{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:2WTDO5PWCK4E3DBBWYSOKIBU2O","short_pith_number":"pith:2WTDO5PW","canonical_record":{"source":{"id":"1206.6346","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-27T17:39:30Z","cross_cats_sorted":[],"title_canon_sha256":"e90f9c6e3ed9bf062845a58c8a297b560aee6d3bc74121701a0bae26cbfb31f7","abstract_canon_sha256":"fce52b6884f06bc59cb463aae0f7d55a2cd6a0c4c56fcecb37727b15a18d38f6"},"schema_version":"1.0"},"canonical_sha256":"d5a63775f612b84d8c21b624e52034d396a87bd1c514dcd083f02c1e62faf53c","source":{"kind":"arxiv","id":"1206.6346","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.6346","created_at":"2026-05-18T01:56:41Z"},{"alias_kind":"arxiv_version","alias_value":"1206.6346v1","created_at":"2026-05-18T01:56:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6346","created_at":"2026-05-18T01:56:41Z"},{"alias_kind":"pith_short_12","alias_value":"2WTDO5PWCK4E","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_16","alias_value":"2WTDO5PWCK4E3DBB","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_8","alias_value":"2WTDO5PW","created_at":"2026-05-18T12:26:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:2WTDO5PWCK4E3DBBWYSOKIBU2O","target":"record","payload":{"canonical_record":{"source":{"id":"1206.6346","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-27T17:39:30Z","cross_cats_sorted":[],"title_canon_sha256":"e90f9c6e3ed9bf062845a58c8a297b560aee6d3bc74121701a0bae26cbfb31f7","abstract_canon_sha256":"fce52b6884f06bc59cb463aae0f7d55a2cd6a0c4c56fcecb37727b15a18d38f6"},"schema_version":"1.0"},"canonical_sha256":"d5a63775f612b84d8c21b624e52034d396a87bd1c514dcd083f02c1e62faf53c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:41.214165Z","signature_b64":"1f4Uf3/fd8rmcwvxtP0c+j0jeIdfDZOw6R/VV7t60LIsBPLUddAPjrVvFXc7hmxWhlf8iQmi8MFB1+lBMo9WCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d5a63775f612b84d8c21b624e52034d396a87bd1c514dcd083f02c1e62faf53c","last_reissued_at":"2026-05-18T01:56:41.213794Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:41.213794Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1206.6346","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":"2026-05-18T01:56:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6np5ZFM4TnXt6GmpqvYlL+aslKEaSZmCYTumtx7pawJhIan4zyfnwnOg8Je/0NhSkcqvuhI4hfEDoeT52yRqCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T08:44:52.624852Z"},"content_sha256":"84f104239678abe6c112503b3d13e3493572da33f992ba53a30fa886c1c38b6d","schema_version":"1.0","event_id":"sha256:84f104239678abe6c112503b3d13e3493572da33f992ba53a30fa886c1c38b6d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:2WTDO5PWCK4E3DBBWYSOKIBU2O","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Interacting fermions and N=2 Chern-Simons-matter theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Marcos Marino, Pavel Putrov","submitted_at":"2012-06-27T17:39:30Z","abstract_excerpt":"The partition function on the three-sphere of N=3 Chern-Simons-matter theories can be formulated in terms of an ideal Fermi gas. In this paper we show that, in theories with N=2 supersymmetry, the partition function corresponds to a gas of interacting fermions in one dimension. The large N limit is the thermodynamic limit of the gas and it can be analyzed with the Hartree and Thomas-Fermi approximations, which lead to the known large N solutions of these models. We use this interacting fermion picture to analyze in detail N=2 theories with one single node. In the case of theories with no long-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6346","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":"2026-05-18T01:56:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"13Yt+sZIWyDE+mTQQy75/dw4g6zvEqLzzSBDFF5qJXb0U5VMPNzWlSVPhU2Q5pMTM+0NFRCQOhCFkU/75YzcCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T08:44:52.625198Z"},"content_sha256":"bd7eb954f7ab945483f9f1b248214872f3d1cf1879968b33b9b9bd43868995a8","schema_version":"1.0","event_id":"sha256:bd7eb954f7ab945483f9f1b248214872f3d1cf1879968b33b9b9bd43868995a8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2WTDO5PWCK4E3DBBWYSOKIBU2O/bundle.json","state_url":"https://pith.science/pith