{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:BCV7HNSHV2OQ6VYZDNK55YJOVC","short_pith_number":"pith:BCV7HNSH","schema_version":"1.0","canonical_sha256":"08abf3b647ae9d0f57191b55dee12ea89a219ad1f4d4e35ca8687d53667f474a","source":{"kind":"arxiv","id":"1609.00327","version":2},"attestation_state":"computed","paper":{"title":"Experimental Evidence for a Structural-Dynamical Transition in Trajectory Space","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"C. Patrick Royall, Francesco Turci, James Hallett, Matteo Campo, Rattachai Pinchaipat, Thomas Speck","submitted_at":"2016-09-01T17:56:54Z","abstract_excerpt":"Among the key insights into the glass transition has been the identification of a non-equilibrium phase transition in trajectory space which reveals phase coexistence between the normal supercooled liquid (active phase) and a glassy state (inactive phase). Here we present evidence that such a transition occurs in experiment. In colloidal hard spheres we find a non-Gaussian distribution of trajectories leaning towards those rich in locally favoured structures (LFS), associated with the emergence of slow dynamics. This we interpret as evidence for an non-equilibrium transition to an inactive LFS"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1609.00327","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2016-09-01T17:56:54Z","cross_cats_sorted":[],"title_canon_sha256":"0670ebf747927eec6baed64b7aa83449548efbbffaea830e1f4f2ab001c27e7a","abstract_canon_sha256":"e60cf29ba4f03f6033268ebe9a0257c3f80a2775df66f203ae9d1a5d01a802e5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:08.076417Z","signature_b64":"+QNMX9uR1eFtqqHRZOJKIc425r5iDjXE4dAuMsSFSeNyQHeNW4cWI4xrErl+QyA9hzG0HqEJ+pDZYEYRn7EaBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08abf3b647ae9d0f57191b55dee12ea89a219ad1f4d4e35ca8687d53667f474a","last_reissued_at":"2026-05-18T00:40:08.075704Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:08.075704Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Experimental Evidence for a Structural-Dynamical Transition in Trajectory Space","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"C. Patrick Royall, Francesco Turci, James Hallett, Matteo Campo, Rattachai Pinchaipat, Thomas Speck","submitted_at":"2016-09-01T17:56:54Z","abstract_excerpt":"Among the key insights into the glass transition has been the identification of a non-equilibrium phase transition in trajectory space which reveals phase coexistence between the normal supercooled liquid (active phase) and a glassy state (inactive phase). Here we present evidence that such a transition occurs in experiment. In colloidal hard spheres we find a non-Gaussian distribution of trajectories leaning towards those rich in locally favoured structures (LFS), associated with the emergence of slow dynamics. This we interpret as evidence for an non-equilibrium transition to an inactive LFS"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.00327","kind":"arxiv","version":2},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1609.00327","created_at":"2026-05-18T00:40:08.075799+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.00327v2","created_at":"2026-05-18T00:40:08.075799+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.00327","created_at":"2026-05-18T00:40:08.075799+00:00"},{"alias_kind":"pith_short_12","alias_value":"BCV7HNSHV2OQ","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_16","alias_value":"BCV7HNSHV2OQ6VYZ","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_8","alias_value":"BCV7HNSH","created_at":"2026-05-18T12:30:07.202191+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC","json":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC.json","graph_json":"https://pith.science/api/pith-number/BCV7HNSHV2OQ6VYZDNK55YJOVC/graph.json","events_json":"https://pith.science/api/pith-number/BCV7HNSHV2OQ6VYZDNK55YJOVC/events.json","paper":"https://pith.science/paper/BCV7HNSH"},"agent_actions":{"view_html":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC","download_json":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC.json","view_paper":"https://pith.science/paper/BCV7HNSH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.00327&json=true","fetch_graph":"https://pith.science/api/pith-number/BCV7HNSHV2OQ6VYZDNK55YJOVC/graph.json","fetch_events":"https://pith.science/api/pith-number/BCV7HNSHV2OQ6VYZDNK55YJOVC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC/action/storage_attestation","attest_author":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC/action/author_attestation","sign_citation":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC/action/citation_signature","submit_replication":"https://pith.science/pith/BCV7HNSHV2OQ6VYZDNK55YJOVC/action/replication_record"}},"created_at":"2026-05-18T00:40:08.075799+00:00","updated_at":"2026-05-18T00:40:08.075799+00:00"}