{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:DVEW57ROIWV5GQSU77MNCP7U2W","short_pith_number":"pith:DVEW57RO","schema_version":"1.0","canonical_sha256":"1d496efe2e45abd34254ffd8d13ff4d5b187c4e892fafea7a6c5a773c0a29aa7","source":{"kind":"arxiv","id":"2511.10934","version":2},"attestation_state":"computed","paper":{"title":"Probing universal imaginary-time relaxation critical dynamics with infinite projected entangled pair states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"He-Yu Lin, Shuai Yin, Zhong-Yi Lu, Z. Y. Xie","submitted_at":"2025-11-14T03:41:38Z","abstract_excerpt":"We investigate the imaginary-time relaxation critical dynamics of the two-dimensional transverse-field Ising model using infinite projected entangled pair states (iPEPS) with the full-update strategy. Simulating directly in the thermodynamic limit, we explore the relaxation process near the critical point with two types of initial states: a fully polarized state and a product state with a small magnetization. For the fully polarized state, the magnetization shows a power law scaling $M\\propto \\tau^{-\\beta/(\\nu z)}$ in the imaginary-time evolution, from which both the critical point and critica"},"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":"2511.10934","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-11-14T03:41:38Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"51f43f3169920fd0670ad0922ee650f2c298a6560beaedd9f89ffc74239855e4","abstract_canon_sha256":"efdb8e5636a504e51490e97b27a9e61c4daba3acb0538fb9ff718266b52ec6c8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-04T01:08:36.051760Z","signature_b64":"tegB4uQTlE0T7fVtdX8AGt24weBkG4x6ubnV/ZTC22o2yb13YPeVjtRHBhz9A7MQC0bL6hGVdH5EPA7iN4JQDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1d496efe2e45abd34254ffd8d13ff4d5b187c4e892fafea7a6c5a773c0a29aa7","last_reissued_at":"2026-06-04T01:08:36.051153Z","signature_status":"signed_v1","first_computed_at":"2026-06-04T01:08:36.051153Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing universal imaginary-time relaxation critical dynamics with infinite projected entangled pair states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"He-Yu Lin, Shuai Yin, Zhong-Yi Lu, Z. Y. Xie","submitted_at":"2025-11-14T03:41:38Z","abstract_excerpt":"We investigate the imaginary-time relaxation critical dynamics of the two-dimensional transverse-field Ising model using infinite projected entangled pair states (iPEPS) with the full-update strategy. Simulating directly in the thermodynamic limit, we explore the relaxation process near the critical point with two types of initial states: a fully polarized state and a product state with a small magnetization. For the fully polarized state, the magnetization shows a power law scaling $M\\propto \\tau^{-\\beta/(\\nu z)}$ in the imaginary-time evolution, from which both the critical point and critica"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.10934","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2511.10934/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":"2511.10934","created_at":"2026-06-04T01:08:36.051226+00:00"},{"alias_kind":"arxiv_version","alias_value":"2511.10934v2","created_at":"2026-06-04T01:08:36.051226+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.10934","created_at":"2026-06-04T01:08:36.051226+00:00"},{"alias_kind":"pith_short_12","alias_value":"DVEW57ROIWV5","created_at":"2026-06-04T01:08:36.051226+00:00"},{"alias_kind":"pith_short_16","alias_value":"DVEW57ROIWV5GQSU","created_at":"2026-06-04T01:08:36.051226+00:00"},{"alias_kind":"pith_short_8","alias_value":"DVEW57RO","created_at":"2026-06-04T01:08:36.051226+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/DVEW57ROIWV5GQSU77MNCP7U2W","json":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W.json","graph_json":"https://pith.science/api/pith-number/DVEW57ROIWV5GQSU77MNCP7U2W/graph.json","events_json":"https://pith.science/api/pith-number/DVEW57ROIWV5GQSU77MNCP7U2W/events.json","paper":"https://pith.science/paper/DVEW57RO"},"agent_actions":{"view_html":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W","download_json":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W.json","view_paper":"https://pith.science/paper/DVEW57RO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2511.10934&json=true","fetch_graph":"https://pith.science/api/pith-number/DVEW57ROIWV5GQSU77MNCP7U2W/graph.json","fetch_events":"https://pith.science/api/pith-number/DVEW57ROIWV5GQSU77MNCP7U2W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W/action/storage_attestation","attest_author":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W/action/author_attestation","sign_citation":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W/action/citation_signature","submit_replication":"https://pith.science/pith/DVEW57ROIWV5GQSU77MNCP7U2W/action/replication_record"}},"created_at":"2026-06-04T01:08:36.051226+00:00","updated_at":"2026-06-04T01:08:36.051226+00:00"}