{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:NR6JGQ7FQPJ6UWRRYCISUBSZXL","short_pith_number":"pith:NR6JGQ7F","schema_version":"1.0","canonical_sha256":"6c7c9343e583d3ea5a31c0912a0659badf7bc98e5d63c08ac84c4d418dd13441","source":{"kind":"arxiv","id":"1401.2100","version":1},"attestation_state":"computed","paper":{"title":"Shear banding of colloidal glasses - a dynamic first order transition?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"B. Nienhuis, D. M. Miedema, P. Schall, V. Chikkadi","submitted_at":"2014-01-09T17:54:12Z","abstract_excerpt":"We demonstrate that application of an increasing shear field on a glass leads to an intriguing dynamic first order transition in analogy to equilibrium transitions. By following the particle dynamics as a function of the driving field in a colloidal glass, we identify a critical shear rate upon which the diffusion time scale of the glass exhibits a sudden discontinuity. Using a new dynamic order parameter, we show that this discontinuity is analogous to a first order transition, in which the applied stress acts as the conjugate field on the system's dynamic evolution. These results offer new p"},"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":"1401.2100","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-01-09T17:54:12Z","cross_cats_sorted":[],"title_canon_sha256":"be571eaa275837a78baa43b18701c78f0af6f2ba157b088f3f3d73768284051d","abstract_canon_sha256":"5161012360440561627a8655aef7645aed3d9a4a60324a416b45c5cceca9a5c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:27.018284Z","signature_b64":"PtjXjJ4YEkWRdAbD7d8ow/UMksvC6wXG25C80gV4Tc3DKzvnxe1ECWk1FqRsog5ByQk4QLyxCswyUB4co/80BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6c7c9343e583d3ea5a31c0912a0659badf7bc98e5d63c08ac84c4d418dd13441","last_reissued_at":"2026-05-18T01:45:27.017863Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:27.017863Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Shear banding of colloidal glasses - a dynamic first order transition?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"B. Nienhuis, D. M. Miedema, P. Schall, V. Chikkadi","submitted_at":"2014-01-09T17:54:12Z","abstract_excerpt":"We demonstrate that application of an increasing shear field on a glass leads to an intriguing dynamic first order transition in analogy to equilibrium transitions. By following the particle dynamics as a function of the driving field in a colloidal glass, we identify a critical shear rate upon which the diffusion time scale of the glass exhibits a sudden discontinuity. Using a new dynamic order parameter, we show that this discontinuity is analogous to a first order transition, in which the applied stress acts as the conjugate field on the system's dynamic evolution. These results offer new p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.2100","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1401.2100","created_at":"2026-05-18T01:45:27.017929+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.2100v1","created_at":"2026-05-18T01:45:27.017929+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.2100","created_at":"2026-05-18T01:45:27.017929+00:00"},{"alias_kind":"pith_short_12","alias_value":"NR6JGQ7FQPJ6","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_16","alias_value":"NR6JGQ7FQPJ6UWRR","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_8","alias_value":"NR6JGQ7F","created_at":"2026-05-18T12:28:41.024544+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/NR6JGQ7FQPJ6UWRRYCISUBSZXL","json":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL.json","graph_json":"https://pith.science/api/pith-number/NR6JGQ7FQPJ6UWRRYCISUBSZXL/graph.json","events_json":"https://pith.science/api/pith-number/NR6JGQ7FQPJ6UWRRYCISUBSZXL/events.json","paper":"https://pith.science/paper/NR6JGQ7F"},"agent_actions":{"view_html":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL","download_json":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL.json","view_paper":"https://pith.science/paper/NR6JGQ7F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.2100&json=true","fetch_graph":"https://pith.science/api/pith-number/NR6JGQ7FQPJ6UWRRYCISUBSZXL/graph.json","fetch_events":"https://pith.science/api/pith-number/NR6JGQ7FQPJ6UWRRYCISUBSZXL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL/action/storage_attestation","attest_author":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL/action/author_attestation","sign_citation":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL/action/citation_signature","submit_replication":"https://pith.science/pith/NR6JGQ7FQPJ6UWRRYCISUBSZXL/action/replication_record"}},"created_at":"2026-05-18T01:45:27.017929+00:00","updated_at":"2026-05-18T01:45:27.017929+00:00"}