{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:6ITU7VEXT66IPYOODQ3VFBSDVX","short_pith_number":"pith:6ITU7VEX","canonical_record":{"source":{"id":"cond-mat/9501106","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1995-01-23T14:24:23Z","cross_cats_sorted":[],"title_canon_sha256":"4d2879f333f9bd96f9b1409d65f3235a25c4fc9f051aa4d9d2f6ad346e4ab94e","abstract_canon_sha256":"9c580ceebaefe70bbd20c0db953b69163c2742fad47144df1205813db936c21f"},"schema_version":"1.0"},"canonical_sha256":"f2274fd4979fbc87e1ce1c37528643adf19f0fb2ae5b8b18add72fe7bae95b1a","source":{"kind":"arxiv","id":"cond-mat/9501106","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9501106","created_at":"2026-05-18T01:07:21Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9501106v1","created_at":"2026-05-18T01:07:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9501106","created_at":"2026-05-18T01:07:21Z"},{"alias_kind":"pith_short_12","alias_value":"6ITU7VEXT66I","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"6ITU7VEXT66IPYOO","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"6ITU7VEX","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:6ITU7VEXT66IPYOODQ3VFBSDVX","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/9501106","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1995-01-23T14:24:23Z","cross_cats_sorted":[],"title_canon_sha256":"4d2879f333f9bd96f9b1409d65f3235a25c4fc9f051aa4d9d2f6ad346e4ab94e","abstract_canon_sha256":"9c580ceebaefe70bbd20c0db953b69163c2742fad47144df1205813db936c21f"},"schema_version":"1.0"},"canonical_sha256":"f2274fd4979fbc87e1ce1c37528643adf19f0fb2ae5b8b18add72fe7bae95b1a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:21.628236Z","signature_b64":"bgjc5vWE5fvvgmaqAGX+bbkLsSPgtiql3BwWmG9Oq/DNkAKd0/8eZTqHSiOkFbC8C2pQW1gRBE/HClSRbwjuDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2274fd4979fbc87e1ce1c37528643adf19f0fb2ae5b8b18add72fe7bae95b1a","last_reissued_at":"2026-05-18T01:07:21.627646Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:21.627646Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/9501106","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":"2026-05-18T01:07:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hovlP4YrvGgekc/2wDcY3GY94I1E6CRNyXxQ4+8FpNaIQ0xeWgrM/XJIgPGWKWc4g7aN41j8kTqz0AI7U0b1CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T17:00:20.562102Z"},"content_sha256":"4e6a6a579195a0b9c294a673cbbc79726769e68e54d5b2baf746130ea0e2f25a","schema_version":"1.0","event_id":"sha256:4e6a6a579195a0b9c294a673cbbc79726769e68e54d5b2baf746130ea0e2f25a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:6ITU7VEXT66IPYOODQ3VFBSDVX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scaling Theory of the Integer Quantum Hall Effect","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Bodo Huckestein","submitted_at":"1995-01-23T14:24:23Z","abstract_excerpt":"The scaling theory of the transitions between plateaus of the Hall conductivity in the integer Quantum Hall effect is reviewed. In the model of two-dimensional noninteracting electrons in strong magnetic fields the transitions are disorder-induced localization-delocalization transitions. While experimental and analytical approaches are surveyed, the main emphasis is on numerical studies, which successfully describe the experiments. The theoretical models for disordered systems are described in detail. An overview of the finite-size scaling theory and its relation to Anderson localization is gi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9501106","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":"2026-05-18T01:07:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hXayV8JbyNylBmUuPW1O5p4Wzqwn6k6HRGKnjfvUPMPCVxpBfNoWQWE3vbMAdSZDzZJ3NwIU1BFmRZDViXnYAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T17:00:20.562456Z"},"content_sha256":"583ec7bd928bf2c08c1b40f6944db70cb6f761364cb571d6486554a6b87f3c2d","schema_version":"1.0","event_id":"sha256:583ec7bd928bf2c08c1b40f6944db70cb6f761364cb571d6486554a6b87f3c2d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6ITU7VEXT66IPYOODQ3VFBSDVX/bundle.json","state_url":"https://pith.science/pith/6ITU7VEXT66IPYOODQ3