{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:RCDMPUXO4Y7XEJNJJMNDFOFDC2","short_pith_number":"pith:RCDMPUXO","canonical_record":{"source":{"id":"1412.5017","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-12-15T16:01:16Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"9cffbd28eb2010af30d977035f757f675f4b5bbd7c2c7d58f741adf26a4f8efe","abstract_canon_sha256":"0c4cf3588c6e78c0825195edcfe1310bf32ac338713d139b6853bac9cd674812"},"schema_version":"1.0"},"canonical_sha256":"8886c7d2eee63f7225a94b1a32b8a3168559d7e2b7fcf799f24e8dd4526ff5e9","source":{"kind":"arxiv","id":"1412.5017","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5017","created_at":"2026-05-18T02:31:09Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5017v1","created_at":"2026-05-18T02:31:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5017","created_at":"2026-05-18T02:31:09Z"},{"alias_kind":"pith_short_12","alias_value":"RCDMPUXO4Y7X","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RCDMPUXO4Y7XEJNJ","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RCDMPUXO","created_at":"2026-05-18T12:28:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:RCDMPUXO4Y7XEJNJJMNDFOFDC2","target":"record","payload":{"canonical_record":{"source":{"id":"1412.5017","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-12-15T16:01:16Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"9cffbd28eb2010af30d977035f757f675f4b5bbd7c2c7d58f741adf26a4f8efe","abstract_canon_sha256":"0c4cf3588c6e78c0825195edcfe1310bf32ac338713d139b6853bac9cd674812"},"schema_version":"1.0"},"canonical_sha256":"8886c7d2eee63f7225a94b1a32b8a3168559d7e2b7fcf799f24e8dd4526ff5e9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:31:09.834303Z","signature_b64":"eZgn01PiLc9Cr+DZIV3xd9Aq/wKbS5OmPAff1T50M1N/HU0vfPuUL7fhu2YC1SlN1yioDwiQj0GMNLtozJa9Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8886c7d2eee63f7225a94b1a32b8a3168559d7e2b7fcf799f24e8dd4526ff5e9","last_reissued_at":"2026-05-18T02:31:09.833623Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:31:09.833623Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.5017","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":"2026-05-18T02:31:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xpJJJgc+v9bp2S5AtKKeTVKri/Ngqsj8eWcDWC3x1xMIDfuuUQsnZ7NzeWR5k3J0BGfJ35bbNmnZTEY+xGYuAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T23:20:00.488162Z"},"content_sha256":"54af94da6447e0280b3cf1d1f53eaaea7c2e27e0e076211be2060405333a1f85","schema_version":"1.0","event_id":"sha256:54af94da6447e0280b3cf1d1f53eaaea7c2e27e0e076211be2060405333a1f85"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:RCDMPUXO4Y7XEJNJJMNDFOFDC2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Random First Order Theory concepts in Biology and Condensed Matter physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"D. Thirumalai, T. R. Kirkpatrick","submitted_at":"2014-12-15T16:01:16Z","abstract_excerpt":"The routine transformation of a liquid, as it is cooled rapidly, resulting in glass formation, is remarkably complex. A theoretical explanation of the dynamics associated with this process has remained one of the major unsolved problems in condensed matter physics. The Random First Order Transition (RFOT) theory, which was proposed over twenty five years ago, provides a theoretical basis for explaining much of the phenomena associated with glass forming materials. It links or relates multiple metastable states, slow or glassy dynamics, dynamic heterogeneity, and both a dynamical and an ideal g"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5017","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":"2026-05-18T02:31:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JV4EaiLZAxP967lGodAS4b3N82N5VdPXz+pbqIh7QiHYZdZUxTp10WyyUHWISAPlSgjGzZMnfBpA74nHmgO0DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T23:20:00.488573Z"},"content_sha256":"5d1a8246103ba1d2fd4d4afdf6de04533c33529b402cb0575cad8e313e657ee8","schema_version":"1.0","event_id":"sha256:5d1a8246103ba1d2fd4d4afdf6de04533c33529b402cb0575cad8e313e657ee8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RCDMPUXO4Y7XEJNJJMNDFOFDC2/bundle.json","state_url":"https://pith