{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:XMRFFYDY2R2J7EBQ656Z436EDV","short_pith_number":"pith:XMRFFYDY","schema_version":"1.0","canonical_sha256":"bb2252e078d4749f9030f77d9e6fc41d73f2e35c5d3ebd4f153d8ee3eb89427b","source":{"kind":"arxiv","id":"hep-th/0206210","version":1},"attestation_state":"computed","paper":{"title":"RG Flows from Super-Liouville Theory to Critical Ising Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Al. B. Zamolodchikov, Chaiho Rim, Changrim Ahn, Chanju Kim","submitted_at":"2002-06-24T06:14:13Z","abstract_excerpt":"We study an integrable deformation of the super-Liouville theory which generates a RG flows to the critical Ising model as the IR fixed point. This model turns out to be a supersymmetric sinh-Gordon model with spontaneously broken N=1 supersymmetry. The resulting massless Goldstino is the only stable on-shell particle which controls the IR behaviours. We propose the exact $S$-matrix of the Goldstino and compare associated thermodynamic Bethe ansatz equations with the quantization conditions derived from the reflection amplitudes of the the super-Liouville theory to provide nonperturbative chec"},"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/0206210","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-06-24T06:14:13Z","cross_cats_sorted":[],"title_canon_sha256":"33ab6219adfa0f73302cbfdddf62c48577ca59aacea753a1674f0b876c3c60fd","abstract_canon_sha256":"3394ee43e1056ff458fbf3861095b25c7b6b0a22f8bae58f83323a2d5b8e3c3f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:48.707066Z","signature_b64":"7UdN9wLGIa5LCbWl/zWirUqJHSx+7MPiyg793I7XTF2eaUGYp83dpeDDHC1XqwVa0sgQTNRCw2f6o13/IsLZDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb2252e078d4749f9030f77d9e6fc41d73f2e35c5d3ebd4f153d8ee3eb89427b","last_reissued_at":"2026-07-04T16:34:48.706715Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:48.706715Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"RG Flows from Super-Liouville Theory to Critical Ising Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Al. B. Zamolodchikov, Chaiho Rim, Changrim Ahn, Chanju Kim","submitted_at":"2002-06-24T06:14:13Z","abstract_excerpt":"We study an integrable deformation of the super-Liouville theory which generates a RG flows to the critical Ising model as the IR fixed point. This model turns out to be a supersymmetric sinh-Gordon model with spontaneously broken N=1 supersymmetry. The resulting massless Goldstino is the only stable on-shell particle which controls the IR behaviours. We propose the exact $S$-matrix of the Goldstino and compare associated thermodynamic Bethe ansatz equations with the quantization conditions derived from the reflection amplitudes of the the super-Liouville theory to provide nonperturbative chec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0206210","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/0206210/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/0206210","created_at":"2026-07-04T16:34:48.706762+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0206210v1","created_at":"2026-07-04T16:34:48.706762+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0206210","created_at":"2026-07-04T16:34:48.706762+00:00"},{"alias_kind":"pith_short_12","alias_value":"XMRFFYDY2R2J","created_at":"2026-07-04T16:34:48.706762+00:00"},{"alias_kind":"pith_short_16","alias_value":"XMRFFYDY2R2J7EBQ","created_at":"2026-07-04T16:34:48.706762+00:00"},{"alias_kind":"pith_short_8","alias_value":"XMRFFYDY","created_at":"2026-07-04T16:34:48.706762+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV","json":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV.json","graph_json":"https://pith.science/api/pith-number/XMRFFYDY2R2J7EBQ656Z436EDV/graph.json","events_json":"https://pith.science/api/pith-number/XMRFFYDY2R2J7EBQ656Z436EDV/events.json","paper":"https://pith.science/paper/XMRFFYDY"},"agent_actions":{"view_html":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV","download_json":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV.json","view_paper":"https://pith.science/paper/XMRFFYDY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0206210&json=true","fetch_graph":"https://pith.science/api/pith-number/XMRFFYDY2R2J7EBQ656Z436EDV/graph.json","fetch_events":"https://pith.science/api/pith-number/XMRFFYDY2R2J7EBQ656Z436EDV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV/action/storage_attestation","attest_author":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV/action/author_attestation","sign_citation":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV/action/citation_signature","submit_replication":"https://pith.science/pith/XMRFFYDY2R2J7EBQ656Z436EDV/action/replication_record"}},"created_at":"2026-07-04T16:34:48.706762+00:00","updated_at":"2026-07-04T16:34:48.706762+00:00"}