{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:XSACWXOYHIAPBZPYTKYYC22SKA","short_pith_number":"pith:XSACWXOY","schema_version":"1.0","canonical_sha256":"bc802b5dd83a00f0e5f89ab1816b525033c8a93a6c65d9cb5894119266058559","source":{"kind":"arxiv","id":"hep-th/0504229","version":2},"attestation_state":"computed","paper":{"title":"From Free Fields to $AdS$ -- III","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Rajesh Gopakumar (Harish-Chandra Research Institute)","submitted_at":"2005-04-28T09:43:44Z","abstract_excerpt":"In previous work we have shown that large $N$ field theory amplitudes, in Schwinger parametrised form, can be organised into integrals over the stringy moduli space ${\\cal M}_{g,n}\\times R_{+}^n$. Here we flesh this out into a concrete implementation of open-closed string duality. In particular, we propose that the closed string worldsheet is reconstructed from the unique Strebel quadratic differential that can be associated to (the dual of) a field theory skeleton graph. We are led, in the process, to identify the inverse Schwinger proper times ($\\s_i={1\\over \\t_i}$) with the lengths of edges"},"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/0504229","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-04-28T09:43:44Z","cross_cats_sorted":[],"title_canon_sha256":"d4eed785db1d9ef67f7adae5aa9151796e0ccd97750b0b5343158222c496a0d0","abstract_canon_sha256":"a8e734dc19c42aa9d2923563f89c9d42d725e9fe8c3e3f36a38bd3cfdfd11d69"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:56:10.094973Z","signature_b64":"+kG+r2kDSAii7oKjxc1FkRdFqV9+AZVziDtF3dzmV083nhvMdpeTS49aduZgivr6uxvcsNY5vcx1QWe5m/SpCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc802b5dd83a00f0e5f89ab1816b525033c8a93a6c65d9cb5894119266058559","last_reissued_at":"2026-07-04T16:56:10.094531Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:56:10.094531Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From Free Fields to $AdS$ -- III","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Rajesh Gopakumar (Harish-Chandra Research Institute)","submitted_at":"2005-04-28T09:43:44Z","abstract_excerpt":"In previous work we have shown that large $N$ field theory amplitudes, in Schwinger parametrised form, can be organised into integrals over the stringy moduli space ${\\cal M}_{g,n}\\times R_{+}^n$. Here we flesh this out into a concrete implementation of open-closed string duality. In particular, we propose that the closed string worldsheet is reconstructed from the unique Strebel quadratic differential that can be associated to (the dual of) a field theory skeleton graph. We are led, in the process, to identify the inverse Schwinger proper times ($\\s_i={1\\over \\t_i}$) with the lengths of edges"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0504229","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/0504229/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/0504229","created_at":"2026-07-04T16:56:10.094624+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0504229v2","created_at":"2026-07-04T16:56:10.094624+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0504229","created_at":"2026-07-04T16:56:10.094624+00:00"},{"alias_kind":"pith_short_12","alias_value":"XSACWXOYHIAP","created_at":"2026-07-04T16:56:10.094624+00:00"},{"alias_kind":"pith_short_16","alias_value":"XSACWXOYHIAPBZPY","created_at":"2026-07-04T16:56:10.094624+00:00"},{"alias_kind":"pith_short_8","alias_value":"XSACWXOY","created_at":"2026-07-04T16:56:10.094624+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.02885","citing_title":"Open-Closed-Open Triality Beyond Matrix Models","ref_index":39,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA","json":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA.json","graph_json":"https://pith.science/api/pith-number/XSACWXOYHIAPBZPYTKYYC22SKA/graph.json","events_json":"https://pith.science/api/pith-number/XSACWXOYHIAPBZPYTKYYC22SKA/events.json","paper":"https://pith.science/paper/XSACWXOY"},"agent_actions":{"view_html":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA","download_json":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA.json","view_paper":"https://pith.science/paper/XSACWXOY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0504229&json=true","fetch_graph":"https://pith.science/api/pith-number/XSACWXOYHIAPBZPYTKYYC22SKA/graph.json","fetch_events":"https://pith.science/api/pith-number/XSACWXOYHIAPBZPYTKYYC22SKA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA/action/storage_attestation","attest_author":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA/action/author_attestation","sign_citation":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA/action/citation_signature","submit_replication":"https://pith.science/pith/XSACWXOYHIAPBZPYTKYYC22SKA/action/replication_record"}},"created_at":"2026-07-04T16:56:10.094624+00:00","updated_at":"2026-07-04T16:56:10.094624+00:00"}