{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:77J3NXEYS4MSIKDKTTBLBF3IY2","short_pith_number":"pith:77J3NXEY","canonical_record":{"source":{"id":"cond-mat/9602113","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1996-02-20T22:32:11Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"06a811a458d7cd406271a513d2bcb04bfdbfd94955a6bd27a566fd43bfd70872","abstract_canon_sha256":"a039cebbfbad2a05e5bdb0920dd68ea616c034bbaf7e75609b02f67ea4d6eba8"},"schema_version":"1.0"},"canonical_sha256":"ffd3b6dc98971924286a9cc2b09768c68dd4a3047781fa94f56f2f005329575b","source":{"kind":"arxiv","id":"cond-mat/9602113","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9602113","created_at":"2026-05-18T04:17:53Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9602113v1","created_at":"2026-05-18T04:17:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9602113","created_at":"2026-05-18T04:17:53Z"},{"alias_kind":"pith_short_12","alias_value":"77J3NXEYS4MS","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"77J3NXEYS4MSIKDK","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"77J3NXEY","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:77J3NXEYS4MSIKDKTTBLBF3IY2","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/9602113","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1996-02-20T22:32:11Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"06a811a458d7cd406271a513d2bcb04bfdbfd94955a6bd27a566fd43bfd70872","abstract_canon_sha256":"a039cebbfbad2a05e5bdb0920dd68ea616c034bbaf7e75609b02f67ea4d6eba8"},"schema_version":"1.0"},"canonical_sha256":"ffd3b6dc98971924286a9cc2b09768c68dd4a3047781fa94f56f2f005329575b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:53.310551Z","signature_b64":"p5RHcM5NawpD1piyO8m/PCPXiRAUhywe4ssSzwY81MeU0xrFbW9RnTDyLVUvmA/TWjo8p8FQAw+z6Fg9DHqiDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ffd3b6dc98971924286a9cc2b09768c68dd4a3047781fa94f56f2f005329575b","last_reissued_at":"2026-05-18T04:17:53.310079Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:53.310079Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/9602113","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":"2026-05-18T04:17:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"m/A+RBm61dTU6xIxK3aEQpeW5gHBE2ijbya8F0yc/KC4StLK+KAuSSkt3CRo73cgoJKy0JDJvr9f7yQKnP80AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T20:45:40.167210Z"},"content_sha256":"f7b3f2aa035fe853196b7f04074d43f6f054a69ba22d2661d8bb09d9f0e4fac1","schema_version":"1.0","event_id":"sha256:f7b3f2aa035fe853196b7f04074d43f6f054a69ba22d2661d8bb09d9f0e4fac1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:77J3NXEYS4MSIKDKTTBLBF3IY2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Edge excitations of paired fractional quantum Hall states","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat","authors_text":"M. Milovanovic, N. Read (Yale University)","submitted_at":"1996-02-20T22:32:11Z","abstract_excerpt":"The Hilbert spaces of the edge excitations of several ``paired'' fractional quantum Hall states, namely the Pfaffian, Haldane-Rezayi and 331 states, are constructed and the states at each angular momentum level are enumerated. The method is based on finding all the zero energy states for those Hamiltonians for which each of these known ground states is the exact, unique, zero-energy eigenstate of lowest angular momentum in the disk geometry. For each state, we find that, in addition to the usual bosonic charge-fluctuation excitations, there are fermionic edge excitations. The edge states can b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9602113","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":"2026-05-18T04:17:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sfAd0yXHB4HxN4x9+Q/OI8QvDBB8yK56hotJ5wV8gMtcSefysOwTjtFCX6ny4y94gzKGWILHmCXW7un1pbpICw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T20:45:40.167893Z"},"content_sha256":"599830dc42c26832467e1f7301d6da04641af09ef45e8737407417c5f38a454d","schema_version":"1.0","event_id":"sha256:599830dc42c26832467e1f7301d6da04641af09ef45e8737407417c5f38a454d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/77J3NXEYS4MSIKDKTTBLBF3IY2/bundle.json","state_url":"https://pith.science/pith/77J3NXEYS4MSIKDKTTBLBF3IY2