{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:EBWRVZVSXF47TY6HEWQOAUM724","short_pith_number":"pith:EBWRVZVS","schema_version":"1.0","canonical_sha256":"206d1ae6b2b979f9e3c725a0e0519fd70e6c1385148fdd938ef0f911ab31a27a","source":{"kind":"arxiv","id":"0906.3008","version":2},"attestation_state":"computed","paper":{"title":"Charges of Monopole Operators in Chern-Simons Yang-Mills Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Igor R. Klebanov, Marcus K. Benna, Thomas Klose","submitted_at":"2009-06-17T17:19:37Z","abstract_excerpt":"We calculate the non-abelian R-charges of BPS monopole operators in three-dimensional gauge theories with N=3 supersymmetry. This class of models includes ABJM theory, the proposed gauge theory dual of M-theory on AdS_4 x S^7/Z_k, as a special case. In the UV limit of the N=3 theories the Yang-Mills coupling becomes weak and the monopole operators are described by classical backgrounds. This allows us to find their SU(2)_R charges in a one-loop computation which by virtue of the non-renormalization of non-abelian R-charges yields the exact result for any value of the coupling. The spectrum of "},"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":"0906.3008","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-06-17T17:19:37Z","cross_cats_sorted":[],"title_canon_sha256":"449a679debc6ecba9e30bc7791f7059e5539f9af5e6f5bf671e61f9a9a2c4615","abstract_canon_sha256":"f09f477039b17f1a611017bb2ec0d7387f9f84634752d86ecaee6dc37cc83748"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:13:19.648971Z","signature_b64":"XaW4PGKczjnkjbhNL43xmHHDVpWdPl7CsJWiBKGBKIHoliiCXqJic2ewW3nlFkU04B7YEpUgWbOiDz8QY74ODg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"206d1ae6b2b979f9e3c725a0e0519fd70e6c1385148fdd938ef0f911ab31a27a","last_reissued_at":"2026-05-18T02:13:19.648414Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:13:19.648414Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charges of Monopole Operators in Chern-Simons Yang-Mills Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Igor R. Klebanov, Marcus K. Benna, Thomas Klose","submitted_at":"2009-06-17T17:19:37Z","abstract_excerpt":"We calculate the non-abelian R-charges of BPS monopole operators in three-dimensional gauge theories with N=3 supersymmetry. This class of models includes ABJM theory, the proposed gauge theory dual of M-theory on AdS_4 x S^7/Z_k, as a special case. In the UV limit of the N=3 theories the Yang-Mills coupling becomes weak and the monopole operators are described by classical backgrounds. This allows us to find their SU(2)_R charges in a one-loop computation which by virtue of the non-renormalization of non-abelian R-charges yields the exact result for any value of the coupling. The spectrum of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0906.3008","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":""},"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":"0906.3008","created_at":"2026-05-18T02:13:19.648488+00:00"},{"alias_kind":"arxiv_version","alias_value":"0906.3008v2","created_at":"2026-05-18T02:13:19.648488+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0906.3008","created_at":"2026-05-18T02:13:19.648488+00:00"},{"alias_kind":"pith_short_12","alias_value":"EBWRVZVSXF47","created_at":"2026-05-18T12:25:59.703012+00:00"},{"alias_kind":"pith_short_16","alias_value":"EBWRVZVSXF47TY6H","created_at":"2026-05-18T12:25:59.703012+00:00"},{"alias_kind":"pith_short_8","alias_value":"EBWRVZVS","created_at":"2026-05-18T12:25:59.703012+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/EBWRVZVSXF47TY6HEWQOAUM724","json":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724.json","graph_json":"https://pith.science/api/pith-number/EBWRVZVSXF47TY6HEWQOAUM724/graph.json","events_json":"https://pith.science/api/pith-number/EBWRVZVSXF47TY6HEWQOAUM724/events.json","paper":"https://pith.science/paper/EBWRVZVS"},"agent_actions":{"view_html":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724","download_json":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724.json","view_paper":"https://pith.science/paper/EBWRVZVS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0906.3008&json=true","fetch_graph":"https://pith.science/api/pith-number/EBWRVZVSXF47TY6HEWQOAUM724/graph.json","fetch_events":"https://pith.science/api/pith-number/EBWRVZVSXF47TY6HEWQOAUM724/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724/action/storage_attestation","attest_author":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724/action/author_attestation","sign_citation":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724/action/citation_signature","submit_replication":"https://pith.science/pith/EBWRVZVSXF47TY6HEWQOAUM724/action/replication_record"}},"created_at":"2026-05-18T02:13:19.648488+00:00","updated_at":"2026-05-18T02:13:19.648488+00:00"}