{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:KMGFZOMH2Q4QLBUUBUC35LOVCE","short_pith_number":"pith:KMGFZOMH","canonical_record":{"source":{"id":"1010.3583","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-10-18T12:55:30Z","cross_cats_sorted":[],"title_canon_sha256":"d33a5f70608e74623dc43d6f2876c47834079d540a11cbfb2e0a40f76853976e","abstract_canon_sha256":"8c4dc4fb53345f8bf41c19c451ea40d7f6f85238a25932f9914fe4cc54fa763a"},"schema_version":"1.0"},"canonical_sha256":"530c5cb987d4390586940d05beadd5113b0e6c487651c8ed92c5e1b35ec536e9","source":{"kind":"arxiv","id":"1010.3583","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.3583","created_at":"2026-05-18T04:21:13Z"},{"alias_kind":"arxiv_version","alias_value":"1010.3583v1","created_at":"2026-05-18T04:21:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3583","created_at":"2026-05-18T04:21:13Z"},{"alias_kind":"pith_short_12","alias_value":"KMGFZOMH2Q4Q","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"KMGFZOMH2Q4QLBUU","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"KMGFZOMH","created_at":"2026-05-18T12:26:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:KMGFZOMH2Q4QLBUUBUC35LOVCE","target":"record","payload":{"canonical_record":{"source":{"id":"1010.3583","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-10-18T12:55:30Z","cross_cats_sorted":[],"title_canon_sha256":"d33a5f70608e74623dc43d6f2876c47834079d540a11cbfb2e0a40f76853976e","abstract_canon_sha256":"8c4dc4fb53345f8bf41c19c451ea40d7f6f85238a25932f9914fe4cc54fa763a"},"schema_version":"1.0"},"canonical_sha256":"530c5cb987d4390586940d05beadd5113b0e6c487651c8ed92c5e1b35ec536e9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:21:13.601579Z","signature_b64":"L6oM9I5CERetPt9Zg7QWtjq8OG2z4D9asR6dTIngw++EQ0A4WlQdj7njzESNgRefxnEYz99wVe9d1G/DRksyBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"530c5cb987d4390586940d05beadd5113b0e6c487651c8ed92c5e1b35ec536e9","last_reissued_at":"2026-05-18T04:21:13.600868Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:21:13.600868Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1010.3583","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:21:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DxHCFt+c1gElYHenjAFIFsqPYGnSgwSjL5OsIKmTmO37r9qSh8g0mSErwEJEF2onLghI7CRBw/FHokD6EERZBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T02:15:25.663838Z"},"content_sha256":"95477e7a3f844900fc948de4b1ed7a8c0e9901dea9c865e2cbca820e2c6bbb1f","schema_version":"1.0","event_id":"sha256:95477e7a3f844900fc948de4b1ed7a8c0e9901dea9c865e2cbca820e2c6bbb1f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:KMGFZOMH2Q4QLBUUBUC35LOVCE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fluids with quenched disorder: Scaling of the free energy barrier near critical points","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"R. L. C. Vink, T. Fischer","submitted_at":"2010-10-18T12:55:30Z","abstract_excerpt":"In the context of Monte Carlo simulations, the analysis of the probability distribution $P_L(m)$ of the order parameter $m$, as obtained in simulation boxes of finite linear extension $L$, allows for an easy estimation of the location of the critical point and the critical exponents. For Ising-like systems without quenched disorder, $P_L(m)$ becomes scale invariant at the critical point, where it assumes a characteristic bimodal shape featuring two overlapping peaks. In particular, the ratio between the value of $P_L(m)$ at the peaks ($P_{L, max}$) and the value at the minimum in-between ($P_{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3583","kind":"arxiv","version":1},"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":"2026-05-18T04:21:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l+nsu3c4ny0mf30Um+rXfYl7Q/mjjjQU4uwdFrqgUiOL08dVpEYZSq/qpZtFeobfHlRBfjbyymoLDNrIAt1QCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T02:15:25.664180Z"},"content_sha256":"dff836db289845acde5656a7045e30d026087d1e33aeeba5a46829da2241fabd","schema_version":"1.0","event_id":"sha256:dff836db289845acde5656a7045e30d026087d1e33aeeba5a46829da2241fabd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KMGFZOMH2Q4QLBUUBUC35LOVCE/bundle.json","state_url":"https://pith