{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:I3TUZK47XM6D6W5LVNXX6PCFHI","short_pith_number":"pith:I3TUZK47","canonical_record":{"source":{"id":"1211.1027","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-11-05T21:00:19Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"1c112128f8c582dfe3deef174e412f2000994078510b3ffd82f9fac853e524bf","abstract_canon_sha256":"3177486ec2833126f6c7568ab38c59c51182d08ecb0079c884e945e85d84efd8"},"schema_version":"1.0"},"canonical_sha256":"46e74cab9fbb3c3f5babab6f7f3c453a397fdbec3207e634f56e419523c6f04a","source":{"kind":"arxiv","id":"1211.1027","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.1027","created_at":"2026-05-18T03:41:28Z"},{"alias_kind":"arxiv_version","alias_value":"1211.1027v1","created_at":"2026-05-18T03:41:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.1027","created_at":"2026-05-18T03:41:28Z"},{"alias_kind":"pith_short_12","alias_value":"I3TUZK47XM6D","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_16","alias_value":"I3TUZK47XM6D6W5L","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_8","alias_value":"I3TUZK47","created_at":"2026-05-18T12:27:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:I3TUZK47XM6D6W5LVNXX6PCFHI","target":"record","payload":{"canonical_record":{"source":{"id":"1211.1027","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-11-05T21:00:19Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"1c112128f8c582dfe3deef174e412f2000994078510b3ffd82f9fac853e524bf","abstract_canon_sha256":"3177486ec2833126f6c7568ab38c59c51182d08ecb0079c884e945e85d84efd8"},"schema_version":"1.0"},"canonical_sha256":"46e74cab9fbb3c3f5babab6f7f3c453a397fdbec3207e634f56e419523c6f04a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:41:28.754816Z","signature_b64":"5QqZPs9vK3opdib1lUOPX/b9wbwLL49P8FaeNbK5Ynx5ol/trpAjEf0J+7yy8p/jWibr4GyH/G6ZCwxHksPMAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"46e74cab9fbb3c3f5babab6f7f3c453a397fdbec3207e634f56e419523c6f04a","last_reissued_at":"2026-05-18T03:41:28.753981Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:41:28.753981Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1211.1027","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":"2026-05-18T03:41:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AKOinF5wp1eoofaUcmW0cKDBXCjxu9HhlZNGimpWYqV+IganAcYoMeriuPe2dWX1eBjYM0e5GTJrZoSZkeQYDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-23T23:51:23.968934Z"},"content_sha256":"2eb88ef60fa76012d8481be50b1a5fde71b4819e69e07c1957dcfd74b10a5a5c","schema_version":"1.0","event_id":"sha256:2eb88ef60fa76012d8481be50b1a5fde71b4819e69e07c1957dcfd74b10a5a5c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:I3TUZK47XM6D6W5LVNXX6PCFHI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Critical exponents of colloid particles in bulk and confinement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Helge Neitsch, Sabine H.L. Klapp","submitted_at":"2012-11-05T21:00:19Z","abstract_excerpt":"Using grand canonical Monte Carlo simulations, we investigate the percolation behavior of a square well fluid with an ultra-short range of attraction in three dimension (3D) and in confined geometry. The latter is defined through two parallel and structureless walls (slit-pore). We focus on temperatures above the critical temperature of the (metastable) condensation transition of the 3D system. Investigating a broad range of systems sizes, we first determine the percolation thresholds, i. e., the critical packing fraction for percolation $\\eta_{c}$. For the slit-pore systems, $\\eta_{c}$ is fou"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.1027","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":"2026-05-18T03:41:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"M8ZY1qdjKlETQv99d7DlY0dD/kwLovkXQyZL0oORTdI8qPEhX2Cg3rtAhzhrU0QTgVVKs8vGpx22YAUUS/7VAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-23T23:51:23.969280Z"},"content_sha256":"cff9b08f3439063a074fb4aa7686cc1ccc9c4daa56f46cc71ed98cec4de372b8","schema_version":"1.0","event_id":"sha256:cff9b08f3439063a074fb4aa7686cc1ccc9c4daa56f46cc71ed98cec4de372b8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/I3TUZK47XM6D6W5LVNXX6PCFHI/bundle.json","state_url":"https://pith.science