{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ZLO6O6H4SCRJXXCBCTSRPFSS4V","short_pith_number":"pith:ZLO6O6H4","schema_version":"1.0","canonical_sha256":"cadde778fc90a29bdc4114e5179652e55f8032e5ec8bc3c2d346def8aba2751b","source":{"kind":"arxiv","id":"1708.06212","version":1},"attestation_state":"computed","paper":{"title":"Phase and vacancy behaviour of hard \"slanted\" cubes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Berend van der Meer, Frank Smallenburg, Jette Janine van den Broeke, Laura Filion, Robin van Damme","submitted_at":"2017-08-21T13:34:33Z","abstract_excerpt":"We use computer simulations to study the phase behaviour for hard, right rhombic prisms as a function of the angle of their rhombic face (the \"slant\" angle). More specifically, using a combination of event-driven molecular dynamics simulations, Monte Carlo simulations, and free-energy calculations, we determine and characterize the equilibrium phases formed by these particles for various slant angles and densities. Surprisingly, we find that the equilibrium crystal structure for a large range of slant angles and densities is the simple cubic crystal - despite the fact that the particles do not"},"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":"1708.06212","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-08-21T13:34:33Z","cross_cats_sorted":[],"title_canon_sha256":"e225fc598e315431977f0b429a47ca1ed3085055a8af65b65a54f19f94945952","abstract_canon_sha256":"bfa12e3751d2354ceb874f03145334a594b39f67aa7d438a5f8fb8bb4bf30d91"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:15.730954Z","signature_b64":"VpFWwKIq98WLIubf9lfSp0wn6+3Q847n1OcWVKzqwPeKjFuQg0YoFuh5Ke3d2C3c2odhjOHRz9CcYRukXVGSDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cadde778fc90a29bdc4114e5179652e55f8032e5ec8bc3c2d346def8aba2751b","last_reissued_at":"2026-05-18T00:33:15.730363Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:15.730363Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase and vacancy behaviour of hard \"slanted\" cubes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Berend van der Meer, Frank Smallenburg, Jette Janine van den Broeke, Laura Filion, Robin van Damme","submitted_at":"2017-08-21T13:34:33Z","abstract_excerpt":"We use computer simulations to study the phase behaviour for hard, right rhombic prisms as a function of the angle of their rhombic face (the \"slant\" angle). More specifically, using a combination of event-driven molecular dynamics simulations, Monte Carlo simulations, and free-energy calculations, we determine and characterize the equilibrium phases formed by these particles for various slant angles and densities. Surprisingly, we find that the equilibrium crystal structure for a large range of slant angles and densities is the simple cubic crystal - despite the fact that the particles do not"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.06212","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":"1708.06212","created_at":"2026-05-18T00:33:15.730446+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.06212v1","created_at":"2026-05-18T00:33:15.730446+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.06212","created_at":"2026-05-18T00:33:15.730446+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZLO6O6H4SCRJ","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZLO6O6H4SCRJXXCB","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZLO6O6H4","created_at":"2026-05-18T12:31:59.375834+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/ZLO6O6H4SCRJXXCBCTSRPFSS4V","json":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V.json","graph_json":"https://pith.science/api/pith-number/ZLO6O6H4SCRJXXCBCTSRPFSS4V/graph.json","events_json":"https://pith.science/api/pith-number/ZLO6O6H4SCRJXXCBCTSRPFSS4V/events.json","paper":"https://pith.science/paper/ZLO6O6H4"},"agent_actions":{"view_html":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V","download_json":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V.json","view_paper":"https://pith.science/paper/ZLO6O6H4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.06212&json=true","fetch_graph":"https://pith.science/api/pith-number/ZLO6O6H4SCRJXXCBCTSRPFSS4V/graph.json","fetch_events":"https://pith.science/api/pith-number/ZLO6O6H4SCRJXXCBCTSRPFSS4V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V/action/storage_attestation","attest_author":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V/action/author_attestation","sign_citation":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V/action/citation_signature","submit_replication":"https://pith.science/pith/ZLO6O6H4SCRJXXCBCTSRPFSS4V/action/replication_record"}},"created_at":"2026-05-18T00:33:15.730446+00:00","updated_at":"2026-05-18T00:33:15.730446+00:00"}