{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:3BTQG2BX44MEA5DV6PJYUU3Y7R","short_pith_number":"pith:3BTQG2BX","canonical_record":{"source":{"id":"1610.04006","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-10-13T10:09:35Z","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math.CO","math.MP"],"title_canon_sha256":"5c8f8d503a4842e9b2e5e66f5d151a30be2c896bcdf8aa1405f6d79bed976fc6","abstract_canon_sha256":"1b343cc22af24f7c4e5b543c1ce8f7786f0e681e93a34d78b67f8e5c92c75f11"},"schema_version":"1.0"},"canonical_sha256":"d867036837e718407475f3d38a5378fc418e811c029a8534fe23408d99d3f975","source":{"kind":"arxiv","id":"1610.04006","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.04006","created_at":"2026-05-18T00:53:58Z"},{"alias_kind":"arxiv_version","alias_value":"1610.04006v2","created_at":"2026-05-18T00:53:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04006","created_at":"2026-05-18T00:53:58Z"},{"alias_kind":"pith_short_12","alias_value":"3BTQG2BX44ME","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"3BTQG2BX44MEA5DV","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"3BTQG2BX","created_at":"2026-05-18T12:29:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:3BTQG2BX44MEA5DV6PJYUU3Y7R","target":"record","payload":{"canonical_record":{"source":{"id":"1610.04006","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-10-13T10:09:35Z","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math.CO","math.MP"],"title_canon_sha256":"5c8f8d503a4842e9b2e5e66f5d151a30be2c896bcdf8aa1405f6d79bed976fc6","abstract_canon_sha256":"1b343cc22af24f7c4e5b543c1ce8f7786f0e681e93a34d78b67f8e5c92c75f11"},"schema_version":"1.0"},"canonical_sha256":"d867036837e718407475f3d38a5378fc418e811c029a8534fe23408d99d3f975","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:58.312578Z","signature_b64":"N7EHmnv/SbsNmaHUuzizLrdo37bAxKXONMO2Vs0rGiLrUpVPvIIx0eSyCMHM7DYnLmZZFGwWmThycCTlJjrWDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d867036837e718407475f3d38a5378fc418e811c029a8534fe23408d99d3f975","last_reissued_at":"2026-05-18T00:53:58.311826Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:58.311826Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.04006","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:53:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AsOEuEaFyLRLtPu17/qn7u8g9lsjdXEoedLPAONkXv1laAgd+5S0ML/ItWaIF7DwbxHoqH38BjTdPJpjctmcAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T16:45:00.993937Z"},"content_sha256":"afe8cd264014b8030708ad98a954967dfff9f46ba8444c7b514ff2b59cf87e19","schema_version":"1.0","event_id":"sha256:afe8cd264014b8030708ad98a954967dfff9f46ba8444c7b514ff2b59cf87e19"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:3BTQG2BX44MEA5DV6PJYUU3Y7R","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite-size corrections for universal boundary entropy in bond percolation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-th","math.CO","math.MP"],"primary_cat":"math-ph","authors_text":"Anita Ponsaing, Jan de Gier, Jesper Lykke Jacobsen","submitted_at":"2016-10-13T10:09:35Z","abstract_excerpt":"We compute the boundary entropy for bond percolation on the square lattice in the presence of a boundary loop weight, and prove explicit and exact expressions on a strip and on a cylinder of size $L$. For the cylinder we provide a rigorous asymptotic analysis which allows for the computation of finite-size corrections to arbitrary order. For the strip we provide exact expressions that have been verified using high-precision numerical analysis. Our rigorous and exact results corroborate an argument based on conformal field theory, in particular concerning universal logarithmic corrections for t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04006","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:53:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L/ON4LohypDveAbGfhDH3awQusYDbyWNNnrUPT6YoyP+/v2PHXKJqT7pVP/iZ6c3pS36t/OpENa/wUjPnkwvDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T16:45:00.994358Z"},"content_sha256":"c762cdaab9b3b49f0ac6365b162077578bc1dd143ed91db85ed98fae554a3849","schema_version":"1.0","event_id":"sha256:c762cdaab9b3b49f0ac6365b162077578bc1dd143ed91db85ed98fae554a3849"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3BTQG2BX44MEA5DV6PJYUU3Y7R/bundle.json","state_url":"https://pith.science/pith/3BTQG2BX44MEA5DV6PJYUU3