{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:SSV2SMGJW57TVH4CYQK22FMF23","short_pith_number":"pith:SSV2SMGJ","schema_version":"1.0","canonical_sha256":"94aba930c9b77f3a9f82c415ad1585d6e4f84816659d5bb6dac4014da1f78765","source":{"kind":"arxiv","id":"1410.0558","version":2},"attestation_state":"computed","paper":{"title":"3D Field Theories with Chern--Simons Term for Large $N$ in the Weyl Gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jean Zinn-Justin, Moshe Moshe","submitted_at":"2014-10-02T14:11:36Z","abstract_excerpt":"Three dimensional, $U(N)$ symmetric, field theory with fermion matter coupled to a topological Chern--Simons term, in the large $N$ limit is analyzed in details. We determine the conditions for the existence of a massless conformal invariant ground state as well as the conditions for a massive phase. We analyze the phase structure and calculate gauge invariant corelators comparing them in several cases to existing results. In addition to the non-critical explicitly broken scale invariance massive case we consider also a massive ground state where the scale symmetry is spontaneously broken. We "},"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":"1410.0558","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-02T14:11:36Z","cross_cats_sorted":[],"title_canon_sha256":"67f05890a28ef45be49187b7bcf6243a864306ee2cb3dbc4b97fd7708d849bc9","abstract_canon_sha256":"d8f6bc2269e69c4c259ef4425312c4456ea511f4bdf49df203e3f5712855b0c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:11:28.465419Z","signature_b64":"pUbDkWv8Y42erKO///iEL9nkjSvSe+nEulSp3MsASY7e7e3cbiSVTYBwyT9xDWDNfsyj0IreVq7+KpXycutaBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"94aba930c9b77f3a9f82c415ad1585d6e4f84816659d5bb6dac4014da1f78765","last_reissued_at":"2026-07-05T00:11:28.465004Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:11:28.465004Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"3D Field Theories with Chern--Simons Term for Large $N$ in the Weyl Gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jean Zinn-Justin, Moshe Moshe","submitted_at":"2014-10-02T14:11:36Z","abstract_excerpt":"Three dimensional, $U(N)$ symmetric, field theory with fermion matter coupled to a topological Chern--Simons term, in the large $N$ limit is analyzed in details. We determine the conditions for the existence of a massless conformal invariant ground state as well as the conditions for a massive phase. We analyze the phase structure and calculate gauge invariant corelators comparing them in several cases to existing results. In addition to the non-critical explicitly broken scale invariance massive case we consider also a massive ground state where the scale symmetry is spontaneously broken. We "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.0558","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1410.0558/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1410.0558","created_at":"2026-07-05T00:11:28.465057+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.0558v2","created_at":"2026-07-05T00:11:28.465057+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.0558","created_at":"2026-07-05T00:11:28.465057+00:00"},{"alias_kind":"pith_short_12","alias_value":"SSV2SMGJW57T","created_at":"2026-07-05T00:11:28.465057+00:00"},{"alias_kind":"pith_short_16","alias_value":"SSV2SMGJW57TVH4C","created_at":"2026-07-05T00:11:28.465057+00:00"},{"alias_kind":"pith_short_8","alias_value":"SSV2SMGJ","created_at":"2026-07-05T00:11:28.465057+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.00107","citing_title":"Dilaton Physics from Asymptotic Freedom","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23","json":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23.json","graph_json":"https://pith.science/api/pith-number/SSV2SMGJW57TVH4CYQK22FMF23/graph.json","events_json":"https://pith.science/api/pith-number/SSV2SMGJW57TVH4CYQK22FMF23/events.json","paper":"https://pith.science/paper/SSV2SMGJ"},"agent_actions":{"view_html":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23","download_json":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23.json","view_paper":"https://pith.science/paper/SSV2SMGJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.0558&json=true","fetch_graph":"https://pith.science/api/pith-number/SSV2SMGJW57TVH4CYQK22FMF23/graph.json","fetch_events":"https://pith.science/api/pith-number/SSV2SMGJW57TVH4CYQK22FMF23/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23/action/storage_attestation","attest_author":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23/action/author_attestation","sign_citation":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23/action/citation_signature","submit_replication":"https://pith.science/pith/SSV2SMGJW57TVH4CYQK22FMF23/action/replication_record"}},"created_at":"2026-07-05T00:11:28.465057+00:00","updated_at":"2026-07-05T00:11:28.465057+00:00"}