{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:LSZM72VW6H55UER5A3T75MSFXW","short_pith_number":"pith:LSZM72VW","schema_version":"1.0","canonical_sha256":"5cb2cfeab6f1fbda123d06e7feb245bdbd0fb175923d1bce21bd255d8b30b102","source":{"kind":"arxiv","id":"1002.0287","version":2},"attestation_state":"computed","paper":{"title":"Mott-insulator phases of spin-3/2 fermions in the presence of quadratic Zeeman coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Arturo Arg\\\"uelles, Karen Rodriguez, Luis Santos, Maria Colom\\'e-Tatch\\'e, Temo Vekua","submitted_at":"2010-02-01T18:49:24Z","abstract_excerpt":"We study the influence of the quadratic Zeeman effect in the Mott-insulator phases of hard-core spin-3/2 fermions. We show that contrary to spinor bosons, any quadratic Zeeman coupling preserves a $SU(2)\\otimes SU(2)$ symmetry, leading for large-enough quadratic Zeeman coupling to an isotropic pseudo-spin-1/2 Heisenberg antiferromagnet. Depending on the scattering lengths, on 1D lattices the quadratic Zeeman coupling can induce either a Kosterlitz-Thouless transition between a gapped dimerized spin-3/2 phase and a gapless pseudo-spin-1/2 antiferromagnet, or a commensurate-incommensurate transi"},"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":"1002.0287","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2010-02-01T18:49:24Z","cross_cats_sorted":[],"title_canon_sha256":"8a4214a12b8aeed2834547e068edf7c5eeed9c52c7ee4f081c377d4e39b58b59","abstract_canon_sha256":"83b14dc4adf744352b14ca6d8d62f99bcca3e3aff4991a074cb5234594ff02ef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:41:44.852131Z","signature_b64":"sCsI3Tkz/Y2hgr1r0r9YywvjuFAmkH63+KpNpVQnh8+DzEZHQCEV6rEbdSJ0EyfV1qtcJMbeT0Mgd7LkcQtABA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5cb2cfeab6f1fbda123d06e7feb245bdbd0fb175923d1bce21bd255d8b30b102","last_reissued_at":"2026-05-18T04:41:44.851708Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:41:44.851708Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mott-insulator phases of spin-3/2 fermions in the presence of quadratic Zeeman coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Arturo Arg\\\"uelles, Karen Rodriguez, Luis Santos, Maria Colom\\'e-Tatch\\'e, Temo Vekua","submitted_at":"2010-02-01T18:49:24Z","abstract_excerpt":"We study the influence of the quadratic Zeeman effect in the Mott-insulator phases of hard-core spin-3/2 fermions. We show that contrary to spinor bosons, any quadratic Zeeman coupling preserves a $SU(2)\\otimes SU(2)$ symmetry, leading for large-enough quadratic Zeeman coupling to an isotropic pseudo-spin-1/2 Heisenberg antiferromagnet. Depending on the scattering lengths, on 1D lattices the quadratic Zeeman coupling can induce either a Kosterlitz-Thouless transition between a gapped dimerized spin-3/2 phase and a gapless pseudo-spin-1/2 antiferromagnet, or a commensurate-incommensurate transi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1002.0287","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":"1002.0287","created_at":"2026-05-18T04:41:44.851773+00:00"},{"alias_kind":"arxiv_version","alias_value":"1002.0287v2","created_at":"2026-05-18T04:41:44.851773+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1002.0287","created_at":"2026-05-18T04:41:44.851773+00:00"},{"alias_kind":"pith_short_12","alias_value":"LSZM72VW6H55","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_16","alias_value":"LSZM72VW6H55UER5","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_8","alias_value":"LSZM72VW","created_at":"2026-05-18T12:26:10.704358+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/LSZM72VW6H55UER5A3T75MSFXW","json":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW.json","graph_json":"https://pith.science/api/pith-number/LSZM72VW6H55UER5A3T75MSFXW/graph.json","events_json":"https://pith.science/api/pith-number/LSZM72VW6H55UER5A3T75MSFXW/events.json","paper":"https://pith.science/paper/LSZM72VW"},"agent_actions":{"view_html":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW","download_json":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW.json","view_paper":"https://pith.science/paper/LSZM72VW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1002.0287&json=true","fetch_graph":"https://pith.science/api/pith-number/LSZM72VW6H55UER5A3T75MSFXW/graph.json","fetch_events":"https://pith.science/api/pith-number/LSZM72VW6H55UER5A3T75MSFXW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW/action/storage_attestation","attest_author":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW/action/author_attestation","sign_citation":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW/action/citation_signature","submit_replication":"https://pith.science/pith/LSZM72VW6H55UER5A3T75MSFXW/action/replication_record"}},"created_at":"2026-05-18T04:41:44.851773+00:00","updated_at":"2026-05-18T04:41:44.851773+00:00"}