{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:IZLEBLZODT4LA6RNY5FQLXKXEI","short_pith_number":"pith:IZLEBLZO","canonical_record":{"source":{"id":"2408.11579","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2024-08-21T12:35:37Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"title_canon_sha256":"3cb528f57c6034a227d92d33b4b68da1f5075fef5557a769cdbc30e1a7929ffb","abstract_canon_sha256":"d6bb8e86f7f9e3e0102e657c6d132bc0fac7e897ab6bf7d64b4d44a47629bb1c"},"schema_version":"1.0"},"canonical_sha256":"465640af2e1cf8b07a2dc74b05dd57223b111a0ea705da50f38a31a60a1619a6","source":{"kind":"arxiv","id":"2408.11579","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.11579","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"arxiv_version","alias_value":"2408.11579v1","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.11579","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"pith_short_12","alias_value":"IZLEBLZODT4L","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"pith_short_16","alias_value":"IZLEBLZODT4LA6RN","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"pith_short_8","alias_value":"IZLEBLZO","created_at":"2026-07-05T08:57:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:IZLEBLZODT4LA6RNY5FQLXKXEI","target":"record","payload":{"canonical_record":{"source":{"id":"2408.11579","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2024-08-21T12:35:37Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"title_canon_sha256":"3cb528f57c6034a227d92d33b4b68da1f5075fef5557a769cdbc30e1a7929ffb","abstract_canon_sha256":"d6bb8e86f7f9e3e0102e657c6d132bc0fac7e897ab6bf7d64b4d44a47629bb1c"},"schema_version":"1.0"},"canonical_sha256":"465640af2e1cf8b07a2dc74b05dd57223b111a0ea705da50f38a31a60a1619a6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:57:45.742786Z","signature_b64":"sMe5PtWeImTho/BZXYmqIEnIbxOLlwqwugWdUw7AnxvXzocZeVEjuZHyI5kEunjgmDeRUYUdfQR47oZ2njlaBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"465640af2e1cf8b07a2dc74b05dd57223b111a0ea705da50f38a31a60a1619a6","last_reissued_at":"2026-07-05T08:57:45.742324Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:57:45.742324Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2408.11579","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":"2026-07-05T08:57:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AQuRnckIBy+Sajmii6TCHhi+aFSUTd/YmCGMij4wP0AeUkZOUcyPYV+nTq9RrO28zLJAs6l9Jsy9/69lAwmGDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T16:42:25.345294Z"},"content_sha256":"18c7ff79b470c9ed0f05ee442196e4d57f51dfbd74ef7bf4f5e05838ede2da78","schema_version":"1.0","event_id":"sha256:18c7ff79b470c9ed0f05ee442196e4d57f51dfbd74ef7bf4f5e05838ede2da78"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:IZLEBLZODT4LA6RNY5FQLXKXEI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dissecting mode-coupling theory for supercooled liquids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"primary_cat":"cond-mat.soft","authors_text":"Ilian Pihlajamaa, Liesbeth M.C. Janssen","submitted_at":"2024-08-21T12:35:37Z","abstract_excerpt":"The mode-coupling theory (MCT) of the glass transition ranks among the most successful first-principles kinetic theories to describe glassy dynamics. However, MCT does not fully account for crucial aspects of the dynamics near the glass transition. To facilitate improving the theory, we critically test the approximations inherent in MCT for a supercooled mixture using Brownian dynamics simulations. Although each MCT approximation significantly impacts the predicted dynamics, our findings show that long-time cancellations of errors occur due to static and dynamic approximations of four-point co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.11579","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2408.11579/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T08:57:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6XbYVy+NFAnzrG1NtFm5xCsJBeegfST+EYJWaWy/F2r+Q+fS9FhLXsGB9jZVQzx3kA6n28kmiV5Uo1gOxGkXBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T16:42:25.345668Z"},"content_sha256":"fd857f04d7b7da9826ae488f99be6fa68a9bdd42bac417f71611a7193f48bcfd","schema_version":"1.0","event_id":"sha256:fd857f04d7b7da9826ae488f99be6fa68a9bdd42bac417f71611a7193f48bcfd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IZLEBLZODT4LA6RNY5FQLXKXEI/bundle.json","state_url":"https://pith.science/pith/IZLEBLZODT4LA6RNY5FQLXKXEI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IZLEBLZODT4LA6RNY5FQLXKXEI/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":"2026-08-03T16:42:25Z","links":{"resolver":"https://pith.science/pith/IZLEBLZODT4LA6RNY5FQLXKXEI","bundle":"https://pith.science/pith/IZLEBLZODT4LA6RNY5FQLXKXEI/bundle.json","state":"https://pith.science/pith/IZLEBLZODT4LA6RNY5FQLXKXEI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IZLEBLZODT4LA6RNY5FQLXKXEI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:IZLEBLZODT4LA6RNY5FQLXKXEI","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":"d6bb8e86f7f9e3e0102e657c6d132bc0fac7e897ab6bf7d64b4d44a47629bb1c","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2024-08-21T12:35:37Z","title_canon_sha256":"3cb528f57c6034a227d92d33b4b68da1f5075fef5557a769cdbc30e1a7929ffb"},"schema_version":"1.0","source":{"id":"2408.11579","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.11579","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"arxiv_version","alias_value":"2408.11579v1","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.11579","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"pith_short_12","alias_value":"IZLEBLZODT4L","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"pith_short_16","alias_value":"IZLEBLZODT4LA6RN","created_at":"2026-07-05T08:57:45Z"},{"alias_kind":"pith_short_8","alias_value":"IZLEBLZO","created_at":"2026-07-05T08:57:45Z"}],"graph_snapshots":[{"event_id":"sha256:fd857f04d7b7da9826ae488f99be6fa68a9bdd42bac417f71611a7193f48bcfd","target":"graph","created_at":"2026-07-05T08:57:45Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2408.11579/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The mode-coupling theory (MCT) of the glass transition ranks among the most successful first-principles kinetic theories to describe glassy dynamics. However, MCT does not fully account for crucial aspects of the dynamics near the glass transition. To facilitate improving the theory, we critically test the approximations inherent in MCT for a supercooled mixture using Brownian dynamics simulations. Although each MCT approximation significantly impacts the predicted dynamics, our findings show that long-time cancellations of errors occur due to static and dynamic approximations of four-point co","authors_text":"Ilian Pihlajamaa, Liesbeth M.C. Janssen","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2024-08-21T12:35:37Z","title":"Dissecting mode-coupling theory for supercooled liquids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.11579","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":"sha256:18c7ff79b470c9ed0f05ee442196e4d57f51dfbd74ef7bf4f5e05838ede2da78","target":"record","created_at":"2026-07-05T08:57:45Z","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":"d6bb8e86f7f9e3e0102e657c6d132bc0fac7e897ab6bf7d64b4d44a47629bb1c","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2024-08-21T12:35:37Z","title_canon_sha256":"3cb528f57c6034a227d92d33b4b68da1f5075fef5557a769cdbc30e1a7929ffb"},"schema_version":"1.0","source":{"id":"2408.11579","kind":"arxiv","version":1}},"canonical_sha256":"465640af2e1cf8b07a2dc74b05dd57223b111a0ea705da50f38a31a60a1619a6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"465640af2e1cf8b07a2dc74b05dd57223b111a0ea705da50f38a31a60a1619a6","first_computed_at":"2026-07-05T08:57:45.742324Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:57:45.742324Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sMe5PtWeImTho/BZXYmqIEnIbxOLlwqwugWdUw7AnxvXzocZeVEjuZHyI5kEunjgmDeRUYUdfQR47oZ2njlaBw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:57:45.742786Z","signed_message":"canonical_sha256_bytes"},"source_id":"2408.11579","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:18c7ff79b470c9ed0f05ee442196e4d57f51dfbd74ef7bf4f5e05838ede2da78","sha256:fd857f04d7b7da9826ae488f99be6fa68a9bdd42bac417f71611a7193f48bcfd"],"state_sha256":"e63cc5b15c3f5171a3dddc13582c944da81176608fd63cd5b652192b8ff66a8e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3wvsdhJs/IFESD5xryzSaUmJTdaV0eb9ZOF7qr+KD9fkw6gtJMcgdzJ0bc99QPt8c18iBTl7cKdTnK52NkZtDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T16:42:25.347928Z","bundle_sha256":"6a1960258c3acc82017645adb2e4f469ba9c4e5975cac138c6927fb368beae15"}}