{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:DPVPUPALQ7KXOEN5IUDUY4PS45","short_pith_number":"pith:DPVPUPAL","canonical_record":{"source":{"id":"1411.0982","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-11-04T17:44:52Z","cross_cats_sorted":[],"title_canon_sha256":"e532964331fffbcf06745a11b5436ccfde149e536c6082738baef6257e5d9051","abstract_canon_sha256":"25ebf095414852fc734efdfa82854ec3d5c712f8af7f8c95f0c800795bfcfb69"},"schema_version":"1.0"},"canonical_sha256":"1beafa3c0b87d57711bd45074c71f2e75a2bf230d1b27475596ef611e1706943","source":{"kind":"arxiv","id":"1411.0982","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.0982","created_at":"2026-05-18T01:35:32Z"},{"alias_kind":"arxiv_version","alias_value":"1411.0982v1","created_at":"2026-05-18T01:35:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.0982","created_at":"2026-05-18T01:35:32Z"},{"alias_kind":"pith_short_12","alias_value":"DPVPUPALQ7KX","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DPVPUPALQ7KXOEN5","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DPVPUPAL","created_at":"2026-05-18T12:28:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:DPVPUPALQ7KXOEN5IUDUY4PS45","target":"record","payload":{"canonical_record":{"source":{"id":"1411.0982","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-11-04T17:44:52Z","cross_cats_sorted":[],"title_canon_sha256":"e532964331fffbcf06745a11b5436ccfde149e536c6082738baef6257e5d9051","abstract_canon_sha256":"25ebf095414852fc734efdfa82854ec3d5c712f8af7f8c95f0c800795bfcfb69"},"schema_version":"1.0"},"canonical_sha256":"1beafa3c0b87d57711bd45074c71f2e75a2bf230d1b27475596ef611e1706943","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:35:32.720791Z","signature_b64":"m18jYT0tI8xskGiarL2ruskY48DbRRSEp9bd4dTwKeiGTPx9NH1FqYS0/Jgi90w95hayGOU+j4cQ54I3/dFADw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1beafa3c0b87d57711bd45074c71f2e75a2bf230d1b27475596ef611e1706943","last_reissued_at":"2026-05-18T01:35:32.720176Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:35:32.720176Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1411.0982","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":"2026-05-18T01:35:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vP5eaZQhes0FPacxlSrwJC1nEZ1+YKAKp+2LeRLYDeVLUukSLAA0SCyx8OXrF0jjLiObHXf0mflS9HSSmZLQAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T02:04:34.417609Z"},"content_sha256":"5893b25a860660f41627f8243192411188f8441711de26878ea38e6f07db9186","schema_version":"1.0","event_id":"sha256:5893b25a860660f41627f8243192411188f8441711de26878ea38e6f07db9186"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:DPVPUPALQ7KXOEN5IUDUY4PS45","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A numerical study of longtime dynamics and ergodic-nonergodic transitions in dense simple fluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"David D. McCowan","submitted_at":"2014-11-04T17:44:52Z","abstract_excerpt":"For over 30 years, mode-coupling theory (MCT) has been the de facto theoretic description of dense fluids and the liquid-glass transition. MCT, however, is limited by its ad hoc construction and lacks a mechanism to institute corrections. We use recent results from a new theoretical framework--developed from first principles via a self-consistent perturbation expansion in terms of an effective two-body potential--to numerically explore the kinetics of systems of classical particles, specifically hard spheres obeying Smoluchowski dynamics. We present here a full solution to the kinetic equation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.0982","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":"2026-05-18T01:35:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2WnFvrW3mexifXigf4pdWqpkNUKe+A/N3YDWIwINLn9TVTa/QM1mHDZ1mzaguNG9FYexBpt43E2e/4yjPXAhDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T02:04:34.417944Z"},"content_sha256":"8450f9973c694dfff4668f748f154dddadea8e30c77198f81e2e37f7fed92dc9","schema_version":"1.0","event_id":"sha256:8450f9973c694dfff4668f748f154dddadea8e30c77198f81e2e37f7fed92dc9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DPVPUPALQ7KXOEN5IUDUY4PS45/bundle.json","state_url":"https://pith.science