{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:SMCQBIDCSI4LMC2FVC2HYSGAVX","short_pith_number":"pith:SMCQBIDC","canonical_record":{"source":{"id":"1604.00122","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-01T03:43:55Z","cross_cats_sorted":[],"title_canon_sha256":"9161529fa83a4e5f4e75dfd5c2ea630aa1dd36bbe0b6d99bc86b15baba929605","abstract_canon_sha256":"9d90c15de501eb5fbf7403cab23e694174cf275928d3d4fec2ac456976b78d5a"},"schema_version":"1.0"},"canonical_sha256":"930500a0629238b60b45a8b47c48c0add872688b37acac5c85e76b39002f1bf0","source":{"kind":"arxiv","id":"1604.00122","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.00122","created_at":"2026-05-18T01:05:43Z"},{"alias_kind":"arxiv_version","alias_value":"1604.00122v1","created_at":"2026-05-18T01:05:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.00122","created_at":"2026-05-18T01:05:43Z"},{"alias_kind":"pith_short_12","alias_value":"SMCQBIDCSI4L","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"SMCQBIDCSI4LMC2F","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"SMCQBIDC","created_at":"2026-05-18T12:30:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:SMCQBIDCSI4LMC2FVC2HYSGAVX","target":"record","payload":{"canonical_record":{"source":{"id":"1604.00122","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-01T03:43:55Z","cross_cats_sorted":[],"title_canon_sha256":"9161529fa83a4e5f4e75dfd5c2ea630aa1dd36bbe0b6d99bc86b15baba929605","abstract_canon_sha256":"9d90c15de501eb5fbf7403cab23e694174cf275928d3d4fec2ac456976b78d5a"},"schema_version":"1.0"},"canonical_sha256":"930500a0629238b60b45a8b47c48c0add872688b37acac5c85e76b39002f1bf0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:43.636928Z","signature_b64":"ZorEwc6+WOrwDeoJGzhSLManefVYuGXhguneeHfbLcR1o/wpBu7NSDxB5RK2H3KKMWMOJRxKmsgzhbJ/XuUuCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"930500a0629238b60b45a8b47c48c0add872688b37acac5c85e76b39002f1bf0","last_reissued_at":"2026-05-18T01:05:43.636262Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:43.636262Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.00122","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":"2026-05-18T01:05:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n09CLhFZgRA+FMAW672uI8g1w26+VyLhdqukYzU2y+t4Ego/zswsPQpqiMnorTaylvz4ert0CMux7asojgOpBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T01:13:05.658282Z"},"content_sha256":"1f5f9edfdac7ba97472eb686b6e9e005de462a8ac6562b6b2a48fdea048a147c","schema_version":"1.0","event_id":"sha256:1f5f9edfdac7ba97472eb686b6e9e005de462a8ac6562b6b2a48fdea048a147c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:SMCQBIDCSI4LMC2FVC2HYSGAVX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Topological edge Mott insulating state in two dimensions at finite temperatures -bulk and edge analysis-","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Norio Kawakami, Tsuneya Yoshida","submitted_at":"2016-04-01T03:43:55Z","abstract_excerpt":"We study a bilayer Kane-Mele-Hubbard model with lattice distortion and inter-layer spin exchange interaction under cylinder geometry. Our analysis based on real-space dynamical mean field theory with continuous-time quantum Monte Carlo demonstrates the emergence of a topological edge Mott insulating (TEMI) state which hosts gapless edge modes only in collective spin excitations. This is confirmed by the numerical calculations at finite temperatures for the spin-Hall conductivity and the single-particle excitation spectrum; the spin Hall conductivity is almost quantized, $\\sigma^{xy}_\\mathrm{sp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.00122","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":"2026-05-18T01:05:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GS4JTXS/U6XqnIWF+wSFNmzQWes/RI50GpgQ3U6xUcFQmhrc1MnEB0FO/3lEeB6HTZPjN7dss30NqhT+I5naDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T01:13:05.658972Z"},"content_sha256":"e8644b69626ed765b4669f76a38d3d5f4b382b09839c27e4760a981c9e98d95f","schema_version":"1.0","event_id":"sha256:e8644b69626ed765b4669f76a38d3d5f4b382b09839c27e4760a981c9e98d95f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SMCQBIDCSI4LMC2FVC2HYSGAVX/bundle.json","state_url":"https://pith.science