.science/pith/RCDMPUXO4Y7XEJNJJMNDFOFDC2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RCDMPUXO4Y7XEJNJJMNDFOFDC2/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":"2026-05-27T23:20:00Z","links":{"resolver":"https://pith.science/pith/RCDMPUXO4Y7XEJNJJMNDFOFDC2","bundle":"https://pith.science/pith/RCDMPUXO4Y7XEJNJJMNDFOFDC2/bundle.json","state":"https://pith.science/pith/RCDMPUXO4Y7XEJNJJMNDFOFDC2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RCDMPUXO4Y7XEJNJJMNDFOFDC2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:RCDMPUXO4Y7XEJNJJMNDFOFDC2","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":"0c4cf3588c6e78c0825195edcfe1310bf32ac338713d139b6853bac9cd674812","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-12-15T16:01:16Z","title_canon_sha256":"9cffbd28eb2010af30d977035f757f675f4b5bbd7c2c7d58f741adf26a4f8efe"},"schema_version":"1.0","source":{"id":"1412.5017","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5017","created_at":"2026-05-18T02:31:09Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5017v1","created_at":"2026-05-18T02:31:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5017","created_at":"2026-05-18T02:31:09Z"},{"alias_kind":"pith_short_12","alias_value":"RCDMPUXO4Y7X","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RCDMPUXO4Y7XEJNJ","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RCDMPUXO","created_at":"2026-05-18T12:28:46Z"}],"graph_snapshots":[{"event_id":"sha256:5d1a8246103ba1d2fd4d4afdf6de04533c33529b402cb0575cad8e313e657ee8","target":"graph","created_at":"2026-05-18T02:31:09Z","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 routine transformation of a liquid, as it is cooled rapidly, resulting in glass formation, is remarkably complex. A theoretical explanation of the dynamics associated with this process has remained one of the major unsolved problems in condensed matter physics. The Random First Order Transition (RFOT) theory, which was proposed over twenty five years ago, provides a theoretical basis for explaining much of the phenomena associated with glass forming materials. It links or relates multiple metastable states, slow or glassy dynamics, dynamic heterogeneity, and both a dynamical and an ideal g","authors_text":"D. Thirumalai, T. R. Kirkpatrick","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-12-15T16:01:16Z","title":"Random First Order Theory concepts in Biology and Condensed Matter physics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5017","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":"sha256:54af94da6447e0280b3cf1d1f53eaaea7c2e27e0e076211be2060405333a1f85","target":"record","created_at":"2026-05-18T02:31:09Z","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":"0c4cf3588c6e78c0825195edcfe1310bf32ac338713d139b6853bac9cd674812","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-12-15T16:01:16Z","title_canon_sha256":"9cffbd28eb2010af30d977035f757f675f4b5bbd7c2c7d58f741adf26a4f8efe"},"schema_version":"1.0","source":{"id":"1412.5017","kind":"arxiv","version":1}},"canonical_sha256":"8886c7d2eee63f7225a94b1a32b8a3168559d7e2b7fcf799f24e8dd4526ff5e9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8886c7d2eee63f7225a94b1a32b8a3168559d7e2b7fcf799f24e8dd4526ff5e9","first_computed_at":"2026-05-18T02:31:09.833623Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:31:09.833623Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"eZgn01PiLc9Cr+DZIV3xd9Aq/wKbS5OmPAff1T50M1N/HU0vfPuUL7fhu2YC1SlN1yioDwiQj0GMNLtozJa9Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:31:09.834303Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.5017","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:54af94da6447e0280b3cf1d1f53eaaea7c2e27e0e076211be2060405333a1f85","sha256:5d1a8246103ba1d2fd4d4afdf6de04533c33529b402cb0575cad8e313e657ee8"],"state_sha256":"ab7be1a433b8078b60f28746b2440e8b47d5b723985ae885ddb9e9f5f83c1253"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bU2d0PiNNAHw3SQjOC7Lz0fsn4J4/oRKGFbkxfa9b9hygeQ8KSM3AsUxPBRqH708tk1qDclKm3fBHJP2eGSKBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T23:20:00.491286Z","bundle_sha256":"d4d036da32e492e0b66cbea20cb252467be673551cf58fc626b3766d9d996877"}}