{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:UACRJITJ6LN2GKGFPE7HTU2QQ5","short_pith_number":"pith:UACRJITJ","canonical_record":{"source":{"id":"1112.2167","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-12-09T18:01:12Z","cross_cats_sorted":[],"title_canon_sha256":"b9716db55df9ca7b5caa22b233ec51fca1df8d384a82ec1f512c50948d006aa2","abstract_canon_sha256":"3bd815e99c92d13a25fea057b298fdfc67d424cfb317451c61cd690ba34b3f18"},"schema_version":"1.0"},"canonical_sha256":"a00514a269f2dba328c5793e79d3508742a628057eea956fff9b815dad8c1f1d","source":{"kind":"arxiv","id":"1112.2167","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.2167","created_at":"2026-05-18T01:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"1112.2167v1","created_at":"2026-05-18T01:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.2167","created_at":"2026-05-18T01:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"UACRJITJ6LN2","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UACRJITJ6LN2GKGF","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UACRJITJ","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:UACRJITJ6LN2GKGFPE7HTU2QQ5","target":"record","payload":{"canonical_record":{"source":{"id":"1112.2167","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-12-09T18:01:12Z","cross_cats_sorted":[],"title_canon_sha256":"b9716db55df9ca7b5caa22b233ec51fca1df8d384a82ec1f512c50948d006aa2","abstract_canon_sha256":"3bd815e99c92d13a25fea057b298fdfc67d424cfb317451c61cd690ba34b3f18"},"schema_version":"1.0"},"canonical_sha256":"a00514a269f2dba328c5793e79d3508742a628057eea956fff9b815dad8c1f1d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:12.519298Z","signature_b64":"hpW1A0Z1vJbWE/vb2fgY5nPPGfWdcR1nz9wt4sVuSTlA5i02plf8GLie/Zn53GQCEjPoPw1zNDO7m4YSJfZcBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a00514a269f2dba328c5793e79d3508742a628057eea956fff9b815dad8c1f1d","last_reissued_at":"2026-05-18T01:59:12.518601Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:12.518601Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.2167","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":"2026-05-18T01:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tFMNiTiNt7HtKOYJj6RsmjGP7+i1+2noMloOPu2GFbprlMhvteFXuQY7dzVto8GV5xgJdml1439sgL50HR+WDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-19T21:42:49.793491Z"},"content_sha256":"4fb1f0c29b5828a6be367131333494b7831b87ab0923fb0e5493166de7e18120","schema_version":"1.0","event_id":"sha256:4fb1f0c29b5828a6be367131333494b7831b87ab0923fb0e5493166de7e18120"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:UACRJITJ6LN2GKGFPE7HTU2QQ5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Universal Edge Physics in Fractional Quantum Hall Liquids","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Kun Yang, R. N. Bhatt, Xin Wan, Zi-Xiang Hu","submitted_at":"2011-12-09T18:01:12Z","abstract_excerpt":"The chiral Luttinger liquid theory for fractional quantum Hall edge transport predicts universal power-law behavior in the current-voltage ($I$-$V$) characteristics for electrons tunneling into the edge. However, it has not been unambiguously observed in experiments in two-dimensional electron gases based on GaAs/GaAlAs heterostructures or quantum wells. One plausible cause is the fractional quantum Hall edge reconstruction, which introduces non-chiral edge modes. The coupling between counterpropagating edge modes can modify the exponent of the $I$-$V$ characteristics. By comparing the $\\nu=1/"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.2167","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":"2026-05-18T01:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0JqYmIydBCKnMy9HPP6HJw0od/2GySlPo2Z8tKhLfzJOOw6iHHTVX5sCJsmx+V6U7ZY3eH8MQDCb8tVkIWOuAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-19T21:42:49.793842Z"},"content_sha256":"7b5c405fe4edd9e33bfbbf3688480f6a7aa7d4a2d98e95702f05b706cddf4e39","schema_version":"1.0","event_id":"sha256:7b5c405fe4edd9e33bfbbf3688480f6a7aa7d4a2d98e95702f05b706cddf4e39"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UACRJITJ6LN2GKGFPE7HTU2QQ5/bundle.json","state_url":"https://pith.science/pith