/pith/I3TUZK47XM6D6W5LVNXX6PCFHI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/I3TUZK47XM6D6W5LVNXX6PCFHI/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":"2026-06-23T23:51:23Z","links":{"resolver":"https://pith.science/pith/I3TUZK47XM6D6W5LVNXX6PCFHI","bundle":"https://pith.science/pith/I3TUZK47XM6D6W5LVNXX6PCFHI/bundle.json","state":"https://pith.science/pith/I3TUZK47XM6D6W5LVNXX6PCFHI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/I3TUZK47XM6D6W5LVNXX6PCFHI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:I3TUZK47XM6D6W5LVNXX6PCFHI","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":"3177486ec2833126f6c7568ab38c59c51182d08ecb0079c884e945e85d84efd8","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-11-05T21:00:19Z","title_canon_sha256":"1c112128f8c582dfe3deef174e412f2000994078510b3ffd82f9fac853e524bf"},"schema_version":"1.0","source":{"id":"1211.1027","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.1027","created_at":"2026-05-18T03:41:28Z"},{"alias_kind":"arxiv_version","alias_value":"1211.1027v1","created_at":"2026-05-18T03:41:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.1027","created_at":"2026-05-18T03:41:28Z"},{"alias_kind":"pith_short_12","alias_value":"I3TUZK47XM6D","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_16","alias_value":"I3TUZK47XM6D6W5L","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_8","alias_value":"I3TUZK47","created_at":"2026-05-18T12:27:09Z"}],"graph_snapshots":[{"event_id":"sha256:cff9b08f3439063a074fb4aa7686cc1ccc9c4daa56f46cc71ed98cec4de372b8","target":"graph","created_at":"2026-05-18T03:41:28Z","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":"Using grand canonical Monte Carlo simulations, we investigate the percolation behavior of a square well fluid with an ultra-short range of attraction in three dimension (3D) and in confined geometry. The latter is defined through two parallel and structureless walls (slit-pore). We focus on temperatures above the critical temperature of the (metastable) condensation transition of the 3D system. Investigating a broad range of systems sizes, we first determine the percolation thresholds, i. e., the critical packing fraction for percolation $\\eta_{c}$. For the slit-pore systems, $\\eta_{c}$ is fou","authors_text":"Helge Neitsch, Sabine H.L. Klapp","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-11-05T21:00:19Z","title":"Critical exponents of colloid particles in bulk and confinement"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.1027","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":"sha256:2eb88ef60fa76012d8481be50b1a5fde71b4819e69e07c1957dcfd74b10a5a5c","target":"record","created_at":"2026-05-18T03:41:28Z","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":"3177486ec2833126f6c7568ab38c59c51182d08ecb0079c884e945e85d84efd8","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-11-05T21:00:19Z","title_canon_sha256":"1c112128f8c582dfe3deef174e412f2000994078510b3ffd82f9fac853e524bf"},"schema_version":"1.0","source":{"id":"1211.1027","kind":"arxiv","version":1}},"canonical_sha256":"46e74cab9fbb3c3f5babab6f7f3c453a397fdbec3207e634f56e419523c6f04a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"46e74cab9fbb3c3f5babab6f7f3c453a397fdbec3207e634f56e419523c6f04a","first_computed_at":"2026-05-18T03:41:28.753981Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:41:28.753981Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5QqZPs9vK3opdib1lUOPX/b9wbwLL49P8FaeNbK5Ynx5ol/trpAjEf0J+7yy8p/jWibr4GyH/G6ZCwxHksPMAg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:41:28.754816Z","signed_message":"canonical_sha256_bytes"},"source_id":"1211.1027","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2eb88ef60fa76012d8481be50b1a5fde71b4819e69e07c1957dcfd74b10a5a5c","sha256:cff9b08f3439063a074fb4aa7686cc1ccc9c4daa56f46cc71ed98cec4de372b8"],"state_sha256":"04a70634cb7cbe2adc2b7e07a4cbe4437905aaa7696e4458a266bbdb48884e95"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SIkhB6SIFtIZZChCO3AKzWqT6q6EO9J3ppry090hHvCaecLIfIaI+lrawgtS2nURaOLglj4T+v9v0JO3OcTdAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-23T23:51:23.971265Z","bundle_sha256":"ff1503e3aa6ccc3212cc9faf8f0a49c465eeb27b9140188cf60f738db14cea43"}}