{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:WESMQI5YQVKUT64L33AXUPPJXX","short_pith_number":"pith:WESMQI5Y","canonical_record":{"source":{"id":"cond-mat/0610253","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2006-10-10T06:07:45Z","cross_cats_sorted":[],"title_canon_sha256":"c0287f690736b0e6e991ce311685f35b3b75fcfbfe3ff144607feb1a92052632","abstract_canon_sha256":"ade4f2dc709f6803a93a37012a4a531ffff6857dfed6b32464f97ef1cf5c3132"},"schema_version":"1.0"},"canonical_sha256":"b124c823b8855549fb8bdec17a3de9bdecc459b0f569fbee16bca0136a468c78","source":{"kind":"arxiv","id":"cond-mat/0610253","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0610253","created_at":"2026-05-18T01:39:42Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0610253v1","created_at":"2026-05-18T01:39:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0610253","created_at":"2026-05-18T01:39:42Z"},{"alias_kind":"pith_short_12","alias_value":"WESMQI5YQVKU","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_16","alias_value":"WESMQI5YQVKUT64L","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_8","alias_value":"WESMQI5Y","created_at":"2026-05-18T12:25:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:WESMQI5YQVKUT64L33AXUPPJXX","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0610253","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2006-10-10T06:07:45Z","cross_cats_sorted":[],"title_canon_sha256":"c0287f690736b0e6e991ce311685f35b3b75fcfbfe3ff144607feb1a92052632","abstract_canon_sha256":"ade4f2dc709f6803a93a37012a4a531ffff6857dfed6b32464f97ef1cf5c3132"},"schema_version":"1.0"},"canonical_sha256":"b124c823b8855549fb8bdec17a3de9bdecc459b0f569fbee16bca0136a468c78","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:42.589281Z","signature_b64":"nnS/SVLBL035ZK1UuNlkkoRge7rEtVV2uSAI3ei2jBGYZ2BLz9aTwzwebmlWD8MuTk8qlyr+co7XBpaRpibnDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b124c823b8855549fb8bdec17a3de9bdecc459b0f569fbee16bca0136a468c78","last_reissued_at":"2026-05-18T01:39:42.588736Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:42.588736Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0610253","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":"2026-05-18T01:39:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B/rS8OvW2q+2uGFp3ivUecmVWAo0Ok/iaWvS27gf4NoFeW/J49kFlBpoCZ+QUeWjEsOd1aiExgYDcpZfHMRxCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T18:15:08.689072Z"},"content_sha256":"c50cb66371049a15103b4cb74e4d7aef08a9867f4a6290a5cfb1feba0f4771ab","schema_version":"1.0","event_id":"sha256:c50cb66371049a15103b4cb74e4d7aef08a9867f4a6290a5cfb1feba0f4771ab"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:WESMQI5YQVKUT64L33AXUPPJXX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Monte-Carlo dynamics of a binary Lennard-Jones glass-forming mixture","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Ludovic Berthier, Walter Kob","submitted_at":"2006-10-10T06:07:45Z","abstract_excerpt":"We use a standard Monte-Carlo algorithm to study the slow dynamics of a binary Lennard-Jones glass-forming mixture at low temperature. We find that Monte-Carlo is by far the most efficient way to simulate a stochastic dynamics since relaxation is about 10 times faster than in Brownian Dynamics and about 30 times faster than in Stochastic Dynamics. Moreover, the average dynamical behaviour of the system is in quantitative agreement with the one obtained using Newtonian dynamics, apart at very short times where thermal vibrations are suppressed. We show, however, that dynamic fluctuations quanti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0610253","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":"2026-05-18T01:39:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0v9MSYXLRWZXiZ4ds6FdrngyKXWOWxmcSdZ0iv54zseZS2ZgC+28kGmAIKebywy8TnUAPlmCnIHJkYRW83OVAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T18:15:08.689828Z"},"content_sha256":"23236880bd539a6cd94d375defb97d582ad87651e085303fa669c4f0173f4acd","schema_version":"1.0","event_id":"sha256:23236880bd539a6cd94d375defb97d582ad87651e085303fa669c4f0173f4acd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WESMQI5YQVKUT64L33AXUPPJXX/bundle.json","state_url":"https://pith.science/pith