{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:JDCIDV6B2LNFHVVSCW62JS7G7T","short_pith_number":"pith:JDCIDV6B","schema_version":"1.0","canonical_sha256":"48c481d7c1d2da53d6b215bda4cbe6fcfb9b1a6c91aa913843510213f2fed25d","source":{"kind":"arxiv","id":"hep-th/9612115","version":2},"attestation_state":"computed","paper":{"title":"A Large-N Reduced Model as Superstring","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Tsuchiya, H. Kawai, N. Ishibashi, Y. Kitazawa","submitted_at":"1996-12-11T08:38:56Z","abstract_excerpt":"A matrix model which has the manifest ten-dimensional N=2 super Poincare invariance is proposed. Interactions between BPS-saturated states are analyzed to show that massless spectrum is the same as that of type IIB string theory. It is conjectured that the large-N reduced model of ten-dimensional super Yang-Mills theory can be regarded as a constructive definition of this model and therefore is equivalent to superstring theory."},"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/9612115","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-12-11T08:38:56Z","cross_cats_sorted":[],"title_canon_sha256":"8f620d4efeb03956096fffa14f28c06fb330ac44bf489c85b9d53419f54d102c","abstract_canon_sha256":"35d9715c9a3c6529a80ef1a068917fabe389e12b75e280f9851fac367f5fe1f5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:27.193589Z","signature_b64":"5Zkqqd8zXxhONHgeRFcGt4lzO55Xl+RWpeY8lChwvr4P3WnqzlyhqRK2cPBN/HeVUKqreviEqTL6IT97FdjhAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"48c481d7c1d2da53d6b215bda4cbe6fcfb9b1a6c91aa913843510213f2fed25d","last_reissued_at":"2026-07-04T16:02:27.193206Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:27.193206Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Large-N Reduced Model as Superstring","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Tsuchiya, H. Kawai, N. Ishibashi, Y. Kitazawa","submitted_at":"1996-12-11T08:38:56Z","abstract_excerpt":"A matrix model which has the manifest ten-dimensional N=2 super Poincare invariance is proposed. Interactions between BPS-saturated states are analyzed to show that massless spectrum is the same as that of type IIB string theory. It is conjectured that the large-N reduced model of ten-dimensional super Yang-Mills theory can be regarded as a constructive definition of this model and therefore is equivalent to superstring theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9612115","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/hep-th/9612115/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/9612115","created_at":"2026-07-04T16:02:27.193267+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9612115v2","created_at":"2026-07-04T16:02:27.193267+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9612115","created_at":"2026-07-04T16:02:27.193267+00:00"},{"alias_kind":"pith_short_12","alias_value":"JDCIDV6B2LNF","created_at":"2026-07-04T16:02:27.193267+00:00"},{"alias_kind":"pith_short_16","alias_value":"JDCIDV6B2LNFHVVS","created_at":"2026-07-04T16:02:27.193267+00:00"},{"alias_kind":"pith_short_8","alias_value":"JDCIDV6B","created_at":"2026-07-04T16:02:27.193267+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":23,"internal_anchor_count":16,"sample":[{"citing_arxiv_id":"2607.08481","citing_title":"Gram--Wishart--Stiefel formulation of the $N=2$, large--$d$ gauge theory in 1D","ref_index":71,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24859","citing_title":"Additional constraints for the tensor bootstrap","ref_index":70,"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":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.27333","citing_title":"The IKKT renormalization group flow is IIB: toward zero-d holography","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":15,"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":27,"is_internal_anchor":true},{"citing_arxiv_id":"2606.07504","citing_title":"On the large N convergence of matrix models","ref_index":6,"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":1,"is_internal_anchor":true},{"citing_arxiv_id":"2605.10720","citing_title":"Regularized Master-Field Approximation for Large-$N$ Reduced Matrix Models","ref_index":6,"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":55,"is_internal_anchor":true},{"citing_arxiv_id":"1907.06280","citing_title":"Noncommutative Gauge Theories and Gravity","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"1907.06280","citing_title":"Noncommutative Gauge Theories and Gravity","ref_index":48,"is_internal_anchor":true},{"citing_arxiv_id":"2311.10565","citing_title":"Worldsheet Formalism for Decoupling Limits in String Theory","ref_index":89,"is_internal_anchor":true},{"citing_arxiv_id":"2507.17802","citing_title":"Instabilities in scale-separated Casimir vacua","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13972","citing_title":"Multi-Matrix Quantum Mechanics, Collective Fields and Emergent Space","ref_index":2,"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":20,"is_internal_anchor":true},{"citing_arxiv_id":"2605.10720","citing_title":"Regularized Master-Field Approximation for Large-$N$ Reduced Matrix Models","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25564","citing_title":"Impact of supersymmetry on the dynamical emergence of the spacetime in the type IIB matrix model with the Lorentz symmetry \"gauge fixed\"","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25052","citing_title":"Path integral for the closed superstring and the matrix model","ref_index":2,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04621","citing_title":"Molien--Weyl Singlet Counting and BFSS$_2$--Factorization in Gaussian Matrix QM","ref_index":60,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19836","citing_title":"The emergence of (3+1)-dimensional expanding spacetime from complex Langevin simulations of the Lorentzian type IIB matrix model with deformations","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2604.04774","citing_title":"Exponentially Long Evaporation of Noncommutative Black Hole","ref_index":52,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14508","citing_title":"Fermionic modes of D-instanton wormholes from broken local supersymmetry","ref_index":3,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T","json":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T.json","graph_json":"https://pith.science/api/pith-number/JDCIDV6B2LNFHVVSCW62JS7G7T/graph.json","events_json":"https://pith.science/api/pith-number/JDCIDV6B2LNFHVVSCW62JS7G7T/events.json","paper":"https://pith.science/paper/JDCIDV6B"},"agent_actions":{"view_html":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T","download_json":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T.json","view_paper":"https://pith.science/paper/JDCIDV6B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9612115&json=true","fetch_graph":"https://pith.science/api/pith-number/JDCIDV6B2LNFHVVSCW62JS7G7T/graph.json","fetch_events":"https://pith.science/api/pith-number/JDCIDV6B2LNFHVVSCW62JS7G7T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T/action/storage_attestation","attest_author":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T/action/author_attestation","sign_citation":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T/action/citation_signature","submit_replication":"https://pith.science/pith/JDCIDV6B2LNFHVVSCW62JS7G7T/action/replication_record"}},"created_at":"2026-07-04T16:02:27.193267+00:00","updated_at":"2026-07-04T16:02:27.193267+00:00"}