.science/pith/KMGFZOMH2Q4QLBUUBUC35LOVCE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KMGFZOMH2Q4QLBUUBUC35LOVCE/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":"2026-05-28T02:15:25Z","links":{"resolver":"https://pith.science/pith/KMGFZOMH2Q4QLBUUBUC35LOVCE","bundle":"https://pith.science/pith/KMGFZOMH2Q4QLBUUBUC35LOVCE/bundle.json","state":"https://pith.science/pith/KMGFZOMH2Q4QLBUUBUC35LOVCE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KMGFZOMH2Q4QLBUUBUC35LOVCE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:KMGFZOMH2Q4QLBUUBUC35LOVCE","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":"8c4dc4fb53345f8bf41c19c451ea40d7f6f85238a25932f9914fe4cc54fa763a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-10-18T12:55:30Z","title_canon_sha256":"d33a5f70608e74623dc43d6f2876c47834079d540a11cbfb2e0a40f76853976e"},"schema_version":"1.0","source":{"id":"1010.3583","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.3583","created_at":"2026-05-18T04:21:13Z"},{"alias_kind":"arxiv_version","alias_value":"1010.3583v1","created_at":"2026-05-18T04:21:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3583","created_at":"2026-05-18T04:21:13Z"},{"alias_kind":"pith_short_12","alias_value":"KMGFZOMH2Q4Q","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"KMGFZOMH2Q4QLBUU","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"KMGFZOMH","created_at":"2026-05-18T12:26:09Z"}],"graph_snapshots":[{"event_id":"sha256:dff836db289845acde5656a7045e30d026087d1e33aeeba5a46829da2241fabd","target":"graph","created_at":"2026-05-18T04:21:13Z","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":"In the context of Monte Carlo simulations, the analysis of the probability distribution $P_L(m)$ of the order parameter $m$, as obtained in simulation boxes of finite linear extension $L$, allows for an easy estimation of the location of the critical point and the critical exponents. For Ising-like systems without quenched disorder, $P_L(m)$ becomes scale invariant at the critical point, where it assumes a characteristic bimodal shape featuring two overlapping peaks. In particular, the ratio between the value of $P_L(m)$ at the peaks ($P_{L, max}$) and the value at the minimum in-between ($P_{","authors_text":"R. L. C. Vink, T. Fischer","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-10-18T12:55:30Z","title":"Fluids with quenched disorder: Scaling of the free energy barrier near critical points"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3583","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":"sha256:95477e7a3f844900fc948de4b1ed7a8c0e9901dea9c865e2cbca820e2c6bbb1f","target":"record","created_at":"2026-05-18T04:21:13Z","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":"8c4dc4fb53345f8bf41c19c451ea40d7f6f85238a25932f9914fe4cc54fa763a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-10-18T12:55:30Z","title_canon_sha256":"d33a5f70608e74623dc43d6f2876c47834079d540a11cbfb2e0a40f76853976e"},"schema_version":"1.0","source":{"id":"1010.3583","kind":"arxiv","version":1}},"canonical_sha256":"530c5cb987d4390586940d05beadd5113b0e6c487651c8ed92c5e1b35ec536e9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"530c5cb987d4390586940d05beadd5113b0e6c487651c8ed92c5e1b35ec536e9","first_computed_at":"2026-05-18T04:21:13.600868Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:21:13.600868Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"L6oM9I5CERetPt9Zg7QWtjq8OG2z4D9asR6dTIngw++EQ0A4WlQdj7njzESNgRefxnEYz99wVe9d1G/DRksyBA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:21:13.601579Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.3583","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:95477e7a3f844900fc948de4b1ed7a8c0e9901dea9c865e2cbca820e2c6bbb1f","sha256:dff836db289845acde5656a7045e30d026087d1e33aeeba5a46829da2241fabd"],"state_sha256":"9f40d9affd97c7e983770e5a15caef653e15fba3395eeae09f2d1d2133110f91"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"d6faL/Meb2PPdg94LwYnIc00TRaitJu52bFaJ5yxrZ79aTo4/+v78ocqEECurQZLNxG3cJwoSKLmLl20/rWADw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T02:15:25.666216Z","bundle_sha256":"fd3ccf62e277a4bc588929cd16170fc8df62dcd9f0d6b2271e4c3a64c0459a26"}}