{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:YDIR2LMXUCVWLEZYNT5B7HGEPB","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"a3135f94693ee357b860406bb376790cb4e1da03c295bb3c951e25b47c4ca555","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-08-12T07:00:01Z","title_canon_sha256":"d1ee51f201b3f4e4e291523b59d5c9a948b11c33562bfb2bd16484622e9a18b2"},"schema_version":"1.0","source":{"id":"1108.2574","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.2574","created_at":"2026-05-18T02:00:54Z"},{"alias_kind":"arxiv_version","alias_value":"1108.2574v1","created_at":"2026-05-18T02:00:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.2574","created_at":"2026-05-18T02:00:54Z"},{"alias_kind":"pith_short_12","alias_value":"YDIR2LMXUCVW","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"YDIR2LMXUCVWLEZY","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"YDIR2LMX","created_at":"2026-05-18T12:26:47Z"}],"graph_snapshots":[{"event_id":"sha256:1a00370a7cc669b5119b22e8b09bc885019b7199dba8e1bb7526cc61dafed6d6","target":"graph","created_at":"2026-05-18T02:00:54Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study the (analytic) finite-size corrections in the Ising model on the strip with fixed ($+ -$) boundary conditions. We find that subdominant finite-size corrections to scaling should be to the form $a_k/N^{2k-1}$ for the free energy $f_N$ and $b_k^{(n)}/N^{2k-1}$ for inverse correlation length $\\xi_n^{-1}$, with integer value of $k$. We investigate the set $\\{a_k, b_k^{(n)}\\}$ by exact evaluation and their changes upon varying anisotropy of coupling. We find that the amplitude ratios $b_k^{(n)}/a_k$ remain constant upon varying coupling anisotropy. Such universal behavior are correctly rep","authors_text":"N. Sh. Izmailian","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-08-12T07:00:01Z","title":"Universal amplitude ratios for scaling corrections on Ising strips with fixed boundary conditions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.2574","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:6ae04eaa725d56d030d12d0ef387887756454fb3cd398b059bbea59e35dba8f9","target":"record","created_at":"2026-05-18T02:00:54Z","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":"a3135f94693ee357b860406bb376790cb4e1da03c295bb3c951e25b47c4ca555","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-08-12T07:00:01Z","title_canon_sha256":"d1ee51f201b3f4e4e291523b59d5c9a948b11c33562bfb2bd16484622e9a18b2"},"schema_version":"1.0","source":{"id":"1108.2574","kind":"arxiv","version":1}},"canonical_sha256":"c0d11d2d97a0ab6593386cfa1f9cc4787e4b8a36aadbefc57ce7effdc3743be3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c0d11d2d97a0ab6593386cfa1f9cc4787e4b8a36aadbefc57ce7effdc3743be3","first_computed_at":"2026-05-18T02:00:54.833077Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:00:54.833077Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cms5j7booOOrpHiA0tnEhzcU9pDoTV8t0MKSTY8GW4GExzCSruC5XSL+Fi32XdgzoEm2XMkJJqDqD8TFW2MRBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:00:54.833667Z","signed_message":"canonical_sha256_bytes"},"source_id":"1108.2574","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6ae04eaa725d56d030d12d0ef387887756454fb3cd398b059bbea59e35dba8f9","sha256:1a00370a7cc669b5119b22e8b09bc885019b7199dba8e1bb7526cc61dafed6d6"],"state_sha256":"fbd9258fff076a4f2ab0afa6979cd5d62d6f128195e144ce938de4ad88d2b291"}