{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:Q46EQ3BTX4NQRXTCS7WRKUULOC","short_pith_number":"pith:Q46EQ3BT","schema_version":"1.0","canonical_sha256":"873c486c33bf1b08de6297ed15528b70b753ae5f0e005302437ab321c9753acc","source":{"kind":"arxiv","id":"hep-th/9407148","version":1},"attestation_state":"computed","paper":{"title":"Aspects of affine Toda field theory on a half line","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"E. Corrigan P.E. Dorey, R.H. Rietdijk","submitted_at":"1994-07-22T15:47:33Z","abstract_excerpt":"The question of the integrability of real-coupling affine toda field theory on a half line is discussed. It is shown, by examining low-spin conserved charges, that the boundary conditions preserving integrability are strongly constrained. In particular, among the cases treated so far, $e_6^{(1)}$, $d_n^{(1)}$ and $a_n^{(1)}, \\ n\\ge 2$, there can be no free parameters introduced by such boundary conditions; indeed the only remaining freedom (apart from choosing the simple condition $\\partial_1\\phi =0$), resides in a choice of signs. For a special case of the boundary condition, accessible only "},"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/9407148","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-07-22T15:47:33Z","cross_cats_sorted":[],"title_canon_sha256":"8edd0b8e93970a38d0c6375232dccb7a898c02e57d71476870d1d526f0e57b0b","abstract_canon_sha256":"bfb95ebc18f70c72087e17043ec6cd3d6a71a629ea2c483c43a47f7ec4c15aa0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:57.001749Z","signature_b64":"5pwEQ0nGgmDKb/oSsYYw58ITKH0RCIH2avqtz6WtqfadeQ27PghAg+KpqNbmDyPn54gCOxza3P9m7MluDEZKAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"873c486c33bf1b08de6297ed15528b70b753ae5f0e005302437ab321c9753acc","last_reissued_at":"2026-07-04T15:23:57.001336Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:57.001336Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Aspects of affine Toda field theory on a half line","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"E. Corrigan P.E. Dorey, R.H. Rietdijk","submitted_at":"1994-07-22T15:47:33Z","abstract_excerpt":"The question of the integrability of real-coupling affine toda field theory on a half line is discussed. It is shown, by examining low-spin conserved charges, that the boundary conditions preserving integrability are strongly constrained. In particular, among the cases treated so far, $e_6^{(1)}$, $d_n^{(1)}$ and $a_n^{(1)}, \\ n\\ge 2$, there can be no free parameters introduced by such boundary conditions; indeed the only remaining freedom (apart from choosing the simple condition $\\partial_1\\phi =0$), resides in a choice of signs. For a special case of the boundary condition, accessible only "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9407148","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/9407148/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/9407148","created_at":"2026-07-04T15:23:57.001399+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9407148v1","created_at":"2026-07-04T15:23:57.001399+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9407148","created_at":"2026-07-04T15:23:57.001399+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q46EQ3BTX4NQ","created_at":"2026-07-04T15:23:57.001399+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q46EQ3BTX4NQRXTC","created_at":"2026-07-04T15:23:57.001399+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q46EQ3BT","created_at":"2026-07-04T15:23:57.001399+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.11647","citing_title":"Boundary Quantum Field Theories Perturbed by ${\\rm T}\\bar{\\rm T}$: Towards a Form Factor Program","ref_index":19,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC","json":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC.json","graph_json":"https://pith.science/api/pith-number/Q46EQ3BTX4NQRXTCS7WRKUULOC/graph.json","events_json":"https://pith.science/api/pith-number/Q46EQ3BTX4NQRXTCS7WRKUULOC/events.json","paper":"https://pith.science/paper/Q46EQ3BT"},"agent_actions":{"view_html":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC","download_json":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC.json","view_paper":"https://pith.science/paper/Q46EQ3BT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9407148&json=true","fetch_graph":"https://pith.science/api/pith-number/Q46EQ3BTX4NQRXTCS7WRKUULOC/graph.json","fetch_events":"https://pith.science/api/pith-number/Q46EQ3BTX4NQRXTCS7WRKUULOC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC/action/storage_attestation","attest_author":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC/action/author_attestation","sign_citation":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC/action/citation_signature","submit_replication":"https://pith.science/pith/Q46EQ3BTX4NQRXTCS7WRKUULOC/action/replication_record"}},"created_at":"2026-07-04T15:23:57.001399+00:00","updated_at":"2026-07-04T15:23:57.001399+00:00"}