{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:ITLC4OPBPBVVIEW5LMBM4YJYNI","short_pith_number":"pith:ITLC4OPB","schema_version":"1.0","canonical_sha256":"44d62e39e1786b5412dd5b02ce61386a12758ba78127699836036259400e8b86","source":{"kind":"arxiv","id":"hep-th/0211094","version":3},"attestation_state":"computed","paper":{"title":"Exact conserved quantities on the cylinder I: conformal case","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Davide Fioravanti (Un. of Durham), Marco Rossi (Heriot-Watt Un.)","submitted_at":"2002-11-11T20:23:43Z","abstract_excerpt":"The nonlinear integral equations describing the spectra of the left and right (continuous) quantum KdV equations on the cylinder are derived from integrable lattice field theories, which turn out to allow the Bethe Ansatz equations of a twisted ``spin -1/2'' chain. A very useful mapping to the more common nonlinear integral equation of the twisted continuous spin $+1/2$ chain is found. The diagonalization of the transfer matrix is performed. The vacua sector is analysed in detail detecting the primary states of the minimal conformal models and giving integral expressions for the eigenvalues of"},"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/0211094","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-11-11T20:23:43Z","cross_cats_sorted":[],"title_canon_sha256":"f34f93169c888526d82f61951ecdbb132a044cd2c0ef5fde699d654e36af538e","abstract_canon_sha256":"db1dbf25e5d9bb7863a849f17f47742f3dc4b075778b724d739cd8cafc477eba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:57.663270Z","signature_b64":"+E3E9LCRINKyajRqRR2ZZV2KCuJAtIKPhguJijqReQmK/Uvhl7OZbT0ajSxSd+qHpNbv5Bg9XpkXqSuGoaIfDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"44d62e39e1786b5412dd5b02ce61386a12758ba78127699836036259400e8b86","last_reissued_at":"2026-07-04T16:34:57.662846Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:57.662846Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exact conserved quantities on the cylinder I: conformal case","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Davide Fioravanti (Un. of Durham), Marco Rossi (Heriot-Watt Un.)","submitted_at":"2002-11-11T20:23:43Z","abstract_excerpt":"The nonlinear integral equations describing the spectra of the left and right (continuous) quantum KdV equations on the cylinder are derived from integrable lattice field theories, which turn out to allow the Bethe Ansatz equations of a twisted ``spin -1/2'' chain. A very useful mapping to the more common nonlinear integral equation of the twisted continuous spin $+1/2$ chain is found. The diagonalization of the transfer matrix is performed. The vacua sector is analysed in detail detecting the primary states of the minimal conformal models and giving integral expressions for the eigenvalues of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0211094","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/hep-th/0211094/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/0211094","created_at":"2026-07-04T16:34:57.662913+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0211094v3","created_at":"2026-07-04T16:34:57.662913+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0211094","created_at":"2026-07-04T16:34:57.662913+00:00"},{"alias_kind":"pith_short_12","alias_value":"ITLC4OPBPBVV","created_at":"2026-07-04T16:34:57.662913+00:00"},{"alias_kind":"pith_short_16","alias_value":"ITLC4OPBPBVVIEW5","created_at":"2026-07-04T16:34:57.662913+00:00"},{"alias_kind":"pith_short_8","alias_value":"ITLC4OPB","created_at":"2026-07-04T16:34:57.662913+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.18695","citing_title":"From classical Lax ODEs to quantum integrable theories: the moduli","ref_index":14,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI","json":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI.json","graph_json":"https://pith.science/api/pith-number/ITLC4OPBPBVVIEW5LMBM4YJYNI/graph.json","events_json":"https://pith.science/api/pith-number/ITLC4OPBPBVVIEW5LMBM4YJYNI/events.json","paper":"https://pith.science/paper/ITLC4OPB"},"agent_actions":{"view_html":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI","download_json":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI.json","view_paper":"https://pith.science/paper/ITLC4OPB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0211094&json=true","fetch_graph":"https://pith.science/api/pith-number/ITLC4OPBPBVVIEW5LMBM4YJYNI/graph.json","fetch_events":"https://pith.science/api/pith-number/ITLC4OPBPBVVIEW5LMBM4YJYNI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI/action/storage_attestation","attest_author":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI/action/author_attestation","sign_citation":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI/action/citation_signature","submit_replication":"https://pith.science/pith/ITLC4OPBPBVVIEW5LMBM4YJYNI/action/replication_record"}},"created_at":"2026-07-04T16:34:57.662913+00:00","updated_at":"2026-07-04T16:34:57.662913+00:00"}