{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:LSR7DVSGTS2ZERM2QREMRXWRJD","short_pith_number":"pith:LSR7DVSG","canonical_record":{"source":{"id":"1812.01944","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-01T10:56:20Z","cross_cats_sorted":[],"title_canon_sha256":"c59e6c816c3eca85b6b3be621439447b2b28c4621976abf9cb17f15849f529b7","abstract_canon_sha256":"d76b0daaee69c99b29ac38912372224a4c9ca355f4161fbcdfe57ad36c333351"},"schema_version":"1.0"},"canonical_sha256":"5ca3f1d6469cb592459a8448c8ded148efa7932a5f19c1022797492da4e94303","source":{"kind":"arxiv","id":"1812.01944","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01944","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01944v1","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01944","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"pith_short_12","alias_value":"LSR7DVSGTS2Z","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"LSR7DVSGTS2ZERM2","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"LSR7DVSG","created_at":"2026-05-18T12:32:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:LSR7DVSGTS2ZERM2QREMRXWRJD","target":"record","payload":{"canonical_record":{"source":{"id":"1812.01944","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-01T10:56:20Z","cross_cats_sorted":[],"title_canon_sha256":"c59e6c816c3eca85b6b3be621439447b2b28c4621976abf9cb17f15849f529b7","abstract_canon_sha256":"d76b0daaee69c99b29ac38912372224a4c9ca355f4161fbcdfe57ad36c333351"},"schema_version":"1.0"},"canonical_sha256":"5ca3f1d6469cb592459a8448c8ded148efa7932a5f19c1022797492da4e94303","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:51:30.669235Z","signature_b64":"IFLrvrjJ0LvhGC9OH8aOzhla/arcm7iAUhZO2vV+tX6Orvc5o15COQpfF/wVMFiCn7kSnzinsb5V8tG8Cz/TAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ca3f1d6469cb592459a8448c8ded148efa7932a5f19c1022797492da4e94303","last_reissued_at":"2026-05-17T23:51:30.668739Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:51:30.668739Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.01944","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:51:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Sspga+lzhAqPmexR1M8KMwIT77sp7rdvoyrrSZ3+Tkg0WX6KE5OBoWjbnYCdLeMRErQjDjCgQEr7WgVkNg0lCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T12:02:58.873552Z"},"content_sha256":"817cb84cb5e14036e563b056133438628540dfd0e379415036bd2af7d56ed4ee","schema_version":"1.0","event_id":"sha256:817cb84cb5e14036e563b056133438628540dfd0e379415036bd2af7d56ed4ee"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:LSR7DVSGTS2ZERM2QREMRXWRJD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strain and onsite-correlation tunable quantum anomalous Hall phases in ferromagnetic (111) LaXO$_3$ bilayers (X$=$Pd, Pt)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Guang-Yu Guo, Hai-Shuang Lu","submitted_at":"2018-12-01T10:56:20Z","abstract_excerpt":"Quantum anomalous Hall (QAH) phases in magnetic topological insulators are characterized by the scattering-free chiral edge currents protected by their nontrivial bulk band topology. To fully explore these intriguing phenomena and application of topological insulators, high temperature material realization of QAH phases is crucial. In this paper, based on extensive first-principles density functional theory calculations, we predict that perovskite bilayers (LaXO$_3$)$_{2}$ (X = Pd, Pt) imbedded in the (111) (LaXO$_3$)$_{2}$/(LaAlO$_3$)$_{10}$ superlattices are high Curie temperature ferromagne"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01944","kind":"arxiv","version":1},"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":"2026-05-17T23:51:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hFp3mCu8onynWi/vVxbFjv/yn4I6K3wcoyqrxFfXBCkGTGZ2Rh78zMcxeAfVqvSUlsqkXj4bKJmHkVVerX1kDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T12:02:58.873882Z"},"content_sha256":"ae35782c79dcc3a8d924e9efdd3927a04195a39a244c0eac74c17187b2243cf7","schema_version":"1.0","event_id":"sha256:ae35782c79dcc3a8d924e9efdd3927a04195a39a244c0eac74c17187b2243cf7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LSR7DVSGTS2ZERM2QREMRXWRJD/bundle.json","state_url":"https://pith.science/pith