{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:F5B6ZL4RKGU4NZ7E6TONZ7FZ3F","short_pith_number":"pith:F5B6ZL4R","schema_version":"1.0","canonical_sha256":"2f43ecaf9151a9c6e7e4f4dcdcfcb9d97fea6a90065a91db891b8b0d536002a3","source":{"kind":"arxiv","id":"1212.6586","version":1},"attestation_state":"computed","paper":{"title":"The Turbulent 'Mixing' Layer as a Problem in the Non-equilibrium Statistical Mechanics of a Vortex Gas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"physics.flu-dyn","authors_text":"N.D. Hari Dass, Roddam Narasimha, Saikishan Suryanarayanan","submitted_at":"2012-12-29T03:21:52Z","abstract_excerpt":"The objective of this paper is to unravel any relations that may exist between turbulent shear flows and statistical mechanics, through a detailed numerical investigation in the simplest case where both can be well defined. The shear flow considered for the purpose is the 2D temporal mixing layer, which is a time-dependent flow that is statistically homogeneous in the streamwise direction (x) and evolves from a plane vortex sheet in the direction normal to it (y) in a periodic-in-x domain with period L. The connections to statistical mechanics are explored by revisiting, via extensive computer"},"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":"1212.6586","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2012-12-29T03:21:52Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"b6599598f14dd9b21c53a1c2d0d7e709278ff87eb2c3d40089f0e927c0495ee5","abstract_canon_sha256":"da368ff8b789cdf1d6932438c393cced5b03459f2e6d5eea95b0fafd836db060"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:37:31.467773Z","signature_b64":"7r7um+Ej80+arOxVpHKtyfpP5lLOXI5sGlsKCG/vuHxE5L0HBs7LvdDN+IPubsuEeGSdvfpt+DlgSM0MP6ZHBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f43ecaf9151a9c6e7e4f4dcdcfcb9d97fea6a90065a91db891b8b0d536002a3","last_reissued_at":"2026-05-18T03:37:31.467038Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:37:31.467038Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Turbulent 'Mixing' Layer as a Problem in the Non-equilibrium Statistical Mechanics of a Vortex Gas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"physics.flu-dyn","authors_text":"N.D. Hari Dass, Roddam Narasimha, Saikishan Suryanarayanan","submitted_at":"2012-12-29T03:21:52Z","abstract_excerpt":"The objective of this paper is to unravel any relations that may exist between turbulent shear flows and statistical mechanics, through a detailed numerical investigation in the simplest case where both can be well defined. The shear flow considered for the purpose is the 2D temporal mixing layer, which is a time-dependent flow that is statistically homogeneous in the streamwise direction (x) and evolves from a plane vortex sheet in the direction normal to it (y) in a periodic-in-x domain with period L. The connections to statistical mechanics are explored by revisiting, via extensive computer"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.6586","kind":"arxiv","version":1},"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":"1212.6586","created_at":"2026-05-18T03:37:31.467147+00:00"},{"alias_kind":"arxiv_version","alias_value":"1212.6586v1","created_at":"2026-05-18T03:37:31.467147+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.6586","created_at":"2026-05-18T03:37:31.467147+00:00"},{"alias_kind":"pith_short_12","alias_value":"F5B6ZL4RKGU4","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"F5B6ZL4RKGU4NZ7E","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"F5B6ZL4R","created_at":"2026-05-18T12:27:04.183437+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/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F","json":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F.json","graph_json":"https://pith.science/api/pith-number/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/graph.json","events_json":"https://pith.science/api/pith-number/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/events.json","paper":"https://pith.science/paper/F5B6ZL4R"},"agent_actions":{"view_html":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F","download_json":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F.json","view_paper":"https://pith.science/paper/F5B6ZL4R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1212.6586&json=true","fetch_graph":"https://pith.science/api/pith-number/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/graph.json","fetch_events":"https://pith.science/api/pith-number/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/action/storage_attestation","attest_author":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/action/author_attestation","sign_citation":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/action/citation_signature","submit_replication":"https://pith.science/pith/F5B6ZL4RKGU4NZ7E6TONZ7FZ3F/action/replication_record"}},"created_at":"2026-05-18T03:37:31.467147+00:00","updated_at":"2026-05-18T03:37:31.467147+00:00"}