{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:COQYFUFV2GYBMDTTFJC5WGYMYV","short_pith_number":"pith:COQYFUFV","canonical_record":{"source":{"id":"1410.5991","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-22T10:58:48Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"5b686dcd5b38b4dd310fa632b3bfa6d888a2f907f0e17a8ab7f6a38e6cd559ab","abstract_canon_sha256":"0e725cb11f58ed0ab53420b94975384a8eccf728f149148e5f69f3ccffb07d09"},"schema_version":"1.0"},"canonical_sha256":"13a182d0b5d1b0160e732a45db1b0cc54c1d32c1450cc8ed76d554625d5a727b","source":{"kind":"arxiv","id":"1410.5991","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.5991","created_at":"2026-05-18T02:28:05Z"},{"alias_kind":"arxiv_version","alias_value":"1410.5991v2","created_at":"2026-05-18T02:28:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.5991","created_at":"2026-05-18T02:28:05Z"},{"alias_kind":"pith_short_12","alias_value":"COQYFUFV2GYB","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"COQYFUFV2GYBMDTT","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"COQYFUFV","created_at":"2026-05-18T12:28:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:COQYFUFV2GYBMDTTFJC5WGYMYV","target":"record","payload":{"canonical_record":{"source":{"id":"1410.5991","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-22T10:58:48Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"5b686dcd5b38b4dd310fa632b3bfa6d888a2f907f0e17a8ab7f6a38e6cd559ab","abstract_canon_sha256":"0e725cb11f58ed0ab53420b94975384a8eccf728f149148e5f69f3ccffb07d09"},"schema_version":"1.0"},"canonical_sha256":"13a182d0b5d1b0160e732a45db1b0cc54c1d32c1450cc8ed76d554625d5a727b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:28:05.065033Z","signature_b64":"Ws0oR0zp6lcbUiCP6ylHKokUC1jXvXk2hRzGbUQGYYTJ8JfK6qalNMHTHWy6rSdd635dkQT0N4WtJYLbNCA8AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"13a182d0b5d1b0160e732a45db1b0cc54c1d32c1450cc8ed76d554625d5a727b","last_reissued_at":"2026-05-18T02:28:05.064615Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:28:05.064615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1410.5991","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":"2026-05-18T02:28:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"y3R5NZIWMRWyTI1zB9Co2Q2CYw8CDv8bLiSpAFjWywfhwBwMm8wP2L9OCOdFO93+9i4VzQIVexm356XXFJhADg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T00:34:06.514094Z"},"content_sha256":"bc4ba207b5282957a61c83627b328eb4581d096ed72a39db28089601b47ef24c","schema_version":"1.0","event_id":"sha256:bc4ba207b5282957a61c83627b328eb4581d096ed72a39db28089601b47ef24c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:COQYFUFV2GYBMDTTFJC5WGYMYV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scattering matrices in the sl(3) twisted Yangian","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","nlin.SI"],"primary_cat":"hep-th","authors_text":"Anastasia Doikou, Jean Avan, Nikos Karaiskos","submitted_at":"2014-10-22T10:58:48Z","abstract_excerpt":"A quantum spin chain with non-conventional boundary conditions is studied. The distinct nature of these boundary conditions arises from the conversion of a soliton to an anti-soliton after being reflected to the boundary, hence the appellation soliton non-preserving boundary conditions. We focus on the simplest non-trivial case of this class of models based on the twisted Yangian quadratic algebra. Our computations are performed through the Bethe ansatz equations in the thermodynamic limit. We formulate a suitable quantization condition describing the scattering process and proceed with explic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.5991","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":"2026-05-18T02:28:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+U50QDpHLzowVJMLJ8jZRyGdjVT5pjwfszfBSdMYqRgkKBtYLOtBS0wq1PmYA97mpKd2ASPBvJyE2Rko5aL5Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T00:34:06.514463Z"},"content_sha256":"81a94475a8aa007444650683c084466ab9f275bbdb850bff482f2bdb70aa4a1d","schema_version":"1.0","event_id":"sha256:81a94475a8aa007444650683c084466ab9f275bbdb850bff482f2bdb70aa4a1d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/COQYFUFV2GYBMDTTFJC5WGYMYV/bundle.json","state_url":"