/pith/DPVPUPALQ7KXOEN5IUDUY4PS45/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DPVPUPALQ7KXOEN5IUDUY4PS45/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":"2026-06-27T02:04:34Z","links":{"resolver":"https://pith.science/pith/DPVPUPALQ7KXOEN5IUDUY4PS45","bundle":"https://pith.science/pith/DPVPUPALQ7KXOEN5IUDUY4PS45/bundle.json","state":"https://pith.science/pith/DPVPUPALQ7KXOEN5IUDUY4PS45/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DPVPUPALQ7KXOEN5IUDUY4PS45/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:DPVPUPALQ7KXOEN5IUDUY4PS45","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":"25ebf095414852fc734efdfa82854ec3d5c712f8af7f8c95f0c800795bfcfb69","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-11-04T17:44:52Z","title_canon_sha256":"e532964331fffbcf06745a11b5436ccfde149e536c6082738baef6257e5d9051"},"schema_version":"1.0","source":{"id":"1411.0982","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.0982","created_at":"2026-05-18T01:35:32Z"},{"alias_kind":"arxiv_version","alias_value":"1411.0982v1","created_at":"2026-05-18T01:35:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.0982","created_at":"2026-05-18T01:35:32Z"},{"alias_kind":"pith_short_12","alias_value":"DPVPUPALQ7KX","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DPVPUPALQ7KXOEN5","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DPVPUPAL","created_at":"2026-05-18T12:28:25Z"}],"graph_snapshots":[{"event_id":"sha256:8450f9973c694dfff4668f748f154dddadea8e30c77198f81e2e37f7fed92dc9","target":"graph","created_at":"2026-05-18T01:35:32Z","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":"For over 30 years, mode-coupling theory (MCT) has been the de facto theoretic description of dense fluids and the liquid-glass transition. MCT, however, is limited by its ad hoc construction and lacks a mechanism to institute corrections. We use recent results from a new theoretical framework--developed from first principles via a self-consistent perturbation expansion in terms of an effective two-body potential--to numerically explore the kinetics of systems of classical particles, specifically hard spheres obeying Smoluchowski dynamics. We present here a full solution to the kinetic equation","authors_text":"David D. McCowan","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-11-04T17:44:52Z","title":"A numerical study of longtime dynamics and ergodic-nonergodic transitions in dense simple fluids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.0982","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":"sha256:5893b25a860660f41627f8243192411188f8441711de26878ea38e6f07db9186","target":"record","created_at":"2026-05-18T01:35:32Z","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":"25ebf095414852fc734efdfa82854ec3d5c712f8af7f8c95f0c800795bfcfb69","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-11-04T17:44:52Z","title_canon_sha256":"e532964331fffbcf06745a11b5436ccfde149e536c6082738baef6257e5d9051"},"schema_version":"1.0","source":{"id":"1411.0982","kind":"arxiv","version":1}},"canonical_sha256":"1beafa3c0b87d57711bd45074c71f2e75a2bf230d1b27475596ef611e1706943","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1beafa3c0b87d57711bd45074c71f2e75a2bf230d1b27475596ef611e1706943","first_computed_at":"2026-05-18T01:35:32.720176Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:35:32.720176Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m18jYT0tI8xskGiarL2ruskY48DbRRSEp9bd4dTwKeiGTPx9NH1FqYS0/Jgi90w95hayGOU+j4cQ54I3/dFADw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:35:32.720791Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.0982","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5893b25a860660f41627f8243192411188f8441711de26878ea38e6f07db9186","sha256:8450f9973c694dfff4668f748f154dddadea8e30c77198f81e2e37f7fed92dc9"],"state_sha256":"519d04ffeca22fc686920306f2df59c3acce75ae074c6c040a9ae8fc7d7359e8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"np8aTHG5IRD3wDbf3T7EJ17We+ueBOSp9c2afk0emXt3VaEuuXjSiQRwtx9QyN8bSB8J4bCHCpLaiQ4JzaYDAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T02:04:34.420013Z","bundle_sha256":"b40482f5cef9f9431a3cf7ccac8cbd7e1ce2c5779fae2c190a7898e2902ef766"}}