{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:FRRYNQZANZGU3QJSO4CAZ33QSX","short_pith_number":"pith:FRRYNQZA","canonical_record":{"source":{"id":"cond-mat/0608346","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2006-08-16T18:36:42Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"5715dc755edb75a2921e666d7a908ddc92a84489dbd532eb7c865448d9ff265d","abstract_canon_sha256":"fbf598514e274206a9f1e924e0520be649827f58b9dfb31a750e85d58101e014"},"schema_version":"1.0"},"canonical_sha256":"2c6386c3206e4d4dc13277040cef7095d01512d12f9d28db22a728793842d806","source":{"kind":"arxiv","id":"cond-mat/0608346","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0608346","created_at":"2026-05-18T01:39:44Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0608346v1","created_at":"2026-05-18T01:39:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0608346","created_at":"2026-05-18T01:39:44Z"},{"alias_kind":"pith_short_12","alias_value":"FRRYNQZANZGU","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"FRRYNQZANZGU3QJS","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"FRRYNQZA","created_at":"2026-05-18T12:25:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:FRRYNQZANZGU3QJSO4CAZ33QSX","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0608346","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2006-08-16T18:36:42Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"5715dc755edb75a2921e666d7a908ddc92a84489dbd532eb7c865448d9ff265d","abstract_canon_sha256":"fbf598514e274206a9f1e924e0520be649827f58b9dfb31a750e85d58101e014"},"schema_version":"1.0"},"canonical_sha256":"2c6386c3206e4d4dc13277040cef7095d01512d12f9d28db22a728793842d806","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:44.144596Z","signature_b64":"mu3jZ10v2yysd1jYC714ZBYIEMVAV9+lD0R/+8lrujBQS3ChefQwQKnkT0c1qQMxI8AeWsEaqjnmBgPoDZHLAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2c6386c3206e4d4dc13277040cef7095d01512d12f9d28db22a728793842d806","last_reissued_at":"2026-05-18T01:39:44.143899Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:44.143899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0608346","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":"2026-05-18T01:39:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ddA6gb2rO46MF5FGh1dvmE7FGa+comaARMj28oDjn1Z9jQF/7pVMpgCtGO9JptfyMj+3tGvo32y/U7Hza2fIDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T21:00:10.997363Z"},"content_sha256":"d9731d29687816819f5ae3483e62769b12477b064b34c0686a10a500dd4efeee","schema_version":"1.0","event_id":"sha256:d9731d29687816819f5ae3483e62769b12477b064b34c0686a10a500dd4efeee"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:FRRYNQZANZGU3QJSO4CAZ33QSX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-Abelian quantized Hall states of electrons at filling factors 12/5 and 13/5 in the first excited Landau level","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"E.H. Rezayi, N. Read","submitted_at":"2006-08-16T18:36:42Z","abstract_excerpt":"We present results of extensive numerical calculations on the ground state of electrons in the first excited (n=1) Landau level with Coulomb interactions, and including non-zero thickness effects, for filling factors 12/5 and 13/5 in the torus geometry. In a region that includes these experimentally-relevant values, we find that the energy spectrum and the overlaps with the trial states support the previous hypothesis that the system is in the non-Abelian k = 3 liquid phase we introduced in a previous paper."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0608346","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":"2026-05-18T01:39:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vcjlnFnOw+BiCMcMKhOVYwONvBI9X1HV3UrkvK4/cy7BArrxlNJiABJSOleB4GdC4N2lRvIiZvDDTE1Rkg7EBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T21:00:10.997701Z"},"content_sha256":"34be7495e90c1577002986128fd2531689795ecdf42f1f8c7da0ce3b464a979a","schema_version":"1.0","event_id":"sha256:34be7495e90c1577002986128fd2531689795ecdf42f1f8c7da0ce3b464a979a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FRRYNQZANZGU3QJSO4CAZ33QSX/bundle.json","state_url":"https://pith.science/pith/FRRYNQZANZGU3QJSO4CAZ33QSX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