{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:MEXFW3I6U5K6TN6AGUPOXUG36E","short_pith_number":"pith:MEXFW3I6","canonical_record":{"source":{"id":"1408.5485","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-08-23T10:35:49Z","cross_cats_sorted":[],"title_canon_sha256":"14d7cfb93b4850443efefdaf6b4468acb5413f3bf9261bf9adf5b3dc907a4280","abstract_canon_sha256":"24a2482e41a212114ee7f3f10168f2d6da8064d0ea5cc6d97316f442c727323e"},"schema_version":"1.0"},"canonical_sha256":"612e5b6d1ea755e9b7c0351eebd0dbf1232d21567fe06bcc44dba5acf9380bb7","source":{"kind":"arxiv","id":"1408.5485","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.5485","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"arxiv_version","alias_value":"1408.5485v1","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.5485","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"pith_short_12","alias_value":"MEXFW3I6U5K6","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MEXFW3I6U5K6TN6A","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MEXFW3I6","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:MEXFW3I6U5K6TN6AGUPOXUG36E","target":"record","payload":{"canonical_record":{"source":{"id":"1408.5485","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-08-23T10:35:49Z","cross_cats_sorted":[],"title_canon_sha256":"14d7cfb93b4850443efefdaf6b4468acb5413f3bf9261bf9adf5b3dc907a4280","abstract_canon_sha256":"24a2482e41a212114ee7f3f10168f2d6da8064d0ea5cc6d97316f442c727323e"},"schema_version":"1.0"},"canonical_sha256":"612e5b6d1ea755e9b7c0351eebd0dbf1232d21567fe06bcc44dba5acf9380bb7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:10.787724Z","signature_b64":"0RfuXglToocLsh1uZiPhkUhP0883S2wKwMwpgOkdmIZxO73R6RLIiZvwMFFmpWTCQB4zwJLL0wL4tT9OySk2Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"612e5b6d1ea755e9b7c0351eebd0dbf1232d21567fe06bcc44dba5acf9380bb7","last_reissued_at":"2026-05-18T02:04:10.786933Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:10.786933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1408.5485","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":"2026-05-18T02:04:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pvnPGwxzHFpfA1peePL/z3yEGf+Samiz2B5ddCVYa2b0H4BeXfkx843dQXxjCAvGI31/GKeoKGa7Gl5VJHv6CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T19:56:00.436501Z"},"content_sha256":"13ca217c2e91dd2f479f054935e07dbc962776b7c4c27c963455c2abe4ba8d6c","schema_version":"1.0","event_id":"sha256:13ca217c2e91dd2f479f054935e07dbc962776b7c4c27c963455c2abe4ba8d6c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:MEXFW3I6U5K6TN6AGUPOXUG36E","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Direct measurements of growing amorphous order and non-monotonic dynamic correlations in a colloidal glass-former","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"A. K. Sood, K. Hima Nagamanasa, Rajesh Ganapathy, Shreyas Gokhale","submitted_at":"2014-08-23T10:35:49Z","abstract_excerpt":"While the transformation of flowing liquids into rigid glasses is omnipresent, a complete understanding of vitrification remains elusive. Of the numerous approaches aimed at solving the glass transition problem, the Random First-Order Theory (RFOT) is the most prominent. However, the existence of the underlying thermodynamic phase transition envisioned by RFOT remains debatable, since its key microscopic predictions concerning the growth of amorphous order and the nature of dynamic correlations lack experimental verification. Here, by using holographic optical tweezers, we freeze a wall of par"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.5485","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":"2026-05-18T02:04:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CU4Mr0dKzaKnXp5biDVLV+ftU4IyrUNYbnKx79WT+ICpelWFt90oP7dkkUj97z1pbvOgDUNFv2qW5xCgMigMAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T19:56:00.437066Z"},"content_sha256":"79f0fb60f3f2cc8f4b82912de2f8c19674b8fe0e107815966f788947014b3688","schema_version":"1.0","event_id":"sha256:79f0fb60f3f2cc8f4b82912de2f8c19674b8fe0e107815966f788947014b3688"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MEXFW3I6U5K6TN6AGUPOXUG36E/bundle.json","state_url":"https://pith.science/pith