{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:4GDOSZUOKGMVLMCEYKM3MPTFD3","short_pith_number":"pith:4GDOSZUO","schema_version":"1.0","canonical_sha256":"e186e9668e519955b044c299b63e651ec3bbddd564cb9df9a8a019f2088a6cde","source":{"kind":"arxiv","id":"1912.01617","version":2},"attestation_state":"computed","paper":{"title":"Random Field Ising Model and Parisi-Sourlas Supersymmetry I. Supersymmetric CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"Apratim Kaviraj, Emilio Trevisani, Slava Rychkov","submitted_at":"2019-12-03T19:00:03Z","abstract_excerpt":"Quenched disorder is very important but notoriously hard. In 1979, Parisi and Sourlas proposed an interesting and powerful conjecture about the infrared fixed points with random field type of disorder: such fixed points should possess an unusual supersymmetry, by which they reduce in two less spatial dimensions to usual non-supersymmetric non-disordered fixed points. This conjecture however is known to fail in some simple cases, but there is no consensus on why this happens. In this paper we give new non-perturbative arguments for dimensional reduction. We recast the problem in the language of"},"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":"1912.01617","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-12-03T19:00:03Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"title_canon_sha256":"22f9d9a4ad808cb0a463668364b79fb3f9291f5c404cd95fb62f7c1cbe6712a5","abstract_canon_sha256":"5abbdf3d6fb0d7dc08b8885530a34f5c49cb0e9232006a1ba5a7b1b1e368c1b3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:04:08.337928Z","signature_b64":"qdJF3S4qefk8vlm1WRygpmx2cOioos3ID/LAI0M1ozMGZXyhGJAveaTw8aZkRT82tRvNbs/3JuabZx9JdK7PCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e186e9668e519955b044c299b63e651ec3bbddd564cb9df9a8a019f2088a6cde","last_reissued_at":"2026-07-05T01:04:08.337494Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:04:08.337494Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Random Field Ising Model and Parisi-Sourlas Supersymmetry I. Supersymmetric CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"Apratim Kaviraj, Emilio Trevisani, Slava Rychkov","submitted_at":"2019-12-03T19:00:03Z","abstract_excerpt":"Quenched disorder is very important but notoriously hard. In 1979, Parisi and Sourlas proposed an interesting and powerful conjecture about the infrared fixed points with random field type of disorder: such fixed points should possess an unusual supersymmetry, by which they reduce in two less spatial dimensions to usual non-supersymmetric non-disordered fixed points. This conjecture however is known to fail in some simple cases, but there is no consensus on why this happens. In this paper we give new non-perturbative arguments for dimensional reduction. We recast the problem in the language of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1912.01617","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/1912.01617/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":"1912.01617","created_at":"2026-07-05T01:04:08.337550+00:00"},{"alias_kind":"arxiv_version","alias_value":"1912.01617v2","created_at":"2026-07-05T01:04:08.337550+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1912.01617","created_at":"2026-07-05T01:04:08.337550+00:00"},{"alias_kind":"pith_short_12","alias_value":"4GDOSZUOKGMV","created_at":"2026-07-05T01:04:08.337550+00:00"},{"alias_kind":"pith_short_16","alias_value":"4GDOSZUOKGMVLMCE","created_at":"2026-07-05T01:04:08.337550+00:00"},{"alias_kind":"pith_short_8","alias_value":"4GDOSZUO","created_at":"2026-07-05T01:04:08.337550+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.22628","citing_title":"Ising surface defects can get dirty","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16119","citing_title":"Boundary anomalous dimensions from BCFT: $\\phi^{3}$ theories with a boundary and higher-derivative generalizations","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3","json":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3.json","graph_json":"https://pith.science/api/pith-number/4GDOSZUOKGMVLMCEYKM3MPTFD3/graph.json","events_json":"https://pith.science/api/pith-number/4GDOSZUOKGMVLMCEYKM3MPTFD3/events.json","paper":"https://pith.science/paper/4GDOSZUO"},"agent_actions":{"view_html":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3","download_json":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3.json","view_paper":"https://pith.science/paper/4GDOSZUO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1912.01617&json=true","fetch_graph":"https://pith.science/api/pith-number/4GDOSZUOKGMVLMCEYKM3MPTFD3/graph.json","fetch_events":"https://pith.science/api/pith-number/4GDOSZUOKGMVLMCEYKM3MPTFD3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3/action/storage_attestation","attest_author":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3/action/author_attestation","sign_citation":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3/action/citation_signature","submit_replication":"https://pith.science/pith/4GDOSZUOKGMVLMCEYKM3MPTFD3/action/replication_record"}},"created_at":"2026-07-05T01:04:08.337550+00:00","updated_at":"2026-07-05T01:04:08.337550+00:00"}