{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:B4ZVTJUGODHQP5QYO5N7SQTZVT","short_pith_number":"pith:B4ZVTJUG","canonical_record":{"source":{"id":"hep-th/9607099","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-07-12T14:56:55Z","cross_cats_sorted":["cond-mat","math.QA","nlin.SI","q-alg","solv-int"],"title_canon_sha256":"b0238bfd5e010251c6bcc38d4638ee12e8b84fdc9f178ea2138c80e2fbd13a92","abstract_canon_sha256":"a356668a4a5ab8325247eb12b54640b8e2c3daab19d65d98c8d04c9c61526b06"},"schema_version":"1.0"},"canonical_sha256":"0f3359a68670cf07f618775bf94279acd07e678b0aaaffae78bfbd40fe6517d0","source":{"kind":"arxiv","id":"hep-th/9607099","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9607099","created_at":"2026-05-18T04:28:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9607099v1","created_at":"2026-05-18T04:28:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9607099","created_at":"2026-05-18T04:28:56Z"},{"alias_kind":"pith_short_12","alias_value":"B4ZVTJUGODHQ","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"B4ZVTJUGODHQP5QY","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"B4ZVTJUG","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:B4ZVTJUGODHQP5QYO5N7SQTZVT","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9607099","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-07-12T14:56:55Z","cross_cats_sorted":["cond-mat","math.QA","nlin.SI","q-alg","solv-int"],"title_canon_sha256":"b0238bfd5e010251c6bcc38d4638ee12e8b84fdc9f178ea2138c80e2fbd13a92","abstract_canon_sha256":"a356668a4a5ab8325247eb12b54640b8e2c3daab19d65d98c8d04c9c61526b06"},"schema_version":"1.0"},"canonical_sha256":"0f3359a68670cf07f618775bf94279acd07e678b0aaaffae78bfbd40fe6517d0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:56.958539Z","signature_b64":"omkkWtylTaBG85jPHo8q/B5jqSaJxM2uetCC5JYejuQS1zAl+zIC4PEyNJ8fk2RqtO/CBtBLfzT/0W3VJGJQBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0f3359a68670cf07f618775bf94279acd07e678b0aaaffae78bfbd40fe6517d0","last_reissued_at":"2026-05-18T04:28:56.958121Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:56.958121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9607099","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:28:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Zp5FLrb1DSmVh6cSpSR377q59rPfutfeV0/kWvnUXw4TS61dgfVTiF99cvAUkttEtJbJz5X2ito1HsBEQrWyBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T22:29:25.600042Z"},"content_sha256":"98f52a5adfb170af395535b816a04d9a3d91185cf988bb6a1bd1cea92338037f","schema_version":"1.0","event_id":"sha256:98f52a5adfb170af395535b816a04d9a3d91185cf988bb6a1bd1cea92338037f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:B4ZVTJUGODHQP5QYO5N7SQTZVT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Integrable Quantum Field Theories in Finite Volume: Excited State Energies","license":"","headline":"","cross_cats":["cond-mat","math.QA","nlin.SI","q-alg","solv-int"],"primary_cat":"hep-th","authors_text":"A.B.Zamolodchikov, S.L.Lukyanov, V.V.Bazhanov","submitted_at":"1996-07-12T14:56:55Z","abstract_excerpt":"We develop a method of computing the excited state energies in Integrable Quantum Field Theories (IQFT) in finite geometry, with spatial coordinate compactified on a circle of circumference R. The IQFT ``commuting transfer-matrices'' introduced by us (BLZ) for Conformal Field Theories (CFT) are generalized to non-conformal IQFT obtained by perturbing CFT with the operator $\\Phi_{1,3}$. We study the models in which the fusion relations for these ``transfer-matrices'' truncate and provide closed integral equations which generalize the equations of Thermodynamic Bethe Ansatz to excited states. Th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9607099","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:28:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/dUH77wGEH2h+tRX1WDL+eDRmJRVSvHSjRSrXmXfH6PVIu6iHXZu1U2WuymeZoPRHM8S3+uBs8khbPq+w6ITBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T22:29:25.600411Z"},"content_sha256":"500d15a3fbe5b8e08e11a71ccdf5c97c7d5bfd52099f056095312a220e808c2a","schema_version":"1.0","event_id":"sha256:500d15a3fbe5b8e08e11a71ccdf5c97c7d5bfd52099f056095312a220e808c2a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/B4ZVTJUGODHQP5QYO5N7SQTZVT/bundle.json","state_url":"https://pith.science/pith/B4ZVTJUGODHQP5QYO5N7SQTZVT