{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:LMAZLVKV4AWTO5BX4C43WMGQNI","short_pith_number":"pith:LMAZLVKV","schema_version":"1.0","canonical_sha256":"5b0195d555e02d377437e0b9bb30d06a130a30e27a20d3fabff5969aa20d142b","source":{"kind":"arxiv","id":"hep-th/9508143","version":5},"attestation_state":"computed","paper":{"title":"An SL(2,Z) Multiplet of Type IIB Superstrings","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"John H. Schwarz","submitted_at":"1995-08-25T23:22:43Z","abstract_excerpt":"An SL(2, Z) family of string solutions of type IIB supergravity in ten dimensions is constructed. The solutions are labeled by a pair of relatively prime integers, which characterize charges of the three-form field strengths. The string tensions depend on these charges in an SL(2, Z) covariant way. Compactifying on a circle and identifying with eleven-dimensional supergravity compactified on a torus implies that the modulus of the IIB theory should be equated to the modular parameter of the torus."},"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/9508143","kind":"arxiv","version":5},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1995-08-25T23:22:43Z","cross_cats_sorted":[],"title_canon_sha256":"56ed25a2b044a0a6f7707e8655e1a4114ad75b645bec5c984a1d53eaa3c005b4","abstract_canon_sha256":"2201df685e2800aa1a296a8fbc10661fc61b5a70e0d3f7917a427844aa7920bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:03.869917Z","signature_b64":"3NRjcyRMBmxO3k1c7i9P4xuLu8sd+CFqtHl2nBUtSTNdseim0TiIFayELr9HcS9/H1I/phBUduG15LqVRfdZCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5b0195d555e02d377437e0b9bb30d06a130a30e27a20d3fabff5969aa20d142b","last_reissued_at":"2026-05-18T02:36:03.869367Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:03.869367Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An SL(2,Z) Multiplet of Type IIB Superstrings","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"John H. Schwarz","submitted_at":"1995-08-25T23:22:43Z","abstract_excerpt":"An SL(2, Z) family of string solutions of type IIB supergravity in ten dimensions is constructed. The solutions are labeled by a pair of relatively prime integers, which characterize charges of the three-form field strengths. The string tensions depend on these charges in an SL(2, Z) covariant way. Compactifying on a circle and identifying with eleven-dimensional supergravity compactified on a torus implies that the modulus of the IIB theory should be equated to the modular parameter of the torus."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9508143","kind":"arxiv","version":5},"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":"hep-th/9508143","created_at":"2026-05-18T02:36:03.869460+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9508143v5","created_at":"2026-05-18T02:36:03.869460+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9508143","created_at":"2026-05-18T02:36:03.869460+00:00"},{"alias_kind":"pith_short_12","alias_value":"LMAZLVKV4AWT","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"LMAZLVKV4AWTO5BX","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"LMAZLVKV","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2605.15276","citing_title":"Bordisms between 9d type IIB supergravities and commutator widths of duality groups","ref_index":172,"is_internal_anchor":true},{"citing_arxiv_id":"2606.18344","citing_title":"Black p-brane Thermodynamics without Constructing Solutions","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2606.21494","citing_title":"Non-relativistic limits of $\\mathcal N=4$ supersymmetric Yang-Mills theory and S-duality","ref_index":38,"is_internal_anchor":true},{"citing_arxiv_id":"2605.15276","citing_title":"Bordisms between 9d type IIB supergravities and commutator widths of duality groups","ref_index":172,"is_internal_anchor":true},{"citing_arxiv_id":"2603.25590","citing_title":"Wilson loop in AdS$_3 \\times S^3 \\times T^4$ from quantum M2 brane","ref_index":43,"is_internal_anchor":true},{"citing_arxiv_id":"2605.03018","citing_title":"Gravitational electric-magnetic duality at the light ring and quasinormal mode isospectrality in effective field theories","ref_index":72,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI","json":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI.json","graph_json":"https://pith.science/api/pith-number/LMAZLVKV4AWTO5BX4C43WMGQNI/graph.json","events_json":"https://pith.science/api/pith-number/LMAZLVKV4AWTO5BX4C43WMGQNI/events.json","paper":"https://pith.science/paper/LMAZLVKV"},"agent_actions":{"view_html":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI","download_json":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI.json","view_paper":"https://pith.science/paper/LMAZLVKV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9508143&json=true","fetch_graph":"https://pith.science/api/pith-number/LMAZLVKV4AWTO5BX4C43WMGQNI/graph.json","fetch_events":"https://pith.science/api/pith-number/LMAZLVKV4AWTO5BX4C43WMGQNI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI/action/storage_attestation","attest_author":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI/action/author_attestation","sign_citation":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI/action/citation_signature","submit_replication":"https://pith.science/pith/LMAZLVKV4AWTO5BX4C43WMGQNI/action/replication_record"}},"created_at":"2026-05-18T02:36:03.869460+00:00","updated_at":"2026-05-18T02:36:03.869460+00:00"}