{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:4IKWFN3SMYCBRSDBCVJA2SEM7B","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":"e4c5e4bf331d70a50de848730d62fca32330e96024f6fd1e952b7210c193b7d0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2011-04-28T08:06:46Z","title_canon_sha256":"aca3a2dca9c3c9b367caa20bac0c07d562255406bae09aca16d1471a8e2abd4f"},"schema_version":"1.0","source":{"id":"1104.5323","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.5323","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"arxiv_version","alias_value":"1104.5323v2","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.5323","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"pith_short_12","alias_value":"4IKWFN3SMYCB","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4IKWFN3SMYCBRSDB","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4IKWFN3S","created_at":"2026-05-18T12:26:20Z"}],"graph_snapshots":[{"event_id":"sha256:a3321f9c2bd6d1a00cf9297717fbe3ecc740de7380d415f10bbddc927708a4af","target":"graph","created_at":"2026-05-18T03:23:34Z","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 simple scheme of forcing turbulence away from decay was introduced by Lundgren some time ago, the `linear forcing', which amounts to a force term linear in the velocity field with a constant coefficient. The evolution of linearly forced turbulence towards a stationary final state, as indicated by direct numerical simulations (DNS), is examined from a theoretical point of view based on symmetry arguments. In order to follow closely the DNS the flow is assumed to live in a cubic domain with periodic boundary conditions. The simplicity of the linear forcing scheme allows one to re-write the pro","authors_text":"E. Akylas, E. Gravanis","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2011-04-28T08:06:46Z","title":"On the stationarity of linearly forced turbulence in finite domains"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.5323","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":"sha256:5e2f62995b26443d8370451cf14491900a1fe809c656ced93341cf1334948e73","target":"record","created_at":"2026-05-18T03:23:34Z","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":"e4c5e4bf331d70a50de848730d62fca32330e96024f6fd1e952b7210c193b7d0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2011-04-28T08:06:46Z","title_canon_sha256":"aca3a2dca9c3c9b367caa20bac0c07d562255406bae09aca16d1471a8e2abd4f"},"schema_version":"1.0","source":{"id":"1104.5323","kind":"arxiv","version":2}},"canonical_sha256":"e21562b772660418c86115520d488cf87a851e3fd75bc44fc4bb2550085c01d6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e21562b772660418c86115520d488cf87a851e3fd75bc44fc4bb2550085c01d6","first_computed_at":"2026-05-18T03:23:34.567893Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:23:34.567893Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+kbrX99aDpoaSPDwhy10pntF8MTiZXAZVQyGkRycVfxAk5E5u3YV+10VMqKKSpXwHlyc5hti5YQfup+VSmfqBA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:23:34.568591Z","signed_message":"canonical_sha256_bytes"},"source_id":"1104.5323","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5e2f62995b26443d8370451cf14491900a1fe809c656ced93341cf1334948e73","sha256:a3321f9c2bd6d1a00cf9297717fbe3ecc740de7380d415f10bbddc927708a4af"],"state_sha256":"26b1658daac3d68e4be6cd68e010fa8f7b4f038ae4bbf3949681cf2b818b8788"}