{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:BDS67254RSEK3M54PTBKKQFZ72","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":"a8f66fb064567a7344f0aaad6d5d5c73278b5a98b01d545c87ac293c32216d98","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-12-04T11:54:09Z","title_canon_sha256":"bbd41242b57332a5b1a67f95c89716a7bad0fb6f8d480d4c73c2b1561fab0664"},"schema_version":"1.0","source":{"id":"1712.01025","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.01025","created_at":"2026-05-18T00:23:58Z"},{"alias_kind":"arxiv_version","alias_value":"1712.01025v1","created_at":"2026-05-18T00:23:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.01025","created_at":"2026-05-18T00:23:58Z"},{"alias_kind":"pith_short_12","alias_value":"BDS67254RSEK","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"BDS67254RSEK3M54","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"BDS67254","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:5cbab9765ea1300e36cbfd9d5d2f84ad5b99cfe932e0c486b3e3bee902bb8ca7","target":"graph","created_at":"2026-05-18T00:23:58Z","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 interplay between shape anisotropy and directed long-range interactions enables the self-assembly of complex colloidal structures. As a recent highlight, ellipsoidal particles polarized in an external electric field were observed to associate into well-defined tubular structures. In this study, we investigate systematically such directed self-assembly using Monte Carlo simulations of a two-point-charge model of polarizable prolate ellipsoids. In spite of its simplicity and computational efficiency, we demonstrate that the model is capable of capturing the complex structures observed in exp","authors_text":"Adriana M. Mihut, Arash Azari, Erik Bialik, J\\'er\\^ome J. Crassous, Joakim Stenhammar, Per Linse, Peter Schurtenberger","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-12-04T11:54:09Z","title":"Directed Self-Assembly of Polarizable Ellipsoids in an External Electric Field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.01025","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":"sha256:976eae1ca0b8e40af56837090eeee4be5afea6a538c1787d48456fe919e7ec0d","target":"record","created_at":"2026-05-18T00:23:58Z","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":"a8f66fb064567a7344f0aaad6d5d5c73278b5a98b01d545c87ac293c32216d98","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-12-04T11:54:09Z","title_canon_sha256":"bbd41242b57332a5b1a67f95c89716a7bad0fb6f8d480d4c73c2b1561fab0664"},"schema_version":"1.0","source":{"id":"1712.01025","kind":"arxiv","version":1}},"canonical_sha256":"08e5efebbc8c88adb3bc7cc2a540b9fe91715a96adc12f811f975179593555c7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"08e5efebbc8c88adb3bc7cc2a540b9fe91715a96adc12f811f975179593555c7","first_computed_at":"2026-05-18T00:23:58.722684Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:23:58.722684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bODlsXd4shOGOGhIRXSdU38w9sYYIIDhXjb6qlwWx88/nhksMDhfX4fOAhQqsgQexDd6mWWonhngJBVYCpk8DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:23:58.723091Z","signed_message":"canonical_sha256_bytes"},"source_id":"1712.01025","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:976eae1ca0b8e40af56837090eeee4be5afea6a538c1787d48456fe919e7ec0d","sha256:5cbab9765ea1300e36cbfd9d5d2f84ad5b99cfe932e0c486b3e3bee902bb8ca7"],"state_sha256":"9b2fbd212d0b4c8f0e59003b669e605b9a7de7dc09d22d70e814e0c9f529f954"}