/UACRJITJ6LN2GKGFPE7HTU2QQ5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UACRJITJ6LN2GKGFPE7HTU2QQ5/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":"2026-06-19T21:42:49Z","links":{"resolver":"https://pith.science/pith/UACRJITJ6LN2GKGFPE7HTU2QQ5","bundle":"https://pith.science/pith/UACRJITJ6LN2GKGFPE7HTU2QQ5/bundle.json","state":"https://pith.science/pith/UACRJITJ6LN2GKGFPE7HTU2QQ5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UACRJITJ6LN2GKGFPE7HTU2QQ5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:UACRJITJ6LN2GKGFPE7HTU2QQ5","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":"3bd815e99c92d13a25fea057b298fdfc67d424cfb317451c61cd690ba34b3f18","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-12-09T18:01:12Z","title_canon_sha256":"b9716db55df9ca7b5caa22b233ec51fca1df8d384a82ec1f512c50948d006aa2"},"schema_version":"1.0","source":{"id":"1112.2167","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.2167","created_at":"2026-05-18T01:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"1112.2167v1","created_at":"2026-05-18T01:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.2167","created_at":"2026-05-18T01:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"UACRJITJ6LN2","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UACRJITJ6LN2GKGF","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UACRJITJ","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:7b5c405fe4edd9e33bfbbf3688480f6a7aa7d4a2d98e95702f05b706cddf4e39","target":"graph","created_at":"2026-05-18T01:59:12Z","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 chiral Luttinger liquid theory for fractional quantum Hall edge transport predicts universal power-law behavior in the current-voltage ($I$-$V$) characteristics for electrons tunneling into the edge. However, it has not been unambiguously observed in experiments in two-dimensional electron gases based on GaAs/GaAlAs heterostructures or quantum wells. One plausible cause is the fractional quantum Hall edge reconstruction, which introduces non-chiral edge modes. The coupling between counterpropagating edge modes can modify the exponent of the $I$-$V$ characteristics. By comparing the $\\nu=1/","authors_text":"Kun Yang, R. N. Bhatt, Xin Wan, Zi-Xiang Hu","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-12-09T18:01:12Z","title":"The Universal Edge Physics in Fractional Quantum Hall Liquids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.2167","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":"sha256:4fb1f0c29b5828a6be367131333494b7831b87ab0923fb0e5493166de7e18120","target":"record","created_at":"2026-05-18T01:59:12Z","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":"3bd815e99c92d13a25fea057b298fdfc67d424cfb317451c61cd690ba34b3f18","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-12-09T18:01:12Z","title_canon_sha256":"b9716db55df9ca7b5caa22b233ec51fca1df8d384a82ec1f512c50948d006aa2"},"schema_version":"1.0","source":{"id":"1112.2167","kind":"arxiv","version":1}},"canonical_sha256":"a00514a269f2dba328c5793e79d3508742a628057eea956fff9b815dad8c1f1d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a00514a269f2dba328c5793e79d3508742a628057eea956fff9b815dad8c1f1d","first_computed_at":"2026-05-18T01:59:12.518601Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:59:12.518601Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hpW1A0Z1vJbWE/vb2fgY5nPPGfWdcR1nz9wt4sVuSTlA5i02plf8GLie/Zn53GQCEjPoPw1zNDO7m4YSJfZcBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:59:12.519298Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.2167","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4fb1f0c29b5828a6be367131333494b7831b87ab0923fb0e5493166de7e18120","sha256:7b5c405fe4edd9e33bfbbf3688480f6a7aa7d4a2d98e95702f05b706cddf4e39"],"state_sha256":"edde5ab379cb792d3060bd12e3bfb5abc7d7f8b58ae21aa853e1b5dde6e9e5e7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l4AP9uehaEn+tCUF8Hoalc2gCOkFWJ8L5HG/vBOsa6EBRH8kZYlYsV9j0gXv6QU6sDYdiXEwanX7CNYYdm2CDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-19T21:42:49.795783Z","bundle_sha256":"3fb0a24c321dbd66ba2219c91d308e78dda3e05b585a18b9f22b14bbc588ce95"}}