{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:FGVLNNLJIVCZQI3GC3A2IYZRHR","short_pith_number":"pith:FGVLNNLJ","schema_version":"1.0","canonical_sha256":"29aab6b569454598236616c1a463313c7e07916dd14a1144767ba8888a239877","source":{"kind":"arxiv","id":"2312.12266","version":3},"attestation_state":"computed","paper":{"title":"A String Theory for Two Dimensional Yang-Mills Theory I","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ofer Aharony, Suman Kundu, Tal Sheaffer","submitted_at":"2023-12-19T15:49:55Z","abstract_excerpt":"Two dimensional gauge theories with charged matter fields are useful toy models for studying gauge theory dynamics, and in particular for studying the duality of large $N$ gauge theories to perturbative string theories. A useful starting point for such studies is the pure Yang-Mills theory, which is exactly solvable. Its $1/N$ expansion was interpreted as a string theory by Gross and Taylor 30 years ago, but they did not provide a worldsheet action for this string theory, and such an action is useful for coupling it to matter fields. The chiral sector of the Yang-Mills theory can be written as"},"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":"2312.12266","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-12-19T15:49:55Z","cross_cats_sorted":[],"title_canon_sha256":"3d1d95c16d52ea4e031114276865d111287381ac1e7048aa8cd3e7b2e224f17f","abstract_canon_sha256":"3d7c67c8bade7f6b5d7311d1cbd3b172cb89719b71317f233dcb40cb0b736dba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:42:00.853465Z","signature_b64":"2DjM+96KtY2JvvRjQZISuOb5MkLp1xSzx0JxN24n4zeWJvfyA3BLGNgHurH88+MIxt66qzGIlSGJlEfzCNNNCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29aab6b569454598236616c1a463313c7e07916dd14a1144767ba8888a239877","last_reissued_at":"2026-07-05T08:42:00.853110Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:42:00.853110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A String Theory for Two Dimensional Yang-Mills Theory I","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ofer Aharony, Suman Kundu, Tal Sheaffer","submitted_at":"2023-12-19T15:49:55Z","abstract_excerpt":"Two dimensional gauge theories with charged matter fields are useful toy models for studying gauge theory dynamics, and in particular for studying the duality of large $N$ gauge theories to perturbative string theories. A useful starting point for such studies is the pure Yang-Mills theory, which is exactly solvable. Its $1/N$ expansion was interpreted as a string theory by Gross and Taylor 30 years ago, but they did not provide a worldsheet action for this string theory, and such an action is useful for coupling it to matter fields. The chiral sector of the Yang-Mills theory can be written as"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.12266","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/2312.12266/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":"2312.12266","created_at":"2026-07-05T08:42:00.853163+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.12266v3","created_at":"2026-07-05T08:42:00.853163+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.12266","created_at":"2026-07-05T08:42:00.853163+00:00"},{"alias_kind":"pith_short_12","alias_value":"FGVLNNLJIVCZ","created_at":"2026-07-05T08:42:00.853163+00:00"},{"alias_kind":"pith_short_16","alias_value":"FGVLNNLJIVCZQI3G","created_at":"2026-07-05T08:42:00.853163+00:00"},{"alias_kind":"pith_short_8","alias_value":"FGVLNNLJ","created_at":"2026-07-05T08:42:00.853163+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.02662","citing_title":"The String Dual to Two-dimensional Yang-Mills Theory Revisited","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR","json":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR.json","graph_json":"https://pith.science/api/pith-number/FGVLNNLJIVCZQI3GC3A2IYZRHR/graph.json","events_json":"https://pith.science/api/pith-number/FGVLNNLJIVCZQI3GC3A2IYZRHR/events.json","paper":"https://pith.science/paper/FGVLNNLJ"},"agent_actions":{"view_html":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR","download_json":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR.json","view_paper":"https://pith.science/paper/FGVLNNLJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.12266&json=true","fetch_graph":"https://pith.science/api/pith-number/FGVLNNLJIVCZQI3GC3A2IYZRHR/graph.json","fetch_events":"https://pith.science/api/pith-number/FGVLNNLJIVCZQI3GC3A2IYZRHR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR/action/storage_attestation","attest_author":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR/action/author_attestation","sign_citation":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR/action/citation_signature","submit_replication":"https://pith.science/pith/FGVLNNLJIVCZQI3GC3A2IYZRHR/action/replication_record"}},"created_at":"2026-07-05T08:42:00.853163+00:00","updated_at":"2026-07-05T08:42:00.853163+00:00"}