{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:37JT4NA2R7LNFP56E3N7WXJRWQ","short_pith_number":"pith:37JT4NA2","schema_version":"1.0","canonical_sha256":"dfd33e341a8fd6d2bfbe26dbfb5d31b4138b08cf3d86ccc86faccd60ec2e9528","source":{"kind":"arxiv","id":"2607.11066","version":1},"attestation_state":"computed","paper":{"title":"Finite-time Scaling of the surface special transition in a 3D classical Heisenberg model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Dongxu Liu, Shuai Yin, Zheng Yan, Zhe Wang","submitted_at":"2026-07-13T04:05:57Z","abstract_excerpt":"We investigate nonequilibrium driven dynamics across the special surface phase transition in the three-dimensional classical Heisenberg model with open boundaries, where tuning the surface coupling gives access to an extraordinary-log boundary critical state characterized by logarithmic, rather than power-law, decay of correlations. Using Monte Carlo simulations, we realize four driving protocols: temperature heating and cooling across the special transition, and surface-coupling ramps from the ordinary and extraordinary-log critical states into the special point. For temperature-driven protoc"},"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":"2607.11066","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-07-13T04:05:57Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"46245ea10545e0ce2984dd299c084a1aa59621518228684fce151785c94a0d3e","abstract_canon_sha256":"92bac6baf610e27593559b86feab334046d176faf11e0c182f54aa1ae4d21a5c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-14T01:22:14.435904Z","signature_b64":"cpo4kSumnBBa+3zT1JnHyrJIAHyiT3VBZ5skiDdYl5dkW8nSjjf6OWGpC5ve8P5FP6dxlhDtsySQdFHvVjVKAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dfd33e341a8fd6d2bfbe26dbfb5d31b4138b08cf3d86ccc86faccd60ec2e9528","last_reissued_at":"2026-07-14T01:22:14.435058Z","signature_status":"signed_v1","first_computed_at":"2026-07-14T01:22:14.435058Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite-time Scaling of the surface special transition in a 3D classical Heisenberg model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Dongxu Liu, Shuai Yin, Zheng Yan, Zhe Wang","submitted_at":"2026-07-13T04:05:57Z","abstract_excerpt":"We investigate nonequilibrium driven dynamics across the special surface phase transition in the three-dimensional classical Heisenberg model with open boundaries, where tuning the surface coupling gives access to an extraordinary-log boundary critical state characterized by logarithmic, rather than power-law, decay of correlations. Using Monte Carlo simulations, we realize four driving protocols: temperature heating and cooling across the special transition, and surface-coupling ramps from the ordinary and extraordinary-log critical states into the special point. For temperature-driven protoc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.11066","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/2607.11066/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":"2607.11066","created_at":"2026-07-14T01:22:14.435499+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.11066v1","created_at":"2026-07-14T01:22:14.435499+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.11066","created_at":"2026-07-14T01:22:14.435499+00:00"},{"alias_kind":"pith_short_12","alias_value":"37JT4NA2R7LN","created_at":"2026-07-14T01:22:14.435499+00:00"},{"alias_kind":"pith_short_16","alias_value":"37JT4NA2R7LNFP56","created_at":"2026-07-14T01:22:14.435499+00:00"},{"alias_kind":"pith_short_8","alias_value":"37JT4NA2","created_at":"2026-07-14T01:22:14.435499+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/37JT4NA2R7LNFP56E3N7WXJRWQ","json":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ.json","graph_json":"https://pith.science/api/pith-number/37JT4NA2R7LNFP56E3N7WXJRWQ/graph.json","events_json":"https://pith.science/api/pith-number/37JT4NA2R7LNFP56E3N7WXJRWQ/events.json","paper":"https://pith.science/paper/37JT4NA2"},"agent_actions":{"view_html":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ","download_json":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ.json","view_paper":"https://pith.science/paper/37JT4NA2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.11066&json=true","fetch_graph":"https://pith.science/api/pith-number/37JT4NA2R7LNFP56E3N7WXJRWQ/graph.json","fetch_events":"https://pith.science/api/pith-number/37JT4NA2R7LNFP56E3N7WXJRWQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ/action/storage_attestation","attest_author":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ/action/author_attestation","sign_citation":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ/action/citation_signature","submit_replication":"https://pith.science/pith/37JT4NA2R7LNFP56E3N7WXJRWQ/action/replication_record"}},"created_at":"2026-07-14T01:22:14.435499+00:00","updated_at":"2026-07-14T01:22:14.435499+00:00"}