{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:DDEL3CUSOCUA2HUWXJOGV7WZXB","short_pith_number":"pith:DDEL3CUS","schema_version":"1.0","canonical_sha256":"18c8bd8a9270a80d1e96ba5c6afed9b8461493c350f53f9ee27f5133b78b7afc","source":{"kind":"arxiv","id":"1306.3124","version":2},"attestation_state":"computed","paper":{"title":"From antiferromagnetic order to magnetic textures in the two dimensional Fermi Hubbard model with synthetic spin orbit interaction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"Beno\\^it Gr\\'emaud, Ji\\v{r}\\'i Min\\'a\\v{r}","submitted_at":"2013-06-13T14:40:05Z","abstract_excerpt":"We study the interacting Fermi-Hubbard model in two spatial dimensions with synthetic gauge coupling of the spin orbit Rashba type, at half-filling. Using real space mean field theory, we numerically determine the phase as a function of the interaction strength for different values of the gauge field parameters. For a fixed value of the gauge field, we observe that when the strength of the repulsive interaction is increased, the system enters into an antiferromagnetic phase, then undergoes a first order phase transition to an non collinear magnetic phase. Depending on the gauge field parameter"},"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":"1306.3124","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-06-13T14:40:05Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"b25b1a04af0a7b6e612e1e2888ae6cd3d91f5643caea56d83938b5d9cd85dc3d","abstract_canon_sha256":"ae28f5fb9288d5fdca23b4474fff9299bc6975a3ce06478e45f5afdcdaa1189d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:03:09.985878Z","signature_b64":"Wt0WjtHr3KKata0eHEL/oTDcRlX5zUn7v14FDSvO17JyvymfikJ36gYJwdajEBKTKp/pB2l93YkSLfldTEQnAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18c8bd8a9270a80d1e96ba5c6afed9b8461493c350f53f9ee27f5133b78b7afc","last_reissued_at":"2026-05-18T03:03:09.985351Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:03:09.985351Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From antiferromagnetic order to magnetic textures in the two dimensional Fermi Hubbard model with synthetic spin orbit interaction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"Beno\\^it Gr\\'emaud, Ji\\v{r}\\'i Min\\'a\\v{r}","submitted_at":"2013-06-13T14:40:05Z","abstract_excerpt":"We study the interacting Fermi-Hubbard model in two spatial dimensions with synthetic gauge coupling of the spin orbit Rashba type, at half-filling. Using real space mean field theory, we numerically determine the phase as a function of the interaction strength for different values of the gauge field parameters. For a fixed value of the gauge field, we observe that when the strength of the repulsive interaction is increased, the system enters into an antiferromagnetic phase, then undergoes a first order phase transition to an non collinear magnetic phase. Depending on the gauge field parameter"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.3124","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":"1306.3124","created_at":"2026-05-18T03:03:09.985439+00:00"},{"alias_kind":"arxiv_version","alias_value":"1306.3124v2","created_at":"2026-05-18T03:03:09.985439+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.3124","created_at":"2026-05-18T03:03:09.985439+00:00"},{"alias_kind":"pith_short_12","alias_value":"DDEL3CUSOCUA","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_16","alias_value":"DDEL3CUSOCUA2HUW","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_8","alias_value":"DDEL3CUS","created_at":"2026-05-18T12:27:40.988391+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/DDEL3CUSOCUA2HUWXJOGV7WZXB","json":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB.json","graph_json":"https://pith.science/api/pith-number/DDEL3CUSOCUA2HUWXJOGV7WZXB/graph.json","events_json":"https://pith.science/api/pith-number/DDEL3CUSOCUA2HUWXJOGV7WZXB/events.json","paper":"https://pith.science/paper/DDEL3CUS"},"agent_actions":{"view_html":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB","download_json":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB.json","view_paper":"https://pith.science/paper/DDEL3CUS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1306.3124&json=true","fetch_graph":"https://pith.science/api/pith-number/DDEL3CUSOCUA2HUWXJOGV7WZXB/graph.json","fetch_events":"https://pith.science/api/pith-number/DDEL3CUSOCUA2HUWXJOGV7WZXB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB/action/storage_attestation","attest_author":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB/action/author_attestation","sign_citation":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB/action/citation_signature","submit_replication":"https://pith.science/pith/DDEL3CUSOCUA2HUWXJOGV7WZXB/action/replication_record"}},"created_at":"2026-05-18T03:03:09.985439+00:00","updated_at":"2026-05-18T03:03:09.985439+00:00"}