{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:66OTION54ULY64Z2MMQWLXDOKO","short_pith_number":"pith:66OTION5","canonical_record":{"source":{"id":"1608.07837","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-08-28T17:53:22Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"737163689e456a61f4ecbce81a32fd5dad9b8ad675e886a66ab95297daa59575","abstract_canon_sha256":"323c5f8498d22856970349481a9c4df996f09b78466b8f619ddebb73a7dabcfe"},"schema_version":"1.0"},"canonical_sha256":"f79d3439bde5178f733a632165dc6e538f74f33e8867f3a9a2d8506626dd34bb","source":{"kind":"arxiv","id":"1608.07837","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.07837","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"arxiv_version","alias_value":"1608.07837v2","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.07837","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"pith_short_12","alias_value":"66OTION54ULY","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"66OTION54ULY64Z2","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"66OTION5","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:66OTION54ULY64Z2MMQWLXDOKO","target":"record","payload":{"canonical_record":{"source":{"id":"1608.07837","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-08-28T17:53:22Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"737163689e456a61f4ecbce81a32fd5dad9b8ad675e886a66ab95297daa59575","abstract_canon_sha256":"323c5f8498d22856970349481a9c4df996f09b78466b8f619ddebb73a7dabcfe"},"schema_version":"1.0"},"canonical_sha256":"f79d3439bde5178f733a632165dc6e538f74f33e8867f3a9a2d8506626dd34bb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:19.954126Z","signature_b64":"9zLvuQdYQ+2tBJ4xEvglIhrlf2hFhEldAecuO89mvPC17paKTzFLe0lUVJZ2a800dxY/FLSYhLuxXx/S0iC0DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f79d3439bde5178f733a632165dc6e538f74f33e8867f3a9a2d8506626dd34bb","last_reissued_at":"2026-05-18T01:07:19.953611Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:19.953611Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.07837","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:07:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/GZPBKYUGhrRJJCUVa014YQVIrX0+rP6HIYpSUxhqOqB7r/DbvUOwUmYLqNAW2XBGWqKVGAJhMVk/U7Qk09iBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T14:44:11.591100Z"},"content_sha256":"efb13dec29760f883a9280b91cbd989153987ec0aeba9c154a1e489786d3ef08","schema_version":"1.0","event_id":"sha256:efb13dec29760f883a9280b91cbd989153987ec0aeba9c154a1e489786d3ef08"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:66OTION54ULY64Z2MMQWLXDOKO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Wedge-local fields in interacting quantum field theories with bound states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Daniela Cadamuro","submitted_at":"2016-08-28T17:53:22Z","abstract_excerpt":"In the context of constructing interacting quantum field theories in the operator-algebraic approach, wedge-local fields play an important role. After the work of Lechner to construct factorizing scattering matrix models with scalar S-matrices without bound states, we recently extended this construction to a class of models with a richer particle spectrum and which are believed to have bound states. These include the Z(N)-Ising model and the affine-Toda field theories. This construction is done by exhibiting wedge-local fields which arise as a deformation of Lechner's fields with the so called"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.07837","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":""},"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":"2026-05-18T01:07:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dzju+LNq2hliFEXmyQV2OdWH89bJ84HBuuU+IXEqo3PNUPXBGTcfoj/kYchTEWSS5yy5B9ebzgLh48tLM1PkBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T14:44:11.591453Z"},"content_sha256":"284b7793296a9352e324a58e13d22082cb70c320ba8b1a7f96e8fab218cbb21b","schema_version":"1.0","event_id":"sha256:284b7793296a9352e324a58e13d22082cb70c320ba8b1a7f96e8fab218cbb21b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/66OTION54ULY64Z2MMQWLXDOKO/bundle.json","state_url":"https://pith.science/pith/66OTION54ULY64Z2MMQWLXDOKO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/66OTION54ULY64Z2MMQWLXDOKO/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":"2026-07-07T14:44:11Z","links":{"resolver":"https://pith.science/pith/66OTION54ULY64Z2MMQWLXDOKO","bundle":"https://pith.science/pith/66OTION54ULY64Z2MMQWLXDOKO/bundle.json","state":"https://pith.science/pith/66OTION54ULY64Z2MMQWLXDOKO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/66OTION54ULY64Z2MMQWLXDOKO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:66OTION54ULY64Z2MMQWLXDOKO","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":"323c5f8498d22856970349481a9c4df996f09b78466b8f619ddebb73a7dabcfe","cross_cats_sorted":["math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-08-28T17:53:22Z","title_canon_sha256":"737163689e456a61f4ecbce81a32fd5dad9b8ad675e886a66ab95297daa59575"},"schema_version":"1.0","source":{"id":"1608.07837","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.07837","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"arxiv_version","alias_value":"1608.07837v2","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.07837","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"pith_short_12","alias_value":"66OTION54ULY","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"66OTION54ULY64Z2","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"66OTION5","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:284b7793296a9352e324a58e13d22082cb70c320ba8b1a7f96e8fab218cbb21b","target":"graph","created_at":"2026-05-18T01:07:19Z","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":"In the context of constructing interacting quantum field theories in the operator-algebraic approach, wedge-local fields play an important role. After the work of Lechner to construct factorizing scattering matrix models with scalar S-matrices without bound states, we recently extended this construction to a class of models with a richer particle spectrum and which are believed to have bound states. These include the Z(N)-Ising model and the affine-Toda field theories. This construction is done by exhibiting wedge-local fields which arise as a deformation of Lechner's fields with the so called","authors_text":"Daniela Cadamuro","cross_cats":["math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-08-28T17:53:22Z","title":"Wedge-local fields in interacting quantum field theories with bound states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.07837","kind":"arxiv","version":2},"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:efb13dec29760f883a9280b91cbd989153987ec0aeba9c154a1e489786d3ef08","target":"record","created_at":"2026-05-18T01:07:19Z","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":"323c5f8498d22856970349481a9c4df996f09b78466b8f619ddebb73a7dabcfe","cross_cats_sorted":["math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-08-28T17:53:22Z","title_canon_sha256":"737163689e456a61f4ecbce81a32fd5dad9b8ad675e886a66ab95297daa59575"},"schema_version":"1.0","source":{"id":"1608.07837","kind":"arxiv","version":2}},"canonical_sha256":"f79d3439bde5178f733a632165dc6e538f74f33e8867f3a9a2d8506626dd34bb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f79d3439bde5178f733a632165dc6e538f74f33e8867f3a9a2d8506626dd34bb","first_computed_at":"2026-05-18T01:07:19.953611Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:07:19.953611Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9zLvuQdYQ+2tBJ4xEvglIhrlf2hFhEldAecuO89mvPC17paKTzFLe0lUVJZ2a800dxY/FLSYhLuxXx/S0iC0DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:07:19.954126Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.07837","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:efb13dec29760f883a9280b91cbd989153987ec0aeba9c154a1e489786d3ef08","sha256:284b7793296a9352e324a58e13d22082cb70c320ba8b1a7f96e8fab218cbb21b"],"state_sha256":"5773aa7cff737784e8cee211c2bcf76aa9713501db4ac54a268139a851f03367"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JAHed2eYZFWLfBgkpFmCp2hdCdQpYbpg4OjVrrYoxkCUAusRCfD/byOYEiumfS3D2CTcicDVh8lnFoN7tkJ/CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-07T14:44:11.593472Z","bundle_sha256":"5fed4c99c9214753c79980b95e7dfb01fce41d183e704364e35a5b6339dd9009"}}