{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:N2AM2XK7VQ27KJYBCMURMH7OPR","short_pith_number":"pith:N2AM2XK7","schema_version":"1.0","canonical_sha256":"6e80cd5d5fac35f527011329161fee7c49b05c61fd4180c1569c779ef236874c","source":{"kind":"arxiv","id":"1411.5962","version":2},"attestation_state":"computed","paper":{"title":"Strongly correlated states of trapped ultracold fermions in deformed Landau levels","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Trombettoni, M. Burrello, M. Rizzi, M. Roncaglia","submitted_at":"2014-11-21T18:03:31Z","abstract_excerpt":"We analyze the strongly correlated regime of a two-component trapped ultracold fermionic gas in a synthetic non-Abelian U(2) gauge potential, that consists of both a magnetic field and a homogeneous spin-orbit coupling. This gauge potential deforms the Landau levels (LLs) with respect to the Abelian case and exchanges their ordering as a function of the spin-orbit coupling. In view of experimental realizations, we show that a harmonic potential combined with a Zeeman term, gives rise to an angular momentum term, which can be used to test the stability of the correlated states obtained through "},"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":"1411.5962","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2014-11-21T18:03:31Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"bc9451885a011c2d6babf65ae3099530639e8718fda101b05531ea2f563be304","abstract_canon_sha256":"32d1a2c481bfe1848dc88080bdeb879826ab6b98fc781f4100faeee76d8795c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:25:19.759267Z","signature_b64":"YJuO68Zd1FZwPFVm7HyfNJg2W+RygK3rsmlKVw3vIjrxF95szXkpAqY+SsDisV7WyPmdK+n3qKEqZH271MDgCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6e80cd5d5fac35f527011329161fee7c49b05c61fd4180c1569c779ef236874c","last_reissued_at":"2026-05-18T02:25:19.758907Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:25:19.758907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strongly correlated states of trapped ultracold fermions in deformed Landau levels","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Trombettoni, M. Burrello, M. Rizzi, M. Roncaglia","submitted_at":"2014-11-21T18:03:31Z","abstract_excerpt":"We analyze the strongly correlated regime of a two-component trapped ultracold fermionic gas in a synthetic non-Abelian U(2) gauge potential, that consists of both a magnetic field and a homogeneous spin-orbit coupling. This gauge potential deforms the Landau levels (LLs) with respect to the Abelian case and exchanges their ordering as a function of the spin-orbit coupling. In view of experimental realizations, we show that a harmonic potential combined with a Zeeman term, gives rise to an angular momentum term, which can be used to test the stability of the correlated states obtained through "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.5962","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1411.5962","created_at":"2026-05-18T02:25:19.758965+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.5962v2","created_at":"2026-05-18T02:25:19.758965+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.5962","created_at":"2026-05-18T02:25:19.758965+00:00"},{"alias_kind":"pith_short_12","alias_value":"N2AM2XK7VQ27","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_16","alias_value":"N2AM2XK7VQ27KJYB","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_8","alias_value":"N2AM2XK7","created_at":"2026-05-18T12:28:41.024544+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/N2AM2XK7VQ27KJYBCMURMH7OPR","json":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR.json","graph_json":"https://pith.science/api/pith-number/N2AM2XK7VQ27KJYBCMURMH7OPR/graph.json","events_json":"https://pith.science/api/pith-number/N2AM2XK7VQ27KJYBCMURMH7OPR/events.json","paper":"https://pith.science/paper/N2AM2XK7"},"agent_actions":{"view_html":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR","download_json":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR.json","view_paper":"https://pith.science/paper/N2AM2XK7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.5962&json=true","fetch_graph":"https://pith.science/api/pith-number/N2AM2XK7VQ27KJYBCMURMH7OPR/graph.json","fetch_events":"https://pith.science/api/pith-number/N2AM2XK7VQ27KJYBCMURMH7OPR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR/action/storage_attestation","attest_author":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR/action/author_attestation","sign_citation":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR/action/citation_signature","submit_replication":"https://pith.science/pith/N2AM2XK7VQ27KJYBCMURMH7OPR/action/replication_record"}},"created_at":"2026-05-18T02:25:19.758965+00:00","updated_at":"2026-05-18T02:25:19.758965+00:00"}