{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:MIS7ELM7QZS46GTI4HJZR6TLBF","short_pith_number":"pith:MIS7ELM7","canonical_record":{"source":{"id":"cond-mat/0310273","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2003-10-13T15:10:02Z","cross_cats_sorted":[],"title_canon_sha256":"cedfcf683c3b0854b223d3b8ed065ecd9fe4affb594b937c1e11068bee8879ce","abstract_canon_sha256":"b6ee972b1b539832c5c004599f3c9c727d88d2dc1d9a9d870749b4af3c181283"},"schema_version":"1.0"},"canonical_sha256":"6225f22d9f8665cf1a68e1d398fa6b09777b3ec42a275004cb26f67cce6a029b","source":{"kind":"arxiv","id":"cond-mat/0310273","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0310273","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0310273v1","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0310273","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"pith_short_12","alias_value":"MIS7ELM7QZS4","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"MIS7ELM7QZS46GTI","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"MIS7ELM7","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:MIS7ELM7QZS46GTI4HJZR6TLBF","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0310273","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2003-10-13T15:10:02Z","cross_cats_sorted":[],"title_canon_sha256":"cedfcf683c3b0854b223d3b8ed065ecd9fe4affb594b937c1e11068bee8879ce","abstract_canon_sha256":"b6ee972b1b539832c5c004599f3c9c727d88d2dc1d9a9d870749b4af3c181283"},"schema_version":"1.0"},"canonical_sha256":"6225f22d9f8665cf1a68e1d398fa6b09777b3ec42a275004cb26f67cce6a029b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:42:22.576078Z","signature_b64":"U830cYKJfl8KCdgBnqMiHJOGIhHZDNXp98oTKHNGogCcFEulw/YzhLexSOC5SPWAR+rrf0/uEGc8xA/NyPhTCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6225f22d9f8665cf1a68e1d398fa6b09777b3ec42a275004cb26f67cce6a029b","last_reissued_at":"2026-05-18T04:42:22.575335Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:42:22.575335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0310273","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":"2026-05-18T04:42:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oOIzmnoo1tD16FNKzEEzr+/EzMp2i8M079KhKP0+XMQ3SMOcyQu3WLJSk8Tw1h4QS3tdsoa2gKoLzjtJRM2gBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T02:52:23.586305Z"},"content_sha256":"159eee3da270d0286efcf2fd4745ebedad09873a2f75aa180a519041c24c2fe8","schema_version":"1.0","event_id":"sha256:159eee3da270d0286efcf2fd4745ebedad09873a2f75aa180a519041c24c2fe8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:MIS7ELM7QZS46GTI4HJZR6TLBF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Geometric phases and quantum entanglement as building blocks for nonabelian quasiparticle statistics","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Ady Stern (Weizmann), Eros Mariani (Hamburg, Felix von Oppen (FU Berlin, Weizmann)","submitted_at":"2003-10-13T15:10:02Z","abstract_excerpt":"Some models describing unconventional fractional quantum Hall states predict quasiparticles that obey nonabelian quantum statistics. The most prominent example is the Moore-Read model for the $\\nu=5/2$ state, in which the ground state is a superconductor of composite fermions, and the charged excitations are vortices in that superconductor. In this paper we develop a physical picture of the nonabelian statistics of these vortices. Considering first the positions of the vortices as fixed, we define a set of single-particle states at and near the core of each vortex, and employ general propertie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0310273","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":"2026-05-18T04:42:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"khZMsmbKX9DPA8bLN1Djjs/NIHpC82Lzq4RxKh2o10HH0JgHcWqVRYJJPXjABWMAtBAy1lBnwPVtTRx37lUZAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T02:52:23.586662Z"},"content_sha256":"9f133b3579e91aa1f129c5803f84cea55e73a225e20a087b6c8fbc52cc160898","schema_version":"1.0","event_id":"sha256:9f133b3579e91aa1f129c5803f84cea55e73a225e20a087b6c8fbc52cc160898"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MIS7ELM7QZS46GTI4HJZR6TLBF/bundle.json","state_url":"https://pith.science/pith/MIS7ELM7QZS46GTI4HJZR6TLBF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MIS7ELM7QZS46GTI4HJZR6TLBF/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":"2026-06-03T02:52:23Z","links":{"resolver":"https://pith.science/pith/MIS7ELM7QZS46GTI4HJZR6TLBF","bundle":"https://pith.science/pith/MIS7ELM7QZS46GTI4HJZR6TLBF/bundle.json","state":"https://pith.science/pith/MIS7ELM7QZS46GTI4HJZR6TLBF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MIS7ELM7QZS46GTI4HJZR6TLBF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:MIS7ELM7QZS46GTI4HJZR6TLBF","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":"b6ee972b1b539832c5c004599f3c9c727d88d2dc1d9a9d870749b4af3c181283","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2003-10-13T15:10:02Z","title_canon_sha256":"cedfcf683c3b0854b223d3b8ed065ecd9fe4affb594b937c1e11068bee8879ce"},"schema_version":"1.0","source":{"id":"cond-mat/0310273","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0310273","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0310273v1","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0310273","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"pith_short_12","alias_value":"MIS7ELM7QZS4","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"MIS7ELM7QZS46GTI","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"MIS7ELM7","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:9f133b3579e91aa1f129c5803f84cea55e73a225e20a087b6c8fbc52cc160898","target":"graph","created_at":"2026-05-18T04:42:22Z","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":"Some models describing unconventional fractional quantum Hall states predict quasiparticles that obey nonabelian quantum statistics. The most prominent example is the Moore-Read model for the $\\nu=5/2$ state, in which the ground state is a superconductor of composite fermions, and the charged excitations are vortices in that superconductor. In this paper we develop a physical picture of the nonabelian statistics of these vortices. Considering first the positions of the vortices as fixed, we define a set of single-particle states at and near the core of each vortex, and employ general propertie","authors_text":"Ady Stern (Weizmann), Eros Mariani (Hamburg, Felix von Oppen (FU Berlin, Weizmann)","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2003-10-13T15:10:02Z","title":"Geometric phases and quantum entanglement as building blocks for nonabelian quasiparticle statistics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0310273","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":"sha256:159eee3da270d0286efcf2fd4745ebedad09873a2f75aa180a519041c24c2fe8","target":"record","created_at":"2026-05-18T04:42:22Z","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":"b6ee972b1b539832c5c004599f3c9c727d88d2dc1d9a9d870749b4af3c181283","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2003-10-13T15:10:02Z","title_canon_sha256":"cedfcf683c3b0854b223d3b8ed065ecd9fe4affb594b937c1e11068bee8879ce"},"schema_version":"1.0","source":{"id":"cond-mat/0310273","kind":"arxiv","version":1}},"canonical_sha256":"6225f22d9f8665cf1a68e1d398fa6b09777b3ec42a275004cb26f67cce6a029b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6225f22d9f8665cf1a68e1d398fa6b09777b3ec42a275004cb26f67cce6a029b","first_computed_at":"2026-05-18T04:42:22.575335Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:42:22.575335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"U830cYKJfl8KCdgBnqMiHJOGIhHZDNXp98oTKHNGogCcFEulw/YzhLexSOC5SPWAR+rrf0/uEGc8xA/NyPhTCw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:42:22.576078Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0310273","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:159eee3da270d0286efcf2fd4745ebedad09873a2f75aa180a519041c24c2fe8","sha256:9f133b3579e91aa1f129c5803f84cea55e73a225e20a087b6c8fbc52cc160898"],"state_sha256":"efcddf6ec6c8614185f14d45a95a7b40e14ad3d4bf6bb1d9140b5b65e8da0848"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BmbB0h/hKNwsS0n9gdOAAdkhFBeUgDBZGRuQUXQ7QYDHQldlrMhHeDR0MYZ/bnKtVJxP+wh4sEb1EpT+I8GkCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T02:52:23.588592Z","bundle_sha256":"97aba6168282252dd6f5733cb6cfbfbfeb5fbab64e8dabb08f2e8be3d8e0cb23"}}