FRRYNQZANZGU3QJSO4CAZ33QSX/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":"2026-06-22T21:00:10Z","links":{"resolver":"https://pith.science/pith/FRRYNQZANZGU3QJSO4CAZ33QSX","bundle":"https://pith.science/pith/FRRYNQZANZGU3QJSO4CAZ33QSX/bundle.json","state":"https://pith.science/pith/FRRYNQZANZGU3QJSO4CAZ33QSX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FRRYNQZANZGU3QJSO4CAZ33QSX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:FRRYNQZANZGU3QJSO4CAZ33QSX","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":"fbf598514e274206a9f1e924e0520be649827f58b9dfb31a750e85d58101e014","cross_cats_sorted":["cond-mat.str-el"],"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2006-08-16T18:36:42Z","title_canon_sha256":"5715dc755edb75a2921e666d7a908ddc92a84489dbd532eb7c865448d9ff265d"},"schema_version":"1.0","source":{"id":"cond-mat/0608346","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0608346","created_at":"2026-05-18T01:39:44Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0608346v1","created_at":"2026-05-18T01:39:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0608346","created_at":"2026-05-18T01:39:44Z"},{"alias_kind":"pith_short_12","alias_value":"FRRYNQZANZGU","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_16","alias_value":"FRRYNQZANZGU3QJS","created_at":"2026-05-18T12:25:53Z"},{"alias_kind":"pith_short_8","alias_value":"FRRYNQZA","created_at":"2026-05-18T12:25:53Z"}],"graph_snapshots":[{"event_id":"sha256:34be7495e90c1577002986128fd2531689795ecdf42f1f8c7da0ce3b464a979a","target":"graph","created_at":"2026-05-18T01:39:44Z","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 present results of extensive numerical calculations on the ground state of electrons in the first excited (n=1) Landau level with Coulomb interactions, and including non-zero thickness effects, for filling factors 12/5 and 13/5 in the torus geometry. In a region that includes these experimentally-relevant values, we find that the energy spectrum and the overlaps with the trial states support the previous hypothesis that the system is in the non-Abelian k = 3 liquid phase we introduced in a previous paper.","authors_text":"E.H. Rezayi, N. Read","cross_cats":["cond-mat.str-el"],"headline":"","license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2006-08-16T18:36:42Z","title":"Non-Abelian quantized Hall states of electrons at filling factors 12/5 and 13/5 in the first excited Landau level"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0608346","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:d9731d29687816819f5ae3483e62769b12477b064b34c0686a10a500dd4efeee","target":"record","created_at":"2026-05-18T01:39:44Z","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":"fbf598514e274206a9f1e924e0520be649827f58b9dfb31a750e85d58101e014","cross_cats_sorted":["cond-mat.str-el"],"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2006-08-16T18:36:42Z","title_canon_sha256":"5715dc755edb75a2921e666d7a908ddc92a84489dbd532eb7c865448d9ff265d"},"schema_version":"1.0","source":{"id":"cond-mat/0608346","kind":"arxiv","version":1}},"canonical_sha256":"2c6386c3206e4d4dc13277040cef7095d01512d12f9d28db22a728793842d806","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2c6386c3206e4d4dc13277040cef7095d01512d12f9d28db22a728793842d806","first_computed_at":"2026-05-18T01:39:44.143899Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:44.143899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mu3jZ10v2yysd1jYC714ZBYIEMVAV9+lD0R/+8lrujBQS3ChefQwQKnkT0c1qQMxI8AeWsEaqjnmBgPoDZHLAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:44.144596Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0608346","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d9731d29687816819f5ae3483e62769b12477b064b34c0686a10a500dd4efeee","sha256:34be7495e90c1577002986128fd2531689795ecdf42f1f8c7da0ce3b464a979a"],"state_sha256":"2b2df95ad3c62b09b393fa5cd22e3e87a8a6adb6c06d394affa53b1b4ff1ffc4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IMTUyiYWzur/iRms5NcW6S8YYFC/ScIURvI5tNixx4Rg5w7VDwyt++Q9h6a5nxocHpI+uRUvcv/Fx4Rb/Z2ABA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T21:00:10.999618Z","bundle_sha256":"8411ba2657832974acbbe1c52963f52f10b3532fb638c72f0724466d7e6da964"}}