{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:BJQRTGRRDMJ4ODEVYKCK3TP74A","short_pith_number":"pith:BJQRTGRR","schema_version":"1.0","canonical_sha256":"0a61199a311b13c70c95c284adcdffe0216e064a1a8cbc8905eb4ccfd34ca0e4","source":{"kind":"arxiv","id":"hep-th/9410117","version":1},"attestation_state":"computed","paper":{"title":"Correlation Functions Along a Massless Flow","license":"","headline":"","cross_cats":["cond-mat"],"primary_cat":"hep-th","authors_text":"G. Delfino, G. Mussardo, P. Simonetti","submitted_at":"1994-10-17T17:08:20Z","abstract_excerpt":"A non-perturbative method based on the Form Factor bootstrap approach is proposed for the analysis of correlation functions of 2-D massless integrable theories and applied to the massless flow between the Tricritical and the Critical Ising Models."},"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/9410117","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-10-17T17:08:20Z","cross_cats_sorted":["cond-mat"],"title_canon_sha256":"ebcdd27b15634db66256af3062b228a4a155a826ba519ad74b2bd2284e940097","abstract_canon_sha256":"c0eedfae0c0cbeeac0d3e983830f0d46381d25bd02f7069a91730951e78eafec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:18:28.686579Z","signature_b64":"Y6coS7Nrcf1d5qH1QtieiwwtIFGP0ZBhmItTNxLUYyBBYcZB3If7b2+ZAyehjn2nZ1Za2oMcXhZi73tQiudGBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0a61199a311b13c70c95c284adcdffe0216e064a1a8cbc8905eb4ccfd34ca0e4","last_reissued_at":"2026-07-04T17:18:28.686126Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:18:28.686126Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Correlation Functions Along a Massless Flow","license":"","headline":"","cross_cats":["cond-mat"],"primary_cat":"hep-th","authors_text":"G. Delfino, G. Mussardo, P. Simonetti","submitted_at":"1994-10-17T17:08:20Z","abstract_excerpt":"A non-perturbative method based on the Form Factor bootstrap approach is proposed for the analysis of correlation functions of 2-D massless integrable theories and applied to the massless flow between the Tricritical and the Critical Ising Models."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9410117","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/9410117/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/9410117","created_at":"2026-07-04T17:18:28.686193+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9410117v1","created_at":"2026-07-04T17:18:28.686193+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9410117","created_at":"2026-07-04T17:18:28.686193+00:00"},{"alias_kind":"pith_short_12","alias_value":"BJQRTGRRDMJ4","created_at":"2026-07-04T17:18:28.686193+00:00"},{"alias_kind":"pith_short_16","alias_value":"BJQRTGRRDMJ4ODEV","created_at":"2026-07-04T17:18:28.686193+00:00"},{"alias_kind":"pith_short_8","alias_value":"BJQRTGRR","created_at":"2026-07-04T17:18:28.686193+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/BJQRTGRRDMJ4ODEVYKCK3TP74A","json":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A.json","graph_json":"https://pith.science/api/pith-number/BJQRTGRRDMJ4ODEVYKCK3TP74A/graph.json","events_json":"https://pith.science/api/pith-number/BJQRTGRRDMJ4ODEVYKCK3TP74A/events.json","paper":"https://pith.science/paper/BJQRTGRR"},"agent_actions":{"view_html":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A","download_json":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A.json","view_paper":"https://pith.science/paper/BJQRTGRR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9410117&json=true","fetch_graph":"https://pith.science/api/pith-number/BJQRTGRRDMJ4ODEVYKCK3TP74A/graph.json","fetch_events":"https://pith.science/api/pith-number/BJQRTGRRDMJ4ODEVYKCK3TP74A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A/action/storage_attestation","attest_author":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A/action/author_attestation","sign_citation":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A/action/citation_signature","submit_replication":"https://pith.science/pith/BJQRTGRRDMJ4ODEVYKCK3TP74A/action/replication_record"}},"created_at":"2026-07-04T17:18:28.686193+00:00","updated_at":"2026-07-04T17:18:28.686193+00:00"}