{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:PWVJN4HVVIUWN7HNO2USQMDNTI","short_pith_number":"pith:PWVJN4HV","schema_version":"1.0","canonical_sha256":"7daa96f0f5aa2966fced76a928306d9a001b943079acd0309a7e30734d5606cb","source":{"kind":"arxiv","id":"1610.06122","version":2},"attestation_state":"computed","paper":{"title":"From dynamical scaling to local scale-invariance: a tutorial","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Malte Henkel","submitted_at":"2016-10-19T17:35:46Z","abstract_excerpt":"Dynamical scaling arises naturally in various many-body systems far from equilibrium. After a short historical overview, the elements of possible extensions of dynamical scaling to a local scale-invariance will be introduced. Schr\\\"odinger-invariance, the most simple example of local scale-invariance, will be introduced as a dynamical symmetry in the Edwards-Wilkinson universality class of interface growth. The Lie algebra construction, its representations and the Bargman superselection rules will be combined with non-equilibrium Janssen-de Dominicis field-theory to produce explicit prediction"},"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":"1610.06122","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-10-19T17:35:46Z","cross_cats_sorted":["hep-th","math-ph","math.MP"],"title_canon_sha256":"da5b9a6a4ecf330367314dd3ea28f0517ad47df781a72e08eb6bbf86656098ed","abstract_canon_sha256":"173cb0aef479621851905a0369ddc64c04f0b5ea1952f40626a84f40fe7f5c6f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:46.601128Z","signature_b64":"X5Khks6FFaUBpEYh3aXlv++3AFdJqMJZ9fH0GdEzq5kBv1h9J5Xr8pB/0lVMllDV4XQNE7lwoLWSiURC0XpXDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7daa96f0f5aa2966fced76a928306d9a001b943079acd0309a7e30734d5606cb","last_reissued_at":"2026-05-18T00:40:46.600443Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:46.600443Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From dynamical scaling to local scale-invariance: a tutorial","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Malte Henkel","submitted_at":"2016-10-19T17:35:46Z","abstract_excerpt":"Dynamical scaling arises naturally in various many-body systems far from equilibrium. After a short historical overview, the elements of possible extensions of dynamical scaling to a local scale-invariance will be introduced. Schr\\\"odinger-invariance, the most simple example of local scale-invariance, will be introduced as a dynamical symmetry in the Edwards-Wilkinson universality class of interface growth. The Lie algebra construction, its representations and the Bargman superselection rules will be combined with non-equilibrium Janssen-de Dominicis field-theory to produce explicit prediction"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.06122","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":"1610.06122","created_at":"2026-05-18T00:40:46.600533+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.06122v2","created_at":"2026-05-18T00:40:46.600533+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.06122","created_at":"2026-05-18T00:40:46.600533+00:00"},{"alias_kind":"pith_short_12","alias_value":"PWVJN4HVVIUW","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"PWVJN4HVVIUWN7HN","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"PWVJN4HV","created_at":"2026-05-18T12:30:39.010887+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.25429","citing_title":"Schr\\\"odinger-invariance in non-equilibrium critical dynamics","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI","json":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI.json","graph_json":"https://pith.science/api/pith-number/PWVJN4HVVIUWN7HNO2USQMDNTI/graph.json","events_json":"https://pith.science/api/pith-number/PWVJN4HVVIUWN7HNO2USQMDNTI/events.json","paper":"https://pith.science/paper/PWVJN4HV"},"agent_actions":{"view_html":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI","download_json":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI.json","view_paper":"https://pith.science/paper/PWVJN4HV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.06122&json=true","fetch_graph":"https://pith.science/api/pith-number/PWVJN4HVVIUWN7HNO2USQMDNTI/graph.json","fetch_events":"https://pith.science/api/pith-number/PWVJN4HVVIUWN7HNO2USQMDNTI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI/action/storage_attestation","attest_author":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI/action/author_attestation","sign_citation":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI/action/citation_signature","submit_replication":"https://pith.science/pith/PWVJN4HVVIUWN7HNO2USQMDNTI/action/replication_record"}},"created_at":"2026-05-18T00:40:46.600533+00:00","updated_at":"2026-05-18T00:40:46.600533+00:00"}