{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:KHAKU36ZSMKKG5PQUBMFO2T4WG","short_pith_number":"pith:KHAKU36Z","schema_version":"1.0","canonical_sha256":"51c0aa6fd99314a375f0a058576a7cb1a84c5e4d0faf1f37a599fb4a2ccf8dfe","source":{"kind":"arxiv","id":"2303.15207","version":2},"attestation_state":"computed","paper":{"title":"Wilson loops at large $N$ and the quantum M2 brane","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Arkady A. Tseytlin, Simone Giombi","submitted_at":"2023-03-27T13:45:44Z","abstract_excerpt":"The Wilson loop operator in the $U(N)_k \\times U(N)_{-k}$ ABJM theory at large $N$ and fixed level $k$ has a dual description in terms of a wrapped M2 brane in the M-theory background AdS$_4 \\times S^7/\\mathbb Z_k$. We consider the localization result for the $1\\over 2$-BPS circular Wilson loop expectation value $W$ in this regime, and compare it to the prediction of the M2 brane theory. The leading large $N$ exponential factor is matched as expected by the classical action of the M2 brane solution with AdS$_2\\times S^1$ geometry. We show that the subleading $k$-dependent prefactor in $W$ is a"},"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":"2303.15207","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-03-27T13:45:44Z","cross_cats_sorted":[],"title_canon_sha256":"a1c4ce543f31941233df7accfd164e6c93f2ee0556f37f84a90bda8e78040f57","abstract_canon_sha256":"3e27934ca97f932456588a0437be537292436b7ce85bce25731be9ff0511abe5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:15:27.703621Z","signature_b64":"AM/pY3czqUslMd80wBt91N19DlMZI1veb1hrCfAAGLobOs1iyGPvbCw+BMvmu4bYD3j5AUbDp+b8GWTtywG4Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"51c0aa6fd99314a375f0a058576a7cb1a84c5e4d0faf1f37a599fb4a2ccf8dfe","last_reissued_at":"2026-07-05T06:15:27.703181Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:15:27.703181Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wilson loops at large $N$ and the quantum M2 brane","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Arkady A. Tseytlin, Simone Giombi","submitted_at":"2023-03-27T13:45:44Z","abstract_excerpt":"The Wilson loop operator in the $U(N)_k \\times U(N)_{-k}$ ABJM theory at large $N$ and fixed level $k$ has a dual description in terms of a wrapped M2 brane in the M-theory background AdS$_4 \\times S^7/\\mathbb Z_k$. We consider the localization result for the $1\\over 2$-BPS circular Wilson loop expectation value $W$ in this regime, and compare it to the prediction of the M2 brane theory. The leading large $N$ exponential factor is matched as expected by the classical action of the M2 brane solution with AdS$_2\\times S^1$ geometry. We show that the subleading $k$-dependent prefactor in $W$ is a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.15207","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/2303.15207/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":"2303.15207","created_at":"2026-07-05T06:15:27.703236+00:00"},{"alias_kind":"arxiv_version","alias_value":"2303.15207v2","created_at":"2026-07-05T06:15:27.703236+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.15207","created_at":"2026-07-05T06:15:27.703236+00:00"},{"alias_kind":"pith_short_12","alias_value":"KHAKU36ZSMKK","created_at":"2026-07-05T06:15:27.703236+00:00"},{"alias_kind":"pith_short_16","alias_value":"KHAKU36ZSMKKG5PQ","created_at":"2026-07-05T06:15:27.703236+00:00"},{"alias_kind":"pith_short_8","alias_value":"KHAKU36Z","created_at":"2026-07-05T06:15:27.703236+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.01167","citing_title":"One-loop divergences for KK theories on $\\mathrm{AdS}\\times S$ spaces; a reanalysis of $\\mathrm{AdS}_4 \\times S^7\\,\\big/$ ABJM precision holography","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2602.10196","citing_title":"Bootstrapping ABJM theory","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2603.25590","citing_title":"Wilson loop in AdS$_3 \\times S^3 \\times T^4$ from quantum M2 brane","ref_index":4,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00987","citing_title":"A gravity interpretation for the complex Euclidean saddles of the ABJM index","ref_index":55,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG","json":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG.json","graph_json":"https://pith.science/api/pith-number/KHAKU36ZSMKKG5PQUBMFO2T4WG/graph.json","events_json":"https://pith.science/api/pith-number/KHAKU36ZSMKKG5PQUBMFO2T4WG/events.json","paper":"https://pith.science/paper/KHAKU36Z"},"agent_actions":{"view_html":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG","download_json":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG.json","view_paper":"https://pith.science/paper/KHAKU36Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2303.15207&json=true","fetch_graph":"https://pith.science/api/pith-number/KHAKU36ZSMKKG5PQUBMFO2T4WG/graph.json","fetch_events":"https://pith.science/api/pith-number/KHAKU36ZSMKKG5PQUBMFO2T4WG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG/action/storage_attestation","attest_author":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG/action/author_attestation","sign_citation":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG/action/citation_signature","submit_replication":"https://pith.science/pith/KHAKU36ZSMKKG5PQUBMFO2T4WG/action/replication_record"}},"created_at":"2026-07-05T06:15:27.703236+00:00","updated_at":"2026-07-05T06:15:27.703236+00:00"}