{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:QO3CSJKKGZS567TBMDE5HOZSDS","short_pith_number":"pith:QO3CSJKK","schema_version":"1.0","canonical_sha256":"83b629254a3665df7e6160c9d3bb321c8d0f0af098395be854b173efb7d1f758","source":{"kind":"arxiv","id":"hep-th/0205256","version":3},"attestation_state":"computed","paper":{"title":"Phenomenology of local scale invariance: from conformal invariance to dynamical scaling","license":"","headline":"","cross_cats":["cond-mat","cond-mat.stat-mech","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Malte Henkel","submitted_at":"2002-05-24T16:47:50Z","abstract_excerpt":"Statistical systems displaying a strongly anisotropic or dynamical scaling behaviour are characterized by an anisotropy exponent theta or a dynamical exponent z. For a given value of theta, we construct local scale transformations which can be viewed as scale transformations with a space-time-dependent dilatation factor. Two distinct types of local scale transformations are found. The first type may describe strongly anisotropic scaling of static systems with a given value of theta, whereas the second type may describe dynamical scaling with a dynamical exponent z. Local scale transformations "},"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/0205256","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-05-24T16:47:50Z","cross_cats_sorted":["cond-mat","cond-mat.stat-mech","math-ph","math.MP"],"title_canon_sha256":"ed0718383c189005e29b9cf4c92d526c29128c82a67400e5cae24385fde5325b","abstract_canon_sha256":"7e36a2ad2230baa7e9cd149c26f9720baddfaca7fe396d3ed1144757116b9c5a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:49.477368Z","signature_b64":"2thL7ANyCKAsBi6RlY6ut3NCPf7z6z5cqL+3bsKhREJjGFl3RZ+jFZipPwDYRcsbjl0MtXWy+t1ilJ1k55MXDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"83b629254a3665df7e6160c9d3bb321c8d0f0af098395be854b173efb7d1f758","last_reissued_at":"2026-05-18T01:38:49.476673Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:49.476673Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phenomenology of local scale invariance: from conformal invariance to dynamical scaling","license":"","headline":"","cross_cats":["cond-mat","cond-mat.stat-mech","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Malte Henkel","submitted_at":"2002-05-24T16:47:50Z","abstract_excerpt":"Statistical systems displaying a strongly anisotropic or dynamical scaling behaviour are characterized by an anisotropy exponent theta or a dynamical exponent z. For a given value of theta, we construct local scale transformations which can be viewed as scale transformations with a space-time-dependent dilatation factor. Two distinct types of local scale transformations are found. The first type may describe strongly anisotropic scaling of static systems with a given value of theta, whereas the second type may describe dynamical scaling with a dynamical exponent z. Local scale transformations "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0205256","kind":"arxiv","version":3},"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":"hep-th/0205256","created_at":"2026-05-18T01:38:49.476782+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0205256v3","created_at":"2026-05-18T01:38:49.476782+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0205256","created_at":"2026-05-18T01:38:49.476782+00:00"},{"alias_kind":"pith_short_12","alias_value":"QO3CSJKKGZS5","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"QO3CSJKKGZS567TB","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"QO3CSJKK","created_at":"2026-05-18T12:25:51.375804+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.19356","citing_title":"Perfect fluid equations with nonrelativistic conformal supersymmetries","ref_index":6,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS","json":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS.json","graph_json":"https://pith.science/api/pith-number/QO3CSJKKGZS567TBMDE5HOZSDS/graph.json","events_json":"https://pith.science/api/pith-number/QO3CSJKKGZS567TBMDE5HOZSDS/events.json","paper":"https://pith.science/paper/QO3CSJKK"},"agent_actions":{"view_html":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS","download_json":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS.json","view_paper":"https://pith.science/paper/QO3CSJKK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0205256&json=true","fetch_graph":"https://pith.science/api/pith-number/QO3CSJKKGZS567TBMDE5HOZSDS/graph.json","fetch_events":"https://pith.science/api/pith-number/QO3CSJKKGZS567TBMDE5HOZSDS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS/action/storage_attestation","attest_author":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS/action/author_attestation","sign_citation":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS/action/citation_signature","submit_replication":"https://pith.science/pith/QO3CSJKKGZS567TBMDE5HOZSDS/action/replication_record"}},"created_at":"2026-05-18T01:38:49.476782+00:00","updated_at":"2026-05-18T01:38:49.476782+00:00"}