{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:RHMHM33QLOBP2ODFJEFCJUHI2W","short_pith_number":"pith:RHMHM33Q","canonical_record":{"source":{"id":"1005.0914","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-05-06T07:51:02Z","cross_cats_sorted":[],"title_canon_sha256":"31dda6354a0e4f6501dbeeca4a7d8b42fb03fbb7c4ebe5f70695c3b32a48f340","abstract_canon_sha256":"4a151e5e94abfece29a77f2f76a108fa2433fbcea6620a58dfcaaa9b52b76452"},"schema_version":"1.0"},"canonical_sha256":"89d8766f705b82fd3865490a24d0e8d5bd0d427ae3f1686fd0edb626ea86e80f","source":{"kind":"arxiv","id":"1005.0914","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1005.0914","created_at":"2026-05-18T04:40:08Z"},{"alias_kind":"arxiv_version","alias_value":"1005.0914v1","created_at":"2026-05-18T04:40:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.0914","created_at":"2026-05-18T04:40:08Z"},{"alias_kind":"pith_short_12","alias_value":"RHMHM33QLOBP","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_16","alias_value":"RHMHM33QLOBP2ODF","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_8","alias_value":"RHMHM33Q","created_at":"2026-05-18T12:26:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:RHMHM33QLOBP2ODFJEFCJUHI2W","target":"record","payload":{"canonical_record":{"source":{"id":"1005.0914","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-05-06T07:51:02Z","cross_cats_sorted":[],"title_canon_sha256":"31dda6354a0e4f6501dbeeca4a7d8b42fb03fbb7c4ebe5f70695c3b32a48f340","abstract_canon_sha256":"4a151e5e94abfece29a77f2f76a108fa2433fbcea6620a58dfcaaa9b52b76452"},"schema_version":"1.0"},"canonical_sha256":"89d8766f705b82fd3865490a24d0e8d5bd0d427ae3f1686fd0edb626ea86e80f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:40:08.249639Z","signature_b64":"BWd/M7TboAqSXNduAAzdn88ZddeDlCTWsPfVIaEVpdrfEHcOuUS69eEgFrY5G3dSgYFMh3fCBz/pltTilPZUCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89d8766f705b82fd3865490a24d0e8d5bd0d427ae3f1686fd0edb626ea86e80f","last_reissued_at":"2026-05-18T04:40:08.249220Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:40:08.249220Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1005.0914","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":"2026-05-18T04:40:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SjjZKmfzErhGPcjFVlrLQYDKxEyvWFW4ohg9486+aFDEUU9DtisUEQGAobh6Qd+bnToR3heXfliEw5wPo9dPBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T21:23:33.293261Z"},"content_sha256":"13cb8fc2630fea928673a6aad28d403182c16da63ae099dfab5e6d14a09c6325","schema_version":"1.0","event_id":"sha256:13cb8fc2630fea928673a6aad28d403182c16da63ae099dfab5e6d14a09c6325"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:RHMHM33QLOBP2ODFJEFCJUHI2W","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A critical test of the mode-coupling theory of the glass transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Gilles Tarjus, Ludovic Berthier","submitted_at":"2010-05-06T07:51:02Z","abstract_excerpt":"The mode-coupling theory of the glass transition predicts the time evolution of the intermediate scattering functions in viscous liquids on the sole basis of the structural information encoded in two-point density correlations. We provide a critical test of this property and show that the theory fails to describe the qualitatively distinct dynamical behavior obtained in two model liquids characterized by very similar pair correlation functions. Because we use `exact' static information provided by numerical simulations, our results are a direct proof that some important information about the d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.0914","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":"2026-05-18T04:40:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HZsxgU3hj9K7a93wf3RXZRnLx02LIZYIBJv77ty6icjAD7rryIP7ZgokTxVhL5LoEhHLqpgqxgpDabyhZNF4AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T21:23:33.293643Z"},"content_sha256":"e21ea3dee987309716bba5b5ceeec55722358ca32e9e6fa2d108cfaf8c4c65d3","schema_version":"1.0","event_id":"sha256:e21ea3dee987309716bba5b5ceeec55722358ca32e9e6fa2d108cfaf8c4c65d3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RHMHM33QLOBP2ODFJEFCJUHI2W/bundle.json","state_url":"https://pith.science/pith