{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:C44FFZ6GAWBW23MKZAJ7O7QRI7","short_pith_number":"pith:C44FFZ6G","schema_version":"1.0","canonical_sha256":"173852e7c605836d6d8ac813f77e1147f178877a21c229e43eea807330af040d","source":{"kind":"arxiv","id":"1501.00425","version":2},"attestation_state":"computed","paper":{"title":"Three-level Haldane-like model on dice optical lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Mekys, E. Anisimovas, G. Juzeli\\=unas, I. B. Spielman, M. Ra\\v{c}i\\=unas, T. Andrijauskas, V. Kudria\\v{s}ov","submitted_at":"2015-01-02T15:46:43Z","abstract_excerpt":"We consider ultracold atoms in a two-dimensional optical lattice of the dice geometry in a tight-binding regime. The atoms experience a laser-assisted tunneling between the nearest neighbour sites of the dice lattice accompanied by the momentum recoil. This allows one to engineer staggered synthetic magnetic fluxes over plaquettes, and thus pave a way towards a realization of topologically nontrivial band structures. In such a lattice the real-valued next-neighbour transitions are not needed to reach a topological regime. Yet, such transitions can increase a variety of the obtained topological"},"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":"1501.00425","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-01-02T15:46:43Z","cross_cats_sorted":[],"title_canon_sha256":"1dee5353632838ba53ef14903e549eaf8fee8ff19f0d2e69a5b78eadd1a232ed","abstract_canon_sha256":"f0b5fd0f43e1298fe5f15a2fbe376f802f7351abfd08bcf93ad77f03dd3e10cc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:32:30.403353Z","signature_b64":"bPcJfl5C/KxFAY3CXSLmeZ6/6by5F5lk9BJ8s59+I4BLeAfeLpne0/42xiY/0wZnmPkuLEFx9akRh+TzAO9FCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"173852e7c605836d6d8ac813f77e1147f178877a21c229e43eea807330af040d","last_reissued_at":"2026-05-18T01:32:30.402802Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:32:30.402802Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three-level Haldane-like model on dice optical lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. Mekys, E. Anisimovas, G. Juzeli\\=unas, I. B. Spielman, M. Ra\\v{c}i\\=unas, T. Andrijauskas, V. Kudria\\v{s}ov","submitted_at":"2015-01-02T15:46:43Z","abstract_excerpt":"We consider ultracold atoms in a two-dimensional optical lattice of the dice geometry in a tight-binding regime. The atoms experience a laser-assisted tunneling between the nearest neighbour sites of the dice lattice accompanied by the momentum recoil. This allows one to engineer staggered synthetic magnetic fluxes over plaquettes, and thus pave a way towards a realization of topologically nontrivial band structures. In such a lattice the real-valued next-neighbour transitions are not needed to reach a topological regime. Yet, such transitions can increase a variety of the obtained topological"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.00425","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":"1501.00425","created_at":"2026-05-18T01:32:30.402892+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.00425v2","created_at":"2026-05-18T01:32:30.402892+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.00425","created_at":"2026-05-18T01:32:30.402892+00:00"},{"alias_kind":"pith_short_12","alias_value":"C44FFZ6GAWBW","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_16","alias_value":"C44FFZ6GAWBW23MK","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_8","alias_value":"C44FFZ6G","created_at":"2026-05-18T12:29:14.074870+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/C44FFZ6GAWBW23MKZAJ7O7QRI7","json":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7.json","graph_json":"https://pith.science/api/pith-number/C44FFZ6GAWBW23MKZAJ7O7QRI7/graph.json","events_json":"https://pith.science/api/pith-number/C44FFZ6GAWBW23MKZAJ7O7QRI7/events.json","paper":"https://pith.science/paper/C44FFZ6G"},"agent_actions":{"view_html":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7","download_json":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7.json","view_paper":"https://pith.science/paper/C44FFZ6G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.00425&json=true","fetch_graph":"https://pith.science/api/pith-number/C44FFZ6GAWBW23MKZAJ7O7QRI7/graph.json","fetch_events":"https://pith.science/api/pith-number/C44FFZ6GAWBW23MKZAJ7O7QRI7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7/action/storage_attestation","attest_author":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7/action/author_attestation","sign_citation":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7/action/citation_signature","submit_replication":"https://pith.science/pith/C44FFZ6GAWBW23MKZAJ7O7QRI7/action/replication_record"}},"created_at":"2026-05-18T01:32:30.402892+00:00","updated_at":"2026-05-18T01:32:30.402892+00:00"}