBQaku9L+nRQyE8WnHk7PV1hDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3e906937d36dcad46603245097903e005feb511de0899f0caac046b390af1a70","last_reissued_at":"2026-05-18T00:54:47.440085Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:47.440085Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.05373","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:54:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SRSX/peFf5gCqE/dFCqDBLnUml+siiEMI6mZ5aYMt0cm3iAOAA4Ht3cx3AdYFP23CKGlQTF0/qENWmncIXeUCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T12:38:48.337139Z"},"content_sha256":"65d5b2cd4da7a7838147c241293284c99e1e4dd0155afb792eab2d3b7cd74fa7","schema_version":"1.0","event_id":"sha256:65d5b2cd4da7a7838147c241293284c99e1e4dd0155afb792eab2d3b7cd74fa7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:H2IGSN6TNXFNIZQDERIJPEB6AB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Zonal-flow dynamics from a phase-space perspective","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ao-ph"],"primary_cat":"physics.plasm-ph","authors_text":"D. E. Ruiz, E. L. Shi, I. Y. Dodin, J. B. Parker","submitted_at":"2016-08-18T18:51:18Z","abstract_excerpt":"The wave kinetic equation (WKE) describing drift-wave (DW) turbulence is widely used in studies of zonal flows (ZFs) emerging from DW turbulence. However, this formulation neglects the exchange of enstrophy between DWs and ZFs and also ignores effects beyond the geometrical-optics limit. We derive a modified theory that takes both of these effects into account, while still treating DW quanta (\"driftons\") as particles in phase space. The drifton dynamics is described by an equation of the Wigner-Moyal type, which is commonly known in the phase-space formulation of quantum mechanics. In the geom"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.05373","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:54:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sRmueZABwlPPtSyqSiOlwDoWy+jA1meQs5DxlsgSxYl+9wrmeyq0sco9rJByTtTOt5LGwIv1pZc3vGkYdbQIAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T12:38:48.337491Z"},"content_sha256":"2c8dce56b874dfc37ad252d5fe1d71daee127f40d63fa52b398076461a5b5ab5","schema_version":"1.0","event_id":"sha256:2c8dce56b874dfc37ad252d5fe1d71daee127f40d63fa52b398076461a5b5ab5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/H2IGSN6TNXFNIZQDERIJPEB6AB/bundle.json","state_url":"https://pith.science/pith/H2IGSN6TNXFNIZQDERIJPEB6AB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/H2IGSN6TNXFNIZQDERIJPEB6AB/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-28T12:38:48Z","links":{"resolver":"https://pith.science/pith/H2IGSN6TNXFNIZQDERIJPEB6AB","bundle":"https://pith.science/pith/H2IGSN6TNXFNIZQDERIJPEB6AB/bundle.json","state":"https://pith.science/pith/H2IGSN6TNXFNIZQDERIJPEB6AB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/H2IGSN6TNXFNIZQDERIJPEB6AB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:H2IGSN6TNXFNIZQDERIJPEB6AB","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":"45b697084a5d2186dd5a76d0b1631547f28aaacec964dcc38673a2e3d4a45fba","cross_cats_sorted":["physics.ao-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-08-18T18:51:18Z","title_canon_sha256":"70a44f8ee1a12f9edd032f33dcbd21236138861c1f748335af007113403a8d44"},"schema_version":"1.0","source":{"id":"1608.05373","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.05373","created_at":"2026-05-18T00:54:47Z"},{"alias_kind":"arxiv_version","alias_value":"1608.05373v2","created_at":"2026-05-18T00:54:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.05373","created_at":"2026-05-18T00:54:47Z"},{"alias_kind":"pith_short_12","alias_value":"H2IGSN6TNXFN","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_16","alias_value":"H2IGSN6TNXFNIZQD","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_8","alias_value":"H2IGSN6T","created_at":"2026-05-18T12:30:19Z"}],"graph_snapshots":[{"event_id":"sha256:2c8dce56b874dfc37ad252d5fe1d71daee127f40d63fa52b398076461a5b5ab5","target":"graph","created_at":"2026-05-18T00:54:47Z","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":"The wave kinetic equation (WKE) describing drift-wave (DW) turbulence is widely used in studies of zonal flows (ZFs) emerging from DW turbulence. However, this formulation neglects the exchange of enstrophy between DWs and ZFs and also ignores effects beyond the geometrical-optics limit. We derive a modified theory that takes both of these effects into account, while still treating DW quanta (\"driftons\") as particles in phase space. The drifton dynamics is described by an equation of the Wigner-Moyal type, which is commonly known in the phase-space formulation of quantum mechanics. In the geom","authors_text":"D. E. Ruiz, E. L. Shi, I. Y. Dodin, J. B. Parker","cross_cats":["physics.ao-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-08-18T18:51:18Z","title":"Zonal-flow dynamics from a phase-space perspective"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.05373","kind":"arxiv","version":2},"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":"sha256:65d5b2cd4da7a7838147c241293284c99e1e4dd0155afb792eab2d3b7cd74fa7","target":"record","created_at":"2026-05-18T00:54:47Z","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":"45b697084a5d2186dd5a76d0b1631547f28aaacec964dcc38673a2e3d4a45fba","cross_cats_sorted":["physics.ao-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-08-18T18:51:18Z","title_canon_sha256":"70a44f8ee1a12f9edd032f33dcbd21236138861c1f748335af007113403a8d44"},"schema_version":"1.0","source":{"id":"1608.05373","kind":"arxiv","version":2}},"canonical_sha256":"3e906937d36dcad46603245097903e005feb511de0899f0caac046b390af1a70","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3e906937d36dcad46603245097903e005feb511de0899f0caac046b390af1a70","first_computed_at":"2026-05-18T00:54:47.440085Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:54:47.440085Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FGDvhCizvJMnY75fKL5PJz8Qn7cLLEoVxUIjx9B1ms9fRBDLNgQmTT567qXDNBQaku9L+nRQyE8WnHk7PV1hDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:54:47.440626Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.05373","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:65d5b2cd4da7a7838147c241293284c99e1e4dd0155afb792eab2d3b7cd74fa7","sha256:2c8dce56b874dfc37ad252d5fe1d71daee127f40d63fa52b398076461a5b5ab5"],"state_sha256":"a16200ed2322e146516a707667d624813db9073ce0290ce9d1bcbc913bff46d0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xHHxJQoQ5iSQ0JtuOtq0tWZB2hBeEA6TR087RcGNsE07iVnRjK+vzM/p8jYM0Hcss5tcbiAOwYH6cnBR2+WLCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-28T12:38:48.339385Z","bundle_sha256":"46b1d192cf441928e904087c413ac38746ae9c89bb835cca5aa07bb8b96e8f9a"}}