Y7R/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3BTQG2BX44MEA5DV6PJYUU3Y7R/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-29T16:45:00Z","links":{"resolver":"https://pith.science/pith/3BTQG2BX44MEA5DV6PJYUU3Y7R","bundle":"https://pith.science/pith/3BTQG2BX44MEA5DV6PJYUU3Y7R/bundle.json","state":"https://pith.science/pith/3BTQG2BX44MEA5DV6PJYUU3Y7R/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3BTQG2BX44MEA5DV6PJYUU3Y7R/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:3BTQG2BX44MEA5DV6PJYUU3Y7R","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":"1b343cc22af24f7c4e5b543c1ce8f7786f0e681e93a34d78b67f8e5c92c75f11","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math.CO","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-10-13T10:09:35Z","title_canon_sha256":"5c8f8d503a4842e9b2e5e66f5d151a30be2c896bcdf8aa1405f6d79bed976fc6"},"schema_version":"1.0","source":{"id":"1610.04006","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.04006","created_at":"2026-05-18T00:53:58Z"},{"alias_kind":"arxiv_version","alias_value":"1610.04006v2","created_at":"2026-05-18T00:53:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04006","created_at":"2026-05-18T00:53:58Z"},{"alias_kind":"pith_short_12","alias_value":"3BTQG2BX44ME","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"3BTQG2BX44MEA5DV","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"3BTQG2BX","created_at":"2026-05-18T12:29:55Z"}],"graph_snapshots":[{"event_id":"sha256:c762cdaab9b3b49f0ac6365b162077578bc1dd143ed91db85ed98fae554a3849","target":"graph","created_at":"2026-05-18T00:53:58Z","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 compute the boundary entropy for bond percolation on the square lattice in the presence of a boundary loop weight, and prove explicit and exact expressions on a strip and on a cylinder of size $L$. For the cylinder we provide a rigorous asymptotic analysis which allows for the computation of finite-size corrections to arbitrary order. For the strip we provide exact expressions that have been verified using high-precision numerical analysis. Our rigorous and exact results corroborate an argument based on conformal field theory, in particular concerning universal logarithmic corrections for t","authors_text":"Anita Ponsaing, Jan de Gier, Jesper Lykke Jacobsen","cross_cats":["cond-mat.stat-mech","hep-th","math.CO","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-10-13T10:09:35Z","title":"Finite-size corrections for universal boundary entropy in bond percolation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04006","kind":"arxiv","version":2},"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:afe8cd264014b8030708ad98a954967dfff9f46ba8444c7b514ff2b59cf87e19","target":"record","created_at":"2026-05-18T00:53:58Z","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":"1b343cc22af24f7c4e5b543c1ce8f7786f0e681e93a34d78b67f8e5c92c75f11","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math.CO","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2016-10-13T10:09:35Z","title_canon_sha256":"5c8f8d503a4842e9b2e5e66f5d151a30be2c896bcdf8aa1405f6d79bed976fc6"},"schema_version":"1.0","source":{"id":"1610.04006","kind":"arxiv","version":2}},"canonical_sha256":"d867036837e718407475f3d38a5378fc418e811c029a8534fe23408d99d3f975","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d867036837e718407475f3d38a5378fc418e811c029a8534fe23408d99d3f975","first_computed_at":"2026-05-18T00:53:58.311826Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:53:58.311826Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"N7EHmnv/SbsNmaHUuzizLrdo37bAxKXONMO2Vs0rGiLrUpVPvIIx0eSyCMHM7DYnLmZZFGwWmThycCTlJjrWDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:53:58.312578Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.04006","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:afe8cd264014b8030708ad98a954967dfff9f46ba8444c7b514ff2b59cf87e19","sha256:c762cdaab9b3b49f0ac6365b162077578bc1dd143ed91db85ed98fae554a3849"],"state_sha256":"b06aa807a8cac2db9cbb6b0f7818de2cf424b2d89153d35ebbf99c96b38b826e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hhk+vTRa6NyVcgvhlIfWRmVArEqh5GzB2DjGLq/92r9inhCWuR1l9xr6+pRh/2zXuLiLkQLwB/tDoq71CFtkDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T16:45:00.997173Z","bundle_sha256":"95c98fb0791400f47e0d097d79695033121986706ac98fd060849313ddf28c8c"}}