{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:YXQ7FLQDEAOEV2BZT4JVNESHH6","short_pith_number":"pith:YXQ7FLQD","canonical_record":{"source":{"id":"1306.2789","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-06-12T11:23:42Z","cross_cats_sorted":[],"title_canon_sha256":"0212bca3a9a671f22cd4cfcbd37a2fdb45e2a0cc390a26df382fcf0e9344959f","abstract_canon_sha256":"6d64647a92e15bce3c9c2daf1616a8a1502a3b26c361366e55d318ab14d4c4a6"},"schema_version":"1.0"},"canonical_sha256":"c5e1f2ae03201c4ae8399f135692473fb1489ecd5e7f24642f69e3fe5b5f7728","source":{"kind":"arxiv","id":"1306.2789","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.2789","created_at":"2026-05-18T03:06:05Z"},{"alias_kind":"arxiv_version","alias_value":"1306.2789v1","created_at":"2026-05-18T03:06:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.2789","created_at":"2026-05-18T03:06:05Z"},{"alias_kind":"pith_short_12","alias_value":"YXQ7FLQDEAOE","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"YXQ7FLQDEAOEV2BZ","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"YXQ7FLQD","created_at":"2026-05-18T12:28:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:YXQ7FLQDEAOEV2BZT4JVNESHH6","target":"record","payload":{"canonical_record":{"source":{"id":"1306.2789","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-06-12T11:23:42Z","cross_cats_sorted":[],"title_canon_sha256":"0212bca3a9a671f22cd4cfcbd37a2fdb45e2a0cc390a26df382fcf0e9344959f","abstract_canon_sha256":"6d64647a92e15bce3c9c2daf1616a8a1502a3b26c361366e55d318ab14d4c4a6"},"schema_version":"1.0"},"canonical_sha256":"c5e1f2ae03201c4ae8399f135692473fb1489ecd5e7f24642f69e3fe5b5f7728","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:05.594828Z","signature_b64":"s1xSVYqWQJLoBzx7q2y5jXNe20ZqqIWtQx0reM9GiwbcvrVXXQqruTHL0MIubbTQyGL0T8qLeDQgf0rCGTIXBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c5e1f2ae03201c4ae8399f135692473fb1489ecd5e7f24642f69e3fe5b5f7728","last_reissued_at":"2026-05-18T03:06:05.594390Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:05.594390Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.2789","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":"2026-05-18T03:06:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"evkz+dz1QGRkzNpnCqh/l2nS/xTm79JG7JvPlP4t9qeWATYmSy8cAcoP0MoDJJ6lzUj+aM+dIN85k9gXyYxFDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T09:53:08.253164Z"},"content_sha256":"80e5c19dbfc93a4c0c6a6e93ff6fa7fee5ddb0f28e83370d78411a32b905e68d","schema_version":"1.0","event_id":"sha256:80e5c19dbfc93a4c0c6a6e93ff6fa7fee5ddb0f28e83370d78411a32b905e68d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:YXQ7FLQDEAOEV2BZT4JVNESHH6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exactly soluble lattice models for non-abelian states of matter in 2 dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Ady Stern, Maciej Koch-Janusz, Michael Levin","submitted_at":"2013-06-12T11:23:42Z","abstract_excerpt":"Following an earlier construction of exactly soluble lattice models for abelian fractional topological insulators in two and three dimensions, we construct here an exactly soluble lattice model for a non-abelian $\\nu=1$ quantum Hall state and a non-abelian topological insulator in two dimensions. We show that both models are topologically ordered, exhibiting fractionalized charge, ground state degeneracy on the torus and protected edge modes. The models feature non-abelian vortices which carry fractional electric charge in the quantum Hall case and spin in the topological insulator case. We an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.2789","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":"2026-05-18T03:06:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qVu/DqjwhqPkvSqmstq5Zmpewe4uVlLRsxis9ajusbucwk39STjf3otRaDlS7gL4JMo0LDNaYRVFxMpBDAJvAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T09:53:08.253544Z"},"content_sha256":"9e6d5b9fc034b93caaa3f0ee9312a5ce6eb1bdcd0258af615191256910385fa6","schema_version":"1.0","event_id":"sha256:9e6d5b9fc034b93caaa3f0ee9312a5ce6eb1bdcd0258af615191256910385fa6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YXQ7FLQDEAOEV2BZT4JVNESHH6/bundle.json","state_url":"https://