{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:QNZ57VJCFT3RRDSDALQNFYPXXO","short_pith_number":"pith:QNZ57VJC","schema_version":"1.0","canonical_sha256":"8373dfd5222cf7188e4302e0d2e1f7bb896300bdba74c374a53545a10a82d34b","source":{"kind":"arxiv","id":"1010.3600","version":2},"attestation_state":"computed","paper":{"title":"Exploiting classical nucleation theory for reverse self-assembly","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Angelo Cacciuto, William L. Miller","submitted_at":"2010-10-18T14:00:38Z","abstract_excerpt":"In this paper we introduce a new method to design interparticle interactions to target arbitrary crystal structures via the process of self-assembly. We show that it is possible to exploit the curvature of the crystal nucleation free-energy barrier to sample and select optimal interparticle interactions for self-assembly into a desired structure. We apply this method to find interactions to target two simple crystal structures: a crystal with simple cubic symmetry and a two-dimensional plane with square symmetry embedded in a three-dimensional space. Finally, we discuss the potential and limit"},"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":"1010.3600","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-10-18T14:00:38Z","cross_cats_sorted":[],"title_canon_sha256":"8dfce3c3fc41afc63a422754727f1d92676764e02783d745a33785f5a3ef99f4","abstract_canon_sha256":"3962144b19fdf8e9f6eab69732c2ec2de39a696292ff3ceb24822eb01ecfc8c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:33:03.354066Z","signature_b64":"KYfj2USXS7l5wo8rpHIounHL6eI7UNPWDNky5icoQGRu5k5noqW7vpjj1jTxpRZX1ciyMBjqZi6OaxjSuwlyBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8373dfd5222cf7188e4302e0d2e1f7bb896300bdba74c374a53545a10a82d34b","last_reissued_at":"2026-05-18T04:33:03.353459Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:33:03.353459Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploiting classical nucleation theory for reverse self-assembly","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Angelo Cacciuto, William L. Miller","submitted_at":"2010-10-18T14:00:38Z","abstract_excerpt":"In this paper we introduce a new method to design interparticle interactions to target arbitrary crystal structures via the process of self-assembly. We show that it is possible to exploit the curvature of the crystal nucleation free-energy barrier to sample and select optimal interparticle interactions for self-assembly into a desired structure. We apply this method to find interactions to target two simple crystal structures: a crystal with simple cubic symmetry and a two-dimensional plane with square symmetry embedded in a three-dimensional space. Finally, we discuss the potential and limit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3600","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":"1010.3600","created_at":"2026-05-18T04:33:03.353553+00:00"},{"alias_kind":"arxiv_version","alias_value":"1010.3600v2","created_at":"2026-05-18T04:33:03.353553+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3600","created_at":"2026-05-18T04:33:03.353553+00:00"},{"alias_kind":"pith_short_12","alias_value":"QNZ57VJCFT3R","created_at":"2026-05-18T12:26:12.377268+00:00"},{"alias_kind":"pith_short_16","alias_value":"QNZ57VJCFT3RRDSD","created_at":"2026-05-18T12:26:12.377268+00:00"},{"alias_kind":"pith_short_8","alias_value":"QNZ57VJC","created_at":"2026-05-18T12:26:12.377268+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/QNZ57VJCFT3RRDSDALQNFYPXXO","json":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO.json","graph_json":"https://pith.science/api/pith-number/QNZ57VJCFT3RRDSDALQNFYPXXO/graph.json","events_json":"https://pith.science/api/pith-number/QNZ57VJCFT3RRDSDALQNFYPXXO/events.json","paper":"https://pith.science/paper/QNZ57VJC"},"agent_actions":{"view_html":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO","download_json":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO.json","view_paper":"https://pith.science/paper/QNZ57VJC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1010.3600&json=true","fetch_graph":"https://pith.science/api/pith-number/QNZ57VJCFT3RRDSDALQNFYPXXO/graph.json","fetch_events":"https://pith.science/api/pith-number/QNZ57VJCFT3RRDSDALQNFYPXXO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO/action/storage_attestation","attest_author":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO/action/author_attestation","sign_citation":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO/action/citation_signature","submit_replication":"https://pith.science/pith/QNZ57VJCFT3RRDSDALQNFYPXXO/action/replication_record"}},"created_at":"2026-05-18T04:33:03.353553+00:00","updated_at":"2026-05-18T04:33:03.353553+00:00"}