/RHMHM33QLOBP2ODFJEFCJUHI2W/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RHMHM33QLOBP2ODFJEFCJUHI2W/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":"2026-05-31T21:23:33Z","links":{"resolver":"https://pith.science/pith/RHMHM33QLOBP2ODFJEFCJUHI2W","bundle":"https://pith.science/pith/RHMHM33QLOBP2ODFJEFCJUHI2W/bundle.json","state":"https://pith.science/pith/RHMHM33QLOBP2ODFJEFCJUHI2W/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RHMHM33QLOBP2ODFJEFCJUHI2W/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:RHMHM33QLOBP2ODFJEFCJUHI2W","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":"4a151e5e94abfece29a77f2f76a108fa2433fbcea6620a58dfcaaa9b52b76452","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-05-06T07:51:02Z","title_canon_sha256":"31dda6354a0e4f6501dbeeca4a7d8b42fb03fbb7c4ebe5f70695c3b32a48f340"},"schema_version":"1.0","source":{"id":"1005.0914","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1005.0914","created_at":"2026-05-18T04:40:08Z"},{"alias_kind":"arxiv_version","alias_value":"1005.0914v1","created_at":"2026-05-18T04:40:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.0914","created_at":"2026-05-18T04:40:08Z"},{"alias_kind":"pith_short_12","alias_value":"RHMHM33QLOBP","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_16","alias_value":"RHMHM33QLOBP2ODF","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_8","alias_value":"RHMHM33Q","created_at":"2026-05-18T12:26:13Z"}],"graph_snapshots":[{"event_id":"sha256:e21ea3dee987309716bba5b5ceeec55722358ca32e9e6fa2d108cfaf8c4c65d3","target":"graph","created_at":"2026-05-18T04:40:08Z","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":"The mode-coupling theory of the glass transition predicts the time evolution of the intermediate scattering functions in viscous liquids on the sole basis of the structural information encoded in two-point density correlations. We provide a critical test of this property and show that the theory fails to describe the qualitatively distinct dynamical behavior obtained in two model liquids characterized by very similar pair correlation functions. Because we use `exact' static information provided by numerical simulations, our results are a direct proof that some important information about the d","authors_text":"Gilles Tarjus, Ludovic Berthier","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-05-06T07:51:02Z","title":"A critical test of the mode-coupling theory of the glass transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.0914","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":"sha256:13cb8fc2630fea928673a6aad28d403182c16da63ae099dfab5e6d14a09c6325","target":"record","created_at":"2026-05-18T04:40:08Z","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":"4a151e5e94abfece29a77f2f76a108fa2433fbcea6620a58dfcaaa9b52b76452","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-05-06T07:51:02Z","title_canon_sha256":"31dda6354a0e4f6501dbeeca4a7d8b42fb03fbb7c4ebe5f70695c3b32a48f340"},"schema_version":"1.0","source":{"id":"1005.0914","kind":"arxiv","version":1}},"canonical_sha256":"89d8766f705b82fd3865490a24d0e8d5bd0d427ae3f1686fd0edb626ea86e80f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"89d8766f705b82fd3865490a24d0e8d5bd0d427ae3f1686fd0edb626ea86e80f","first_computed_at":"2026-05-18T04:40:08.249220Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:40:08.249220Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BWd/M7TboAqSXNduAAzdn88ZddeDlCTWsPfVIaEVpdrfEHcOuUS69eEgFrY5G3dSgYFMh3fCBz/pltTilPZUCw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:40:08.249639Z","signed_message":"canonical_sha256_bytes"},"source_id":"1005.0914","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:13cb8fc2630fea928673a6aad28d403182c16da63ae099dfab5e6d14a09c6325","sha256:e21ea3dee987309716bba5b5ceeec55722358ca32e9e6fa2d108cfaf8c4c65d3"],"state_sha256":"d0c6a5ce60e1d24c5dd702e72836b153a35327255b43fac1b6a26195dfac932a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O+e1GWiYuY1fX+41dUn17R189H+TUGoJ25Om4dyxAbPV4C1CVyByXtbzkEAUxAOljvndWo6vGaz7xlNNuHOJBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T21:23:33.295625Z","bundle_sha256":"d8c13d1d1284c48a2c755e92ca8b95d9ac395a7abc2f30acb5f4f762bccd4ca3"}}