{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:MB7MFA7ZXTF4PEU7WSZKZO7F5Z","short_pith_number":"pith:MB7MFA7Z","schema_version":"1.0","canonical_sha256":"607ec283f9bccbc7929fb4b2acbbe5ee4740465d329b17abcdd7c8c6f65cf22f","source":{"kind":"arxiv","id":"hep-th/9303157","version":2},"attestation_state":"computed","paper":{"title":"Explicit Resolution of an Integrable c(4,3) Open String Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Laurent Houart","submitted_at":"1993-03-29T14:26:51Z","abstract_excerpt":"We study the two-matrix model which represents the sum over closed and open random surfaces coupled to an Ising Model. The boundary conditions are characterized by the fact that the Ising spins sitting at the vertices of the boundaries are all in the same state. We obtain the string equation and discuss the results. (No change in physics, only some misprints are corrected)"},"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/9303157","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-03-29T14:26:51Z","cross_cats_sorted":[],"title_canon_sha256":"2a1ab4847f9ab8469a436ef6aca063236919a33faf2c7511bd39490f5580b128","abstract_canon_sha256":"67384b2d6572280c3166ee18a06fe8878717222e9f8fff51163ca966e8ec119d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:37:43.570405Z","signature_b64":"DD+0t5GrYUxzR+h91E6bxhHaxns3WzHGjXiKBWLcZecuZcBeTrgcH0jmhAUmSK1vM2NpZWwTp/AQWNkNI6OyCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"607ec283f9bccbc7929fb4b2acbbe5ee4740465d329b17abcdd7c8c6f65cf22f","last_reissued_at":"2026-05-18T04:37:43.569819Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:37:43.569819Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Explicit Resolution of an Integrable c(4,3) Open String Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Laurent Houart","submitted_at":"1993-03-29T14:26:51Z","abstract_excerpt":"We study the two-matrix model which represents the sum over closed and open random surfaces coupled to an Ising Model. The boundary conditions are characterized by the fact that the Ising spins sitting at the vertices of the boundaries are all in the same state. We obtain the string equation and discuss the results. (No change in physics, only some misprints are corrected)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9303157","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":"hep-th/9303157","created_at":"2026-05-18T04:37:43.569894+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9303157v2","created_at":"2026-05-18T04:37:43.569894+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9303157","created_at":"2026-05-18T04:37:43.569894+00:00"},{"alias_kind":"pith_short_12","alias_value":"MB7MFA7ZXTF4","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"MB7MFA7ZXTF4PEU7","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"MB7MFA7Z","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z","json":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z.json","graph_json":"https://pith.science/api/pith-number/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/graph.json","events_json":"https://pith.science/api/pith-number/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/events.json","paper":"https://pith.science/paper/MB7MFA7Z"},"agent_actions":{"view_html":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z","download_json":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z.json","view_paper":"https://pith.science/paper/MB7MFA7Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9303157&json=true","fetch_graph":"https://pith.science/api/pith-number/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/graph.json","fetch_events":"https://pith.science/api/pith-number/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/action/storage_attestation","attest_author":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/action/author_attestation","sign_citation":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/action/citation_signature","submit_replication":"https://pith.science/pith/MB7MFA7ZXTF4PEU7WSZKZO7F5Z/action/replication_record"}},"created_at":"2026-05-18T04:37:43.569894+00:00","updated_at":"2026-05-18T04:37:43.569894+00:00"}