{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:3FBTAZHSW5IMNTLGCIGL2N22SN","short_pith_number":"pith:3FBTAZHS","canonical_record":{"source":{"id":"1206.0584","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2012-06-04T11:26:54Z","cross_cats_sorted":[],"title_canon_sha256":"75f8a51f8326c8ed58e74b0fdabeb28116b55abd991126197a2a70e00864b47e","abstract_canon_sha256":"6a33efce389aed4972317b724f6ca17136800ba5e7db8327b97ff6e4b6a2c332"},"schema_version":"1.0"},"canonical_sha256":"d9433064f2b750c6cd66120cbd375a9361ca41d2a338afacaea368e16124fb57","source":{"kind":"arxiv","id":"1206.0584","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.0584","created_at":"2026-05-18T03:42:55Z"},{"alias_kind":"arxiv_version","alias_value":"1206.0584v4","created_at":"2026-05-18T03:42:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.0584","created_at":"2026-05-18T03:42:55Z"},{"alias_kind":"pith_short_12","alias_value":"3FBTAZHSW5IM","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_16","alias_value":"3FBTAZHSW5IMNTLG","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_8","alias_value":"3FBTAZHS","created_at":"2026-05-18T12:26:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:3FBTAZHSW5IMNTLGCIGL2N22SN","target":"record","payload":{"canonical_record":{"source":{"id":"1206.0584","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2012-06-04T11:26:54Z","cross_cats_sorted":[],"title_canon_sha256":"75f8a51f8326c8ed58e74b0fdabeb28116b55abd991126197a2a70e00864b47e","abstract_canon_sha256":"6a33efce389aed4972317b724f6ca17136800ba5e7db8327b97ff6e4b6a2c332"},"schema_version":"1.0"},"canonical_sha256":"d9433064f2b750c6cd66120cbd375a9361ca41d2a338afacaea368e16124fb57","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:42:55.773151Z","signature_b64":"koS2vRZknTEZFHgJjKaAPp1lBETdKIbWOLcyo9emsjlv10BQeEZlCmpXYpvBZQtwN5Jz9e0ajwd9lt+d4KzwBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9433064f2b750c6cd66120cbd375a9361ca41d2a338afacaea368e16124fb57","last_reissued_at":"2026-05-18T03:42:55.772489Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:42:55.772489Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1206.0584","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:42:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7AXRP17RnnXcMY3UCrrhQ+YbPPya88lCLnjPu8HeYUlaqUTvv2sbZal6clV6bG0Xg8RDYnObDXJebqQdXiHECg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T06:31:36.052773Z"},"content_sha256":"cd435d71e7af2b42201d9908ff4ebafbceb0667bc7582b002492ed8411e420cd","schema_version":"1.0","event_id":"sha256:cd435d71e7af2b42201d9908ff4ebafbceb0667bc7582b002492ed8411e420cd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:3FBTAZHSW5IMNTLGCIGL2N22SN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Considering Fluctuation Energy as a Measure of Gyrokinetic Turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"G. G. Plunk, T. Tatsuno, W. Dorland","submitted_at":"2012-06-04T11:26:54Z","abstract_excerpt":"In gyrokinetic theory there are two quadratic measures of fluctuation energy, left invariant under nonlinear interactions, that constrain the turbulence. The recent work of Plunk and Tatsuno [Phys. Rev. Lett. 106, 165003 (2011)] reported on the novel consequences that this constraint has on the direction and locality of spectral energy transfer. This paper builds on that work. We provide detailed analysis in support of the results of Plunk and Tatsuno but also significantly broaden the scope and use additional methods to address the problem of energy transfer. The perspective taken here is tha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.0584","kind":"arxiv","version":4},"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":"2026-05-18T03:42:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qjd1JwGUvtzfTk192rIJsdvJ4u3IOAsEVSZequJCXt+4nirKH1ogexBdNHdFTvSKpOikiHfN10YVCFpkc20yBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T06:31:36.053512Z"},"content_sha256":"7c64e470c2a3b9480dd90ed297cc0c3b0475a135976f831e84062a112c215388","schema_version":"1.0","event_id":"sha256:7c64e470c2a3b9480dd90ed297cc0c3b0475a135976f831e84062a112c215388"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3FBTAZHSW5IMNTLGCIGL2N22SN/bundle.json","state_url":"https://pith.science/pith/3