{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:53UWIQLFGSLDVHWUY7ARV2GLR3","short_pith_number":"pith:53UWIQLF","schema_version":"1.0","canonical_sha256":"eee964416534963a9ed4c7c11ae8cb8eddcd18ecd83b28f68b8f14084473b4ca","source":{"kind":"arxiv","id":"1703.04522","version":3},"attestation_state":"computed","paper":{"title":"Odd viscosity in two-dimensional incompressible fluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.flu-dyn","authors_text":"Alexander G. Abanov, Sriram Ganeshan","submitted_at":"2017-03-01T21:34:51Z","abstract_excerpt":"In this work, we present observable consequences of parity-violating odd viscosity term in incompressible 2+1D hydrodynamics. For boundary conditions depending on the velocity field (flow) alone we show that: (i) The fluid flow quantified by the velocity field is independent of odd viscosity, (ii) The force acting on a closed contour is independent of odd viscosity, and (iii) The odd viscosity part of torque on a closed contour is proportional to the rate of change of area enclosed by the contour with the proportionality constant being twice the odd viscosity. The last statement allows us to d"},"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":"1703.04522","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-03-01T21:34:51Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"0891a7b63ee1143c93a7ec6284c3b32251a25e9ae4defb17dd747f4aa5dff6d6","abstract_canon_sha256":"3a80cd42984cd5d2efde9ddd68a93732028600d94f21878e08d3996a7bb37649"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:50.480090Z","signature_b64":"Q4aDPvOoji5212bilGq1vowOH2xaBTGSKPYxllGb4dO7Erok9SVtp1Cwq5J36xraRTs9kvunGqZ5//xFXFLlAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eee964416534963a9ed4c7c11ae8cb8eddcd18ecd83b28f68b8f14084473b4ca","last_reissued_at":"2026-05-18T00:33:50.479605Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:50.479605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Odd viscosity in two-dimensional incompressible fluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.flu-dyn","authors_text":"Alexander G. Abanov, Sriram Ganeshan","submitted_at":"2017-03-01T21:34:51Z","abstract_excerpt":"In this work, we present observable consequences of parity-violating odd viscosity term in incompressible 2+1D hydrodynamics. For boundary conditions depending on the velocity field (flow) alone we show that: (i) The fluid flow quantified by the velocity field is independent of odd viscosity, (ii) The force acting on a closed contour is independent of odd viscosity, and (iii) The odd viscosity part of torque on a closed contour is proportional to the rate of change of area enclosed by the contour with the proportionality constant being twice the odd viscosity. The last statement allows us to d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.04522","kind":"arxiv","version":3},"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":"1703.04522","created_at":"2026-05-18T00:33:50.479696+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.04522v3","created_at":"2026-05-18T00:33:50.479696+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.04522","created_at":"2026-05-18T00:33:50.479696+00:00"},{"alias_kind":"pith_short_12","alias_value":"53UWIQLFGSLD","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"53UWIQLFGSLDVHWU","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"53UWIQLF","created_at":"2026-05-18T12:31:00.734936+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/53UWIQLFGSLDVHWUY7ARV2GLR3","json":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3.json","graph_json":"https://pith.science/api/pith-number/53UWIQLFGSLDVHWUY7ARV2GLR3/graph.json","events_json":"https://pith.science/api/pith-number/53UWIQLFGSLDVHWUY7ARV2GLR3/events.json","paper":"https://pith.science/paper/53UWIQLF"},"agent_actions":{"view_html":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3","download_json":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3.json","view_paper":"https://pith.science/paper/53UWIQLF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.04522&json=true","fetch_graph":"https://pith.science/api/pith-number/53UWIQLFGSLDVHWUY7ARV2GLR3/graph.json","fetch_events":"https://pith.science/api/pith-number/53UWIQLFGSLDVHWUY7ARV2GLR3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3/action/storage_attestation","attest_author":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3/action/author_attestation","sign_citation":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3/action/citation_signature","submit_replication":"https://pith.science/pith/53UWIQLFGSLDVHWUY7ARV2GLR3/action/replication_record"}},"created_at":"2026-05-18T00:33:50.479696+00:00","updated_at":"2026-05-18T00:33:50.479696+00:00"}