{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:YK7LKTPUVNL2YBANLHRUWO6LWB","short_pith_number":"pith:YK7LKTPU","canonical_record":{"source":{"id":"1306.0422","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-06-03T14:13:19Z","cross_cats_sorted":["cond-mat.str-el","physics.flu-dyn","quant-ph"],"title_canon_sha256":"b30e54664c4e0c8f66b2fb5a1b885c7eab4ea326ea47900add89710cad8ed432","abstract_canon_sha256":"4dbd11d5abab736335e1857bedcfd06679a520d9e9c62da1e1ed7a27684c82d0"},"schema_version":"1.0"},"canonical_sha256":"c2beb54df4ab57ac040d59e34b3bcbb07a774e15133a66fd604d00b4afbd25b9","source":{"kind":"arxiv","id":"1306.0422","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.0422","created_at":"2026-05-18T03:10:44Z"},{"alias_kind":"arxiv_version","alias_value":"1306.0422v2","created_at":"2026-05-18T03:10:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.0422","created_at":"2026-05-18T03:10:44Z"},{"alias_kind":"pith_short_12","alias_value":"YK7LKTPUVNL2","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YK7LKTPUVNL2YBAN","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YK7LKTPU","created_at":"2026-05-18T12:28:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:YK7LKTPUVNL2YBANLHRUWO6LWB","target":"record","payload":{"canonical_record":{"source":{"id":"1306.0422","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-06-03T14:13:19Z","cross_cats_sorted":["cond-mat.str-el","physics.flu-dyn","quant-ph"],"title_canon_sha256":"b30e54664c4e0c8f66b2fb5a1b885c7eab4ea326ea47900add89710cad8ed432","abstract_canon_sha256":"4dbd11d5abab736335e1857bedcfd06679a520d9e9c62da1e1ed7a27684c82d0"},"schema_version":"1.0"},"canonical_sha256":"c2beb54df4ab57ac040d59e34b3bcbb07a774e15133a66fd604d00b4afbd25b9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:10:44.695728Z","signature_b64":"lqhEMXxSX7E5mZAS68kEZW5rlwSzqkddO78I3jOLuLgw84fcHbVBMHtheSp8ZJN0kuZ00BE2moDAD9WHbz7jCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c2beb54df4ab57ac040d59e34b3bcbb07a774e15133a66fd604d00b4afbd25b9","last_reissued_at":"2026-05-18T03:10:44.695082Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:10:44.695082Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.0422","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:10:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QhQZiXmsoEUGoRUkK/yiLJY4paC3KqrJzbE9trXwJ2t21tlwD3WvmVTRpv26t/WQ/H4SeQVBUDFcQPw2wjjBCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T10:48:35.732651Z"},"content_sha256":"7abd7dd91921f646a0c4858d43ed5a0b98b7a4cb927f33f13a8858dcf553322a","schema_version":"1.0","event_id":"sha256:7abd7dd91921f646a0c4858d43ed5a0b98b7a4cb927f33f13a8858dcf553322a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:YK7LKTPUVNL2YBANLHRUWO6LWB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum-statistics-induced flow patterns in driven ideal Fermi gases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","physics.flu-dyn","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Marco Beria, Markus M\\\"uller, Massimiliano Di Ventra, Yasir Iqbal","submitted_at":"2013-06-03T14:13:19Z","abstract_excerpt":"While classical or quantum interacting liquids become turbulent under sufficiently strong driving, it is not obvious what flow pattern an ideal quantum gas develops under similar conditions. Unlike classical noninteracting particles which exhibit rather trivial flow, ideal fermions have to satisfy the exclusion principle, which acts as a form of collective repulsion. We thus study the flow of an ideal Fermi gas as it is driven out of a narrow orifice of width comparable to the Fermi wavelength, employing both a microcanonical approach to transport, and solving a Lindblad equation for Markovian"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.0422","kind":"arxiv","version":2},"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":"2026-05-18T03:10:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z8nA742oL7bXne5B3Gizv13vvpcegoUhBOIpxvcgXYyatApe9GYEIzw5qBjm8bbf8uxVWe/DWNRA6UKVtntfAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T10:48:35.733307Z"},"content_sha256":"8fb5460747eabcbd30a1374ad16c4bb649c8b139aec38808a8db31ed0f7e8086","schema_version":"1.0","event_id":"sha256:8fb5460747eabcbd30a1374ad16c4bb649c8b139aec38808a8db31ed0f7e8086"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YK7LKTPUVNL2YBANLHRUWO6LWB/bundle.json","state_url":"https://pith.science