{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:QCMYW47FH2ASAWKRSI52H75IXW","short_pith_number":"pith:QCMYW47F","canonical_record":{"source":{"id":"1805.00945","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-05-02T18:00:02Z","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"title_canon_sha256":"1802eda142c97c72e80272df4e9d978e8f395fe54ebfb40e30d7123b1633ec34","abstract_canon_sha256":"94f2fcc458b58536ff2b1f946431ff1a8ac723e083f4108751aeee77e76c974a"},"schema_version":"1.0"},"canonical_sha256":"80998b73e53e81205951923ba3ffa8bd9891442d90719dcdfeef0586ea896da6","source":{"kind":"arxiv","id":"1805.00945","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.00945","created_at":"2026-05-17T23:57:36Z"},{"alias_kind":"arxiv_version","alias_value":"1805.00945v1","created_at":"2026-05-17T23:57:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.00945","created_at":"2026-05-17T23:57:36Z"},{"alias_kind":"pith_short_12","alias_value":"QCMYW47FH2AS","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"QCMYW47FH2ASAWKR","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"QCMYW47F","created_at":"2026-05-18T12:32:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:QCMYW47FH2ASAWKRSI52H75IXW","target":"record","payload":{"canonical_record":{"source":{"id":"1805.00945","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-05-02T18:00:02Z","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"title_canon_sha256":"1802eda142c97c72e80272df4e9d978e8f395fe54ebfb40e30d7123b1633ec34","abstract_canon_sha256":"94f2fcc458b58536ff2b1f946431ff1a8ac723e083f4108751aeee77e76c974a"},"schema_version":"1.0"},"canonical_sha256":"80998b73e53e81205951923ba3ffa8bd9891442d90719dcdfeef0586ea896da6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:57:36.579950Z","signature_b64":"bq3RcRmgue1OBczS/WZe4yWngi/iOJ9EbDQDS56BANfFQxrrNs2iBgfyDhFAoyBXeig3AJ+iglXGSnxkaKc8CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"80998b73e53e81205951923ba3ffa8bd9891442d90719dcdfeef0586ea896da6","last_reissued_at":"2026-05-17T23:57:36.579541Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:57:36.579541Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1805.00945","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":"2026-05-17T23:57:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EgBXAJgddsGeVM3cS1FsA+P1KtIDuWUn2tbT3Y9rJy2tmmyVKDC6lIWIdbFNWKxsLyaXpvgH4KzMDNu06IO+DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-19T23:40:27.871097Z"},"content_sha256":"10a918d665c393513ede47c411b5bad552c5c30dc0cd6ad7184e9be7c4d5777b","schema_version":"1.0","event_id":"sha256:10a918d665c393513ede47c411b5bad552c5c30dc0cd6ad7184e9be7c4d5777b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:QCMYW47FH2ASAWKRSI52H75IXW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Algebraic Approach to Fractional Quantum Hall Effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Dam Thanh Son, Dung Xuan Nguyen","submitted_at":"2018-05-02T18:00:02Z","abstract_excerpt":"We construct an algebraic description for the ground state and for the static response of the quantum Hall plateaux with filling factor $\\nu=N/(2N+1)$ in the large $N$ limit. By analyzing the algebra of the fluctuations of the shape of the Fermi surface of the composite fermions, we find the explicit form of the projected static structure factor at large $N$ and fixed $z=(2N+1) q\\ell_B\\sim 1$. When $z<3.8$, the result does not depend on the particular form of the Hamiltonian."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.00945","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":"2026-05-17T23:57:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ALZEFXGIZFdWYBHFZRbrMYTihVmlx4j6EfAoUIceuU+WlGIVYc5sRJbq2jw3HG1ATDhKeU5qHm944rhdqziQBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-19T23:40:27.871460Z"},"content_sha256":"3fea6d9336b481d1e3ba7c678b13012485dad250692dd4fcaa4a4cccc351b2b4","schema_version":"1.0","event_id":"sha256:3fea6d9336b481d1e3ba7c678b13012485dad250692dd4fcaa4a4cccc351b2b4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QCMYW47FH2ASAWKRSI52H75IXW/bundle.json","state_url":