/LSR7DVSGTS2ZERM2QREMRXWRJD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LSR7DVSGTS2ZERM2QREMRXWRJD/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":"2026-06-11T12:02:58Z","links":{"resolver":"https://pith.science/pith/LSR7DVSGTS2ZERM2QREMRXWRJD","bundle":"https://pith.science/pith/LSR7DVSGTS2ZERM2QREMRXWRJD/bundle.json","state":"https://pith.science/pith/LSR7DVSGTS2ZERM2QREMRXWRJD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LSR7DVSGTS2ZERM2QREMRXWRJD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:LSR7DVSGTS2ZERM2QREMRXWRJD","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":"d76b0daaee69c99b29ac38912372224a4c9ca355f4161fbcdfe57ad36c333351","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-01T10:56:20Z","title_canon_sha256":"c59e6c816c3eca85b6b3be621439447b2b28c4621976abf9cb17f15849f529b7"},"schema_version":"1.0","source":{"id":"1812.01944","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01944","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01944v1","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01944","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"pith_short_12","alias_value":"LSR7DVSGTS2Z","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"LSR7DVSGTS2ZERM2","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"LSR7DVSG","created_at":"2026-05-18T12:32:37Z"}],"graph_snapshots":[{"event_id":"sha256:ae35782c79dcc3a8d924e9efdd3927a04195a39a244c0eac74c17187b2243cf7","target":"graph","created_at":"2026-05-17T23:51:30Z","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":"Quantum anomalous Hall (QAH) phases in magnetic topological insulators are characterized by the scattering-free chiral edge currents protected by their nontrivial bulk band topology. To fully explore these intriguing phenomena and application of topological insulators, high temperature material realization of QAH phases is crucial. In this paper, based on extensive first-principles density functional theory calculations, we predict that perovskite bilayers (LaXO$_3$)$_{2}$ (X = Pd, Pt) imbedded in the (111) (LaXO$_3$)$_{2}$/(LaAlO$_3$)$_{10}$ superlattices are high Curie temperature ferromagne","authors_text":"Guang-Yu Guo, Hai-Shuang Lu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-01T10:56:20Z","title":"Strain and onsite-correlation tunable quantum anomalous Hall phases in ferromagnetic (111) LaXO$_3$ bilayers (X$=$Pd, Pt)"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01944","kind":"arxiv","version":1},"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":"sha256:817cb84cb5e14036e563b056133438628540dfd0e379415036bd2af7d56ed4ee","target":"record","created_at":"2026-05-17T23:51:30Z","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":"d76b0daaee69c99b29ac38912372224a4c9ca355f4161fbcdfe57ad36c333351","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-01T10:56:20Z","title_canon_sha256":"c59e6c816c3eca85b6b3be621439447b2b28c4621976abf9cb17f15849f529b7"},"schema_version":"1.0","source":{"id":"1812.01944","kind":"arxiv","version":1}},"canonical_sha256":"5ca3f1d6469cb592459a8448c8ded148efa7932a5f19c1022797492da4e94303","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5ca3f1d6469cb592459a8448c8ded148efa7932a5f19c1022797492da4e94303","first_computed_at":"2026-05-17T23:51:30.668739Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:51:30.668739Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IFLrvrjJ0LvhGC9OH8aOzhla/arcm7iAUhZO2vV+tX6Orvc5o15COQpfF/wVMFiCn7kSnzinsb5V8tG8Cz/TAQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:51:30.669235Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.01944","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:817cb84cb5e14036e563b056133438628540dfd0e379415036bd2af7d56ed4ee","sha256:ae35782c79dcc3a8d924e9efdd3927a04195a39a244c0eac74c17187b2243cf7"],"state_sha256":"564abb1a8318fa09096bf8ee25fbad82b3343e91ebd2c4771a568e4b69d98281"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JydmqGLN+3qxR/fVLbJImg2YDylAoxNNpo6C3DXcq8xO93r+4hcrfaPi1uJMCzBSBCqW1o2EWz6fQo+RH09kCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T12:02:58.875665Z","bundle_sha256":"70d1acad99272ea41d3038c537bee8cdb37c80e3920f053e148c20b863ae4019"}}