{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:PGLYARLIBJHPVR75F42VP4CID7","short_pith_number":"pith:PGLYARLI","canonical_record":{"source":{"id":"hep-th/9404173","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-04-28T16:07:44Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3deb59fa5220dba92dc325a7df317fa224fa88609815f517948960b14d72995f","abstract_canon_sha256":"ab7bc87d7cf76838e2a7dff82fea0c7123be8167db3a47ba87a533b5e37e9318"},"schema_version":"1.0"},"canonical_sha256":"79978045680a4efac7fd2f3557f0481fd9cc2ef7ef629af80ae7c09ae3686625","source":{"kind":"arxiv","id":"hep-th/9404173","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9404173","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9404173v1","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9404173","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"pith_short_12","alias_value":"PGLYARLIBJHP","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"pith_short_16","alias_value":"PGLYARLIBJHPVR75","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"pith_short_8","alias_value":"PGLYARLI","created_at":"2026-07-04T15:57:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:PGLYARLIBJHPVR75F42VP4CID7","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9404173","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-04-28T16:07:44Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3deb59fa5220dba92dc325a7df317fa224fa88609815f517948960b14d72995f","abstract_canon_sha256":"ab7bc87d7cf76838e2a7dff82fea0c7123be8167db3a47ba87a533b5e37e9318"},"schema_version":"1.0"},"canonical_sha256":"79978045680a4efac7fd2f3557f0481fd9cc2ef7ef629af80ae7c09ae3686625","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:57:44.390975Z","signature_b64":"XkXEU6ZcBDN3KRfGtgxHMXrhnwpkFY6ljIRgwuXwZqQUj5e7YLbp7A0JtK6+yPw29Fi1DT7XA+yktj4M7iVHAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"79978045680a4efac7fd2f3557f0481fd9cc2ef7ef629af80ae7c09ae3686625","last_reissued_at":"2026-07-04T15:57:44.390635Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:57:44.390635Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9404173","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":"2026-07-04T15:57:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KuI0wdlrilrlw37tHZcsDd1mdggs9C5FS/ULmY4Me15C1HACfByvy3HNHh+XnLj8jZimL5W3WVXOYbb0ZNQjAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T14:08:48.261646Z"},"content_sha256":"40a4edfe59d4c2e88e7056a871a0437f0f8b9010848a38534bf9ec24ace5c453","schema_version":"1.0","event_id":"sha256:40a4edfe59d4c2e88e7056a871a0437f0f8b9010848a38534bf9ec24ace5c453"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:PGLYARLIBJHPVR75F42VP4CID7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High energy QCD as a completely integrable model","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"G.P.Korchemsky, L.D.Faddeev","submitted_at":"1994-04-28T16:07:44Z","abstract_excerpt":"We show that the one-dimensional lattice model proposed by Lipatov to describe the high energy scattering of hadrons in multicolor QCD is completely integrable. We identify this model as the XXX Heisenberg chain of noncompact spin $s=0$ and find the conservation laws of the model. A generalized Bethe ansatz is developed for the diagonalization of the hamiltonian and for the calculation of hadron-hadron scattering amplitude."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9404173","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/9404173/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:57:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pkegCrwF7ype24BNp0ckmd/qWYVmTXiFJn9H2wIKHRfJq9mrVWvkOvaUdWlV4m0he7XnNgNl1EE8SIqSOfg/Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T14:08:48.262237Z"},"content_sha256":"99e40404e6ccd3170ce9d1049e7ab8d5b878368703228102fbc5adfcd0ad4d89","schema_version":"1.0","event_id":"sha256:99e40404e6ccd3170ce9d1049e7ab8d5b878368703228102fbc5adfcd0ad4d89"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PGLYARLIBJHPVR75F42VP4CID7/bundle.json","state_url":"https://pith.science/pith/PGLYARLIBJHPVR75F42VP4CID7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PGLYARLIBJHPVR75F42VP4CID7/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":"2026-08-03T14:08:48Z","links":{"resolver":"https://pith.science/pith/PGLYARLIBJHPVR75F42VP4CID7","bundle":"https://pith.science/pith/PGLYARLIBJHPVR75F42VP4CID7/bundle.json","state":"https://pith.science/pith/PGLYARLIBJHPVR75F42VP4CID7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PGLYARLIBJHPVR75F42VP4CID7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:PGLYARLIBJHPVR75F42VP4CID7","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":"ab7bc87d7cf76838e2a7dff82fea0c7123be8167db3a47ba87a533b5e37e9318","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"1994-04-28T16:07:44Z","title_canon_sha256":"3deb59fa5220dba92dc325a7df317fa224fa88609815f517948960b14d72995f"},"schema_version":"1.0","source":{"id":"hep-th/9404173","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9404173","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9404173v1","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9404173","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"pith_short_12","alias_value":"PGLYARLIBJHP","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"pith_short_16","alias_value":"PGLYARLIBJHPVR75","created_at":"2026-07-04T15:57:44Z"},{"alias_kind":"pith_short_8","alias_value":"PGLYARLI","created_at":"2026-07-04T15:57:44Z"}],"graph_snapshots":[{"event_id":"sha256:99e40404e6ccd3170ce9d1049e7ab8d5b878368703228102fbc5adfcd0ad4d89","target":"graph","created_at":"2026-07-04T15:57:44Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/9404173/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We show that the one-dimensional lattice model proposed by Lipatov to describe the high energy scattering of hadrons in multicolor QCD is completely integrable. We identify this model as the XXX Heisenberg chain of noncompact spin $s=0$ and find the conservation laws of the model. A generalized Bethe ansatz is developed for the diagonalization of the hamiltonian and for the calculation of hadron-hadron scattering amplitude.","authors_text":"G.P.Korchemsky, L.D.Faddeev","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1994-04-28T16:07:44Z","title":"High energy QCD as a completely integrable model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9404173","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":"sha256:40a4edfe59d4c2e88e7056a871a0437f0f8b9010848a38534bf9ec24ace5c453","target":"record","created_at":"2026-07-04T15:57:44Z","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":"ab7bc87d7cf76838e2a7dff82fea0c7123be8167db3a47ba87a533b5e37e9318","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"1994-04-28T16:07:44Z","title_canon_sha256":"3deb59fa5220dba92dc325a7df317fa224fa88609815f517948960b14d72995f"},"schema_version":"1.0","source":{"id":"hep-th/9404173","kind":"arxiv","version":1}},"canonical_sha256":"79978045680a4efac7fd2f3557f0481fd9cc2ef7ef629af80ae7c09ae3686625","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"79978045680a4efac7fd2f3557f0481fd9cc2ef7ef629af80ae7c09ae3686625","first_computed_at":"2026-07-04T15:57:44.390635Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:57:44.390635Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XkXEU6ZcBDN3KRfGtgxHMXrhnwpkFY6ljIRgwuXwZqQUj5e7YLbp7A0JtK6+yPw29Fi1DT7XA+yktj4M7iVHAw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:57:44.390975Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9404173","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:40a4edfe59d4c2e88e7056a871a0437f0f8b9010848a38534bf9ec24ace5c453","sha256:99e40404e6ccd3170ce9d1049e7ab8d5b878368703228102fbc5adfcd0ad4d89"],"state_sha256":"6635e1404849ebbe694491445bcd9bede84b277044825890d3643fa3f05d1401"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2RwSg+A4nfQpYXlL99P7LhUwI2OJUNSgKpex3dcoJACpkPulw3G2wzwGkyLPtC+aUL951n5AVNcZQ2xuwE/lBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T14:08:48.266164Z","bundle_sha256":"f357ce26f1e95ada92d938ba10070d5f107b0e63e487f7dea3df8bb664f0c60d"}}