FBTAZHSW5IMNTLGCIGL2N22SN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3FBTAZHSW5IMNTLGCIGL2N22SN/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":"2026-06-09T06:31:36Z","links":{"resolver":"https://pith.science/pith/3FBTAZHSW5IMNTLGCIGL2N22SN","bundle":"https://pith.science/pith/3FBTAZHSW5IMNTLGCIGL2N22SN/bundle.json","state":"https://pith.science/pith/3FBTAZHSW5IMNTLGCIGL2N22SN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3FBTAZHSW5IMNTLGCIGL2N22SN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:3FBTAZHSW5IMNTLGCIGL2N22SN","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":"6a33efce389aed4972317b724f6ca17136800ba5e7db8327b97ff6e4b6a2c332","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2012-06-04T11:26:54Z","title_canon_sha256":"75f8a51f8326c8ed58e74b0fdabeb28116b55abd991126197a2a70e00864b47e"},"schema_version":"1.0","source":{"id":"1206.0584","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.0584","created_at":"2026-05-18T03:42:55Z"},{"alias_kind":"arxiv_version","alias_value":"1206.0584v4","created_at":"2026-05-18T03:42:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.0584","created_at":"2026-05-18T03:42:55Z"},{"alias_kind":"pith_short_12","alias_value":"3FBTAZHSW5IM","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_16","alias_value":"3FBTAZHSW5IMNTLG","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_8","alias_value":"3FBTAZHS","created_at":"2026-05-18T12:26:50Z"}],"graph_snapshots":[{"event_id":"sha256:7c64e470c2a3b9480dd90ed297cc0c3b0475a135976f831e84062a112c215388","target":"graph","created_at":"2026-05-18T03:42:55Z","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":"In gyrokinetic theory there are two quadratic measures of fluctuation energy, left invariant under nonlinear interactions, that constrain the turbulence. The recent work of Plunk and Tatsuno [Phys. Rev. Lett. 106, 165003 (2011)] reported on the novel consequences that this constraint has on the direction and locality of spectral energy transfer. This paper builds on that work. We provide detailed analysis in support of the results of Plunk and Tatsuno but also significantly broaden the scope and use additional methods to address the problem of energy transfer. The perspective taken here is tha","authors_text":"G. G. Plunk, T. Tatsuno, W. Dorland","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2012-06-04T11:26:54Z","title":"Considering Fluctuation Energy as a Measure of Gyrokinetic Turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.0584","kind":"arxiv","version":4},"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:cd435d71e7af2b42201d9908ff4ebafbceb0667bc7582b002492ed8411e420cd","target":"record","created_at":"2026-05-18T03:42:55Z","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":"6a33efce389aed4972317b724f6ca17136800ba5e7db8327b97ff6e4b6a2c332","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2012-06-04T11:26:54Z","title_canon_sha256":"75f8a51f8326c8ed58e74b0fdabeb28116b55abd991126197a2a70e00864b47e"},"schema_version":"1.0","source":{"id":"1206.0584","kind":"arxiv","version":4}},"canonical_sha256":"d9433064f2b750c6cd66120cbd375a9361ca41d2a338afacaea368e16124fb57","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d9433064f2b750c6cd66120cbd375a9361ca41d2a338afacaea368e16124fb57","first_computed_at":"2026-05-18T03:42:55.772489Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:42:55.772489Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"koS2vRZknTEZFHgJjKaAPp1lBETdKIbWOLcyo9emsjlv10BQeEZlCmpXYpvBZQtwN5Jz9e0ajwd9lt+d4KzwBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:42:55.773151Z","signed_message":"canonical_sha256_bytes"},"source_id":"1206.0584","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cd435d71e7af2b42201d9908ff4ebafbceb0667bc7582b002492ed8411e420cd","sha256:7c64e470c2a3b9480dd90ed297cc0c3b0475a135976f831e84062a112c215388"],"state_sha256":"363320f9fffdd3a33e0452c74ed2a85fbd3a93b9d833d76515153e02bfe08ae7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mhvYaGTC6QtA1dUUb0Fs2KbVgrr4vyq698LccXJ9bgVhElNKg14SyJBB+SQsm7rp0GHv3yllppDY7qEaBdNZCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T06:31:36.058107Z","bundle_sha256":"e9bd46334d30492ec724828c60219e4825b7b4018d1ffd7ad648fd09483c3698"}}