{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D","short_pith_number":"pith:3DR7Q7EC","schema_version":"1.0","canonical_sha256":"d8e3f87c8224100b3a49dc92687449d8fe506a83ce2f34223704dc7e486ac1ed","source":{"kind":"arxiv","id":"2408.05805","version":2},"attestation_state":"computed","paper":{"title":"Supersymmetric brick wall diagrams and the dynamical fishnet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Matthias Staudacher, Moritz Kade","submitted_at":"2024-08-11T15:53:07Z","abstract_excerpt":"We consider the double scaling limit of $\\beta$-deformed planar N = 4 supersymmetric Yang-Mills theory (SYM), which has been argued to be conformal and integrable. It is a special point in the three-parameter space of double-scaled $\\gamma_i$-deformed N = 4 SYM, preserving N = 1 supersymmetry. The Feynman diagrams of the general three-parameter models form a \"dynamical fishnet\" that is much harder to analyze than the original one-parameter fishnet, where major progress in uncovering the model's integrable structure has been made in recent years. Here we show that by applying N = 1 superspace t"},"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":"2408.05805","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-08-11T15:53:07Z","cross_cats_sorted":[],"title_canon_sha256":"d5b97aafad4fc16c75ac7f1ba67c7a328842a4f6f59208b93f9aefbcf542c5be","abstract_canon_sha256":"1b9e5e3742e8beaf5b5af7975adec003d3e7ba92b1c33d38b26ba3d35648318d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:55:59.521180Z","signature_b64":"DeFXINe/krTh6UMxQidUd+nKP/JjEOU4KXEnIUidd/9lVRFNPF4sOP4+KJqY7ERgek+8mOvYVbAJbj2Xj7qCCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8e3f87c8224100b3a49dc92687449d8fe506a83ce2f34223704dc7e486ac1ed","last_reissued_at":"2026-07-05T09:55:59.520680Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:55:59.520680Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supersymmetric brick wall diagrams and the dynamical fishnet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Matthias Staudacher, Moritz Kade","submitted_at":"2024-08-11T15:53:07Z","abstract_excerpt":"We consider the double scaling limit of $\\beta$-deformed planar N = 4 supersymmetric Yang-Mills theory (SYM), which has been argued to be conformal and integrable. It is a special point in the three-parameter space of double-scaled $\\gamma_i$-deformed N = 4 SYM, preserving N = 1 supersymmetry. The Feynman diagrams of the general three-parameter models form a \"dynamical fishnet\" that is much harder to analyze than the original one-parameter fishnet, where major progress in uncovering the model's integrable structure has been made in recent years. Here we show that by applying N = 1 superspace t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.05805","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2408.05805/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":"2408.05805","created_at":"2026-07-05T09:55:59.520736+00:00"},{"alias_kind":"arxiv_version","alias_value":"2408.05805v2","created_at":"2026-07-05T09:55:59.520736+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.05805","created_at":"2026-07-05T09:55:59.520736+00:00"},{"alias_kind":"pith_short_12","alias_value":"3DR7Q7ECEQIA","created_at":"2026-07-05T09:55:59.520736+00:00"},{"alias_kind":"pith_short_16","alias_value":"3DR7Q7ECEQIAWOSJ","created_at":"2026-07-05T09:55:59.520736+00:00"},{"alias_kind":"pith_short_8","alias_value":"3DR7Q7EC","created_at":"2026-07-05T09:55:59.520736+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/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D","json":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D.json","graph_json":"https://pith.science/api/pith-number/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/graph.json","events_json":"https://pith.science/api/pith-number/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/events.json","paper":"https://pith.science/paper/3DR7Q7EC"},"agent_actions":{"view_html":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D","download_json":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D.json","view_paper":"https://pith.science/paper/3DR7Q7EC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2408.05805&json=true","fetch_graph":"https://pith.science/api/pith-number/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/graph.json","fetch_events":"https://pith.science/api/pith-number/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/action/storage_attestation","attest_author":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/action/author_attestation","sign_citation":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/action/citation_signature","submit_replication":"https://pith.science/pith/3DR7Q7ECEQIAWOSJ3SJGQ5CJ3D/action/replication_record"}},"created_at":"2026-07-05T09:55:59.520736+00:00","updated_at":"2026-07-05T09:55:59.520736+00:00"}