{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:XH3O5THTGXD4PCTKUUMO6SE36R","short_pith_number":"pith:XH3O5THT","schema_version":"1.0","canonical_sha256":"b9f6eeccf335c7c78a6aa518ef489bf45206f39e20f4b4bf1340595defc8bb69","source":{"kind":"arxiv","id":"2309.12923","version":2},"attestation_state":"computed","paper":{"title":"Non-Abelian dynamical gauge field and topological superfluids in optical Raman lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Tian-Hua Yang, Xin-Chi Zhou, Xiong-jun Liu, Zhi-Yuan Wang","submitted_at":"2023-09-22T15:23:41Z","abstract_excerpt":"We propose an experimental scheme to realize non-Abelian dynamical gauge field for ultracold fermions, which induces a novel pairing mechanism of topological superfluidity. The dynamical gauge fields arise from nontrivial interplay effect between the strong Zeeman splitting and Hubbard interaction in a two-dimensional (2D) optical Raman lattice. The spin-flip transitions are forbidden by the large Zeeman detuning, but are restored when the Zeeman splitting is compensated by Hubbard interaction. This scheme allows to generate a dynamical non-Abelian gauge field that leads to a Dirac type correl"},"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":"2309.12923","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2023-09-22T15:23:41Z","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con","quant-ph"],"title_canon_sha256":"8bc0ac96ef163b348e5bb75e57490deaa56d3deff91a220c98fffb2040ed4822","abstract_canon_sha256":"120d989c6b23f250b1b7afb64b26807a12a47cfc3982c6c2ee2890c3ffafe207"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:54:23.639225Z","signature_b64":"+U3mamEBqLq3E27suC1OAmoB3L7GuWr3dnd6+9WdButjq+4mNs/7ThKNaQtBngVT3IndYELIlGmdpSkj9fMAAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b9f6eeccf335c7c78a6aa518ef489bf45206f39e20f4b4bf1340595defc8bb69","last_reissued_at":"2026-07-05T06:54:23.638757Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:54:23.638757Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Abelian dynamical gauge field and topological superfluids in optical Raman lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Tian-Hua Yang, Xin-Chi Zhou, Xiong-jun Liu, Zhi-Yuan Wang","submitted_at":"2023-09-22T15:23:41Z","abstract_excerpt":"We propose an experimental scheme to realize non-Abelian dynamical gauge field for ultracold fermions, which induces a novel pairing mechanism of topological superfluidity. The dynamical gauge fields arise from nontrivial interplay effect between the strong Zeeman splitting and Hubbard interaction in a two-dimensional (2D) optical Raman lattice. The spin-flip transitions are forbidden by the large Zeeman detuning, but are restored when the Zeeman splitting is compensated by Hubbard interaction. This scheme allows to generate a dynamical non-Abelian gauge field that leads to a Dirac type correl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.12923","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2309.12923/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2309.12923","created_at":"2026-07-05T06:54:23.638815+00:00"},{"alias_kind":"arxiv_version","alias_value":"2309.12923v2","created_at":"2026-07-05T06:54:23.638815+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.12923","created_at":"2026-07-05T06:54:23.638815+00:00"},{"alias_kind":"pith_short_12","alias_value":"XH3O5THTGXD4","created_at":"2026-07-05T06:54:23.638815+00:00"},{"alias_kind":"pith_short_16","alias_value":"XH3O5THTGXD4PCTK","created_at":"2026-07-05T06:54:23.638815+00:00"},{"alias_kind":"pith_short_8","alias_value":"XH3O5THT","created_at":"2026-07-05T06:54:23.638815+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.13940","citing_title":"Preparation and observation of anomalous counterpropagating edge states in a periodically driven optical Raman lattice","ref_index":82,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R","json":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R.json","graph_json":"https://pith.science/api/pith-number/XH3O5THTGXD4PCTKUUMO6SE36R/graph.json","events_json":"https://pith.science/api/pith-number/XH3O5THTGXD4PCTKUUMO6SE36R/events.json","paper":"https://pith.science/paper/XH3O5THT"},"agent_actions":{"view_html":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R","download_json":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R.json","view_paper":"https://pith.science/paper/XH3O5THT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2309.12923&json=true","fetch_graph":"https://pith.science/api/pith-number/XH3O5THTGXD4PCTKUUMO6SE36R/graph.json","fetch_events":"https://pith.science/api/pith-number/XH3O5THTGXD4PCTKUUMO6SE36R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R/action/storage_attestation","attest_author":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R/action/author_attestation","sign_citation":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R/action/citation_signature","submit_replication":"https://pith.science/pith/XH3O5THTGXD4PCTKUUMO6SE36R/action/replication_record"}},"created_at":"2026-07-05T06:54:23.638815+00:00","updated_at":"2026-07-05T06:54:23.638815+00:00"}