{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:INHM3YCEJXZ5T6I3F5SCBUOG6K","short_pith_number":"pith:INHM3YCE","schema_version":"1.0","canonical_sha256":"434ecde0444df3d9f91b2f6420d1c6f299029be6c17d5e85637a3e288848c05a","source":{"kind":"arxiv","id":"1711.07343","version":2},"attestation_state":"computed","paper":{"title":"Solving M-theory with the Conformal Bootstrap","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Nathan B. Agmon, Shai M. Chester, Silviu S. Pufu","submitted_at":"2017-11-20T14:54:48Z","abstract_excerpt":"We use the conformal bootstrap to perform a precision study of 3d maximally supersymmetric ($\\mathcal{N}=8$) SCFTs that describe the IR physics on $N$ coincident M2-branes placed either in flat space or at a $\\C^4/\\Z_2$ singularity. First, using the explicit Lagrangians of ABJ(M) \\cite{Aharony:2008ug,Aharony:2008gk} and recent supersymmetric localization results, we calculate certain half and quarter-BPS OPE coefficients, both exactly at small $N$, and approximately in a large $N$ expansion that we perform to all orders in $1/N$. Comparing these values with the numerical bootstrap bounds leads"},"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":"1711.07343","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-11-20T14:54:48Z","cross_cats_sorted":[],"title_canon_sha256":"d6ef7e0e6cc21ab0ddaabce51b4cfb27dd28701ac078feb08ee9c77594b48954","abstract_canon_sha256":"5c1889d8e69579fadf824e7fda4183fa0dd23c670c9908aa6a617c70a795d748"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:09:30.239932Z","signature_b64":"1OApGDwrFrsimPO/T3n+7fVeRu3Pd4ryFknNOxp8m4J5p4PTKBqGJdR8M6g6nXRZSgxCF8nhqrK4Pd6KWQuZBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"434ecde0444df3d9f91b2f6420d1c6f299029be6c17d5e85637a3e288848c05a","last_reissued_at":"2026-05-18T00:09:30.239251Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:09:30.239251Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Solving M-theory with the Conformal Bootstrap","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Nathan B. Agmon, Shai M. Chester, Silviu S. Pufu","submitted_at":"2017-11-20T14:54:48Z","abstract_excerpt":"We use the conformal bootstrap to perform a precision study of 3d maximally supersymmetric ($\\mathcal{N}=8$) SCFTs that describe the IR physics on $N$ coincident M2-branes placed either in flat space or at a $\\C^4/\\Z_2$ singularity. First, using the explicit Lagrangians of ABJ(M) \\cite{Aharony:2008ug,Aharony:2008gk} and recent supersymmetric localization results, we calculate certain half and quarter-BPS OPE coefficients, both exactly at small $N$, and approximately in a large $N$ expansion that we perform to all orders in $1/N$. Comparing these values with the numerical bootstrap bounds leads"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.07343","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":"1711.07343","created_at":"2026-05-18T00:09:30.239373+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.07343v2","created_at":"2026-05-18T00:09:30.239373+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.07343","created_at":"2026-05-18T00:09:30.239373+00:00"},{"alias_kind":"pith_short_12","alias_value":"INHM3YCEJXZ5","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_16","alias_value":"INHM3YCEJXZ5T6I3","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_8","alias_value":"INHM3YCE","created_at":"2026-05-18T12:31:21.493067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.04606","citing_title":"An Airy Tale at Large $N$","ref_index":30,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K","json":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K.json","graph_json":"https://pith.science/api/pith-number/INHM3YCEJXZ5T6I3F5SCBUOG6K/graph.json","events_json":"https://pith.science/api/pith-number/INHM3YCEJXZ5T6I3F5SCBUOG6K/events.json","paper":"https://pith.science/paper/INHM3YCE"},"agent_actions":{"view_html":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K","download_json":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K.json","view_paper":"https://pith.science/paper/INHM3YCE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.07343&json=true","fetch_graph":"https://pith.science/api/pith-number/INHM3YCEJXZ5T6I3F5SCBUOG6K/graph.json","fetch_events":"https://pith.science/api/pith-number/INHM3YCEJXZ5T6I3F5SCBUOG6K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K/action/storage_attestation","attest_author":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K/action/author_attestation","sign_citation":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K/action/citation_signature","submit_replication":"https://pith.science/pith/INHM3YCEJXZ5T6I3F5SCBUOG6K/action/replication_record"}},"created_at":"2026-05-18T00:09:30.239373+00:00","updated_at":"2026-05-18T00:09:30.239373+00:00"}