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/77J3NXEYS4MSIKDKTTBLBF3IY2/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":"2026-05-29T20:45:40Z","links":{"resolver":"https://pith.science/pith/77J3NXEYS4MSIKDKTTBLBF3IY2","bundle":"https://pith.science/pith/77J3NXEYS4MSIKDKTTBLBF3IY2/bundle.json","state":"https://pith.science/pith/77J3NXEYS4MSIKDKTTBLBF3IY2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/77J3NXEYS4MSIKDKTTBLBF3IY2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:77J3NXEYS4MSIKDKTTBLBF3IY2","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":"a039cebbfbad2a05e5bdb0920dd68ea616c034bbaf7e75609b02f67ea4d6eba8","cross_cats_sorted":["hep-th"],"license":"","primary_cat":"cond-mat","submitted_at":"1996-02-20T22:32:11Z","title_canon_sha256":"06a811a458d7cd406271a513d2bcb04bfdbfd94955a6bd27a566fd43bfd70872"},"schema_version":"1.0","source":{"id":"cond-mat/9602113","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9602113","created_at":"2026-05-18T04:17:53Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9602113v1","created_at":"2026-05-18T04:17:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9602113","created_at":"2026-05-18T04:17:53Z"},{"alias_kind":"pith_short_12","alias_value":"77J3NXEYS4MS","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"77J3NXEYS4MSIKDK","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"77J3NXEY","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:599830dc42c26832467e1f7301d6da04641af09ef45e8737407417c5f38a454d","target":"graph","created_at":"2026-05-18T04:17:53Z","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 Hilbert spaces of the edge excitations of several ``paired'' fractional quantum Hall states, namely the Pfaffian, Haldane-Rezayi and 331 states, are constructed and the states at each angular momentum level are enumerated. The method is based on finding all the zero energy states for those Hamiltonians for which each of these known ground states is the exact, unique, zero-energy eigenstate of lowest angular momentum in the disk geometry. For each state, we find that, in addition to the usual bosonic charge-fluctuation excitations, there are fermionic edge excitations. The edge states can b","authors_text":"M. Milovanovic, N. Read (Yale University)","cross_cats":["hep-th"],"headline":"","license":"","primary_cat":"cond-mat","submitted_at":"1996-02-20T22:32:11Z","title":"Edge excitations of paired fractional quantum Hall states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9602113","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:f7b3f2aa035fe853196b7f04074d43f6f054a69ba22d2661d8bb09d9f0e4fac1","target":"record","created_at":"2026-05-18T04:17:53Z","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":"a039cebbfbad2a05e5bdb0920dd68ea616c034bbaf7e75609b02f67ea4d6eba8","cross_cats_sorted":["hep-th"],"license":"","primary_cat":"cond-mat","submitted_at":"1996-02-20T22:32:11Z","title_canon_sha256":"06a811a458d7cd406271a513d2bcb04bfdbfd94955a6bd27a566fd43bfd70872"},"schema_version":"1.0","source":{"id":"cond-mat/9602113","kind":"arxiv","version":1}},"canonical_sha256":"ffd3b6dc98971924286a9cc2b09768c68dd4a3047781fa94f56f2f005329575b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ffd3b6dc98971924286a9cc2b09768c68dd4a3047781fa94f56f2f005329575b","first_computed_at":"2026-05-18T04:17:53.310079Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:17:53.310079Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"p5RHcM5NawpD1piyO8m/PCPXiRAUhywe4ssSzwY81MeU0xrFbW9RnTDyLVUvmA/TWjo8p8FQAw+z6Fg9DHqiDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:17:53.310551Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/9602113","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f7b3f2aa035fe853196b7f04074d43f6f054a69ba22d2661d8bb09d9f0e4fac1","sha256:599830dc42c26832467e1f7301d6da04641af09ef45e8737407417c5f38a454d"],"state_sha256":"936bca60d3dfb13e4571b594f9826042c496e0807619ed077309de1da6fd323a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oHQdFBTcxwAC9Hc5qVRNRm3XD7GerzlUT0srhfaI7Aub7jfKc0lUnF7XKtVTIc3Mt3aH6Sz/tDBFGaI+NnQCAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T20:45:40.170948Z","bundle_sha256":"158719dd3b2378e22600facb024fe246d96371bc2145db49402c1163cb390681"}}