https://pith.science/pith/COQYFUFV2GYBMDTTFJC5WGYMYV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/COQYFUFV2GYBMDTTFJC5WGYMYV/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":"2026-06-12T00:34:06Z","links":{"resolver":"https://pith.science/pith/COQYFUFV2GYBMDTTFJC5WGYMYV","bundle":"https://pith.science/pith/COQYFUFV2GYBMDTTFJC5WGYMYV/bundle.json","state":"https://pith.science/pith/COQYFUFV2GYBMDTTFJC5WGYMYV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/COQYFUFV2GYBMDTTFJC5WGYMYV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:COQYFUFV2GYBMDTTFJC5WGYMYV","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":"0e725cb11f58ed0ab53420b94975384a8eccf728f149148e5f69f3ccffb07d09","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-22T10:58:48Z","title_canon_sha256":"5b686dcd5b38b4dd310fa632b3bfa6d888a2f907f0e17a8ab7f6a38e6cd559ab"},"schema_version":"1.0","source":{"id":"1410.5991","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.5991","created_at":"2026-05-18T02:28:05Z"},{"alias_kind":"arxiv_version","alias_value":"1410.5991v2","created_at":"2026-05-18T02:28:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.5991","created_at":"2026-05-18T02:28:05Z"},{"alias_kind":"pith_short_12","alias_value":"COQYFUFV2GYB","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"COQYFUFV2GYBMDTT","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"COQYFUFV","created_at":"2026-05-18T12:28:22Z"}],"graph_snapshots":[{"event_id":"sha256:81a94475a8aa007444650683c084466ab9f275bbdb850bff482f2bdb70aa4a1d","target":"graph","created_at":"2026-05-18T02:28:05Z","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":"A quantum spin chain with non-conventional boundary conditions is studied. The distinct nature of these boundary conditions arises from the conversion of a soliton to an anti-soliton after being reflected to the boundary, hence the appellation soliton non-preserving boundary conditions. We focus on the simplest non-trivial case of this class of models based on the twisted Yangian quadratic algebra. Our computations are performed through the Bethe ansatz equations in the thermodynamic limit. We formulate a suitable quantization condition describing the scattering process and proceed with explic","authors_text":"Anastasia Doikou, Jean Avan, Nikos Karaiskos","cross_cats":["math-ph","math.MP","nlin.SI"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-22T10:58:48Z","title":"Scattering matrices in the sl(3) twisted Yangian"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.5991","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:bc4ba207b5282957a61c83627b328eb4581d096ed72a39db28089601b47ef24c","target":"record","created_at":"2026-05-18T02:28:05Z","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":"0e725cb11f58ed0ab53420b94975384a8eccf728f149148e5f69f3ccffb07d09","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-22T10:58:48Z","title_canon_sha256":"5b686dcd5b38b4dd310fa632b3bfa6d888a2f907f0e17a8ab7f6a38e6cd559ab"},"schema_version":"1.0","source":{"id":"1410.5991","kind":"arxiv","version":2}},"canonical_sha256":"13a182d0b5d1b0160e732a45db1b0cc54c1d32c1450cc8ed76d554625d5a727b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"13a182d0b5d1b0160e732a45db1b0cc54c1d32c1450cc8ed76d554625d5a727b","first_computed_at":"2026-05-18T02:28:05.064615Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:28:05.064615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ws0oR0zp6lcbUiCP6ylHKokUC1jXvXk2hRzGbUQGYYTJ8JfK6qalNMHTHWy6rSdd635dkQT0N4WtJYLbNCA8AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:28:05.065033Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.5991","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bc4ba207b5282957a61c83627b328eb4581d096ed72a39db28089601b47ef24c","sha256:81a94475a8aa007444650683c084466ab9f275bbdb850bff482f2bdb70aa4a1d"],"state_sha256":"1935448298c1c9e78673a5a6aab61c08faa03d9de867eb9aead9f960b28c7137"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jsvmD7KQca3qlJP+wuWnkiLM1gw+EHb8SRxYhzkRbyfnFPVAFUNp8WogXaQXigqsslqq87/hBI71z+xdLFaoCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T00:34:06.516458Z","bundle_sha256":"a1635776f551930096314c3b64688a7390022a7f29b4b42c1b4d0a92aaeba3ba"}}