VFBSDVX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6ITU7VEXT66IPYOODQ3VFBSDVX/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":"2026-06-30T17:00:20Z","links":{"resolver":"https://pith.science/pith/6ITU7VEXT66IPYOODQ3VFBSDVX","bundle":"https://pith.science/pith/6ITU7VEXT66IPYOODQ3VFBSDVX/bundle.json","state":"https://pith.science/pith/6ITU7VEXT66IPYOODQ3VFBSDVX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6ITU7VEXT66IPYOODQ3VFBSDVX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:6ITU7VEXT66IPYOODQ3VFBSDVX","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":"9c580ceebaefe70bbd20c0db953b69163c2742fad47144df1205813db936c21f","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"1995-01-23T14:24:23Z","title_canon_sha256":"4d2879f333f9bd96f9b1409d65f3235a25c4fc9f051aa4d9d2f6ad346e4ab94e"},"schema_version":"1.0","source":{"id":"cond-mat/9501106","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9501106","created_at":"2026-05-18T01:07:21Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9501106v1","created_at":"2026-05-18T01:07:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9501106","created_at":"2026-05-18T01:07:21Z"},{"alias_kind":"pith_short_12","alias_value":"6ITU7VEXT66I","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"6ITU7VEXT66IPYOO","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"6ITU7VEX","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:583ec7bd928bf2c08c1b40f6944db70cb6f761364cb571d6486554a6b87f3c2d","target":"graph","created_at":"2026-05-18T01:07:21Z","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":"The scaling theory of the transitions between plateaus of the Hall conductivity in the integer Quantum Hall effect is reviewed. In the model of two-dimensional noninteracting electrons in strong magnetic fields the transitions are disorder-induced localization-delocalization transitions. While experimental and analytical approaches are surveyed, the main emphasis is on numerical studies, which successfully describe the experiments. The theoretical models for disordered systems are described in detail. An overview of the finite-size scaling theory and its relation to Anderson localization is gi","authors_text":"Bodo Huckestein","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat","submitted_at":"1995-01-23T14:24:23Z","title":"Scaling Theory of the Integer Quantum Hall Effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9501106","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":"sha256:4e6a6a579195a0b9c294a673cbbc79726769e68e54d5b2baf746130ea0e2f25a","target":"record","created_at":"2026-05-18T01:07:21Z","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":"9c580ceebaefe70bbd20c0db953b69163c2742fad47144df1205813db936c21f","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"1995-01-23T14:24:23Z","title_canon_sha256":"4d2879f333f9bd96f9b1409d65f3235a25c4fc9f051aa4d9d2f6ad346e4ab94e"},"schema_version":"1.0","source":{"id":"cond-mat/9501106","kind":"arxiv","version":1}},"canonical_sha256":"f2274fd4979fbc87e1ce1c37528643adf19f0fb2ae5b8b18add72fe7bae95b1a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f2274fd4979fbc87e1ce1c37528643adf19f0fb2ae5b8b18add72fe7bae95b1a","first_computed_at":"2026-05-18T01:07:21.627646Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:07:21.627646Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bgjc5vWE5fvvgmaqAGX+bbkLsSPgtiql3BwWmG9Oq/DNkAKd0/8eZTqHSiOkFbC8C2pQW1gRBE/HClSRbwjuDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:07:21.628236Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/9501106","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4e6a6a579195a0b9c294a673cbbc79726769e68e54d5b2baf746130ea0e2f25a","sha256:583ec7bd928bf2c08c1b40f6944db70cb6f761364cb571d6486554a6b87f3c2d"],"state_sha256":"7ea9b35db36f17e1cc8b48d312ca062da70a3a66b5579069b6a66fe863f3bf23"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"M52i58WPSNqdPedMX7qZnBu+ZIkp4o7BOxYc5p+lk/GIvY7Od1cz0YOP9l720GNuDIt94AJAQlZaqwho5i7jDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-30T17:00:20.564835Z","bundle_sha256":"592900f824436f123a95aebfcd8340c99413ca4cf2d7de72d74e3b1b23ad5426"}}