{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:MIQETXSKENIYUERE2WPYTH5SA7","short_pith_number":"pith:MIQETXSK","schema_version":"1.0","canonical_sha256":"622049de4a23518a1224d59f899fb207c5ca8d28686071f2c623326aebffc118","source":{"kind":"arxiv","id":"hep-th/9512182","version":1},"attestation_state":"computed","paper":{"title":"N=2 Supersymmetry and Bailey Pairs","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alexander Berkovich, Anne Schilling, Barry M. McCoy","submitted_at":"1995-12-21T18:00:21Z","abstract_excerpt":"We demonstrate that the Bailey pair formulation of Rogers-Ramanujan identities unifies the calculations of the characters of $N=1$ and $N=2$ supersymmetric conformal field theories with the counterpart theory with no supersymmetry. We illustrate this construction for the $M(3,4)$ (Ising) model where the Bailey pairs have been given by Slater. We then present the general unitary case. We demonstrate that the model $M(p,p+1)$ is derived from $M(p-1,p)$ by a Bailey renormalization flow and conclude by obtaining the $N=1$ model $SM(p,p+2)$ and the unitary $N=2$ model with central charge $c=3(1-2/p"},"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":"hep-th/9512182","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1995-12-21T18:00:21Z","cross_cats_sorted":[],"title_canon_sha256":"a30b13a625d43416b12420c5a7d82271610758f1d8db8ba42dc6d9e22c1b6808","abstract_canon_sha256":"e2417ddc56ade7bb7037d64e6a603de21fd4da9acb7c9ada10f41c0b75570599"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:38.472421Z","signature_b64":"PykqR8QIx95KYi48vD/MclP0pO3G6rDYuzTGIEa7vM/UDZnV0SAZdCoCD1FXCkKM3bRC7lV5uvO1rocpziFfBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"622049de4a23518a1224d59f899fb207c5ca8d28686071f2c623326aebffc118","last_reissued_at":"2026-05-18T01:38:38.471941Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:38.471941Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"N=2 Supersymmetry and Bailey Pairs","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alexander Berkovich, Anne Schilling, Barry M. McCoy","submitted_at":"1995-12-21T18:00:21Z","abstract_excerpt":"We demonstrate that the Bailey pair formulation of Rogers-Ramanujan identities unifies the calculations of the characters of $N=1$ and $N=2$ supersymmetric conformal field theories with the counterpart theory with no supersymmetry. We illustrate this construction for the $M(3,4)$ (Ising) model where the Bailey pairs have been given by Slater. We then present the general unitary case. We demonstrate that the model $M(p,p+1)$ is derived from $M(p-1,p)$ by a Bailey renormalization flow and conclude by obtaining the $N=1$ model $SM(p,p+2)$ and the unitary $N=2$ model with central charge $c=3(1-2/p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9512182","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":"hep-th/9512182","created_at":"2026-05-18T01:38:38.472013+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9512182v1","created_at":"2026-05-18T01:38:38.472013+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9512182","created_at":"2026-05-18T01:38:38.472013+00:00"},{"alias_kind":"pith_short_12","alias_value":"MIQETXSKENIY","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"MIQETXSKENIYUERE","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"MIQETXSK","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/MIQETXSKENIYUERE2WPYTH5SA7","json":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7.json","graph_json":"https://pith.science/api/pith-number/MIQETXSKENIYUERE2WPYTH5SA7/graph.json","events_json":"https://pith.science/api/pith-number/MIQETXSKENIYUERE2WPYTH5SA7/events.json","paper":"https://pith.science/paper/MIQETXSK"},"agent_actions":{"view_html":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7","download_json":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7.json","view_paper":"https://pith.science/paper/MIQETXSK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9512182&json=true","fetch_graph":"https://pith.science/api/pith-number/MIQETXSKENIYUERE2WPYTH5SA7/graph.json","fetch_events":"https://pith.science/api/pith-number/MIQETXSKENIYUERE2WPYTH5SA7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7/action/storage_attestation","attest_author":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7/action/author_attestation","sign_citation":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7/action/citation_signature","submit_replication":"https://pith.science/pith/MIQETXSKENIYUERE2WPYTH5SA7/action/replication_record"}},"created_at":"2026-05-18T01:38:38.472013+00:00","updated_at":"2026-05-18T01:38:38.472013+00:00"}