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/B4ZVTJUGODHQP5QYO5N7SQTZVT/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-21T22:29:25Z","links":{"resolver":"https://pith.science/pith/B4ZVTJUGODHQP5QYO5N7SQTZVT","bundle":"https://pith.science/pith/B4ZVTJUGODHQP5QYO5N7SQTZVT/bundle.json","state":"https://pith.science/pith/B4ZVTJUGODHQP5QYO5N7SQTZVT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/B4ZVTJUGODHQP5QYO5N7SQTZVT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:B4ZVTJUGODHQP5QYO5N7SQTZVT","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"a356668a4a5ab8325247eb12b54640b8e2c3daab19d65d98c8d04c9c61526b06","cross_cats_sorted":["cond-mat","math.QA","nlin.SI","q-alg","solv-int"],"license":"","primary_cat":"hep-th","submitted_at":"1996-07-12T14:56:55Z","title_canon_sha256":"b0238bfd5e010251c6bcc38d4638ee12e8b84fdc9f178ea2138c80e2fbd13a92"},"schema_version":"1.0","source":{"id":"hep-th/9607099","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9607099","created_at":"2026-05-18T04:28:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9607099v1","created_at":"2026-05-18T04:28:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9607099","created_at":"2026-05-18T04:28:56Z"},{"alias_kind":"pith_short_12","alias_value":"B4ZVTJUGODHQ","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"B4ZVTJUGODHQP5QY","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"B4ZVTJUG","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:500d15a3fbe5b8e08e11a71ccdf5c97c7d5bfd52099f056095312a220e808c2a","target":"graph","created_at":"2026-05-18T04:28:56Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We develop a method of computing the excited state energies in Integrable Quantum Field Theories (IQFT) in finite geometry, with spatial coordinate compactified on a circle of circumference R. The IQFT ``commuting transfer-matrices'' introduced by us (BLZ) for Conformal Field Theories (CFT) are generalized to non-conformal IQFT obtained by perturbing CFT with the operator $\\Phi_{1,3}$. We study the models in which the fusion relations for these ``transfer-matrices'' truncate and provide closed integral equations which generalize the equations of Thermodynamic Bethe Ansatz to excited states. Th","authors_text":"A.B.Zamolodchikov, S.L.Lukyanov, V.V.Bazhanov","cross_cats":["cond-mat","math.QA","nlin.SI","q-alg","solv-int"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1996-07-12T14:56:55Z","title":"Integrable Quantum Field Theories in Finite Volume: Excited State Energies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9607099","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:98f52a5adfb170af395535b816a04d9a3d91185cf988bb6a1bd1cea92338037f","target":"record","created_at":"2026-05-18T04:28:56Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"a356668a4a5ab8325247eb12b54640b8e2c3daab19d65d98c8d04c9c61526b06","cross_cats_sorted":["cond-mat","math.QA","nlin.SI","q-alg","solv-int"],"license":"","primary_cat":"hep-th","submitted_at":"1996-07-12T14:56:55Z","title_canon_sha256":"b0238bfd5e010251c6bcc38d4638ee12e8b84fdc9f178ea2138c80e2fbd13a92"},"schema_version":"1.0","source":{"id":"hep-th/9607099","kind":"arxiv","version":1}},"canonical_sha256":"0f3359a68670cf07f618775bf94279acd07e678b0aaaffae78bfbd40fe6517d0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0f3359a68670cf07f618775bf94279acd07e678b0aaaffae78bfbd40fe6517d0","first_computed_at":"2026-05-18T04:28:56.958121Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:28:56.958121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"omkkWtylTaBG85jPHo8q/B5jqSaJxM2uetCC5JYejuQS1zAl+zIC4PEyNJ8fk2RqtO/CBtBLfzT/0W3VJGJQBA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:28:56.958539Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9607099","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:98f52a5adfb170af395535b816a04d9a3d91185cf988bb6a1bd1cea92338037f","sha256:500d15a3fbe5b8e08e11a71ccdf5c97c7d5bfd52099f056095312a220e808c2a"],"state_sha256":"78fd644c7a9ec4ae87156eaaabbe4319d1ea16ffbcba5a0781e375ec2846e176"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DlpPOUL76c5zJ20OrvY1wWn2Q2OTK73jJ8lZbvlM8ppouiSIpK0xkqK10tB/cWxboqGrdR7QrHlvLKpsKqgpDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T22:29:25.602575Z","bundle_sha256":"826612dc9218c38f540aa81201dd6b3c609859232571c50138d846a888f62bf2"}}