{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:A3J2OXBKCM62IXZ3NAPLMB6JAO","short_pith_number":"pith:A3J2OXBK","schema_version":"1.0","canonical_sha256":"06d3a75c2a133da45f3b681eb607c903bc3288048fd3a847fce2f5a38e5dc1d7","source":{"kind":"arxiv","id":"2411.10266","version":1},"attestation_state":"computed","paper":{"title":"Universal non-equilibrium scaling of cumulants across a critical point","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Leon J. Sieke, Lorenz von Smekal, Mattis Harhoff, S\\\"oren Schlichting","submitted_at":"2024-11-15T15:15:04Z","abstract_excerpt":"We study the critical dynamics of a scalar field theory with $Z_2$ symmetry in the dynamic universality class of Model A in two and three spatial dimensions with classical-statistical lattice simulations. In particular, we measure the non-equilibrium behavior of the system under a quench protocol in which the symmetry-breaking external field is changed at a constant rate through the critical point. Using the well-established Kibble-Zurek scaling theory we compute non-equilibrium scaling functions of cumulants of the order parameter up to fourth order. Together with the static critical exponent"},"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":"2411.10266","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-15T15:15:04Z","cross_cats_sorted":[],"title_canon_sha256":"cf4ddfab71c3c9e9ee58b0f0829fbe511cc8a592782b6d91d58b5345840b19ea","abstract_canon_sha256":"7433056de99c31768149f122afce6a2675af89d2f61556012364eba0a6612538"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:36:02.434329Z","signature_b64":"F7JSF7tEo2m6pIJ9NBoq2QlntGI7CXikFLCNWJFLLM/C+dsM+V3EDCjTnNiHPMIJDkJuSyLS6EJkkYY6ojyqDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"06d3a75c2a133da45f3b681eb607c903bc3288048fd3a847fce2f5a38e5dc1d7","last_reissued_at":"2026-07-05T09:36:02.433812Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:36:02.433812Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal non-equilibrium scaling of cumulants across a critical point","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Leon J. Sieke, Lorenz von Smekal, Mattis Harhoff, S\\\"oren Schlichting","submitted_at":"2024-11-15T15:15:04Z","abstract_excerpt":"We study the critical dynamics of a scalar field theory with $Z_2$ symmetry in the dynamic universality class of Model A in two and three spatial dimensions with classical-statistical lattice simulations. In particular, we measure the non-equilibrium behavior of the system under a quench protocol in which the symmetry-breaking external field is changed at a constant rate through the critical point. Using the well-established Kibble-Zurek scaling theory we compute non-equilibrium scaling functions of cumulants of the order parameter up to fourth order. Together with the static critical exponent"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.10266","kind":"arxiv","version":1},"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/2411.10266/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":"2411.10266","created_at":"2026-07-05T09:36:02.433869+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.10266v1","created_at":"2026-07-05T09:36:02.433869+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.10266","created_at":"2026-07-05T09:36:02.433869+00:00"},{"alias_kind":"pith_short_12","alias_value":"A3J2OXBKCM62","created_at":"2026-07-05T09:36:02.433869+00:00"},{"alias_kind":"pith_short_16","alias_value":"A3J2OXBKCM62IXZ3","created_at":"2026-07-05T09:36:02.433869+00:00"},{"alias_kind":"pith_short_8","alias_value":"A3J2OXBK","created_at":"2026-07-05T09:36:02.433869+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/A3J2OXBKCM62IXZ3NAPLMB6JAO","json":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO.json","graph_json":"https://pith.science/api/pith-number/A3J2OXBKCM62IXZ3NAPLMB6JAO/graph.json","events_json":"https://pith.science/api/pith-number/A3J2OXBKCM62IXZ3NAPLMB6JAO/events.json","paper":"https://pith.science/paper/A3J2OXBK"},"agent_actions":{"view_html":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO","download_json":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO.json","view_paper":"https://pith.science/paper/A3J2OXBK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.10266&json=true","fetch_graph":"https://pith.science/api/pith-number/A3J2OXBKCM62IXZ3NAPLMB6JAO/graph.json","fetch_events":"https://pith.science/api/pith-number/A3J2OXBKCM62IXZ3NAPLMB6JAO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO/action/storage_attestation","attest_author":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO/action/author_attestation","sign_citation":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO/action/citation_signature","submit_replication":"https://pith.science/pith/A3J2OXBKCM62IXZ3NAPLMB6JAO/action/replication_record"}},"created_at":"2026-07-05T09:36:02.433869+00:00","updated_at":"2026-07-05T09:36:02.433869+00:00"}