{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:NPBQLFTRUYCIJH7Z2E7SXTYTQF","short_pith_number":"pith:NPBQLFTR","schema_version":"1.0","canonical_sha256":"6bc3059671a604849ff9d13f2bcf138146c358937b813380b9846fd41b514e9f","source":{"kind":"arxiv","id":"0909.2661","version":2},"attestation_state":"computed","paper":{"title":"Conformal Invariance in (2+1)-Dimensional Stochastic Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"L. Moriconi, M. Moriconi","submitted_at":"2009-09-14T23:34:48Z","abstract_excerpt":"Stochastic partial differential equations can be used to model second order thermodynamical phase transitions, as well as a number of critical out-of-equilibrium phenomena. In (2+1) dimensions, many of these systems are conjectured (and some are indeed proved) to be described by conformal field theories. We advance, in the framework of the Martin-Siggia-Rose field theoretical formalism of stochastic dynamics, a general solution of the translation Ward identities, which yields a putative conformal energy-momentum tensor. Even though the computation of energy-momentum correlators is obstructed, "},"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":"0909.2661","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2009-09-14T23:34:48Z","cross_cats_sorted":["cond-mat.dis-nn","hep-th"],"title_canon_sha256":"ffb7f8142247f54cf62013f83e9f9f2b19aa11f99594d4e241047cd4f2535f64","abstract_canon_sha256":"dc3fbd6eb25e5d3faab6c3b6d8b9cd84ee8babc35a43a84d6a6ffd3daf5fb2e5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:57.740968Z","signature_b64":"wc6PIi82RaFf8CTYKIc7wdOGy49cseLk+GhctzHypU1qW2slh3ZoEWdIcMGtQix+cmqXqZX549DhB1c5qWj5BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6bc3059671a604849ff9d13f2bcf138146c358937b813380b9846fd41b514e9f","last_reissued_at":"2026-05-18T03:23:57.740496Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:57.740496Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conformal Invariance in (2+1)-Dimensional Stochastic Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"L. Moriconi, M. Moriconi","submitted_at":"2009-09-14T23:34:48Z","abstract_excerpt":"Stochastic partial differential equations can be used to model second order thermodynamical phase transitions, as well as a number of critical out-of-equilibrium phenomena. In (2+1) dimensions, many of these systems are conjectured (and some are indeed proved) to be described by conformal field theories. We advance, in the framework of the Martin-Siggia-Rose field theoretical formalism of stochastic dynamics, a general solution of the translation Ward identities, which yields a putative conformal energy-momentum tensor. Even though the computation of energy-momentum correlators is obstructed, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0909.2661","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0909.2661","created_at":"2026-05-18T03:23:57.740574+00:00"},{"alias_kind":"arxiv_version","alias_value":"0909.2661v2","created_at":"2026-05-18T03:23:57.740574+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0909.2661","created_at":"2026-05-18T03:23:57.740574+00:00"},{"alias_kind":"pith_short_12","alias_value":"NPBQLFTRUYCI","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_16","alias_value":"NPBQLFTRUYCIJH7Z","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_8","alias_value":"NPBQLFTR","created_at":"2026-05-18T12:26:00.592388+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/NPBQLFTRUYCIJH7Z2E7SXTYTQF","json":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF.json","graph_json":"https://pith.science/api/pith-number/NPBQLFTRUYCIJH7Z2E7SXTYTQF/graph.json","events_json":"https://pith.science/api/pith-number/NPBQLFTRUYCIJH7Z2E7SXTYTQF/events.json","paper":"https://pith.science/paper/NPBQLFTR"},"agent_actions":{"view_html":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF","download_json":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF.json","view_paper":"https://pith.science/paper/NPBQLFTR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0909.2661&json=true","fetch_graph":"https://pith.science/api/pith-number/NPBQLFTRUYCIJH7Z2E7SXTYTQF/graph.json","fetch_events":"https://pith.science/api/pith-number/NPBQLFTRUYCIJH7Z2E7SXTYTQF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF/action/storage_attestation","attest_author":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF/action/author_attestation","sign_citation":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF/action/citation_signature","submit_replication":"https://pith.science/pith/NPBQLFTRUYCIJH7Z2E7SXTYTQF/action/replication_record"}},"created_at":"2026-05-18T03:23:57.740574+00:00","updated_at":"2026-05-18T03:23:57.740574+00:00"}