"https://pith.science/pith/QCMYW47FH2ASAWKRSI52H75IXW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QCMYW47FH2ASAWKRSI52H75IXW/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":"2026-06-19T23:40:27Z","links":{"resolver":"https://pith.science/pith/QCMYW47FH2ASAWKRSI52H75IXW","bundle":"https://pith.science/pith/QCMYW47FH2ASAWKRSI52H75IXW/bundle.json","state":"https://pith.science/pith/QCMYW47FH2ASAWKRSI52H75IXW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QCMYW47FH2ASAWKRSI52H75IXW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:QCMYW47FH2ASAWKRSI52H75IXW","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":"94f2fcc458b58536ff2b1f946431ff1a8ac723e083f4108751aeee77e76c974a","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-05-02T18:00:02Z","title_canon_sha256":"1802eda142c97c72e80272df4e9d978e8f395fe54ebfb40e30d7123b1633ec34"},"schema_version":"1.0","source":{"id":"1805.00945","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.00945","created_at":"2026-05-17T23:57:36Z"},{"alias_kind":"arxiv_version","alias_value":"1805.00945v1","created_at":"2026-05-17T23:57:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.00945","created_at":"2026-05-17T23:57:36Z"},{"alias_kind":"pith_short_12","alias_value":"QCMYW47FH2AS","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"QCMYW47FH2ASAWKR","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"QCMYW47F","created_at":"2026-05-18T12:32:46Z"}],"graph_snapshots":[{"event_id":"sha256:3fea6d9336b481d1e3ba7c678b13012485dad250692dd4fcaa4a4cccc351b2b4","target":"graph","created_at":"2026-05-17T23:57:36Z","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 construct an algebraic description for the ground state and for the static response of the quantum Hall plateaux with filling factor $\\nu=N/(2N+1)$ in the large $N$ limit. By analyzing the algebra of the fluctuations of the shape of the Fermi surface of the composite fermions, we find the explicit form of the projected static structure factor at large $N$ and fixed $z=(2N+1) q\\ell_B\\sim 1$. When $z<3.8$, the result does not depend on the particular form of the Hamiltonian.","authors_text":"Dam Thanh Son, Dung Xuan Nguyen","cross_cats":["cond-mat.mes-hall","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-05-02T18:00:02Z","title":"Algebraic Approach to Fractional Quantum Hall Effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.00945","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":"sha256:10a918d665c393513ede47c411b5bad552c5c30dc0cd6ad7184e9be7c4d5777b","target":"record","created_at":"2026-05-17T23:57:36Z","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":"94f2fcc458b58536ff2b1f946431ff1a8ac723e083f4108751aeee77e76c974a","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-05-02T18:00:02Z","title_canon_sha256":"1802eda142c97c72e80272df4e9d978e8f395fe54ebfb40e30d7123b1633ec34"},"schema_version":"1.0","source":{"id":"1805.00945","kind":"arxiv","version":1}},"canonical_sha256":"80998b73e53e81205951923ba3ffa8bd9891442d90719dcdfeef0586ea896da6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"80998b73e53e81205951923ba3ffa8bd9891442d90719dcdfeef0586ea896da6","first_computed_at":"2026-05-17T23:57:36.579541Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:57:36.579541Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bq3RcRmgue1OBczS/WZe4yWngi/iOJ9EbDQDS56BANfFQxrrNs2iBgfyDhFAoyBXeig3AJ+iglXGSnxkaKc8CQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:57:36.579950Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.00945","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:10a918d665c393513ede47c411b5bad552c5c30dc0cd6ad7184e9be7c4d5777b","sha256:3fea6d9336b481d1e3ba7c678b13012485dad250692dd4fcaa4a4cccc351b2b4"],"state_sha256":"58446325a398bf93fa128e293bcda32907c2c8f5e2456772ff03165c81839442"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ImolB2yBbILgf9OL5lDMC1MmXSp5CaTn7gbQr/3OYjW9P8pDPemNF8fWQrWvwZ60pwlj2CL3aENPTknGIbIMAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-19T23:40:27.873444Z","bundle_sha256":"f0b5b564572891b85326eed3fc90308f86b356208b6dbf1c50f2db5c012f2668"}}