pith.science/pith/YXQ7FLQDEAOEV2BZT4JVNESHH6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YXQ7FLQDEAOEV2BZT4JVNESHH6/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":"2026-06-11T09:53:08Z","links":{"resolver":"https://pith.science/pith/YXQ7FLQDEAOEV2BZT4JVNESHH6","bundle":"https://pith.science/pith/YXQ7FLQDEAOEV2BZT4JVNESHH6/bundle.json","state":"https://pith.science/pith/YXQ7FLQDEAOEV2BZT4JVNESHH6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YXQ7FLQDEAOEV2BZT4JVNESHH6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:YXQ7FLQDEAOEV2BZT4JVNESHH6","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":"6d64647a92e15bce3c9c2daf1616a8a1502a3b26c361366e55d318ab14d4c4a6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-06-12T11:23:42Z","title_canon_sha256":"0212bca3a9a671f22cd4cfcbd37a2fdb45e2a0cc390a26df382fcf0e9344959f"},"schema_version":"1.0","source":{"id":"1306.2789","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.2789","created_at":"2026-05-18T03:06:05Z"},{"alias_kind":"arxiv_version","alias_value":"1306.2789v1","created_at":"2026-05-18T03:06:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.2789","created_at":"2026-05-18T03:06:05Z"},{"alias_kind":"pith_short_12","alias_value":"YXQ7FLQDEAOE","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"YXQ7FLQDEAOEV2BZ","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"YXQ7FLQD","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:9e6d5b9fc034b93caaa3f0ee9312a5ce6eb1bdcd0258af615191256910385fa6","target":"graph","created_at":"2026-05-18T03:06:05Z","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":"Following an earlier construction of exactly soluble lattice models for abelian fractional topological insulators in two and three dimensions, we construct here an exactly soluble lattice model for a non-abelian $\\nu=1$ quantum Hall state and a non-abelian topological insulator in two dimensions. We show that both models are topologically ordered, exhibiting fractionalized charge, ground state degeneracy on the torus and protected edge modes. The models feature non-abelian vortices which carry fractional electric charge in the quantum Hall case and spin in the topological insulator case. We an","authors_text":"Ady Stern, Maciej Koch-Janusz, Michael Levin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-06-12T11:23:42Z","title":"Exactly soluble lattice models for non-abelian states of matter in 2 dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.2789","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":"sha256:80e5c19dbfc93a4c0c6a6e93ff6fa7fee5ddb0f28e83370d78411a32b905e68d","target":"record","created_at":"2026-05-18T03:06:05Z","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":"6d64647a92e15bce3c9c2daf1616a8a1502a3b26c361366e55d318ab14d4c4a6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-06-12T11:23:42Z","title_canon_sha256":"0212bca3a9a671f22cd4cfcbd37a2fdb45e2a0cc390a26df382fcf0e9344959f"},"schema_version":"1.0","source":{"id":"1306.2789","kind":"arxiv","version":1}},"canonical_sha256":"c5e1f2ae03201c4ae8399f135692473fb1489ecd5e7f24642f69e3fe5b5f7728","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c5e1f2ae03201c4ae8399f135692473fb1489ecd5e7f24642f69e3fe5b5f7728","first_computed_at":"2026-05-18T03:06:05.594390Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:06:05.594390Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"s1xSVYqWQJLoBzx7q2y5jXNe20ZqqIWtQx0reM9GiwbcvrVXXQqruTHL0MIubbTQyGL0T8qLeDQgf0rCGTIXBw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:06:05.594828Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.2789","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:80e5c19dbfc93a4c0c6a6e93ff6fa7fee5ddb0f28e83370d78411a32b905e68d","sha256:9e6d5b9fc034b93caaa3f0ee9312a5ce6eb1bdcd0258af615191256910385fa6"],"state_sha256":"c77d45b2fc09a4c2ed1a3fec7c376260531b59686438a95478e39790037ebe4a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UE/OmRe9pPHAz1dmXL7PBSuC1/eDe0bha/tL8A1RWux8TjRt8IUu+wPZxZrqNsdhJ2Obc4DTVwLyVq6MY7uIAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T09:53:08.255918Z","bundle_sha256":"d9522f95df89638d6a5106a11839cd823ec9f78cfd1c0d83876b3a14fa2a455f"}}