/MEXFW3I6U5K6TN6AGUPOXUG36E/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MEXFW3I6U5K6TN6AGUPOXUG36E/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":"2026-06-04T19:56:00Z","links":{"resolver":"https://pith.science/pith/MEXFW3I6U5K6TN6AGUPOXUG36E","bundle":"https://pith.science/pith/MEXFW3I6U5K6TN6AGUPOXUG36E/bundle.json","state":"https://pith.science/pith/MEXFW3I6U5K6TN6AGUPOXUG36E/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MEXFW3I6U5K6TN6AGUPOXUG36E/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:MEXFW3I6U5K6TN6AGUPOXUG36E","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":"24a2482e41a212114ee7f3f10168f2d6da8064d0ea5cc6d97316f442c727323e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-08-23T10:35:49Z","title_canon_sha256":"14d7cfb93b4850443efefdaf6b4468acb5413f3bf9261bf9adf5b3dc907a4280"},"schema_version":"1.0","source":{"id":"1408.5485","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.5485","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"arxiv_version","alias_value":"1408.5485v1","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.5485","created_at":"2026-05-18T02:04:10Z"},{"alias_kind":"pith_short_12","alias_value":"MEXFW3I6U5K6","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MEXFW3I6U5K6TN6A","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MEXFW3I6","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:79f0fb60f3f2cc8f4b82912de2f8c19674b8fe0e107815966f788947014b3688","target":"graph","created_at":"2026-05-18T02:04:10Z","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":"While the transformation of flowing liquids into rigid glasses is omnipresent, a complete understanding of vitrification remains elusive. Of the numerous approaches aimed at solving the glass transition problem, the Random First-Order Theory (RFOT) is the most prominent. However, the existence of the underlying thermodynamic phase transition envisioned by RFOT remains debatable, since its key microscopic predictions concerning the growth of amorphous order and the nature of dynamic correlations lack experimental verification. Here, by using holographic optical tweezers, we freeze a wall of par","authors_text":"A. K. Sood, K. Hima Nagamanasa, Rajesh Ganapathy, Shreyas Gokhale","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-08-23T10:35:49Z","title":"Direct measurements of growing amorphous order and non-monotonic dynamic correlations in a colloidal glass-former"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.5485","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":"sha256:13ca217c2e91dd2f479f054935e07dbc962776b7c4c27c963455c2abe4ba8d6c","target":"record","created_at":"2026-05-18T02:04:10Z","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":"24a2482e41a212114ee7f3f10168f2d6da8064d0ea5cc6d97316f442c727323e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-08-23T10:35:49Z","title_canon_sha256":"14d7cfb93b4850443efefdaf6b4468acb5413f3bf9261bf9adf5b3dc907a4280"},"schema_version":"1.0","source":{"id":"1408.5485","kind":"arxiv","version":1}},"canonical_sha256":"612e5b6d1ea755e9b7c0351eebd0dbf1232d21567fe06bcc44dba5acf9380bb7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"612e5b6d1ea755e9b7c0351eebd0dbf1232d21567fe06bcc44dba5acf9380bb7","first_computed_at":"2026-05-18T02:04:10.786933Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:04:10.786933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0RfuXglToocLsh1uZiPhkUhP0883S2wKwMwpgOkdmIZxO73R6RLIiZvwMFFmpWTCQB4zwJLL0wL4tT9OySk2Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:04:10.787724Z","signed_message":"canonical_sha256_bytes"},"source_id":"1408.5485","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:13ca217c2e91dd2f479f054935e07dbc962776b7c4c27c963455c2abe4ba8d6c","sha256:79f0fb60f3f2cc8f4b82912de2f8c19674b8fe0e107815966f788947014b3688"],"state_sha256":"50b6b1a63e90a194b949fdef5f358111fd500b3b61fa14b89381cc7d64a9c93e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"f343WnR7utJEATD1iSIUuy8z3kgQ6f0/fyLFxQ/BxwUWBOt3n+blprT9FX/y/3406ndEUs25JLnM7+btIHkjCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T19:56:00.438965Z","bundle_sha256":"599d50aa30da6c4ea115865daef8da34f66ae8deb82b41307e9836b861ad3043"}}