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Lett. 100, 017203 (2008)","work_id":"ad4e4f7b-d7ef-4676-8161-e8c4617191ea","year":2008}],"snapshot_sha256":"b23f2fbac5354a15acf078e29ae21025ec6835080857b63499207eb0540a639c"},"source":{"id":"2605.15730","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-19T19:49:12.156687Z","id":"423fb1af-9e8f-435a-a299-262f7786ceb8","model_set":{"reader":"grok-4.3"},"one_line_summary":"Monte Carlo simulations of short-time dynamics in the 3D cubic dimer model extract Tc = 0.672(1), β/ν = 0.581(5), z = 1.92(1), and negative θ = -1.052(5), attributed to SO(5) symmetry and U(1) gauge constraint.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"The cubic dimer model shows a negative critical initial slip exponent of -1.052 due to emergent SO(5) symmetry and U(1) gauge constraint.","strongest_claim":"From these scaling behaviors, we accurately determine the critical temperature Tc = 0.672(1) and the static critical exponent β/ν = 0.581(5) according to the scaling theory of the short-time dynamics. ... we extract the dynamic critical exponent z = 1.92(1) and, notably, find a negative critical initial slip exponent θ = -1.052(5).","weakest_assumption":"The assumption that the initial states have vanishing initial correlation length, which is required for the short-time scaling theory to apply directly (stated in the abstract as the condition for the quenches from ordered and disordered states)."}},"verdict_id":"423fb1af-9e8f-435a-a299-262f7786ceb8"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:fe98c03d42e7476cfb6a5731b528a2836fde562d8b8451400bab2f8a5a0f54f8","target":"record","created_at":"2026-05-20T00:01:15Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"fd476b114defb148a28120d47d6de4676295829412e59c44e7ec7976d76b4a08","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-15T08:33:48Z","title_canon_sha256":"13204948a28fcfd7b2bd48c0185e9a8c304cfaa522eb240c2d23700d08b9b150"},"schema_version":"1.0","source":{"id":"2605.15730","kind":"arxiv","version":1}},"canonical_sha256":"6848466e4c90236378c109fa68c27b68c35caea7e717a7f6089d3883348f94c8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6848466e4c90236378c109fa68c27b68c35caea7e717a7f6089d3883348f94c8","first_computed_at":"2026-05-20T00:01:15.256726Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:01:15.256726Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MQFGcrdL95OCKg0jabIqDxs42ND7r9ARdfSiaI87O0M11vTCHNNWwXj0rat0JYSAri/8dhpU0EHveNrFZ0RZBg==","signature_status":"signed_v1","signed_at":"2026-05-20T00:01:15.257508Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.15730","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fe98c03d42e7476cfb6a5731b528a2836fde562d8b8451400bab2f8a5a0f54f8","sha256:a0c43d263815a41a24d19a4fef7923203aaf8d73de6c80380c0fab9a8edf242d"],"state_sha256":"324e5167018e3006129de259e27534c5c2d47653e3b31dd57b6b57f4d5ded0ae"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rGnLJKSyWhge0K+KCzrUQVKELSRf8Z5qzEzVb5f9JY6cT356VbbcWtPsyc/DrChKhpAAkI1uZHvbMUhS+dTADw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T15:21:14.340079Z","bundle_sha256":"41aecd3909416d5466b55a49da2bfbe1067d2e31c26bb577b9772bf6cd09be12"}}