{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:5RIEP7UDYUHVUCSCTMRBFE7G4M","short_pith_number":"pith:5RIEP7UD","canonical_record":{"source":{"id":"1409.6237","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-22T16:45:35Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"7a2bab9b2a716f44066edf40bcab1b6b86b0c11d612319c3b21eb99ffb099ce7","abstract_canon_sha256":"69c33f5ab7870719ceb27ac364beda0d11152b80c836fbef308de9a84ba7ead4"},"schema_version":"1.0"},"canonical_sha256":"ec5047fe83c50f5a0a429b221293e6e32d507053ba35efe5de0916a79767a9d4","source":{"kind":"arxiv","id":"1409.6237","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.6237","created_at":"2026-05-18T01:13:45Z"},{"alias_kind":"arxiv_version","alias_value":"1409.6237v2","created_at":"2026-05-18T01:13:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6237","created_at":"2026-05-18T01:13:45Z"},{"alias_kind":"pith_short_12","alias_value":"5RIEP7UDYUHV","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"5RIEP7UDYUHVUCSC","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"5RIEP7UD","created_at":"2026-05-18T12:28:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:5RIEP7UDYUHVUCSCTMRBFE7G4M","target":"record","payload":{"canonical_record":{"source":{"id":"1409.6237","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-22T16:45:35Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"7a2bab9b2a716f44066edf40bcab1b6b86b0c11d612319c3b21eb99ffb099ce7","abstract_canon_sha256":"69c33f5ab7870719ceb27ac364beda0d11152b80c836fbef308de9a84ba7ead4"},"schema_version":"1.0"},"canonical_sha256":"ec5047fe83c50f5a0a429b221293e6e32d507053ba35efe5de0916a79767a9d4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:13:45.044392Z","signature_b64":"HcbnJ9RVX9G80zSzySvYNR1WD6eZEFGIX0pyD/ODEWUHfdY9bFe0NXkRVNP0cjMTzUFc/Fybk9ssGQT+4oPWCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec5047fe83c50f5a0a429b221293e6e32d507053ba35efe5de0916a79767a9d4","last_reissued_at":"2026-05-18T01:13:45.043869Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:13:45.043869Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.6237","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:13:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Okt43BP//p++S4wsXcWyukpraHPRmJoaEguxRvYRGjyuc7E62zmN+gWRGASsPwhbq+N3MYBvc75gdSrgISpRAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T17:07:31.456154Z"},"content_sha256":"a06c50e348faf38ee08bcc4f2a93594422b166b0550bd0924218dd52c6b86c97","schema_version":"1.0","event_id":"sha256:a06c50e348faf38ee08bcc4f2a93594422b166b0550bd0924218dd52c6b86c97"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:5RIEP7UDYUHVUCSCTMRBFE7G4M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Realizing Topological Mott Insulators from the RKKY Interaction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"cond-mat.str-el","authors_text":"Beno\\^it Dou\\c{c}ot, Karyn Le Hur, Tianhan Liu","submitted_at":"2014-09-22T16:45:35Z","abstract_excerpt":"We engineer topological insulating phases in a fermion-fermion mixture on the honeycomb lattice, without resorting to artificial gauge fields or spin-orbit couplings and considering only local interactions. Essentially, upon integrating out the fast component (characterized by a larger hopping amplitude) in a finite region of dopings, we obtain an effective interaction between the slow fermions at half-filling, which acquires a Haldane mass with opposite parity in the two valleys of the Dirac cones, thus triggering a quantum anomalous Hall effect. We carefully analyze the competition between t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6237","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:13:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dg5aO7Je0fBRX+c2OaSMTsYilT+lkZjHlUwyniJ8QV2LFiHp/FzU1ecpym4s1cJe7a6DbJ4Gt1c8b4FsBrN2Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T17:07:31.456827Z"},"content_sha256":"2a299ec621362d3ec36ca861ae27db456b3b382d962c5e823d2cee32104fea73","schema_version":"1.0","event_id":"sha256:2a299ec621362d3ec36ca861ae27db456b3b382d962c5e823d2cee32104fea73"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5RIEP7UDYUHVUCSCTMRBFE7G4M/bundle.json","state_url":"https://pith.science/pith/5RIEP7UDYUHVUCSCTMRBFE7G4M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5RIEP7UDYUHVUCSCTMRBFE7G4M/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-09T17:07:31Z","links":{"resolver":"https://pith.science/pith/5RIEP7UDYUHVUCSCTMRBFE7G4M","bundle":"https://pith.science/pith/5RIEP7UDYUHVUCSCTMRBFE7G4M/bundle.json","state":"https://pith.science/pith/5RIEP7UDYUHVUCSCTMRBFE7G4M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5RIEP7UDYUHVUCSCTMRBFE7G4M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:5RIEP7UDYUHVUCSCTMRBFE7G4M","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"69c33f5ab7870719ceb27ac364beda0d11152b80c836fbef308de9a84ba7ead4","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-22T16:45:35Z","title_canon_sha256":"7a2bab9b2a716f44066edf40bcab1b6b86b0c11d612319c3b21eb99ffb099ce7"},"schema_version":"1.0","source":{"id":"1409.6237","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.6237","created_at":"2026-05-18T01:13:45Z"},{"alias_kind":"arxiv_version","alias_value":"1409.6237v2","created_at":"2026-05-18T01:13:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.6237","created_at":"2026-05-18T01:13:45Z"},{"alias_kind":"pith_short_12","alias_value":"5RIEP7UDYUHV","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"5RIEP7UDYUHVUCSC","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"5RIEP7UD","created_at":"2026-05-18T12:28:14Z"}],"graph_snapshots":[{"event_id":"sha256:2a299ec621362d3ec36ca861ae27db456b3b382d962c5e823d2cee32104fea73","target":"graph","created_at":"2026-05-18T01:13:45Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We engineer topological insulating phases in a fermion-fermion mixture on the honeycomb lattice, without resorting to artificial gauge fields or spin-orbit couplings and considering only local interactions. Essentially, upon integrating out the fast component (characterized by a larger hopping amplitude) in a finite region of dopings, we obtain an effective interaction between the slow fermions at half-filling, which acquires a Haldane mass with opposite parity in the two valleys of the Dirac cones, thus triggering a quantum anomalous Hall effect. We carefully analyze the competition between t","authors_text":"Beno\\^it Dou\\c{c}ot, Karyn Le Hur, Tianhan Liu","cross_cats":["cond-mat.quant-gas"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-22T16:45:35Z","title":"Realizing Topological Mott Insulators from the RKKY Interaction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.6237","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a06c50e348faf38ee08bcc4f2a93594422b166b0550bd0924218dd52c6b86c97","target":"record","created_at":"2026-05-18T01:13:45Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"69c33f5ab7870719ceb27ac364beda0d11152b80c836fbef308de9a84ba7ead4","cross_cats_sorted":["cond-mat.quant-gas"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-22T16:45:35Z","title_canon_sha256":"7a2bab9b2a716f44066edf40bcab1b6b86b0c11d612319c3b21eb99ffb099ce7"},"schema_version":"1.0","source":{"id":"1409.6237","kind":"arxiv","version":2}},"canonical_sha256":"ec5047fe83c50f5a0a429b221293e6e32d507053ba35efe5de0916a79767a9d4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ec5047fe83c50f5a0a429b221293e6e32d507053ba35efe5de0916a79767a9d4","first_computed_at":"2026-05-18T01:13:45.043869Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:13:45.043869Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HcbnJ9RVX9G80zSzySvYNR1WD6eZEFGIX0pyD/ODEWUHfdY9bFe0NXkRVNP0cjMTzUFc/Fybk9ssGQT+4oPWCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:13:45.044392Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.6237","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a06c50e348faf38ee08bcc4f2a93594422b166b0550bd0924218dd52c6b86c97","sha256:2a299ec621362d3ec36ca861ae27db456b3b382d962c5e823d2cee32104fea73"],"state_sha256":"50226904f7066175dc033f6b22ac555b34290d3f8447fa4531ae993b94aeda9a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CbnAkvokmY0YrHLerRBGJaQIAu6kDR/4+P4Y8e98eAuC93oqRwRSCTjEBizGOR1xv/zCo6fghzDXDABCJuT1Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T17:07:31.460821Z","bundle_sha256":"0af1e2d850d111782d7ddfc2966215321b124eaa744b869d74f1cc31a5f5ef39"}}