{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:J4PFHENVEDITREB4ZSUYEQCWCL","short_pith_number":"pith:J4PFHENV","schema_version":"1.0","canonical_sha256":"4f1e5391b520d138903ccca982405612c0b5dcd2269d26a4753d13b2c6acd10a","source":{"kind":"arxiv","id":"2305.09502","version":2},"attestation_state":"computed","paper":{"title":"Domain wall fluctuations of the six-vertex model at the ice point","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Herbert Spohn, Michael Praehofer","submitted_at":"2023-05-16T14:56:11Z","abstract_excerpt":"We report on Monte-Carlo simulations of the six-vertex model with domain wall boundary conditions. In thermal equilibrium such boundary conditions force a fluctuating line separating the disordered region from the perfectly ordered ones. Specifically we study the ice point at which all vertex weights are equal. With high precision the one-point fluctuations of the line are confirmed to be of order $N^{1/3}$ and governed by the Tracy-Widom distribution. Furthermore, the non-universal scaling coefficients are computed for a wide range of interaction strengths. A draft of this paper was completed"},"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":"2305.09502","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-16T14:56:11Z","cross_cats_sorted":[],"title_canon_sha256":"2c709d9fe6e595371864009d8c720b272f8ef07f82fe570f80a6f7433dcf51ff","abstract_canon_sha256":"aab8f0f5a85b49609bc9ee573615a211f1efe6c4a9823edaa2fdca5b3e7e70a8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:27:04.584999Z","signature_b64":"ta+ZIoJ+eaE481842lJhYcuO2saKZMS2qny51wFnUd5QxLwms3aAvTP8PpHKf4JYGV3Wzyig8nY+9FPDvvspDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f1e5391b520d138903ccca982405612c0b5dcd2269d26a4753d13b2c6acd10a","last_reissued_at":"2026-07-05T07:27:04.584539Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:27:04.584539Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Domain wall fluctuations of the six-vertex model at the ice point","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Herbert Spohn, Michael Praehofer","submitted_at":"2023-05-16T14:56:11Z","abstract_excerpt":"We report on Monte-Carlo simulations of the six-vertex model with domain wall boundary conditions. In thermal equilibrium such boundary conditions force a fluctuating line separating the disordered region from the perfectly ordered ones. Specifically we study the ice point at which all vertex weights are equal. With high precision the one-point fluctuations of the line are confirmed to be of order $N^{1/3}$ and governed by the Tracy-Widom distribution. Furthermore, the non-universal scaling coefficients are computed for a wide range of interaction strengths. A draft of this paper was completed"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.09502","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/2305.09502/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":"2305.09502","created_at":"2026-07-05T07:27:04.584603+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.09502v2","created_at":"2026-07-05T07:27:04.584603+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.09502","created_at":"2026-07-05T07:27:04.584603+00:00"},{"alias_kind":"pith_short_12","alias_value":"J4PFHENVEDIT","created_at":"2026-07-05T07:27:04.584603+00:00"},{"alias_kind":"pith_short_16","alias_value":"J4PFHENVEDITREB4","created_at":"2026-07-05T07:27:04.584603+00:00"},{"alias_kind":"pith_short_8","alias_value":"J4PFHENV","created_at":"2026-07-05T07:27:04.584603+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/J4PFHENVEDITREB4ZSUYEQCWCL","json":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL.json","graph_json":"https://pith.science/api/pith-number/J4PFHENVEDITREB4ZSUYEQCWCL/graph.json","events_json":"https://pith.science/api/pith-number/J4PFHENVEDITREB4ZSUYEQCWCL/events.json","paper":"https://pith.science/paper/J4PFHENV"},"agent_actions":{"view_html":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL","download_json":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL.json","view_paper":"https://pith.science/paper/J4PFHENV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.09502&json=true","fetch_graph":"https://pith.science/api/pith-number/J4PFHENVEDITREB4ZSUYEQCWCL/graph.json","fetch_events":"https://pith.science/api/pith-number/J4PFHENVEDITREB4ZSUYEQCWCL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL/action/storage_attestation","attest_author":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL/action/author_attestation","sign_citation":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL/action/citation_signature","submit_replication":"https://pith.science/pith/J4PFHENVEDITREB4ZSUYEQCWCL/action/replication_record"}},"created_at":"2026-07-05T07:27:04.584603+00:00","updated_at":"2026-07-05T07:27:04.584603+00:00"}