/pith/SMCQBIDCSI4LMC2FVC2HYSGAVX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SMCQBIDCSI4LMC2FVC2HYSGAVX/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":"2026-06-05T01:13:05Z","links":{"resolver":"https://pith.science/pith/SMCQBIDCSI4LMC2FVC2HYSGAVX","bundle":"https://pith.science/pith/SMCQBIDCSI4LMC2FVC2HYSGAVX/bundle.json","state":"https://pith.science/pith/SMCQBIDCSI4LMC2FVC2HYSGAVX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SMCQBIDCSI4LMC2FVC2HYSGAVX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:SMCQBIDCSI4LMC2FVC2HYSGAVX","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":"9d90c15de501eb5fbf7403cab23e694174cf275928d3d4fec2ac456976b78d5a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-01T03:43:55Z","title_canon_sha256":"9161529fa83a4e5f4e75dfd5c2ea630aa1dd36bbe0b6d99bc86b15baba929605"},"schema_version":"1.0","source":{"id":"1604.00122","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.00122","created_at":"2026-05-18T01:05:43Z"},{"alias_kind":"arxiv_version","alias_value":"1604.00122v1","created_at":"2026-05-18T01:05:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.00122","created_at":"2026-05-18T01:05:43Z"},{"alias_kind":"pith_short_12","alias_value":"SMCQBIDCSI4L","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"SMCQBIDCSI4LMC2F","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"SMCQBIDC","created_at":"2026-05-18T12:30:44Z"}],"graph_snapshots":[{"event_id":"sha256:e8644b69626ed765b4669f76a38d3d5f4b382b09839c27e4760a981c9e98d95f","target":"graph","created_at":"2026-05-18T01:05:43Z","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 study a bilayer Kane-Mele-Hubbard model with lattice distortion and inter-layer spin exchange interaction under cylinder geometry. Our analysis based on real-space dynamical mean field theory with continuous-time quantum Monte Carlo demonstrates the emergence of a topological edge Mott insulating (TEMI) state which hosts gapless edge modes only in collective spin excitations. This is confirmed by the numerical calculations at finite temperatures for the spin-Hall conductivity and the single-particle excitation spectrum; the spin Hall conductivity is almost quantized, $\\sigma^{xy}_\\mathrm{sp","authors_text":"Norio Kawakami, Tsuneya Yoshida","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-01T03:43:55Z","title":"Topological edge Mott insulating state in two dimensions at finite temperatures -bulk and edge analysis-"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.00122","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":"sha256:1f5f9edfdac7ba97472eb686b6e9e005de462a8ac6562b6b2a48fdea048a147c","target":"record","created_at":"2026-05-18T01:05:43Z","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":"9d90c15de501eb5fbf7403cab23e694174cf275928d3d4fec2ac456976b78d5a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-01T03:43:55Z","title_canon_sha256":"9161529fa83a4e5f4e75dfd5c2ea630aa1dd36bbe0b6d99bc86b15baba929605"},"schema_version":"1.0","source":{"id":"1604.00122","kind":"arxiv","version":1}},"canonical_sha256":"930500a0629238b60b45a8b47c48c0add872688b37acac5c85e76b39002f1bf0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"930500a0629238b60b45a8b47c48c0add872688b37acac5c85e76b39002f1bf0","first_computed_at":"2026-05-18T01:05:43.636262Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:05:43.636262Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZorEwc6+WOrwDeoJGzhSLManefVYuGXhguneeHfbLcR1o/wpBu7NSDxB5RK2H3KKMWMOJRxKmsgzhbJ/XuUuCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:05:43.636928Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.00122","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1f5f9edfdac7ba97472eb686b6e9e005de462a8ac6562b6b2a48fdea048a147c","sha256:e8644b69626ed765b4669f76a38d3d5f4b382b09839c27e4760a981c9e98d95f"],"state_sha256":"a37bafce1e9ca653c6db1e48847390cd59847ef7ecfb715d538934117c393b96"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Amojkc/II7mD1XOOUbOLHiyrV7RbpTCqnyUfMqYe752K8i+UW5KZusgDhxhdUBPJd7SvYysPqQGx1ZInm+tbCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T01:13:05.663019Z","bundle_sha256":"db589f3f61f54c270a36afd29691f38ef6a1d2f837d2ee2ee41275b675e9440d"}}