{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:DXI2RQZFHSQQXR5OEG7KGC4ZMR","short_pith_number":"pith:DXI2RQZF","schema_version":"1.0","canonical_sha256":"1dd1a8c3253ca10bc7ae21bea30b99646a0b8dd947c50c86d041d5390621b08d","source":{"kind":"arxiv","id":"1206.0145","version":1},"attestation_state":"computed","paper":{"title":"A Dynamical Self-Consistent Finite Temperature Kinetic Theory: The ZNG Scheme","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. J. Allen, C. F. Barenghi, E. Zaremba, N. P. Proukakis","submitted_at":"2012-06-01T11:06:41Z","abstract_excerpt":"We review a self-consistent scheme for modelling trapped weakly-interacting quantum gases at temperatures where the condensate coexists with a significant thermal cloud. This method has been applied to atomic gases by Zaremba, Nikuni, and Griffin, and is often referred to as ZNG. It describes both mean-field-dominated and hydrodynamic regimes, except at very low temperatures or in the regime of large fluctuations. Condensate dynamics are described by a dissipative Gross-Pitaevskii equation (or the corresponding quantum hydrodynamic equation with a source term), while the non-condensate evoluti"},"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":"1206.0145","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2012-06-01T11:06:41Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"fb3e2738e0dde2facb5d5d9f244910dcbebf59b2ce7caf71b18135a3d3fd6a02","abstract_canon_sha256":"3e81f0138a030effc845f110ccdcb11a70248728bb339f7b196bbd1608c0243b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:02.648522Z","signature_b64":"Sfk6k3bZJadFgaXssWZtGSGzU3olVLSreXPq4d/SMsAnl3DHpJXQW08+ymKh/tEnWuyF4iausMtdRIgybE1DCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1dd1a8c3253ca10bc7ae21bea30b99646a0b8dd947c50c86d041d5390621b08d","last_reissued_at":"2026-05-18T00:37:02.647979Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:02.647979Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Dynamical Self-Consistent Finite Temperature Kinetic Theory: The ZNG Scheme","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. J. Allen, C. F. Barenghi, E. Zaremba, N. P. Proukakis","submitted_at":"2012-06-01T11:06:41Z","abstract_excerpt":"We review a self-consistent scheme for modelling trapped weakly-interacting quantum gases at temperatures where the condensate coexists with a significant thermal cloud. This method has been applied to atomic gases by Zaremba, Nikuni, and Griffin, and is often referred to as ZNG. It describes both mean-field-dominated and hydrodynamic regimes, except at very low temperatures or in the regime of large fluctuations. Condensate dynamics are described by a dissipative Gross-Pitaevskii equation (or the corresponding quantum hydrodynamic equation with a source term), while the non-condensate evoluti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.0145","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":"1206.0145","created_at":"2026-05-18T00:37:02.648076+00:00"},{"alias_kind":"arxiv_version","alias_value":"1206.0145v1","created_at":"2026-05-18T00:37:02.648076+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.0145","created_at":"2026-05-18T00:37:02.648076+00:00"},{"alias_kind":"pith_short_12","alias_value":"DXI2RQZFHSQQ","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"DXI2RQZFHSQQXR5O","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"DXI2RQZF","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/DXI2RQZFHSQQXR5OEG7KGC4ZMR","json":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR.json","graph_json":"https://pith.science/api/pith-number/DXI2RQZFHSQQXR5OEG7KGC4ZMR/graph.json","events_json":"https://pith.science/api/pith-number/DXI2RQZFHSQQXR5OEG7KGC4ZMR/events.json","paper":"https://pith.science/paper/DXI2RQZF"},"agent_actions":{"view_html":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR","download_json":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR.json","view_paper":"https://pith.science/paper/DXI2RQZF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1206.0145&json=true","fetch_graph":"https://pith.science/api/pith-number/DXI2RQZFHSQQXR5OEG7KGC4ZMR/graph.json","fetch_events":"https://pith.science/api/pith-number/DXI2RQZFHSQQXR5OEG7KGC4ZMR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR/action/storage_attestation","attest_author":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR/action/author_attestation","sign_citation":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR/action/citation_signature","submit_replication":"https://pith.science/pith/DXI2RQZFHSQQXR5OEG7KGC4ZMR/action/replication_record"}},"created_at":"2026-05-18T00:37:02.648076+00:00","updated_at":"2026-05-18T00:37:02.648076+00:00"}