/pith/YK7LKTPUVNL2YBANLHRUWO6LWB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YK7LKTPUVNL2YBANLHRUWO6LWB/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":"2026-06-01T10:48:35Z","links":{"resolver":"https://pith.science/pith/YK7LKTPUVNL2YBANLHRUWO6LWB","bundle":"https://pith.science/pith/YK7LKTPUVNL2YBANLHRUWO6LWB/bundle.json","state":"https://pith.science/pith/YK7LKTPUVNL2YBANLHRUWO6LWB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YK7LKTPUVNL2YBANLHRUWO6LWB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:YK7LKTPUVNL2YBANLHRUWO6LWB","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":"4dbd11d5abab736335e1857bedcfd06679a520d9e9c62da1e1ed7a27684c82d0","cross_cats_sorted":["cond-mat.str-el","physics.flu-dyn","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-06-03T14:13:19Z","title_canon_sha256":"b30e54664c4e0c8f66b2fb5a1b885c7eab4ea326ea47900add89710cad8ed432"},"schema_version":"1.0","source":{"id":"1306.0422","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.0422","created_at":"2026-05-18T03:10:44Z"},{"alias_kind":"arxiv_version","alias_value":"1306.0422v2","created_at":"2026-05-18T03:10:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.0422","created_at":"2026-05-18T03:10:44Z"},{"alias_kind":"pith_short_12","alias_value":"YK7LKTPUVNL2","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YK7LKTPUVNL2YBAN","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YK7LKTPU","created_at":"2026-05-18T12:28:06Z"}],"graph_snapshots":[{"event_id":"sha256:8fb5460747eabcbd30a1374ad16c4bb649c8b139aec38808a8db31ed0f7e8086","target":"graph","created_at":"2026-05-18T03:10:44Z","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":"While classical or quantum interacting liquids become turbulent under sufficiently strong driving, it is not obvious what flow pattern an ideal quantum gas develops under similar conditions. Unlike classical noninteracting particles which exhibit rather trivial flow, ideal fermions have to satisfy the exclusion principle, which acts as a form of collective repulsion. We thus study the flow of an ideal Fermi gas as it is driven out of a narrow orifice of width comparable to the Fermi wavelength, employing both a microcanonical approach to transport, and solving a Lindblad equation for Markovian","authors_text":"Marco Beria, Markus M\\\"uller, Massimiliano Di Ventra, Yasir Iqbal","cross_cats":["cond-mat.str-el","physics.flu-dyn","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-06-03T14:13:19Z","title":"Quantum-statistics-induced flow patterns in driven ideal Fermi gases"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.0422","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":"sha256:7abd7dd91921f646a0c4858d43ed5a0b98b7a4cb927f33f13a8858dcf553322a","target":"record","created_at":"2026-05-18T03:10:44Z","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":"4dbd11d5abab736335e1857bedcfd06679a520d9e9c62da1e1ed7a27684c82d0","cross_cats_sorted":["cond-mat.str-el","physics.flu-dyn","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2013-06-03T14:13:19Z","title_canon_sha256":"b30e54664c4e0c8f66b2fb5a1b885c7eab4ea326ea47900add89710cad8ed432"},"schema_version":"1.0","source":{"id":"1306.0422","kind":"arxiv","version":2}},"canonical_sha256":"c2beb54df4ab57ac040d59e34b3bcbb07a774e15133a66fd604d00b4afbd25b9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c2beb54df4ab57ac040d59e34b3bcbb07a774e15133a66fd604d00b4afbd25b9","first_computed_at":"2026-05-18T03:10:44.695082Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:10:44.695082Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lqhEMXxSX7E5mZAS68kEZW5rlwSzqkddO78I3jOLuLgw84fcHbVBMHtheSp8ZJN0kuZ00BE2moDAD9WHbz7jCg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:10:44.695728Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.0422","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7abd7dd91921f646a0c4858d43ed5a0b98b7a4cb927f33f13a8858dcf553322a","sha256:8fb5460747eabcbd30a1374ad16c4bb649c8b139aec38808a8db31ed0f7e8086"],"state_sha256":"be16e72fb1386b6e250aea2e94926f36a1867a49d0c95d90b922fe7dc9967053"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"142dK0WLEIAnXv/coAZ+fpXrgoRWmbTj8JZDM7OOG4NNxiQos/z6+krPhUWYUYxPtWrUW3grOBzDxITaCPykBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T10:48:35.736543Z","bundle_sha256":"867c7770a9d389217a4ea03175e0b20b5f9a5d8aca443fd410c6182309712104"}}