{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:F4FYTVPCPO3L3UDERCSGWDPFCY","short_pith_number":"pith:F4FYTVPC","schema_version":"1.0","canonical_sha256":"2f0b89d5e27bb6bdd06488a46b0de516201a0e2817cb77294565e5b7fd9a4ab0","source":{"kind":"arxiv","id":"hep-th/9610043","version":3},"attestation_state":"computed","paper":{"title":"M Theory As A Matrix Model: A Conjecture","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"L. Susskind, S.H. Shenker, T. Banks, W. Fischler","submitted_at":"1996-10-07T21:32:58Z","abstract_excerpt":"We suggest and motivate a precise equivalence between uncompactified eleven dimensional M-theory and the N = infinity limit of the supersymmetric matrix quantum mechanics describing D0-branes. The evidence for the conjecture consists of several correspondences between the two theories. As a consequence of supersymmetry the simple matrix model is rich enough to describe the properties of the entire Fock space of massless well separated particles of the supergravity theory. In one particular kinematic situation the leading large distance interaction of these particles is exactly described by sup"},"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":"hep-th/9610043","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-10-07T21:32:58Z","cross_cats_sorted":[],"title_canon_sha256":"baaa378d282762ee6235a86686a6b51a27eb50ac0eeaf4052a6161f09b25cff8","abstract_canon_sha256":"c81debe164f235cddcd489e3bc52bb7fda6731247bb7d6b9571f1e13723e3a4c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:45:47.345050Z","signature_b64":"QhiwV1f21pPQ0QmoH1ZK8BU37z+GDKZ/lR9gttAZFc+SZVtodPBy1LyYkYpZO3zHJ+cVSTzKSBVx14SYox6zBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f0b89d5e27bb6bdd06488a46b0de516201a0e2817cb77294565e5b7fd9a4ab0","last_reissued_at":"2026-07-04T15:45:47.344643Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:45:47.344643Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"M Theory As A Matrix Model: A Conjecture","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"L. Susskind, S.H. Shenker, T. Banks, W. Fischler","submitted_at":"1996-10-07T21:32:58Z","abstract_excerpt":"We suggest and motivate a precise equivalence between uncompactified eleven dimensional M-theory and the N = infinity limit of the supersymmetric matrix quantum mechanics describing D0-branes. The evidence for the conjecture consists of several correspondences between the two theories. As a consequence of supersymmetry the simple matrix model is rich enough to describe the properties of the entire Fock space of massless well separated particles of the supergravity theory. In one particular kinematic situation the leading large distance interaction of these particles is exactly described by sup"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9610043","kind":"arxiv","version":3},"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/hep-th/9610043/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":"hep-th/9610043","created_at":"2026-07-04T15:45:47.344702+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9610043v3","created_at":"2026-07-04T15:45:47.344702+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9610043","created_at":"2026-07-04T15:45:47.344702+00:00"},{"alias_kind":"pith_short_12","alias_value":"F4FYTVPCPO3L","created_at":"2026-07-04T15:45:47.344702+00:00"},{"alias_kind":"pith_short_16","alias_value":"F4FYTVPCPO3L3UDE","created_at":"2026-07-04T15:45:47.344702+00:00"},{"alias_kind":"pith_short_8","alias_value":"F4FYTVPC","created_at":"2026-07-04T15:45:47.344702+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":35,"internal_anchor_count":26,"sample":[{"citing_arxiv_id":"2607.08481","citing_title":"Gram--Wishart--Stiefel formulation of the $N=2$, large--$d$ gauge theory in 1D","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24859","citing_title":"Additional constraints for the tensor bootstrap","ref_index":65,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24577","citing_title":"Description of curved spacetimes by finite-size matrices in the type IIB matrix model","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2606.18396","citing_title":"An effective field theory approach to the sign problem in BFSS","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17758","citing_title":"A Double--Scaling Large--\\(d\\) Saddle of BFSS/BMN Matrix Quantum Mechanics","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2606.09521","citing_title":"Negative heat capacities in spherically symmetric sectors of $d$-matrix quantum mechanics","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2606.07504","citing_title":"On the large N convergence of matrix models","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2606.05388","citing_title":"BPS Non-Renormalization in the BMN Matrix Model","ref_index":12,"is_internal_anchor":true},{"citing_arxiv_id":"2606.05314","citing_title":"Mass-Flow Invariance of $Q$-Cohomology in BMN Matrix Quantum Mechanics","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.03496","citing_title":"Off-Shell Supersymmetry Algebra in the Lorentzian IIB Matrix Model: Algebraic Constraints and a $\\kappa$-Minkowski-Like Sector","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2605.10720","citing_title":"Regularized Master-Field Approximation for Large-$N$ Reduced Matrix Models","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25560","citing_title":"Finite-$N$ BMN index across all vacuum sectors","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25647","citing_title":"Endpoint formulation and Molien--Weyl structure for the \\(N=2\\), large--\\(d\\) BFSS/BMN models","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2605.26055","citing_title":"Krylov Complexity for Plane Wave Matrix Model","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2605.27359","citing_title":"Wilson coefficients from a non-renormalization theorem in 2D SYM","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"1907.06280","citing_title":"Noncommutative Gauge Theories and Gravity","ref_index":47,"is_internal_anchor":true},{"citing_arxiv_id":"2206.09952","citing_title":"Tachyonic AdS/QCD, Determining the Strong Running Coupling and \\beta-function in both UV and IR Regions of AdS Space","ref_index":87,"is_internal_anchor":true},{"citing_arxiv_id":"2311.10565","citing_title":"Worldsheet Formalism for Decoupling Limits in String Theory","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2411.11096","citing_title":"An extremal black hole with a unique ground state","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16507","citing_title":"Krylov complexity from a simple quantum mechanical model for a radiating black hole","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"2506.16164","citing_title":"The Carrollian Kaleidoscope","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2511.08560","citing_title":"Bootstrapping Euclidean Two-point Correlators","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13972","citing_title":"Multi-Matrix Quantum Mechanics, Collective Fields and Emergent Space","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2603.27824","citing_title":"Higher-spin composites and emergent AdS$_3$ geometry in the $(1+1)$-dimensional Gross-Neveu model","ref_index":48,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13294","citing_title":"Quantum spacetime and quantum fluctuations in the IKKT model at weak coupling","ref_index":44,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY","json":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY.json","graph_json":"https://pith.science/api/pith-number/F4FYTVPCPO3L3UDERCSGWDPFCY/graph.json","events_json":"https://pith.science/api/pith-number/F4FYTVPCPO3L3UDERCSGWDPFCY/events.json","paper":"https://pith.science/paper/F4FYTVPC"},"agent_actions":{"view_html":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY","download_json":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY.json","view_paper":"https://pith.science/paper/F4FYTVPC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9610043&json=true","fetch_graph":"https://pith.science/api/pith-number/F4FYTVPCPO3L3UDERCSGWDPFCY/graph.json","fetch_events":"https://pith.science/api/pith-number/F4FYTVPCPO3L3UDERCSGWDPFCY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY/action/storage_attestation","attest_author":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY/action/author_attestation","sign_citation":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY/action/citation_signature","submit_replication":"https://pith.science/pith/F4FYTVPCPO3L3UDERCSGWDPFCY/action/replication_record"}},"created_at":"2026-07-04T15:45:47.344702+00:00","updated_at":"2026-07-04T15:45:47.344702+00:00"}