{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:LR4VFCIVNXDJE2B7EB3QSJJTFS","short_pith_number":"pith:LR4VFCIV","schema_version":"1.0","canonical_sha256":"5c795289156dc692683f20770925332c85d75ac55ebfc0a298b719a577732e77","source":{"kind":"arxiv","id":"1507.04926","version":2},"attestation_state":"computed","paper":{"title":"Order-disorder transitions in a sheared many body system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.CD","physics.flu-dyn"],"primary_cat":"cond-mat.soft","authors_text":"Bruno Eckhardt, Georg Ehlers, Jens C. Pfeifer, Tobias Bischoff","submitted_at":"2015-07-17T11:18:10Z","abstract_excerpt":"Motivated by experiments on sheared suspensions that show a transition between ordered and disordered phases, we here study the long-time behavior of a sheared and overdamped 2-d system of particles interacting by repulsive forces. As a function of interaction strength and shear rate we find transitions between phases with vanishing and large single-particle diffusion. In the phases with vanishing single-particle diffusion, the system evolves towards regular lattices, usually on very slow time scales. Different lattices can be approached, depending on interaction strength and forcing amplitude"},"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":"1507.04926","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-07-17T11:18:10Z","cross_cats_sorted":["nlin.CD","physics.flu-dyn"],"title_canon_sha256":"741354f49f683d79d612ea5bf53a6c8d1010888ca27eb11277ac2e6d8118ec81","abstract_canon_sha256":"9b347e213a51cde7a278f08f432b3f5fa7d02cc4927857644b23b03a1f263276"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:23:23.825835Z","signature_b64":"ABgzcjH18qZODS1b3VwUnSOl1dnUGeuFsS4CaxH2SQ+2v7FYFlvF0KRpYCymd9uiGimDB6iC+quI1w/knEarAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c795289156dc692683f20770925332c85d75ac55ebfc0a298b719a577732e77","last_reissued_at":"2026-05-18T01:23:23.825155Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:23:23.825155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Order-disorder transitions in a sheared many body system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.CD","physics.flu-dyn"],"primary_cat":"cond-mat.soft","authors_text":"Bruno Eckhardt, Georg Ehlers, Jens C. Pfeifer, Tobias Bischoff","submitted_at":"2015-07-17T11:18:10Z","abstract_excerpt":"Motivated by experiments on sheared suspensions that show a transition between ordered and disordered phases, we here study the long-time behavior of a sheared and overdamped 2-d system of particles interacting by repulsive forces. As a function of interaction strength and shear rate we find transitions between phases with vanishing and large single-particle diffusion. In the phases with vanishing single-particle diffusion, the system evolves towards regular lattices, usually on very slow time scales. Different lattices can be approached, depending on interaction strength and forcing amplitude"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.04926","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":"1507.04926","created_at":"2026-05-18T01:23:23.825253+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.04926v2","created_at":"2026-05-18T01:23:23.825253+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.04926","created_at":"2026-05-18T01:23:23.825253+00:00"},{"alias_kind":"pith_short_12","alias_value":"LR4VFCIVNXDJ","created_at":"2026-05-18T12:29:29.992203+00:00"},{"alias_kind":"pith_short_16","alias_value":"LR4VFCIVNXDJE2B7","created_at":"2026-05-18T12:29:29.992203+00:00"},{"alias_kind":"pith_short_8","alias_value":"LR4VFCIV","created_at":"2026-05-18T12:29:29.992203+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/LR4VFCIVNXDJE2B7EB3QSJJTFS","json":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS.json","graph_json":"https://pith.science/api/pith-number/LR4VFCIVNXDJE2B7EB3QSJJTFS/graph.json","events_json":"https://pith.science/api/pith-number/LR4VFCIVNXDJE2B7EB3QSJJTFS/events.json","paper":"https://pith.science/paper/LR4VFCIV"},"agent_actions":{"view_html":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS","download_json":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS.json","view_paper":"https://pith.science/paper/LR4VFCIV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.04926&json=true","fetch_graph":"https://pith.science/api/pith-number/LR4VFCIVNXDJE2B7EB3QSJJTFS/graph.json","fetch_events":"https://pith.science/api/pith-number/LR4VFCIVNXDJE2B7EB3QSJJTFS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS/action/storage_attestation","attest_author":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS/action/author_attestation","sign_citation":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS/action/citation_signature","submit_replication":"https://pith.science/pith/LR4VFCIVNXDJE2B7EB3QSJJTFS/action/replication_record"}},"created_at":"2026-05-18T01:23:23.825253+00:00","updated_at":"2026-05-18T01:23:23.825253+00:00"}