{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:D5GT4MGTXANUI6CH75LN75F6EP","short_pith_number":"pith:D5GT4MGT","schema_version":"1.0","canonical_sha256":"1f4d3e30d3b81b447847ff56dff4be23f0b40c03d6ae27a6df8f17620afbb4eb","source":{"kind":"arxiv","id":"cond-mat/9505027","version":1},"attestation_state":"computed","paper":{"title":"Abelian Hall Fluids and Edge States: a Conformal Field Theory Approach","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A. De Martino, R. Musto","submitted_at":"1995-05-08T10:50:34Z","abstract_excerpt":"We show that a Coulomb gas Vertex Operator representation of 2D Conformal Field Theory gives a complete description of abelian Hall fluids: as an euclidean theory in two space dimensions leads to the construction of the ground state wave function for planar and toroidal geometry and characterizes the spectrum of low energy excitations; as a $1+1$ Minkowski theory gives the corresponding dynamics of the edge states. The difference between a generic Hall fluid and states of the Jain's sequences is emphasized and the presence, in the latter case, of of an $\\hat {U}(1)\\otimes \\hat {SU}(n)$ extende"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"cond-mat/9505027","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1995-05-08T10:50:34Z","cross_cats_sorted":[],"title_canon_sha256":"058ab7af71ec4c05eac060812a2c3dc74ee0556c7543d9036d3d1714cb4763db","abstract_canon_sha256":"15e01188dc4aae866998d8faf8669f35b8476d25ac60e57e0cba660547e1889a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:44:45.535968Z","signature_b64":"8t5WFYzJ3S86BPx0ZmZRIs6CTNvwZCr5ITo3tIcy9TmNu3a5M6OUKvF4rs/FmbXXW2ggcfxpEg6pLH9/Gi0PCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1f4d3e30d3b81b447847ff56dff4be23f0b40c03d6ae27a6df8f17620afbb4eb","last_reissued_at":"2026-05-18T03:44:45.535302Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:44:45.535302Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Abelian Hall Fluids and Edge States: a Conformal Field Theory Approach","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A. De Martino, R. Musto","submitted_at":"1995-05-08T10:50:34Z","abstract_excerpt":"We show that a Coulomb gas Vertex Operator representation of 2D Conformal Field Theory gives a complete description of abelian Hall fluids: as an euclidean theory in two space dimensions leads to the construction of the ground state wave function for planar and toroidal geometry and characterizes the spectrum of low energy excitations; as a $1+1$ Minkowski theory gives the corresponding dynamics of the edge states. The difference between a generic Hall fluid and states of the Jain's sequences is emphasized and the presence, in the latter case, of of an $\\hat {U}(1)\\otimes \\hat {SU}(n)$ extende"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9505027","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9505027","created_at":"2026-05-18T03:44:45.535424+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9505027v1","created_at":"2026-05-18T03:44:45.535424+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9505027","created_at":"2026-05-18T03:44:45.535424+00:00"},{"alias_kind":"pith_short_12","alias_value":"D5GT4MGTXANU","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"D5GT4MGTXANUI6CH","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"D5GT4MGT","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP","json":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP.json","graph_json":"https://pith.science/api/pith-number/D5GT4MGTXANUI6CH75LN75F6EP/graph.json","events_json":"https://pith.science/api/pith-number/D5GT4MGTXANUI6CH75LN75F6EP/events.json","paper":"https://pith.science/paper/D5GT4MGT"},"agent_actions":{"view_html":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP","download_json":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP.json","view_paper":"https://pith.science/paper/D5GT4MGT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9505027&json=true","fetch_graph":"https://pith.science/api/pith-number/D5GT4MGTXANUI6CH75LN75F6EP/graph.json","fetch_events":"https://pith.science/api/pith-number/D5GT4MGTXANUI6CH75LN75F6EP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP/action/storage_attestation","attest_author":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP/action/author_attestation","sign_citation":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP/action/citation_signature","submit_replication":"https://pith.science/pith/D5GT4MGTXANUI6CH75LN75F6EP/action/replication_record"}},"created_at":"2026-05-18T03:44:45.535424+00:00","updated_at":"2026-05-18T03:44:45.535424+00:00"}