/2WTDO5PWCK4E3DBBWYSOKIBU2O/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2WTDO5PWCK4E3DBBWYSOKIBU2O/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":"2026-06-12T08:44:52Z","links":{"resolver":"https://pith.science/pith/2WTDO5PWCK4E3DBBWYSOKIBU2O","bundle":"https://pith.science/pith/2WTDO5PWCK4E3DBBWYSOKIBU2O/bundle.json","state":"https://pith.science/pith/2WTDO5PWCK4E3DBBWYSOKIBU2O/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2WTDO5PWCK4E3DBBWYSOKIBU2O/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:2WTDO5PWCK4E3DBBWYSOKIBU2O","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":"fce52b6884f06bc59cb463aae0f7d55a2cd6a0c4c56fcecb37727b15a18d38f6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-27T17:39:30Z","title_canon_sha256":"e90f9c6e3ed9bf062845a58c8a297b560aee6d3bc74121701a0bae26cbfb31f7"},"schema_version":"1.0","source":{"id":"1206.6346","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.6346","created_at":"2026-05-18T01:56:41Z"},{"alias_kind":"arxiv_version","alias_value":"1206.6346v1","created_at":"2026-05-18T01:56:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6346","created_at":"2026-05-18T01:56:41Z"},{"alias_kind":"pith_short_12","alias_value":"2WTDO5PWCK4E","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_16","alias_value":"2WTDO5PWCK4E3DBB","created_at":"2026-05-18T12:26:50Z"},{"alias_kind":"pith_short_8","alias_value":"2WTDO5PW","created_at":"2026-05-18T12:26:50Z"}],"graph_snapshots":[{"event_id":"sha256:bd7eb954f7ab945483f9f1b248214872f3d1cf1879968b33b9b9bd43868995a8","target":"graph","created_at":"2026-05-18T01:56:41Z","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":"The partition function on the three-sphere of N=3 Chern-Simons-matter theories can be formulated in terms of an ideal Fermi gas. In this paper we show that, in theories with N=2 supersymmetry, the partition function corresponds to a gas of interacting fermions in one dimension. The large N limit is the thermodynamic limit of the gas and it can be analyzed with the Hartree and Thomas-Fermi approximations, which lead to the known large N solutions of these models. We use this interacting fermion picture to analyze in detail N=2 theories with one single node. In the case of theories with no long-","authors_text":"Marcos Marino, Pavel Putrov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-27T17:39:30Z","title":"Interacting fermions and N=2 Chern-Simons-matter theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6346","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":"sha256:84f104239678abe6c112503b3d13e3493572da33f992ba53a30fa886c1c38b6d","target":"record","created_at":"2026-05-18T01:56:41Z","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":"fce52b6884f06bc59cb463aae0f7d55a2cd6a0c4c56fcecb37727b15a18d38f6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-27T17:39:30Z","title_canon_sha256":"e90f9c6e3ed9bf062845a58c8a297b560aee6d3bc74121701a0bae26cbfb31f7"},"schema_version":"1.0","source":{"id":"1206.6346","kind":"arxiv","version":1}},"canonical_sha256":"d5a63775f612b84d8c21b624e52034d396a87bd1c514dcd083f02c1e62faf53c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d5a63775f612b84d8c21b624e52034d396a87bd1c514dcd083f02c1e62faf53c","first_computed_at":"2026-05-18T01:56:41.213794Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:56:41.213794Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1f4Uf3/fd8rmcwvxtP0c+j0jeIdfDZOw6R/VV7t60LIsBPLUddAPjrVvFXc7hmxWhlf8iQmi8MFB1+lBMo9WCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:56:41.214165Z","signed_message":"canonical_sha256_bytes"},"source_id":"1206.6346","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:84f104239678abe6c112503b3d13e3493572da33f992ba53a30fa886c1c38b6d","sha256:bd7eb954f7ab945483f9f1b248214872f3d1cf1879968b33b9b9bd43868995a8"],"state_sha256":"f8ee47b95491f1e6cd361cda40a814da6f084e9b765831e9c67dbe863c56044f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6xmZu/eVccbC9P4pSeTMk7GwTJrs6Nd+vsFFNJNzUdJPms1pqSKEHxarCfZLOe7Y/wykgDxmDOeOxOZoSG6+AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T08:44:52.627272Z","bundle_sha256":"275c46b1530824d0a910d9f8e1e4ec4132625a7aac74b434c8ec515707f3bc69"}}