{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:B64KMWQYNRS2M42JGID7RZ6AJR","short_pith_number":"pith:B64KMWQY","schema_version":"1.0","canonical_sha256":"0fb8a65a186c65a673493207f8e7c04c46096d8443b34d1328a7d8dea56fdfb9","source":{"kind":"arxiv","id":"hep-th/9809165","version":1},"attestation_state":"computed","paper":{"title":"On Exact Supersymmetry in DLCQ","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"F. Antonuccio, O. Lunin, S. Pinsky","submitted_at":"1998-09-22T23:07:56Z","abstract_excerpt":"In recent years a supersymmetric form of discrete light-cone quantization (hereafter `SDLCQ') has emerged as a very powerful tool for solving supersymmetric field theories. In this scheme, one calculates the light-cone supercharge with respect to a discretized light-cone Fock basis, instead of working with the light-cone Hamiltonian. This procedure has the advantage of preserving supersymmetry even in the discretized theory, and eliminates the need for explicit renormalizations in 1+1 dimensions. In order to compare the usual DLCQ prescription with the supersymmetric prescription, we consider "},"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/9809165","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-09-22T23:07:56Z","cross_cats_sorted":[],"title_canon_sha256":"766c708d6f470935fc48ac0ea3ef3af9f5fa7bdd00ed91039922e70f52f9707e","abstract_canon_sha256":"37e95376fe13195aada6c8af379e1e0b47d2077fe8fce44b4f5b0a7cebc562ad"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:55.166169Z","signature_b64":"OgIhhDCK5FDJ1419A+T6fnAJ+u+w6KWtUP7FElfhLjMeLu7rCGIgB4WEWAUy5oMB+IV72GO89MEb0lzkBgEoCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0fb8a65a186c65a673493207f8e7c04c46096d8443b34d1328a7d8dea56fdfb9","last_reissued_at":"2026-07-04T16:09:55.165754Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:55.165754Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On Exact Supersymmetry in DLCQ","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"F. Antonuccio, O. Lunin, S. Pinsky","submitted_at":"1998-09-22T23:07:56Z","abstract_excerpt":"In recent years a supersymmetric form of discrete light-cone quantization (hereafter `SDLCQ') has emerged as a very powerful tool for solving supersymmetric field theories. In this scheme, one calculates the light-cone supercharge with respect to a discretized light-cone Fock basis, instead of working with the light-cone Hamiltonian. This procedure has the advantage of preserving supersymmetry even in the discretized theory, and eliminates the need for explicit renormalizations in 1+1 dimensions. In order to compare the usual DLCQ prescription with the supersymmetric prescription, we consider "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9809165","kind":"arxiv","version":1},"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/9809165/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/9809165","created_at":"2026-07-04T16:09:55.165819+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9809165v1","created_at":"2026-07-04T16:09:55.165819+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9809165","created_at":"2026-07-04T16:09:55.165819+00:00"},{"alias_kind":"pith_short_12","alias_value":"B64KMWQYNRS2","created_at":"2026-07-04T16:09:55.165819+00:00"},{"alias_kind":"pith_short_16","alias_value":"B64KMWQYNRS2M42J","created_at":"2026-07-04T16:09:55.165819+00:00"},{"alias_kind":"pith_short_8","alias_value":"B64KMWQY","created_at":"2026-07-04T16:09:55.165819+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.17138","citing_title":"Supercurrents and (Partial) Supersymmetry in Adjoint QCD$_2$ and Its Generalizations","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR","json":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR.json","graph_json":"https://pith.science/api/pith-number/B64KMWQYNRS2M42JGID7RZ6AJR/graph.json","events_json":"https://pith.science/api/pith-number/B64KMWQYNRS2M42JGID7RZ6AJR/events.json","paper":"https://pith.science/paper/B64KMWQY"},"agent_actions":{"view_html":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR","download_json":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR.json","view_paper":"https://pith.science/paper/B64KMWQY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9809165&json=true","fetch_graph":"https://pith.science/api/pith-number/B64KMWQYNRS2M42JGID7RZ6AJR/graph.json","fetch_events":"https://pith.science/api/pith-number/B64KMWQYNRS2M42JGID7RZ6AJR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR/action/storage_attestation","attest_author":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR/action/author_attestation","sign_citation":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR/action/citation_signature","submit_replication":"https://pith.science/pith/B64KMWQYNRS2M42JGID7RZ6AJR/action/replication_record"}},"created_at":"2026-07-04T16:09:55.165819+00:00","updated_at":"2026-07-04T16:09:55.165819+00:00"}