/WESMQI5YQVKUT64L33AXUPPJXX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WESMQI5YQVKUT64L33AXUPPJXX/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":"2026-05-31T18:15:08Z","links":{"resolver":"https://pith.science/pith/WESMQI5YQVKUT64L33AXUPPJXX","bundle":"https://pith.science/pith/WESMQI5YQVKUT64L33AXUPPJXX/bundle.json","state":"https://pith.science/pith/WESMQI5YQVKUT64L33AXUPPJXX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WESMQI5YQVKUT64L33AXUPPJXX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:WESMQI5YQVKUT64L33AXUPPJXX","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":"ade4f2dc709f6803a93a37012a4a531ffff6857dfed6b32464f97ef1cf5c3132","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2006-10-10T06:07:45Z","title_canon_sha256":"c0287f690736b0e6e991ce311685f35b3b75fcfbfe3ff144607feb1a92052632"},"schema_version":"1.0","source":{"id":"cond-mat/0610253","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0610253","created_at":"2026-05-18T01:39:42Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0610253v1","created_at":"2026-05-18T01:39:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0610253","created_at":"2026-05-18T01:39:42Z"},{"alias_kind":"pith_short_12","alias_value":"WESMQI5YQVKU","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_16","alias_value":"WESMQI5YQVKUT64L","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_8","alias_value":"WESMQI5Y","created_at":"2026-05-18T12:25:54Z"}],"graph_snapshots":[{"event_id":"sha256:23236880bd539a6cd94d375defb97d582ad87651e085303fa669c4f0173f4acd","target":"graph","created_at":"2026-05-18T01:39:42Z","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 use a standard Monte-Carlo algorithm to study the slow dynamics of a binary Lennard-Jones glass-forming mixture at low temperature. We find that Monte-Carlo is by far the most efficient way to simulate a stochastic dynamics since relaxation is about 10 times faster than in Brownian Dynamics and about 30 times faster than in Stochastic Dynamics. Moreover, the average dynamical behaviour of the system is in quantitative agreement with the one obtained using Newtonian dynamics, apart at very short times where thermal vibrations are suppressed. We show, however, that dynamic fluctuations quanti","authors_text":"Ludovic Berthier, Walter Kob","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2006-10-10T06:07:45Z","title":"The Monte-Carlo dynamics of a binary Lennard-Jones glass-forming mixture"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0610253","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:c50cb66371049a15103b4cb74e4d7aef08a9867f4a6290a5cfb1feba0f4771ab","target":"record","created_at":"2026-05-18T01:39:42Z","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":"ade4f2dc709f6803a93a37012a4a531ffff6857dfed6b32464f97ef1cf5c3132","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2006-10-10T06:07:45Z","title_canon_sha256":"c0287f690736b0e6e991ce311685f35b3b75fcfbfe3ff144607feb1a92052632"},"schema_version":"1.0","source":{"id":"cond-mat/0610253","kind":"arxiv","version":1}},"canonical_sha256":"b124c823b8855549fb8bdec17a3de9bdecc459b0f569fbee16bca0136a468c78","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b124c823b8855549fb8bdec17a3de9bdecc459b0f569fbee16bca0136a468c78","first_computed_at":"2026-05-18T01:39:42.588736Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:42.588736Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nnS/SVLBL035ZK1UuNlkkoRge7rEtVV2uSAI3ei2jBGYZ2BLz9aTwzwebmlWD8MuTk8qlyr+co7XBpaRpibnDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:42.589281Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0610253","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c50cb66371049a15103b4cb74e4d7aef08a9867f4a6290a5cfb1feba0f4771ab","sha256:23236880bd539a6cd94d375defb97d582ad87651e085303fa669c4f0173f4acd"],"state_sha256":"40c59b6e851337459d77e95c2e7be5b5525701cb197ae51e83b6232d7cd07f01"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"srgiciWDUK5S3p9DQS063ddxM6632Jp2R1xvpEZi8s1KS8Jjm710cGMCjpylVX65huoSA7LvLwXNhM1dLioADA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T18:15:08.693824Z","bundle_sha256":"be8b4a509b6a544b8f82735dabeb07ce181633d23847708cd118815c59c9041d"}}