{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:YJEWRIAMH6T2O6NGFXSF4RI6HZ","short_pith_number":"pith:YJEWRIAM","schema_version":"1.0","canonical_sha256":"c24968a00c3fa7a779a62de45e451e3e62a28c7eab86b4bc40dc8da45b2af75e","source":{"kind":"arxiv","id":"1211.1251","version":2},"attestation_state":"computed","paper":{"title":"Instanton Effects in ABJM Theory from Fermi Gas Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kazumi Okuyama, Sanefumi Moriyama, Yasuyuki Hatsuda","submitted_at":"2012-11-06T15:07:34Z","abstract_excerpt":"We study the instanton effects of the ABJM partition function using the Fermi gas formalism. We compute the exact values of the partition function at the Chern-Simons levels k=1,2,3,4,6 up to N=44,20,18,16,14 respectively, and extract non-perturbative corrections from these exact results. Fitting the resulting non-perturbative corrections by their expected forms from the Fermi gas, we determine unknown parameters in them. After separating the oscillating behavior of the grand potential, which originates in the periodicity of the grand partition function, and the worldsheet instanton contributi"},"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":"1211.1251","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-11-06T15:07:34Z","cross_cats_sorted":[],"title_canon_sha256":"cf2b1b25509096da44433a306ff943eeac0308736deec7aab225494717c14e85","abstract_canon_sha256":"28eecc9629335b5e96639476a7667152bb0d2996253f00196605dc0d14181d45"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:53:25.030341Z","signature_b64":"GL2Wnak0gN8VfMI7V9x3Hgaj4Mehot0SH2IfdZAya2VLzfiO4Zuhq+S1gIaBeh8piEl4ZMe8ju+DKMdvFW/aAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c24968a00c3fa7a779a62de45e451e3e62a28c7eab86b4bc40dc8da45b2af75e","last_reissued_at":"2026-05-18T01:53:25.029781Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:53:25.029781Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Instanton Effects in ABJM Theory from Fermi Gas Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kazumi Okuyama, Sanefumi Moriyama, Yasuyuki Hatsuda","submitted_at":"2012-11-06T15:07:34Z","abstract_excerpt":"We study the instanton effects of the ABJM partition function using the Fermi gas formalism. We compute the exact values of the partition function at the Chern-Simons levels k=1,2,3,4,6 up to N=44,20,18,16,14 respectively, and extract non-perturbative corrections from these exact results. Fitting the resulting non-perturbative corrections by their expected forms from the Fermi gas, we determine unknown parameters in them. After separating the oscillating behavior of the grand potential, which originates in the periodicity of the grand partition function, and the worldsheet instanton contributi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.1251","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":"1211.1251","created_at":"2026-05-18T01:53:25.029853+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.1251v2","created_at":"2026-05-18T01:53:25.029853+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.1251","created_at":"2026-05-18T01:53:25.029853+00:00"},{"alias_kind":"pith_short_12","alias_value":"YJEWRIAMH6T2","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_16","alias_value":"YJEWRIAMH6T2O6NG","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_8","alias_value":"YJEWRIAM","created_at":"2026-05-18T12:27:27.928770+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2602.10196","citing_title":"Bootstrapping ABJM theory","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2603.19159","citing_title":"$S^3$ partition functions and Equivariant CY$_4 $/CY$_3$ correspondence from Quantum curves","ref_index":30,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ","json":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ.json","graph_json":"https://pith.science/api/pith-number/YJEWRIAMH6T2O6NGFXSF4RI6HZ/graph.json","events_json":"https://pith.science/api/pith-number/YJEWRIAMH6T2O6NGFXSF4RI6HZ/events.json","paper":"https://pith.science/paper/YJEWRIAM"},"agent_actions":{"view_html":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ","download_json":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ.json","view_paper":"https://pith.science/paper/YJEWRIAM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.1251&json=true","fetch_graph":"https://pith.science/api/pith-number/YJEWRIAMH6T2O6NGFXSF4RI6HZ/graph.json","fetch_events":"https://pith.science/api/pith-number/YJEWRIAMH6T2O6NGFXSF4RI6HZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ/action/storage_attestation","attest_author":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ/action/author_attestation","sign_citation":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ/action/citation_signature","submit_replication":"https://pith.science/pith/YJEWRIAMH6T2O6NGFXSF4RI6HZ/action/replication_record"}},"created_at":"2026-05-18T01:53:25.029853+00:00","updated_at":"2026-05-18T01:53:25.029853+00:00"}